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Author name code: yurchyshyn
ADS astronomy entries on 2022-09-14
author:Yurchyshyn, V. B.

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Title: Solar Chromospheric Network as a Source for Solar Wind
    Switchbacks
Authors: Lee, Jeongwoo; Yurchyshyn, Vasyl; Wang, Haimin; Yang, Xu;
   Cao, Wenda; Carlos Martínez Oliveros, Juan
2022ApJ...935L..27L    Altcode:
  Recent studies suggest that the magnetic switchbacks (SBs) detected
  by the Parker Solar Probe carry information on the scales of solar
  supergranulation (large scale) and granulation (medium scale). We test
  this claim using high-resolution Hα images obtained with the visible
  spectropolarimeters of the Goode Solar Telescope in Big Bear Solar
  Observatory. As possible solar sources, we count all the spicule-like
  features standing along the chromospheric networks near the coronal
  hole boundary visible in the Hα blue-wing but absent in the red-wing
  images and measure the geometric parameters of dense sections of
  individual flux tubes. Intervals between adjacent spicules located
  along the chromospheric networks are found in the range of 0.4-1.5
  Mm (0.°03-0.°12) tending to be smaller than the medium scale of
  SBs. Interdistances between all pairs of the flux tubes are also counted
  and they appear in a single peak distribution around 0.7 Mm (0.°06)
  unlike the waiting-time distribution of SBs in a scale-free single
  power-law form. The length-to-diameter ratio of the dense section
  of flux tubes is as high as 6-40, similar to the aspect ratio of
  SBs. The number of spicules along a network can be as high as 40-100,
  consistent with numerous SBs within a patch. With these numbers, it is
  argued that the medium scale of SBs can be understood as an equilibrium
  distance resulting from a random walk within each diverging magnetic
  field funnel connected to the chromospheric networks.

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Title: Erratum: "A Study of Sunspot 3 Minute Oscillations Using ALMA
    and GST" (2022, ApJ, 924, 100)
Authors: Chai, Yi; Gary, Dale E.; Reardon, Kevin P.; Yurchyshyn, Vasyl
2022ApJ...933..247C    Altcode:
  No abstract at ADS

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Title: Triggering Mechanism for Eruption of Two Filaments Observed by
    the Solar Dynamics Observatory, Nobeyama Radioheliograph, and RHESSI
Authors: Kim, Sujin; Yurchyshyn, Vasyl
2022ApJ...932L..18K    Altcode:
  We investigate the eruptive process of two filaments, which is
  associated with an M-class flare that occurred in 2011 August 4. The
  filaments are partly overlapped, one in the active region and the
  other just beside it, and erupt together as a halo coronal mass
  ejection. For this study, we used the Atmospheric Imaging Assembly
  and the Heliospheric Magnetic Imager on board the Solar Dynamics
  Observatory, the Nobeyama Radioheliograph 17 GHz, and the RHESSI Hard
  X-ray satellite. We found three distinct phases in the microwave flux
  profile and in the rising pattern of the filaments during the event. In
  the first phase, there was weak nonthermal emission at 17 GHz and hard
  X-rays. Those nonthermal sources appeared on one edge of the western
  filament (F2) in the active region. The F2 began to be bright and rose
  upward rapidly, while the eastern filament (F1), which was extended to
  the quiet region, started to brighten from the peak time of the 17 GHz
  flux. In the second phase, the nonthermal emission weakened and the
  F2 rose up slowly, while the F1 began to rise up. In the third phase,
  two filaments erupted together. Since the F1 was stable for a long time
  in the quiet region, breaking the equilibrium state of the F1 would be
  decisive for the successful eruption of two filaments and it seems clear
  that the evolution of the F2 provoked the unstable F1. We suggest that
  tether-cutting reconnection between two overlapped filaments triggers
  the eruption of the two filaments as a tangled identity.

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Title: Magnetic Field Re-configuration Associated With a Slow Rise
    Eruptive X1.2 Flare in NOAA Active Region 11944
Authors: Yurchyshyn, Vasyl; Yang, Xu; Nita, Gelu; Fleishman, Gregory;
   Abramenko, Valentina; Inoue, Satoshi; Lim, Eun-Kyung; Cao, Wenda
2022FrASS...916523Y    Altcode:
  Using multi-wavelength observations, we analysed magnetic field
  variations associated with a gradual X1.2 flare that erupted on
  January 7, 2014 in active region (AR) NOAA 11944 located near the disk
  center. A fast coronal mass ejection (CME) was observed following the
  flare, which was noticeably deflected in the south-west direction. A
  chromospheric filament was observed at the eruption site prior to and
  after the flare. We used SDO/HMI data to perform non-linear force-free
  field extrapolation of coronal magnetic fields above the AR and to
  study the evolution of AR magnetic fields prior to the eruption. The
  extrapolated data allowed us to detect signatures of several magnetic
  flux ropes present at the eruption site several hours before the
  event. The eruption site was located under slanted sunspot fields
  with a varying decay index of 1.0-1.5. That might have caused the
  erupting fields to slide along this slanted magnetic boundary rather
  than vertically erupt, thus explaining the slow rise of the flare
  as well as the observed direction of the resulting CME. We employed
  sign-singularity tools to quantify the evolutionary changes in the
  model twist and observed current helicity data, and found rapid and
  coordinated variations of current systems in both data sets prior to
  the event as well as their rapid exhaustion after the event onset.

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Title: Observations of Extremely Strong Magnetic Fields in Active
    Region NOAA 12673 Using GST Magnetic Field Measurement
Authors: Lozitsky, Vsevolod; Yurchyshyn, Vasyl; Ahn, Kwangsu; Wang,
   Haimin
2022ApJ...928...41L    Altcode:
  We present a detailed study of very strong magnetic fields in the
  NOAA Active Region (AR) 12673, which was the most flare productive
  AR in solar cycle 24. It produced four X-class flares including the
  X9.3 flare on 2017 September 6 and the X8.2 limb event on September
  10. Our analysis is based on direct measurements of full Zeeman
  splitting of the Fe I 1564.85 nm line using all Stokes I, Q, U, and
  V profiles. This approach allowed us to obtain reliable estimates
  of the magnitude of magnetic fields independent of the filling
  factor and atmosphere models. Thus, the strongest fields up to 5.5
  kG were found in a light bridge (LB) of a spot, while in the dark
  umbra magnetic fields did not exceed 4 kG. In the case of the LB,
  the magnitude of the magnetic field is not related to the underlying
  continuum intensity, while in the case of umbral fields we observed
  a well-known anticorrelation between the continuum intensity and the
  field magnitude. In this study, the LB was cospatial with a polarity
  inversion line of δ-sunspot, and we speculate that the 5.5 kG strong
  horizontal fields may be associated with a compact twisted flux rope
  at or near the photosphere. A comparison of the depth of the Zeeman
  π and σ components showed that in the LB magnetic fields are, on
  average, more horizontal than those in the dark umbra.

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Title: A Study of Sunspot 3 Minute Oscillations Using ALMA and GST
Authors: Chai, Yi; Gary, Dale E.; Reardon, Kevin P.; Yurchyshyn, Vasyl
2022ApJ...924..100C    Altcode: 2021arXiv211105812C
  Waves and oscillations are important solar phenomena, not only because
  they can propagate and dissipate energy in the chromosphere, but also
  because they carry information about the structure of the atmosphere
  in which they propagate. The nature of the 3 minute oscillations
  observed in the umbral region of sunspots is considered to be an
  effect of propagation of magnetohydrodynamic waves upward from below
  the photosphere. We present a study of sunspot oscillations and wave
  propagation in NOAA Active Region 12470 using an approximately 1
  hr long data set acquired on 2015 December 17 by the Atacama Large
  Millimeter/submillimeter Array (ALMA), the Goode Solar Telescope
  (GST) operating at the Big Bear Solar Observatory, the Atmospheric
  Imaging Assembly on board the Solar Dynamics Observatory, and the
  Interface Region Imaging Spectrograph. The ALMA data are unique in
  providing a time series of direct temperature measurements in the
  sunspot chromosphere. The 2 s cadence of ALMA images allows us to well
  resolve the 3 minute periods typical of sunspot oscillations in the
  chromosphere. Fourier analysis is applied to ALMA Band 3 (~100 GHz, ~3
  mm) and GST Hα data sets to obtain power spectra as well as oscillation
  phase information. We analyzed properties of the wave propagation by
  combining multiple wavelengths that probe physical parameters of solar
  atmosphere at different heights. We find that the ALMA temperature
  fluctuations are consistent with that expected for a propagating
  acoustic wave, with a slight asymmetry indicating nonlinear steepening.

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Title: Solar Chromospheric Ejections and Solar Wind Switchbacks
Authors: Lee, Jeongwoo; Yang, Xu; Yurchyshyn, Vasyl; Wang, Haimin
2021AGUFMSH33B..01L    Altcode:
  Small-scale jet-like ejections in the solar atmosphere are of renewed
  interest to NASA's Parker Solar Probe (PSP) mission, because they may
  develop into the mysterious solar wind structure of plasma and magnetic
  field called switchbacks detected by the PSP. We investigate high
  resolution H-alpha images and magnetograms obtained with the visible
  (VIS) and near-infrared (NIRIS) spectro-polarimeters of the Goode
  Solar Telescope (GST) in Big Bear Solar Observatory (BBSO) to explore
  solar origin for the switchbacks. In this effort, we measure spatial
  dimensions, orientation, eruption speed of tiny magnetic arcades,
  mini-filaments, and plumelets for comparison with the properties of
  the switchbacks established from the PSP observations. The spatial
  dimensions of these objects range from tens of arcsecond down to sub
  arcsecond (200 km), small enough to produce short duration switchbacks
  in the PSP locations. However, the orientation combined with the
  speed can be tested against the surprisingly high aspect ratio of
  the switchbacks, thus providing a strong constraint on the possible
  candidates. Other properties of the switchbacks such as clustering and
  one-sidedness make this search a narrower choice. We argue that the most
  ideal solar candidate should be the tiny upright flux tubes that can
  develop into an S-shape after ejection, and that the KelvinHelmholtz
  instability arising from the density inhomogeneity along the flux
  tube could be a plausible mechanism for transforming the chromospheric
  structure into the solar wind switchbacks.

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Title: Exploring Nature Of Type II Spicules With GST Data
Authors: Yurchyshyn, V.
2021AAS...23820504Y    Altcode:
  Large- and small-scale jets and upflows observed in the lower
  atmosphere of the quiet Sun (QS) are thought to play an important
  role in the transfer of mass and energy from the dense chromosphere
  into the corona. However, their origin and connection to dynamic
  magnetic fields are not yet well understood and explored. Type II
  spicules are a subset of these small-scale phenomena discovered in
  off-limb Hinode data. Although their formation may affect the corona
  by generating shocks, flows, waves, and electric currents, their
  detailed physical cause and role in providing mass and energy to the
  corona remain largely unknown. Here we will present recent progress
  in studying type II spicules facilitated by data from the Goode Solar
  Telescope. Various data sets and approaches to analysis all seem to
  indicate that these events result from magnetic reconnection driven by
  rapidly varying small-scale magnetic fields present in highly turbulent
  solar photosphere. In particular, we observe very rapid morphological
  changes on timescales of the order of 1 s. They very frequently appear
  in situ without any clear evidence of H-alpha material being injected
  from below. Their evolution includes various splitting patterns as well
  as sudden formation of a diffuse region followed by branching. These
  observations suggest that faint and numerous type II spicules may
  be formed as a result of component reconnection within a bundle of
  unipolar large scale fields.

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Title: Magnetic Field Configuration Associated With A Slow Rise
    Eruptive X1.2 Flare In Active Region 11944
Authors: Yang, X.; Yurchyshyn, V.; Nita, G.; Abramenko, V.; Lim, E.;
   Cao, W.
2021AAS...23812707Y    Altcode:
  Using multi-wavelength observations, we studied a gradual X1.2 flare
  that erupted on January 7, 2014, in active region (AR) NOAA 11944
  located near the disk center. A fast coronal mass ejection (CME) was
  observed following the flare; however, it was strongly deflected in the
  south-west direction. We used SDO/HMI data to perform extrapolation of
  coronal magnetic fields and to study the evolution of AR magnetic fields
  before the eruption. Extrapolated data allowed us to detect a flux rope
  (FR) present at the eruption site several hours before the event. That
  was the only well-defined FR present in the AR. Although the strapping
  and core fields in the model have significantly changed after the flare,
  the model FR did not erupt. We note that a chromospheric filament
  was observed at the eruption site prior to and after the flare. The
  eruption site was located under sunspot canopy fields with a decay
  index of about 0.5, which is not favorable for torus instability to
  develop. That might have caused the erupting fields to slide along the
  canopy rather than vertically erupt, thus explaining the slow rise of
  the flare as well as the observed direction of the resulting CME. We
  employed sign-singularity tools to quantify the evolutionary changes
  in a model twist and observed current helicity data, and found rapid
  enhancements in the current systems in both data sets prior to the
  event as well as their rapid exhaustion after the event onset.

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Title: Detection of Opposite Magnetic Polarity in a Light Bridge:
    Its Emergence and Cancellation in Association with LB Fan-shaped Jets
Authors: Lim, Eun-Kyung; Yang, Heesu; Yurchyshyn, Vasyl; Chae,
   Jongchul; Song, Donguk; Madjarska, Maria S.
2020ApJ...904...84L    Altcode: 2020arXiv201010713L
  Light bridges (LBs) are relatively bright structures that divide
  sunspot umbrae into two or more parts. Chromospheric LBs are known to
  be associated with various activities including fan-shaped jet-like
  ejections and brightenings. Although magnetic reconnection is
  frequently suggested to be responsible for such activities, not many
  studies present firm evidence to support the scenario. We carry out
  magnetic field measurements and imaging spectroscopy of an LB where
  fan-shaped jet-like ejections occur with co-spatial brightenings
  at their footpoints. We study LB fine structure and magnetic field
  changes using TiO images, Near-InfraRed Imaging Spectropolarimeter,
  and Hα data taken by the 1.6 m Goode Solar Telescope. We detect
  magnetic flux emergence in the LB that is of opposite polarity to that
  of the sunspot. The new magnetic flux cancels with the pre-existing
  flux at a rate of 5.6 × 10<SUP>18</SUP> Mx hr<SUP>-1</SUP>. Both
  the recurrent jet-like ejections and their base brightenings are
  initiated at the vicinity of the magnetic flux cancellation, and show
  apparent horizontal extension along the LB at a projected speed of up
  to $18.4$ km s<SUP>-1</SUP> to form a fan-shaped appearance. Based on
  these observations, we suggest that the fan-shaped ejections may have
  resulted from slipping reconnection between the new flux emerging in
  the LB and the ambient sunspot field.

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Title: Accelerating and Supersonic Density Disturbances in Solar
    Polar Plumes
Authors: Cho, I. H.; Moon, Y. J.; Nakariakov, V. M.; Lee, J. Y.; Yu,
   D. J.; Cho, K. S. F.; Yurchyshyn, V.; Lee, H.
2020AGUFMSH0290003C    Altcode:
  Propagating intensity disturbances in solar coronal holes are often
  considered as wave propagations or mass flows. By applying the
  differential emission measure technique for the extreme ultraviolet
  images taken by the Atmospheric Imaging Assembly on board the Solar
  Dynamics Observatory, we analyze the propagation speed of density
  disturbances of plume structure in an off-limb coronal hole for a
  given temperature. We construct the map of cross-correlation between
  density profile for a given height and the profile at the height
  of 50 Mm. The evolution of density disturbances is well fitted by
  the second-order polynomial. The acceleration is calculated to be
  36 m s<SUP>-2</SUP>. The initial speed is 134 km s<SUP>-1</SUP>
  which is comparable with the sound speed given by the DEM-weighted
  temperature. Hence, density disturbances are accelerating and supersonic
  at around the base of the solar corona. The excess speed relative
  to the sound speed is ∼ 30 km s<SUP>-1</SUP> at the height of 1.23
  solar radii, which is consistent with the Doppler speeds and Doppler
  dimming speeds observed by different instruments. The extrapolated
  sonic distance of the excess speed is ∼ 2.16 solar radii which is
  consistent with those of solar winds. The lower limit of the mass
  flux corresponds to 7% of the global solar wind. Hence, we interpret
  that the observed density disturbances are slow magnetoacoustic waves
  propagating in subsonic and accelerating solar winds.

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Title: Temporal and Periodic Variation of the MCMESI for the Last
    Two Solar Cycles; Comparison with the Number of Different Class
    X-ray Solar Flares
Authors: Kilcik, Ali; Chowdhury, Partha; Sarp, Volkan; Yurchyshyn,
   Vasyl; Donmez, Burcin; Rozelot, Jean-Pierre; Ozguc, Atila
2020SoPh..295..159K    Altcode: 2020arXiv200811506K
  In this study we compared the temporal and periodic variations of
  the Maximum CME Speed Index (MCMESI) and the the number of different
  class (C, M, and X) solar X-ray flares for the last two solar cycles
  (Solar Cycles 23 and 24). To obtain the correlation between the MCMESI
  and solar flare numbers the cross-correlation analysis was applied to
  monthly data sets. Also to investigate the periodic behavior of all
  data sets the Multi Taper Method (MTM) and the Morlet wavelet analysis
  method were performed with daily data from 2009 to 2018. To evaluate our
  wavelet analysis Cross Wavelet Transform (XWT) and Wavelet Transform
  Coherence (WTC) methods were performed. Causal relationship between
  data sets were further examined by Convergence Cross Mapping (CCM)
  method. As results of our analysis we found the following: i) The C
  class X-ray flare numbers increased about 16% during the Solar Cycle 24
  compared to Cycle 23, while all other data sets decreased; the MCMESI
  decreased about 16% and the number of M and X class flares decreased
  about 32%. ii) All the X-ray solar flare classes show remarkable
  positive correlation with the MCMESI. While the correlation between the
  MCMESI and C class flares comes from the general solar cycle trend,
  it mainly results from the fluctuations in the data in case of the X
  class flares. iii) In general, all class flare numbers and the MCMESI
  show similar periodic behavior. iv) The 546-day periodicity detected
  in the MCMESI may not be of solar origin or at least the solar flares
  are not the source of this periodicity. v) C and M class solar flares
  have a stronger causative effect on the MCMESI compared to X class
  solar flares. However, the only bidirectional causal relationship is
  obtained between the MCMESI and C class flare numbers.

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Title: Decoding the Pre-Eruptive Magnetic Field Configurations of
    Coronal Mass Ejections
Authors: Patsourakos, S.; Vourlidas, A.; Török, T.; Kliem, B.;
   Antiochos, S. K.; Archontis, V.; Aulanier, G.; Cheng, X.; Chintzoglou,
   G.; Georgoulis, M. K.; Green, L. M.; Leake, J. E.; Moore, R.; Nindos,
   A.; Syntelis, P.; Yardley, S. L.; Yurchyshyn, V.; Zhang, J.
2020SSRv..216..131P    Altcode: 2020arXiv201010186P
  A clear understanding of the nature of the pre-eruptive magnetic
  field configurations of Coronal Mass Ejections (CMEs) is required
  for understanding and eventually predicting solar eruptions. Only
  two, but seemingly disparate, magnetic configurations are considered
  viable; namely, sheared magnetic arcades (SMA) and magnetic flux ropes
  (MFR). They can form via three physical mechanisms (flux emergence,
  flux cancellation, helicity condensation). Whether the CME culprit
  is an SMA or an MFR, however, has been strongly debated for thirty
  years. We formed an International Space Science Institute (ISSI) team to
  address and resolve this issue and report the outcome here. We review
  the status of the field across modeling and observations, identify
  the open and closed issues, compile lists of SMA and MFR observables
  to be tested against observations and outline research activities
  to close the gaps in our current understanding. We propose that the
  combination of multi-viewpoint multi-thermal coronal observations
  and multi-height vector magnetic field measurements is the optimal
  approach for resolving the issue conclusively. We demonstrate the
  approach using MHD simulations and synthetic coronal images.

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Title: Analysis of quiet-sun turbulence on the basis of SDO/HMI and
    goode solar telescope data
Authors: Abramenko, Valentina I.; Yurchyshyn, Vasyl B.
2020MNRAS.497.5405A    Altcode: 2020arXiv200806264A; 2020MNRAS.tmp.2438A
  We analysed line-of-sight magnetic fields and magnetic power
  spectra of an undisturbed photosphere using magnetograms acquired
  by the Helioseismic and Magnetic Imager (HMI) on-board the Solar
  Dynamic Observatory and the Near InfraRed Imaging Spectrapolarimeter
  (NIRIS) operating at the Goode Solar Telescope of the Big Bear Solar
  Observatory. In the NIRIS data, we revealed thin flux tubes of 200-400
  km in diameter and of 1000-2000 G field strength. The HMI power spectra
  determined for a coronal hole, a quiet sun, and a plage areas exhibit
  the same spectral index of -1 on a broad range of spatial scales from
  10-20 Mm down to 2.4 Mm. This implies that the same mechanism(s)
  of magnetic field generation operate everywhere in the undisturbed
  photosphere. The most plausible one is the local turbulent dynamo. When
  compared to the HMI spectra, the -1.2 slope of the NIRIS spectrum
  appears to be more extended into the short spatial range until the
  cut-off at 0.8-0.9 Mm, after which it continues with a steeper slope of
  -2.2. Comparison of the observed and Kolmogorov-type spectra allowed
  us to infer that the Kolmogorov turbulent cascade cannot account for
  more than 35 per cent of the total magnetic energy observed in the
  scale range of 3.5-0.3 Mm. The energy excess can be attributed to other
  mechanisms of field generation such as the local turbulent dynamo and
  magnetic superdiffusivity observed in an undisturbed photosphere that
  can slow down the rate of the Kolmogorov cascade leading to a shallower
  resulting spectrum.

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Title: Accelerating and Supersonic Density Fluctuations in Coronal
Hole Plumes: Signature of Nascent Solar Winds
Authors: Cho, Il-Hyun; Nakariakov, Valery M.; Moon, Yong-Jae; Lee,
   Jin-Yi; Yu, Dae Jung; Cho, Kyung-Suk; Yurchyshyn, Vasyl; Lee, Harim
2020ApJ...900L..19C    Altcode: 2020arXiv200807848C
  Slow magnetoacoustic waves in a static background provide a
  seismological tool to probe the solar atmosphere in the analytic
  frame. By analyzing the spatiotemporal variation of the electron
  number density of plume structure in coronal holes above the limb for
  a given temperature, we find that the density perturbations accelerate
  with supersonic speeds in the distance range from 1.02 to 1.23 solar
  radii. We interpret them as slow magnetoacoustic waves propagating at
  about the sound speed with accelerating subsonic flows. The average
  sonic height of the subsonic flows is calculated to be 1.27 solar
  radii. The mass flux of the subsonic flows is estimated to be 44.1%
  relative to the global solar wind. Hence, the subsonic flow is likely
  to be the nascent solar wind. In other words, the evolution of the
  nascent solar wind in plumes at the low corona is quantified for the
  first time from imaging observations. Based on the interpretation,
  propagating density perturbations present in plumes could be used as
  a seismological probe of the gradually accelerating solar wind.

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Title: Date Co-alignment for Ground-Based High-Resolution Solar
    Imaging
Authors: Yang, X.; Ji, K.; Cao, W.; Yurchyshyn, V.; Xu, Z.
2020SPD....5120501Y    Altcode:
  The multi-wavelength analysis is a well-spread method in solar
  physics studies, and the community increasingly relies on coordinated
  observations involving multiple instruments. The calibration of
  heliographic coordinates is therefore vital for the co-alignment
  of such multi-instrument, multi-wavelength data. However, this is
  particularly difficult for ground-based high-resolution observations
  because of the limited field of view. Manually co-aligning data with
  low-contrast features (e.g., photospheric observations of quiet Sun
  regions) between different telescopes requires exceptional efforts
  and patience. Here, we developed a technique to accurately determine
  coordinates of high-resolution images acquired by the Goode Solar
  Telescope (GST) at the Big Bear Solar Observatory. The technique employs
  a scale-invariant feature transform (SIFT) method, which performs
  without human interference. With this new approach, we co-aligned
  multi-wavelength GST data sets to the continuum intensity data from
  the Helioseismic and Magnetic Imager (HMI) precisely. The inferred
  heliographic coordinates are saved in each FITS file header, which
  is compatible with the common mapping methods available in the Solar
  SoftWare (SSW) package. GST data are fully open to the scientific
  community, and a substantial portion of observing time on the GST
  opens to the community as well.

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Title: Hard X-Ray Emission from an Activated Flux Rope and Subsequent
    Evolution of an Eruptive Long-duration Solar Flare
Authors: Sahu, Suraj; Joshi, Bhuwan; Mitra, Prabir K.; Veronig,
   Astrid M.; Yurchyshyn, V.
2020ApJ...897..157S    Altcode: 2020arXiv200506221S
  In this paper, we present a comprehensive study of the evolutionary
  phases of a major M6.6 long duration event with special emphasize on
  its pre-flare phase. The event occurred in NOAA 12371 on 2015 June
  22. A remarkable aspect of the event was an active pre-flare phase
  lasting for about an hour during which a hot EUV coronal channel
  was in the build-up stage and displayed cospatial hard X-ray (HXR)
  emission up to energies of 25 keV. This is the first evidence of the
  HXR coronal channel. The coronal magnetic field configuration based
  on nonlinear-force-free-field modeling clearly exhibited a magnetic
  flux rope (MFR) oriented along the polarity inversion line (PIL) and
  cospatial with the coronal channel. We observed significant changes
  in the AR's photospheric magnetic field during an extended period of
  ≍42 hr in the form of rotation of sunspots, moving magnetic features,
  and flux cancellation along the PIL. Prior to the flare onset, the MFR
  underwent a slow rise phase (≍14 km s<SUP>-1</SUP>) for ≍12 minutes,
  which we attribute to the faster build-up and activation of the MFR
  by tether-cutting reconnection occurring at multiple locations along
  the MFR itself. The sudden transition in the kinematic evolution of
  the MFR from the phase of slow to fast rise (≍109 km s<SUP>-1</SUP>
  with acceleration ≍110 m s<SUP>-2</SUP>) precisely divides the
  pre-flare and impulsive phase of the flare, which points toward the
  feedback process between the early dynamics of the eruption and the
  strength of the flare magnetic reconnection.

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Title: Spatial Distribution of the Origin of Umbral Waves in a
    Sunspot Umbra
Authors: Yurchyshyn, Vasyl; Kilcik, Ali; Şahin, Seray; Abramenko,
   Valentina; Lim, Eun-Kyung
2020ApJ...896..150Y    Altcode: 2020arXiv200504202Y
  Umbral flashes (UFs) are emissions in the core of chromospheric lines
  caused by upward propagating waves steepening into shocks. UFs are
  followed by an expanding blueshifted umbral wave and redshifted plasma
  returning to the initial state. Here we use 5 s cadence images acquired
  at ±0.04 nm off the H ${}_{\alpha }$ line center by the Visible Imaging
  Spectrometer installed on the Goode Solar Telescope (GST) to detect
  the origin of UFs and umbral waves (UWs) in a sunspot with a uniform
  umbra free of light bridges and clusters of umbral dots. The data
  showed that UFs do not randomly originate over the umbra. Instead, they
  appear to be repeatedly triggered at locations with the lowest umbral
  intensity and the most powerful oscillations of H ${}_{\alpha }$ -0.04
  nm intensity. GST magnetic field measurements using the Near-Infrared
  Imaging Spectropolarimeter also showed that the dominant location of
  prevalent UF origin is cospatial associated with the strongest fields
  in the umbra. Interface Region Imaging Spectrograph 149.0 nm images
  showed that no bright UV loops were anchored in the umbra in general,
  and near the UF patches in particular, suggesting that UFs and UWs
  alone cannot be responsible for the origin of warm coronal loops. We
  thus conclude that the existence of locations with prevalent origin of
  UFs confirms the idea that they may be driven by a subsurface source
  located near the axis of a flux rope, while the presence of several UFs
  trigger centers may indicate the complex structure of a sunspot umbra.

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Title: Possible Production of Solar Spicules by Microfilament
    Eruptions
Authors: Sterling, Alphonse C.; Moore, Ronald L.; Samanta, Tanmoy;
   Yurchyshyn, Vasyl
2020ApJ...893L..45S    Altcode: 2020arXiv200404187S
  We examine Big Bear Solar Observatory (BBSO) Goode Solar Telescope
  (GST) high spatial resolution (0"06), high-cadence (3.45 s), Hα-0.8
  Å images of central-disk solar spicules, using data of Samanta et
  al. We compare with coronal-jet chromospheric-component observations
  of Sterling et al. Morphologically, bursts of spicules, referred to as
  "enhanced spicular activities" by Samanta et al., appear as scaled-down
  versions of the jet's chromospheric component. Both the jet and the
  enhanced spicular activities appear as chromospheric-material strands,
  undergoing twisting-type motions of ∼20-50 km s<SUP>-1</SUP>
  in the jet and ∼20-30 km s<SUP>-1</SUP> in the enhanced spicular
  activities. Presumably, the jet resulted from a minifilament-carrying
  magnetic eruption. For two enhanced spicular activities that we
  examine in detail, we find tentative candidates for corresponding
  erupting microfilaments, but not the expected corresponding base
  brightenings. Nonetheless, the enhanced-spicular-activities'
  interacting mixed-polarity base fields, frequent-apparent-twisting
  motions, and morphological similarities to the coronal jet's
  chromospheric-temperature component, suggest that erupting
  microfilaments might drive the enhanced spicular activities but be hard
  to detect, perhaps due to Hα opacity. Degrading the BBSO/GST-image
  resolution with a 1"0-FWHM smoothing function yields enhanced spicular
  activities resembling the "classical spicules" described by, e.g.,
  Beckers. Thus, a microfilament eruption might be the fundamental driver
  of many spicules, just as a minifilament eruption is the fundamental
  driver of many coronal jets. Similarly, a 0"5-FWHM smoothing renders
  some enhanced spicular activities to resemble previously reported
  "twinned" spicules, while the full-resolution features might account
  for spicules sometimes appearing as 2D-sheet-like structures.

---------------------------------------------------------
Title: Physical Characteristics of Umbral Dots Derived from a
    High-Resolution Observations
Authors: Kilcik, Ali; Sarp, Volkan; Yurchyshyn, Vasyl; Rozelot,
   Jean-Pierre; Ozguc, Atila
2020SoPh..295...58K    Altcode: 2020arXiv200407687K
  The aim of this study is to revisit the physical parameters of
  umbral dots (UDs) with the latest high-resolution observations and
  contribute to the scientific understanding of their formation and
  evolution. In this study, we applied a particle tracking algorithm for
  detecting UDs in NOAA AR 12384 observed on June 14, 2015 by the Goode
  Solar Telescope (GST). We analyzed average position distributions,
  location dependencies, and general properties of the detected total
  2892 UDs separately during their life time and the periodic behavior
  of ten selected long-lived UDs. We found: i) the brightest, largest,
  fastest and most elliptic UDs tend to be located at the umbra-penumbra
  boundary while their lifetime does not display any meaningful location
  dependency, ii) average dynamic velocity of all detected UDs is about
  twice (0.76 km s<SUP>−1</SUP>) of the previously reported average
  values, iii) obtained trajectories from the longest-lived 354 UDs show
  that they have generally inward motion, iv) chosen 10 long-lived UDs
  generally have similar periodic behavior showing 8.5 - 32, 3.5 - 4.1,
  1.5 - 1.9, and 1.1 - 1.3 minutes periodicities, v) generally, detected
  UDs have an elliptical shape with the averaged eccentricity of 0.29,
  with a 0.11 standard deviation, vi) larger UDs tend to be more elliptic
  and more dynamic.

---------------------------------------------------------
Title: Rapid Evolution of Type II Spicules Observed in Goode Solar
    Telescope On-disk H<SUB>α</SUB> Images
Authors: Yurchyshyn, Vasyl; Cao, Wenda; Abramenko, Valentina; Yang,
   Xu; Cho, Kyung-Suk
2020ApJ...891L..21Y    Altcode: 2020arXiv200504253Y
  We analyze ground-based chromospheric data acquired at a high temporal
  cadence of 2 s in wings of the H<SUB>α</SUB> spectral line using the
  Goode Solar Telescope operating at the Big Bear Solar Observatory. We
  inspected a 30 minute long H<SUB>α</SUB>-0.08 nm data set to find
  that rapid blueshifted H<SUB>α</SUB> excursions (RBEs), which are a
  cool component of type II spicules, experience very rapid morphological
  changes on timescales of the order of 1 s. Unlike typical reconnection
  jets, RBEs very frequently appear in situ without any clear evidence
  of H<SUB>α</SUB> material being injected from below. Their evolution
  includes inverted "Y," "V," "N," and parallel splitting (doubling)
  patterns as well as sudden formation of a diffuse region followed
  by branching. We also find that the same feature may undergo several
  splitting episodes within about a 1 minute time interval.

---------------------------------------------------------
Title: Magnetic Field Dynamics and Varying Plasma Emission in Large
    Scale Coronal Loops
Authors: Yurchyshyn, V.; Sahin, S.; Goode, P. R.; Kumar, P.; Kilcik,
   A.; Ahn, K.; Yang, X.
2019AGUFMSH11C3399Y    Altcode:
  We studied the evolution of magnetic fields at footpoints of two warm
  coronal loops observed on 5 May 2016 in NOAA AR 12542 (Loop I) and
  17 Dec 2015 in NOAA AR 12470 (Loop II). These loops were connecting
  a plage region with sunspot periphery (Loop I) and a sunspot umbra
  (Loop II). We used Solar Dynamics Observatory (SDO) and Goode Solar
  Telescope (GST) data to describe the phenomenon and understand its
  causes. The study indicates loop brightening episodes were associated
  with magnetic flux emergence and cancellation processes observed in
  SDO's Helioseismic and Magnetic Imager (HMI) and GST's Near InfraRed
  Imaging Spectrapolarimeter (NIRIS) data. The observed activity was
  driven by magnetic reconnection between small-scale emerging dipoles
  and large-scale pre-existing fields, suggesting that the reconnection
  occurred in the lower chromosphere at the edge of an extended plage
  region, where the loops were rooted. We suggest that plasma, evaporated
  during these reconnection events, gradually filled the loops and as it
  cooled the visible density front propagated from one footpoint of the
  loop to another at a rate of 90-110 km/s. This study also indicates
  that at least some of the bright loops seen in SDO Atmospheric Imaging
  Assembly images rooted in sunspot umbra may be heated due to magnetic
  activity taking place at the remote (non-sunspot) footpoint.

---------------------------------------------------------
Title: Generation of solar spicules and subsequent atmospheric heating
Authors: Samanta, Tanmoy; Tian, Hui; Yurchyshyn, Vasyl; Peter, Hardi;
   Cao, Wenda; Sterling, Alphonse; Erdélyi, Robertus; Ahn, Kwangsu;
   Feng, Song; Utz, Dominik; Banerjee, Dipankar; Chen, Yajie
2019Sci...366..890S    Altcode: 2020arXiv200602571S
  Spicules are rapidly evolving fine-scale jets of magnetized plasma in
  the solar chromosphere. It remains unclear how these prevalent jets
  originate from the solar surface and what role they play in heating
  the solar atmosphere. Using the Goode Solar Telescope at the Big Bear
  Solar Observatory, we observed spicules emerging within minutes of the
  appearance of opposite-polarity magnetic flux around dominant-polarity
  magnetic field concentrations. Data from the Solar Dynamics Observatory
  showed subsequent heating of the adjacent corona. The dynamic
  interaction of magnetic fields (likely due to magnetic reconnection)
  in the partially ionized lower solar atmosphere appears to generate
  these spicules and heat the upper solar atmosphere.

---------------------------------------------------------
Title: Light Bridge Brightening and Plasma Ejection Driven by a
    Magnetic Flux Emergence Event
Authors: Yang, Xu; Yurchyshyn, Vasyl; Ahn, Kwangsu; Penn, Matt;
   Cao, Wenda
2019ApJ...886...64Y    Altcode:
  Observations with the Goode Solar Telescope (GST) are presented
  here showing that the emergence of 1.91 × 10<SUP>18</SUP> Mx of
  new magnetic flux occurred at the edge of a filamentary light bridge
  (LB). This emergence was accompanied by brightness enhancement of a
  photospheric overturning convection cell (OCC) at the endpoints of the
  emerging magnetic structure. We present an analysis of the origin and
  the dynamics of this event using high-resolution GST Fe I 1564.85 nm
  vector magnetic field data, TiO photospheric, and Hα chromospheric
  images. The emerged structure was 1.5 × 0.3 Mm in size at the peak
  of development and lasted for 17 minutes. Doppler observations showed
  presence of systematic upflows before the appearance of the magnetic
  field signal and downflows during the decay phase. Changes in the
  orientation of the associated transverse fields, determined from
  the differential angle, suggest the emergence of a twisted magnetic
  structure. A fan-shaped jet was observed to be spatially and temporally
  correlated with the endpoint of the OCC intruding into the LB. Our data
  suggest that the emerging fields may have reconnected with the magnetic
  fields in the vicinity of the LB, which could lead to the formation of
  the jet. Our observation is the first report of flux emergence within
  a granular LB with evidence in the evolution of vector magnetic field,
  as well as photosphere convection motions, and supports the idea that
  the impulsive jets above the LB are caused by magnetic reconnection.

---------------------------------------------------------
Title: Analysis of the Hemispheric Sunspot Number Time Series for
    the Solar Cycles 18 to 24
Authors: Chowdhury, P.; Kilcik, A.; Yurchyshyn, V.; Obridko, V. N.;
   Rozelot, J. P.
2019SoPh..294..142C    Altcode:
  In this article, we investigate temporal and periodic variations of the
  hemispheric sunspot number using sunspot data from Kanzelhöhe Solar
  Observatory (KSO) for the time period of 1944 - 2017, which covers Solar
  Cycles 18 to 23 and almost the entire Solar Cycle 24 (2009 - 2017). The
  KSO data set was verified against the International Sunspot Number
  (ISSN) data. Temporal and periodic variations in the KSO data were
  analyzed using cross-correlation analysis, Morlet wavelet and multitaper
  (MTM) period analysis methods. We find that: i) sunspot numbers, as
  derived from both KSO and ISSN time series, are highly correlated with
  one another; ii) the temporal evolution of the sunspot number differs
  from one hemisphere to another with the solar cycle peaking at different
  times in each hemisphere; iii) the northern hemisphere showed two-
  and seven-month lead in Solar Cycles 18 and 19, respectively, while
  the southern hemisphere was leading in the rest of the cycles with
  the varying lead time ranging from 2 to 14 months; iv) apart from the
  fundamental mode of ≈ 11 years, Solar Cycle, the KSO data also show
  several midterm variations in the opposite hemispheres, specifically,
  Rieger-type and quasi-biennial periodicities - the detected midterm
  periodicities also differ in the northern and southern hemispheres;
  v) our results confirm the Waldmeier effect, which correlates the rise
  time with the cycle amplitude using the new sunspot data set from KSO.

---------------------------------------------------------
Title: Vortex Formations and Its Associated Surges in a Sunspot
    Light Bridge
Authors: Yang, Heesu; Lim, Eun-Kyung; Iijima, Haruhisa; Yurchyshyn,
   Vasyl; Cho, Kyung-Suk; Lee, Jeongwoo; Schmieder, Brigitte; Kim,
   Yeon-Han; Kim, Sujin; Bong, Su-Chan
2019ApJ...882..175Y    Altcode:
  We report on the successive occurrence of 0.″5 wide photospheric
  vortices with strong transverse shear flows at the edge of a sunspot
  light bridge (LB), and the subsequent ejection of chromospheric surges
  observed using a Visible Inteferometry Spectrograph, a broadband
  TiO filter, and a Near InfRared Imaging Spectrograph of the Goode
  Solar Telescope operating at Big Bear Solar Observatory. The Hα
  surges ejected at the location of the vortices often appeared in
  a hollow cylindrical structure. We also observed quasi-periodic
  vortex-associated bright Hα plasma blobs moving upward with a speed
  of up to 4 km s<SUP>-1</SUP>. In view of the strong shear flow at
  the edge of the LB, it is likely that the vortices form under the
  Kelvin-Helmholtz instability. The surges may result from either the
  magnetic tension generated after magnetic reconnection or an acoustic
  impulse of a fast photospheric transverse flow. Otherwise, the surges
  could also be associated with Alfvénic waves, in which case their
  origin could be torsional magnetic fields generated in the process of
  the vortex formation.

---------------------------------------------------------
Title: Cosmic Ray Modulation with the Maximum CME Speed Index During
    Solar Cycles 23 and 24
Authors: Sarp, Volkan; Kilcik, Ali; Yurchyshyn, Vasyl; Ozguc, Atila;
   Rozelot, Jean-Pierre
2019SoPh..294...86S    Altcode:
  We analyzed modulation of cosmic-ray intensities (CRIs) during
  Solar Cycles 23 and 24 by using the international sunspot numbers
  (ISSN) and the maximum CME speed index (MCMESI) as proxies for solar
  activity. Temporal variations, cross-correlations, and hysteresis
  patterns of CRI, MCMESI, and ISSN data were investigated. As a result,
  we concluded that the MCMESI better describes solar modulation of the
  CRI as compared to the ISSN. This is mainly because the correlation
  between CRI and ISSN is caused by the general cyclic trend of solar
  activity, while the correlation between the CRI and the MCMESI is
  mainly due to short-term fluctuations related to Forbush decreases. In
  contrast to the ISSN, there is no time lag between the CRI and the
  MCMESI variations.

---------------------------------------------------------
Title: Magnetic Field Dynamics and Varying Plasma Emission in Large
    Scale Coronal Loops
Authors: Yurchyshyn, Vasyl B.; Sahin, Seray; Kumar, Pankaj; Kilcik,
   Ali; Ahn, Kwangsu; Yang, Xu
2019AAS...23431104Y    Altcode:
  We report detailed observations of magnetic environment at four
  footpoints of two warm coronal loops observed on 5 May 2016 in NOAA
  AR 12542 (Loop I) and 17 Dec 2015 in NOAA AR 12470 (Loop II). These
  loops were connecting a plage region with sunspot periphery (Loop I)
  and a sunspot umbra (Loop II). We used Solar Dynamics Observatory (SDO)
  and Goode Solar Telescope (GST) data to describe the phenomenon and
  understand its causes. The study indicates loop brightening episodes
  were associated with magnetic flux emergence and cancellation processes
  observed in SDO's Helioseismic and Magnetic Imager (HMI) and GST's Near
  InfraRed Imaging Spectrapolarimeter (NIRIS) data. The observed activity
  was driven by magnetic reconnection between small-scale emerging dipoles
  and large-scale pre-existing fields, suggesting that the reconnection
  occurred in the lower chromosphere at the edge of an extended plage
  region, where the loops were rooted. We suggest that plasma, evaporated
  during these reconnection events, gradually filled the loops and as it
  cooled the visible density front propagated from one footpoint of the
  loop to another at a rate of 90-110 km/s. This study also indicates
  that at least some of the bright loops seen in SDO Atmospheric Imaging
  Assembly images rooted in sunspot umbra may be heated due to magnetic
  activity taking place at the remote (non-sunspot) footpoint.

---------------------------------------------------------
Title: Multi-wavelength Multi-height Study of Super Strong Surface
    and Coronal Magnetic Fields in Active Region 12673
Authors: Wang, Haimin; Chen, Bin; Jing, Ju; Yu, Sijie; Liu, Chang;
   Yurchyshyn, Vasyl B.; Ahn, Kwangsu; Okamoto, Takenori; Toriumi, Shin;
   Cao, Wenda; Gary, Dale E.
2019AAS...23440205W    Altcode:
  Using the joint observations of Goode Solar telescope (GST), Expanded
  Owens Valley Solar Array (EOVSA), Solar Dynamics Observatory (SDO)
  and Hinode, we study the Solar Active Region (AR) 12673 in September
  2017, which is the most flare productive AR in the solar cycle 24. GST
  observations show the strong photospheric magnetic fields (nearly
  6000 G) in polarity inversion line (PIL) and apparent photospheric
  twist. Consistent upward flows are also observed in Dopplergrams
  of Hinode, HMI and GST at the center part of that section of PIL,
  while the down flows are observed in two ends, indicating that the
  structure was rising from subsurface. Combining Non-Linear Force Free
  Extrapolation and EOVSA microwave imaging spectroscopy, we also look
  into the coronal structure of magnetic fields in this unusual AR,
  including the evolution before and after the X9.3 flare on September
  6, 2017. Coronal fields between 1000 and 2000 gauss are found above
  the flaring PIL at the height range between 8 and 4Mm, outlining the
  structure of a fluxrope or sheared arcade.

---------------------------------------------------------
Title: Sheared Magnetic Arcades and the Pre-eruptive Magnetic
Configuration of Coronal Mass Ejections: Diagnostics, Challenges
    and Future Observables
Authors: Patsourakos, Spiros; Vourlidas, A.; Anthiochos, S. K.;
   Archontis, V.; Aulanier, G.; Cheng, X.; Chintzoglou, G.; Georgoulis,
   M. K.; Green, L. M.; Kliem, B.; Leake, J.; Moore, R. L.; Nindos, A.;
   Syntelis, P.; Torok, T.; Yardley, S. L.; Yurchyshyn, V.; Zhang, J.
2019shin.confE.194P    Altcode:
  Our thinking about the pre-eruptive magnetic configuration of Coronal
  Mass Ejections has been effectively dichotomized into two opposing
  and often fiercely contested views: namely, sheared magnetic arcades
  and magnetic flux ropes. Finding a solution to this issue will have
  important implications for our understanding of CME initiation. We
  first discuss the very value of embarking into the arcade vs. flux rope
  dilemma and illustrate the corresponding challenges and difficulties to
  address it. Next, we are compiling several observational diagnostics of
  pre-eruptive sheared magnetic arcades stemming from theory/modeling,
  discuss their merits, and highlight potential ambiguities that could
  arise in their interpretation. We finally conclude with a discussion
  of possible new observables, in the frame of upcoming or proposed
  instrumentation, that could help to circumvent the issues we are
  currently facing.

---------------------------------------------------------
Title: Oscillation of a Small Hα Surge in a Solar Polar Coronal Hole
Authors: Cho, Kyung-Suk; Cho, Il-Hyun; Nakariakov, V. M.; Yurchyshyn,
   Vasyl B.; Yang, Heesu; Kim, Yeon-Han; Kumar, Pankaj; Magara, Tetsuya
2019ApJ...877L...1C    Altcode:
  Hα surges (i.e., cool/dense collimated plasma ejections) may act as
  a guide for a propagation of magnetohydrodynamic waves. We report
  a high-resolution observation of a surge observed with 1.6 m Goode
  Solar Telescope (GST) on 2009 August 26, from 18:20 UT to 18:45
  UT. Characteristics of plasma motions in the surge are determined
  with the normalizing radial gradient filter and the Fourier motion
  filter. The shape of the surge is found to change from a “C”
  shape to an inverse “C” shape after a formation of a cusp, a
  signature of reconnection. There are apparent upflows seen above
  the cusp top and downflows below it. The upflows show rising and
  rotational motions in the right-hand direction, with the rotational
  speed decreasing with height. Near the cusp top, we find a transverse
  oscillation of the surge, with the period of ∼2 minutes. There is no
  change of the oscillation phase below the cusp top, but above the top
  a phase change is identified, giving a vertical phase speed about 86
  km s<SUP>-1</SUP>. As the height increases, the initial amplitude of
  the oscillation increases, and the oscillation damping time decreases
  from 5.13 to 1.18 minutes. We conclude that the oscillation is a
  propagating kink wave that is possibly excited by the repetitive
  spontaneous magnetic reconnection.

---------------------------------------------------------
Title: Flame-like Ellerman Bombs and Their Connection to Solar
    Ultraviolet Bursts
Authors: Chen, Yajie; Tian, Hui; Peter, Hardi; Samanta, Tanmoy;
   Yurchyshyn, Vasyl; Wang, Haimin; Cao, Wenda; Wang, Linghua; He, Jiansen
2019ApJ...875L..30C    Altcode: 2019arXiv190301981C
  Ellerman bombs (EBs) are small-scale intense brightenings in Hα
  wing images, which are generally believed to be signatures of
  magnetic reconnection around the temperature minimum region of the
  solar atmosphere. They have a flame-like morphology when observed
  near the solar limb. Recent observations from the Interface Region
  Imaging Spectrograph (IRIS) reveal another type of small-scale
  reconnection event called an ultraviolet (UV) burst, in the lower solar
  atmosphere. Though previous observations have shown a clear coincidence
  between the occurrence of some UV bursts and EBs, the exact relationship
  between these two phenomena is still debated. We investigate the spatial
  and temporal relationship between flame-like EBs and UV bursts using
  joint near-limb observations between the 1.6 m Goode Solar Telescope
  (GST) and IRIS. In total, 161 EBs have been identified from the GST
  observations, and ∼20 of them reveal signatures of UV bursts in
  the IRIS images. Interestingly, we find that these UV bursts have a
  tendency to appear at the upper parts of their associated flame-like
  EBs. The intensity variations of most EB-related UV bursts and their
  corresponding EBs match well. Our results suggest that some of these
  UV bursts and EBs likely form at different heights during a common
  reconnection process.

---------------------------------------------------------
Title: Magnetic Field Dynamics and Varying Plasma Emission in
    Large-scale Coronal Loops
Authors: Şahin, S.; Yurchyshyn, V.; Kumar, P.; Kilcik, A.; Ahn, K.;
   Yang, X.
2019ApJ...873...75S    Altcode: 2019arXiv190312148S
  In this study we report detailed observations of magnetic environment at
  four footpoints of two warm coronal loops observed on 2016 May 5 in NOAA
  AR 12542 (Loop I) and 2015 December 17 in NOAA AR 12470 (Loop II). These
  loops were connecting a plage region with sunspot periphery (Loop I)
  and a sunspot umbra (Loop II). We used Solar Dynamics Observatory (SDO)
  and Goode Solar Telescope (GST) data to describe the phenomenon and
  understand its causes. The study indicates loop brightening episodes
  were associated with magnetic flux emergence and cancellation processes
  observed in SDO’s Helioseismic and Magnetic Imager and GST’s Near
  InfraRed Imaging Spectrapolarimeter data. The observed activity was
  driven by magnetic reconnection between small-scale emerging dipoles
  and large-scale pre-existing fields, suggesting that the reconnection
  occurred in the lower chromosphere at the edge of an extended plage
  region, where the loops were rooted. We suggest that plasma, evaporated
  during these reconnection events, gradually filled the loops and as it
  cooled the visible density front propagated from one footpoint of the
  loop to another at a rate of 90-110 km s<SUP>-1</SUP>. This study also
  indicates that at least some of the bright loops seen in SDO Atmospheric
  Imaging Assembly images rooted in sunspot umbra may be heated due to
  magnetic activity taking place at the remote (nonsunspot) footpoint.

---------------------------------------------------------
Title: Prediction of solar cycle 25: a non-linear approach
Authors: Sarp, V.; Kilcik, A.; Yurchyshyn, V.; Rozelot, J. P.;
   Ozguc, A.
2018MNRAS.481.2981S    Altcode: 2018MNRAS.tmp.2359S
  Predicting the solar activity is an important task for space weather
  and solar physics. There are various approaches to predict the
  solar activity and these predictions are used in various areas such
  as planning space missions, approximating the mechanism of solar
  dynamo, etc. In this paper, a non-linear prediction algorithm based
  on delay-time and phase space reconstruction is used to forecast the
  maximum of Solar Cycle 25. Apart from embedding dimension and delay-time
  which are the key parameters of such methods, we further found a new
  parameter (starting point) that should be taken into account to get
  better solar cycle predictions. This method was tested on last five
  solar cycles and the results are quite acceptable. We predicted that
  the maximum of Solar Cycle 25 will be at the year 2023.2 ± 1.1 with a
  peak sunspot number of 154 ± 12. Our results are compared with other
  available predictions.

---------------------------------------------------------
Title: First high-resolution look at the quiet Sun with ALMA at 3mm
Authors: Nindos, A.; Alissandrakis, C. E.; Bastian, T. S.; Patsourakos,
   S.; De Pontieu, B.; Warren, H.; Ayres, T.; Hudson, H. S.; Shimizu,
   T.; Vial, J. -C.; Wedemeyer, S.; Yurchyshyn, V.
2018A&A...619L...6N    Altcode: 2018arXiv181005223N
  We present an overview of high-resolution quiet Sun observations,
  from disk center to the limb, obtained with the Atacama Large
  millimeter and sub-millimeter Array (ALMA) at 3 mm. Seven quiet-Sun
  regions were observed at a resolution of up to 2.5″ by 4.5″. We
  produced both average and snapshot images by self-calibrating the ALMA
  visibilities and combining the interferometric images with full-disk
  solar images. The images show well the chromospheric network, which,
  based on the unique segregation method we used, is brighter than the
  average over the fields of view of the observed regions by ∼305
  K while the intranetwork is less bright by ∼280 K, with a slight
  decrease of the network/intranetwork contrast toward the limb. At 3
  mm the network is very similar to the 1600 Å images, with somewhat
  larger size. We detect, for the first time, spicular structures,
  rising up to 15″ above the limb with a width down to the image
  resolution and brightness temperature of ∼1800 K above the local
  background. No trace of spicules, either in emission or absorption,
  is found on the disk. Our results highlight the potential of ALMA for
  the study of the quiet chromosphere.

---------------------------------------------------------
Title: Magnetic Flux Emergence Triggered Light Bridge Brightening
    and Reconnection Jets
Authors: Yang, Xu; Cao, Wenda; Yurchyshyn, Vasyl; Ahn, Kwangsu
2018cosp...42E3744Y    Altcode:
  Light bridges (LBs) are elongated, bright, granular structures that
  divide the umbra of a large and complex sunspot into two or more umbral
  regions with the same magnetic polarity. Surge-like activities are
  common phenomenon appear above the LBs which always accompanied by the
  magnetic flux emergence process. Former works tried to interpret the
  triggering mechanism for them, however they often lacked the support of
  high spatial and temporal resolution vector magnetic measurement. Our
  recent Observation shows a strong magnetic flux emergence happened
  at the edge of a filamentary Light Bridge (LB) and accompanied by
  brightness enhancement of photospheric granulations at the endpoints
  of the emerged magnetic structure. We study the origin and dynamics of
  this magnetic flux emergence event with high resolution Fe I 1.56 μm
  polarimetry magnetogram, TiO photosphere image and Hα chromosphere
  image from the Goode Solar Telescope. The emerged magnetic structure
  was 1.5 Mm × 0.3 Mm in size at its peak time and lasted for 17
  minutes. Doppler map detected upflows before its formation and downflows
  during the destruction. The magnetic orientation change was obtained by
  calculating the shear angle and plotting the magnetic field vectors. The
  result indicates that the new emerged more transverse magnetic field
  reconnected with the pre-existing more vertical field, which triggered
  the fan-shaped jets. The expanding fields at the endpoints due to the
  flux emergence pushed and compressed the existing granulations and
  led to their enhanced brightness.

---------------------------------------------------------
Title: Erupting Solar Magnetic Flux Ropes and the Bz Challenge:
    Understanding details of CME propagation in the Interplanetary Media
Authors: Yurchyshyn, Vasyl
2018cosp...42E3786Y    Altcode:
  Understanding the connection between magnetic topologies of a
  coronal mass ejection (CME) as observed closer to the Sun and in
  the interplanetary medium close to the Earth is vital for successful
  predictions of geomagnetic storms. Recent solar and magnetospheric
  data convincingly demonstrate that fast CME originating from near
  the solar disk center are the major cause of extreme space weather
  events. Moreover, topology and helicity of the ejected fields tends
  to be mainly preserved as the ejecta propagates and evolves in the
  interplanetary space. The interplanetary CME that is often observed near
  the Earth as a well organized helical structure called _ a magnetic
  cloud (MC) is the result of expansion of the original ejecta and its
  interaction with the heliospheric plasma and magnetic fields that
  may cause the ejecta to alter its shape, rotate and shed its magnetic
  flux. Therefore the probability of a strong geomagnetic storm to occur
  as well as its intensity depend on both initial properties of the
  erupted structure and the further interactions that the ejecta may be
  subjected to as it expands into the heliosphere. Detailed understanding
  of this interaction may shed light on the problems related to connecting
  solar surface phenomena to their interplanetary counterparts. In this
  talk I will briefly review current progress on the CME evolution in
  the heliosphere.

---------------------------------------------------------
Title: The evolution of flaring and non-flaring active regions
Authors: Kilcik, A.; Yurchyshyn, V.; Sahin, S.; Sarp, V.; Obridko,
   V.; Ozguc, A.; Rozelot, J. P.
2018MNRAS.477..293K    Altcode:
  According to the modified Zurich classification, sunspot groups are
  classified into seven different classes (A, B, C, D, E, F and H) based
  on their morphology and evolution. In this classification, classes
  A and B, which are small groups, describe the beginning of sunspot
  evolution, while classes D, E and F describe the large and evolved
  groups. Class C describes the middle phase of sunspot evolution and
  the class H describes the end of sunspot evolution. Here, we compare
  the lifetime and temporal evolution of flaring and non-flaring active
  regions (ARs), and the flaring effect on ARs in these groups in detail
  for the last two solar cycles (1996 through 2016). Our main findings
  are as follows: (i) Flaring sunspot groups have longer lifetimes
  than non-flaring ones. (ii) Most of the class A, B and C flaring
  ARs rapidly evolve to higher classes, while this is not applicable
  for non-flaring ARs. More than 50 per cent of the flaring A, B and
  C groups changed morphologically, while the remaining D, E, F and
  H groups did not change remarkably after the flare activity. (iii)
  75 per cent of all flaring sunspot groups are large and complex. (iv)
  There is a significant increase in the sunspot group area in classes A,
  B, C, D and H after flaring activity. In contrast, the sunspot group
  area of classes E and F decreased. The sunspot counts of classes D, E
  and F decreased as well, while classes A, B, C and H showed an increase.

---------------------------------------------------------
Title: Signature of a possible relationship between the maximum CME
    speed index and the critical frequencies of the F1 and F2 ionospheric
layers: Data analysis for a mid-latitude ionospheric station during
    the solar cycles 23 and 24
Authors: Kilcik, Ali; Ozguc, Atila; Yiğit, Erdal; Yurchyshyn, Vasyl;
   Donmez, Burcin
2018JASTP.171..131K    Altcode:
  We analyze temporal variations of two solar indices, the monthly
  mean Maximum CME Speed Index (MCMESI) and the International Sunspot
  Number (ISSN) as well as the monthly median ionospheric critical
  frequencies (foF1, and foF2) for the time period of 1996-2013,
  which covers the entire solar cycle 23 and the ascending branch of
  the cycle 24. We found that the maximum of foF1 and foF2 occurred
  respectively during the first and second maximum of the ISSN solar
  activity index in the solar cycle 23. We compared these data sets by
  using the cross-correlation and hysteresis analysis and found that
  both foF1 and foF2 show higher correlation with ISSN than the MCMESI
  during the investigated time period, but when significance levels are
  considered correlation coefficients between the same indices become
  comparable. Cross-correlation analysis showed that the agreement between
  these data sets (solar indices and ionospheric critical frequencies)
  is better pronounced during the ascending phases of solar cycles, while
  they display significant deviations during the descending phase. We
  conclude that there exists a signature of a possible relationship
  between MCMESI and foF1 and foF2, which means that MCMESI could be
  used as a possible indicator of solar and geomagnetic activity, even
  though other investigations are needed.

---------------------------------------------------------
Title: High-resolution Observations of a White-light Flare with
    Goode Solar Telescope
Authors: Yurchyshyn, Vasyl; Kumar, Pankaj; Abramenko, Valentyna; Xu,
   Yan; Goode, Philip R.; Cho, Kyung-Suk F.
2018tess.conf21702Y    Altcode:
  Using high resolution data from the Goode Solar Telescope (GST)
  we studied the fine spatial and temporal structure of an M1.3 white
  light (WL) flare, which was one of the three homologous solar flares
  (C6.8, M1.3, and M2.3) observed in a close proximity to the west solar
  limb. The RHESSI photon spectra for the M1.3 flare showed strongly
  accelerated electrons with energies above 100 keV. Comparison of
  HXR photon spectra for the three flares suggests that either thermal
  energy of order of 10<SUP>30</SUP> ergs and/or high energy electrons
  (&gt;50 keV) are necessary to produce a WL flare. The strong and
  compact WL cores were ≈0.15 Mm across with an area of about
  10<SUP>14</SUP> cm<SUP>2</SUP> . The observed TiO enhancements are
  not normally distributed and are structured by the magnetic field of
  the penumbra. Several of the TiO cores were not co-spatial with the Hα
  emission, which suggests that the TiO and chromospheric emission did not
  originate in the same chromospheric volume as some models suggest. We
  thus conclude that fine temporal and spatial structure of the WL flare
  was largely defined by the associated magnetic fields, which favors
  the direct heating models, where the flare energy is directly deposited
  in the temperature minimum region by the accelerated electrons.

---------------------------------------------------------
Title: Observation of Light Bridge Brightening and Plasma Ejection
    Triggered by a Magnetic Flux Emergence Event
Authors: Yang, Xu; Yurchyshyn, Vasyl; Ahn, Kwangsu; Cao, Wenda
2018tess.conf10906Y    Altcode:
  Light bridges (LBs) are elongated, bright, granular structures that
  divide the umbra of a large and complex sunspot into two or more umbral
  regions with the same magnetic polarity. Surge-like activities are
  common phenomenon appear above the LBs which always accompanied by the
  magnetic flux emergence process. Former works tried to interpret the
  triggering mechanism for them, however they often lacked the support of
  high spatial and temporal resolution vector magnetic measurement. Our
  recent Observation shows a strong magnetic flux emergence happened
  at the edge of a filamentary Light Bridge (LB) and accompanied by
  brightness enhancement of photospheric granulations at the endpoints
  of the emerged magnetic structure. We study the origin and dynamics of
  this magnetic flux emergence event with high resolution Fe I 1.56 μm
  polarimetry magnetogram, TiO photosphere image and Hα chromosphere
  image from the Goode Solar Telescope. The emerged magnetic structure
  was 1.5 Mm × 0.3 Mm in size at its peak time and lasted for 17
  minutes. Doppler map detected upflows before its formation and downflows
  during the destruction. The magnetic orientation change was obtained by
  calculating the shear angle and plotting the magnetic field vectors. The
  result indicates that the new emerged more transverse magnetic field
  reconnected with the pre-existing more vertical field, which triggered
  the fan-shaped jets. The expanding fields at the endpoints due to the
  flux emergence pushed and compressed the existing granulations and
  led to their enhanced brightness.

---------------------------------------------------------
Title: Study of 3D magnetic Structure Corresponding to Extremely
    Strong Photospheric Magnetic Fields in Active Region 12673
Authors: Wang, Haimin; Yurchyshyn, Vasyl; Liu, Chang; Chen, Bin;
   Jing, Ju; Ahn, Kwangsu; Toriumi, Shin; Cao, Wenda
2018tess.conf31902W    Altcode:
  Solar Active Region (AR) 12673 is the most flare productive AR in the
  solar cycle 24. It produced four X-class flares including the X9.3 flare
  on 06 September 2017 and the X8.2 limb event on 10 September. Sun and
  Norton (2017) reported that this region had an unusual high rate of
  flux emergence, while Huang et al. (2018) reported that the X9.3 flare
  had extremely strong white-light flare emission. Yang et al. (2017)
  described the detailed morphological evolution of this AR. In this work,
  we first study the unusual behaviors of the light bridge (LB) dividing
  the delta configuration of this AR, namely the strong magnetic fields
  (above 5500 G) in the LB and the apparent photospheric twist as seen in
  observations with a 0.1 arcsec spatial resolution obtained by the 1.6m
  Goode Solar Telescope (GST) at the Big Bear Solar Observatory. Using the
  newly commissioned Expanded Owens Valley Solar Array (EOVSA), we carried
  out diagnoses of magnetic fields in this AR with microwave imaging
  spectroscopy from 2.5 to 18 GHz. Finally, we utilized Non-Linear Force
  Free Field (NLFFF) extrapolation to reveal 3-D magnetic structure to
  gain a physical understanding of GST and EOVSA observations of this AR.

---------------------------------------------------------
Title: The evolution of a small complex active region AR 12550
    observed by the GST
Authors: Kim, Yeon-Han; Xu, Yan; Yurchyshyn, Vasyl; Lim, Eun-Kyung
2018EGUGA..2013133K    Altcode:
  The 1.6m Goode Solar Telescope (GST: formerly NST) at Big Bear Solar
  Observatory (BBSO) provides us with unprecedented high-resolution
  data of the Sun since 2009. On 2016 May 30, we observed a small
  complex active region AR 12550 using the GST equipped with the He I D3
  filter, the photospheric broadband filter (G-band), and Near IR imaging
  spectrograph (NIRIS). This active region showed a small loop eruption
  in He I D3 images associated with several B class brightenings from
  17:00 UT to 18:00 UT and dynamic variations of photospheric features
  in G-band and NIRIS images. Additionally, we examined the SDO data
  and found several brightenings and loop activities in the higher
  temperature plasmas. Interestingly, the loop activities appeared as
  dark features in D3 images and did as bright ones in SDO data. In
  order to interpret both data, we performed DEM analysis using SDO AIA
  data. In this presentation, we will describe the whole evolution of
  the AR 12550 and give the observation results.

---------------------------------------------------------
Title: Temporal and Periodic Variations of Sunspot Counts in Flaring
    and Non-Flaring Active Regions
Authors: Kilcik, A.; Yurchyshyn, V.; Donmez, B.; Obridko, V. N.;
   Ozguc, A.; Rozelot, J. P.
2018SoPh..293...63K    Altcode: 2017arXiv170509065K
  We analyzed temporal and periodic variations of sunspot counts (SSCs)
  in flaring (C-, M-, or X-class flares), and non-flaring active regions
  (ARs) for nearly three solar cycles (1986 through 2016). Our main
  findings are as follows: i) temporal variations of monthly means of
  the daily total SSCs in flaring and non-flaring ARs behave differently
  during a solar cycle and the behavior varies from one cycle to another;
  during Solar Cycle 23 temporal SSC profiles of non-flaring ARs are wider
  than those of flaring ARs, while they are almost the same during Solar
  Cycle 22 and the current Cycle 24. The SSC profiles show a multi-peak
  structure and the second peak of flaring ARs dominates the current
  Cycle 24, while the difference between peaks is less pronounced during
  Solar Cycles 22 and 23. The first and second SSC peaks of non-flaring
  ARs have comparable magnitude in the current solar cycle, while the
  first peak is nearly absent in the case of the flaring ARs of the same
  cycle. ii) Periodic variations observed in the SSCs profiles of flaring
  and non-flaring ARs derived from the multi-taper method (MTM) spectrum
  and wavelet scalograms are quite different as well, and they vary from
  one solar cycle to another. The largest detected period in flaring
  ARs is 113 ±1.6 days while we detected much longer periodicities (327
  ±13 , 312 ±11 , and 256 ±8 days) in the non-flaring AR profiles. No
  meaningful periodicities were detected in the MTM spectrum of flaring
  ARs exceeding 55 ±0.7 days during Solar Cycles 22 and 24, while a 113
  ±1.3 days period was detected in flaring ARs of Solar Cycle 23. For
  the non-flaring ARs the largest detected period was only 31 ±0.2
  days for Cycle 22 and 72 ±1.3 days for the current Cycle 24, while
  the largest measured period was 327 ±13 days during Solar Cycle 23.

---------------------------------------------------------
Title: Frequently Occurring Reconnection Jets from Sunspot Light
    Bridges
Authors: Tian, Hui; Yurchyshyn, Vasyl; Peter, Hardi; Solanki, Sami
   K.; Young, Peter R.; Ni, Lei; Cao, Wenda; Ji, Kaifan; Zhu, Yingjie;
   Zhang, Jingwen; Samanta, Tanmoy; Song, Yongliang; He, Jiansen; Wang,
   Linghua; Chen, Yajie
2018ApJ...854...92T    Altcode: 2018arXiv180106802T
  Solid evidence of magnetic reconnection is rarely reported within
  sunspots, the darkest regions with the strongest magnetic fields
  and lowest temperatures in the solar atmosphere. Using the world’s
  largest solar telescope, the 1.6 m Goode Solar Telescope, we detect
  prevalent reconnection through frequently occurring fine-scale jets
  in the Hα line wings at light bridges, the bright lanes that may
  divide the dark sunspot core into multiple parts. Many jets have an
  inverted Y-shape, shown by models to be typical of reconnection in a
  unipolar field environment. Simultaneous spectral imaging data from
  the Interface Region Imaging Spectrograph show that the reconnection
  drives bidirectional flows up to 200 km s<SUP>-1</SUP>, and that the
  weakly ionized plasma is heated by at least an order of magnitude up
  to ∼80,000 K. Such highly dynamic reconnection jets and efficient
  heating should be properly accounted for in future modeling efforts
  of sunspots. Our observations also reveal that the surge-like activity
  previously reported above light bridges in some chromospheric passbands
  such as the Hα core has two components: the ever-present short surges
  likely to be related to the upward leakage of magnetoacoustic waves
  from the photosphere, and the occasionally occurring long and fast
  surges that are obviously caused by the intermittent reconnection jets.

---------------------------------------------------------
Title: Strong Transverse Photosphere Magnetic Fields and Twist in
    Light Bridge Dividing Delta Sunspot of Active Region 12673
Authors: Wang, Haimin; Yurchyshyn, Vasyl; Liu, Chang; Ahn, Kwangsu;
   Toriumi, Shin; Cao, Wenda
2018RNAAS...2....8W    Altcode: 2018RNAAS...2a...8W; 2018arXiv180102928W
  Solar Active Region (AR) 12673 is the most flare productive AR in the
  solar cycle 24. It produced four X-class flares including the X9.3 flare
  on 06 September 2017 and the X8.2 limb event on 10 September. Sun and
  Norton (2017) reported that this region had an unusual high rate of
  flux emergence, while Huang et al. (2018) reported that the X9.3 flare
  had extremely strong white-light flare emissions. Yang at al. (2017)
  described the detailed morphological evolution of this AR. In this
  report, we focus on usual behaviors of the light bridge (LB) dividing
  the delta configuration of this AR, namely the strong magnetic fields
  (above 5500 G) in the LB and apparent photospheric twist as shown in
  observations with a 0.1 arcsec spatial resolution obtained by the 1.6m
  telescope at Big Bear Solar Observatory.

---------------------------------------------------------
Title: Problem of Super-Strong Magnetic Fields on the Sun: Brief
    Chronology and New Observational Data
Authors: Lozitsky, V. G.; Yurchyshyn, V. B.; Ahn, K.; Wang, H.;
   Lozitska, N. I.
2018OAP....31..152L    Altcode:
  In this study we present the old and new observational data
  concerning the problem of extreme magnetic fields (≥ 5 kG)
  in the Sun's atmosphere. We emphasize that the upper limit of the
  intensity of the magnetic field in the solar atmosphere is unknown to
  date. Severny (1957) heuristically suggested that the magnetic fields
  in the sunspots could reach 50 kG. As for the observational data, at
  least three arguments in favor of the magnetic fields of the order
  of ≤10<SUP>4</SUP> G can be specified: (1) the dependence of the
  measured magnetic field on the factor g<SUB>eff</SUB>λ<SUP>2</SUP>
  of magnetosensitive lines (Gopasyuk et al., 1973; Lozitsky, 1980),
  (2) local extremums in splitting of bisectors in the profiles I
  ± V for lines with different Lande factors (Lozitsky, 1980; 2015)
  and (3) the reliable splitting of emission peaks in Fe I lines with
  very low Lande factors, about 0.01, in the spectra of powerful solar
  flares (Lozitsky, 1993; 1998). Theoretically, superstrong fields
  should have gigantic magnetic pressure and can exist only with a
  specific topology of field lines, apparently of a force-free type
  (Soloviev and Lozitsky, 1986). To further develop this problem,
  we are analyzing new observational data obtained with the NIRIS
  spectropolarimeter of the largest GST solar telescope of the Big Bear
  Solar Observatory (BBSO). Our observations relate to the active region
  NOAA 12673, which was the most flare-productive in the 24<SUP>th</SUP>
  cycle. Stokes-metric measurements are made in the FeI 15648.5 Å line
  with a signal-to-noise ratio of about 10<SUP>-4</SUP>. In this active
  region, superstrong magnetic field of 5.57 kG was discovered recently by
  Wang et al. (2018). An additional study of about 70 different places in
  this active region suggested that there were two types of places that
  can be conventionally called "typical" and "peculiar". In "typical"
  areas, the magnitude of the magnetic field in general is the greater,
  the less the intensity in the spectral continuum, and the maximum field
  here does not exceed 4 kG. All "peculiar" places correspond to positions
  with the highest intensity in the spectral continuum, and the magnetic
  field strength is here in the range of 3.0-5.7 kG. Notice, such strong
  magnetic fields were firstly discovered outside the sunspot umbra. The
  orientation of the magnetic field vector in "peculiar" places is close
  to the transversal, which is also atypical for "typical" regions and
  can reflect strong twisting of field lines.

---------------------------------------------------------
Title: Multi-wavelength Observation of Filament Eruption associated
    with M-class Flare
Authors: Kim, S.; Yurchyshyn, V.; Jiang, C.
2017AGUFMSH41A2748K    Altcode:
  We have investigated a M-class flare associated with filament eruption
  which developed into a Halo CME. The M-class flare occurred in 2011
  August 4. For this study, we used the Nobryama Radioheliograph (NoRH)
  17 and 34 GHz, RHESSI Hard X-ray satellite, and Atmo- spheric Imaging
  Assembly (AIA) and the Heliospheric Magentic Imager(HMI) onboard the
  Solar Dynamic Observatory (SDO). During the pre-eruption phase, clear
  nonthermal emission was detected in microwaves of NoRH and hard-X-ray
  of RHESSI. At the moment that the nonthermal emission start, the
  nonthermal sources appeared at the one edge of the filament structure on
  a polarity inversion line, and the slowing rising filament structure in
  AIA 94A underwent a sudden acceleration on its ascendance. Magnetograms
  showed converging motion of magnetic elements at the source position
  of HXR and MW. Based on the results, we conjecture that the plausible
  trigger of the filament eruption is magnetic reconnections at the HXR
  source position by converging motion of magnetic elements. In addition,
  we will discuss on the magnetic flux variation before and after the
  eruption based on the result of Nonlinear force-free field model.

---------------------------------------------------------
Title: Observation of a Large-scale Quasi-circular Secondary Ribbon
    Associated with Successive Flares and a Halo CME
Authors: Lim, Eun-Kyung; Yurchyshyn, Vasyl; Kumar, Pankaj; Cho,
   Kyuhyoun; Jiang, Chaowei; Kim, Sujin; Yang, Heesu; Chae, Jongchul;
   Cho, Kyung-Suk; Lee, Jeongwoo
2017ApJ...850..167L    Altcode: 2017arXiv171100622L
  Solar flare ribbons provide an important clue to the magnetic
  reconnection process and associated magnetic field topology in the
  solar corona. We detected a large-scale secondary flare ribbon of
  a circular shape that developed in association with two successive
  M-class flares and one coronal mass ejection. The ribbon revealed
  interesting properties such as (1) a quasi-circular shape and enclosing
  the central active region (AR); (2) the size as large as 500″ by
  650″ (3) successive brightenings in the clockwise direction at a
  speed of 160 km s<SUP>-1</SUP> starting from the nearest position to
  the flaring sunspots; (4) radial contraction and expansion in the
  northern and the southern part, respectively, at speeds of ≤10
  km s<SUP>-1</SUP>. Using multi-wavelength data from Solar Dynamics
  Observatory, RHESSI, XRT, and Nobeyama, along with magnetic field
  extrapolations, we found that: (1) the secondary ribbon location is
  consistent with those of the field line footpoints of a fan-shaped
  magnetic structure that connects the flaring region and the ambient
  decaying field; (2) the second M2.6 flare occurred when the expanding
  coronal loops driven by the first M2.0 flare encountered the background
  decayed field; (3) immediately after the second flare, the secondary
  ribbon developed along with dimming regions. Based on our findings,
  we suggest that interaction between the expanding sigmoid field and
  the overlying fan-shaped field triggered the secondary reconnection
  that resulted in the field opening and formation of the quasi-circular
  secondary ribbon. We thus conclude that interaction between the AR and
  the ambient large-scale fields should be taken into account to fully
  understand the entire eruption process.

---------------------------------------------------------
Title: Three-minute Sunspot Oscillations Driven by Magnetic
    Reconnection in a Light Bridge
Authors: Song, Donguk; Chae, Jongchul; Kwak, Hannah; Kano, Ryouhei;
   Yurchyshyn, Vasyl; Moon, Yong-Jae; Lim, Eun-Kyung; Lee, Jeongwoo
2017ApJ...850L..33S    Altcode: 2017arXiv171106489S
  We report a different type of three-minute chromospheric oscillation
  above a sunspot in association with a small-scale impulsive event
  in a light bridge (LB). During our observations, we found a transient
  brightening in the LB. The brightening was composed of elementary bursts
  that may be a manifestation of fast repetitive magnetic reconnections
  in the LB. Interestingly, the oscillations in the nearby sunspot umbra
  were impulsively excited when the intensity of the brightening reached
  its peak. The initial period of the oscillations was about 2.3 minutes
  and then gradually increased to 3.0 minutes with time. In addition,
  we found that the amplitude of the excited oscillations was twice the
  amplitude of oscillations before the brightening. Based on our results,
  we propose that magnetic reconnection occurring in an LB can excite
  oscillations in the nearby sunspot umbra.

---------------------------------------------------------
Title: Contribution to the Solar Mean Magnetic Field from Different
    Solar Regions
Authors: Kutsenko, A. S.; Abramenko, V. I.; Yurchyshyn, V. B.
2017SoPh..292..121K    Altcode: 2017arXiv170705971K
  Seven-year-long seeing-free observations of solar magnetic fields
  with the Helioseismic and Magnetic Imager (HMI) on board the Solar
  Dynamics Observatory (SDO) were used to study the sources of the solar
  mean magnetic field, SMMF, defined as the net line-of-sight magnetic
  flux divided over the solar disk area. To evaluate the contribution
  of different regions to the SMMF, we separated all the pixels of
  each SDO/HMI magnetogram into three subsets: weak (B<SUP>W</SUP>),
  intermediate (B<SUP>I</SUP>), and strong (B<SUP>S</SUP>) fields. The
  B<SUP>W</SUP> component represents areas with magnetic flux densities
  below the chosen threshold; the B<SUP>I</SUP> component is mainly
  represented by network fields, remains of decayed active regions (ARs),
  and ephemeral regions. The B<SUP>S</SUP> component consists of magnetic
  elements in ARs. To derive the contribution of a subset to the total
  SMMF, the linear regression coefficients between the corresponding
  component and the SMMF were calculated. We found that i) when the
  threshold level of 30 Mx cm<SUP>−2</SUP> is applied, the B<SUP>I</SUP>
  and B<SUP>S</SUP> components together contribute from 65% to 95% of the
  SMMF, while the fraction of the occupied area varies in a range of 2 -
  6% of the disk area; ii) as the threshold magnitude is lowered to 6 Mx
  cm<SUP>−2</SUP>, the contribution from B<SUP>I</SUP>+B<SUP>S</SUP>
  grows to 98%, and the fraction of the occupied area reaches a value
  of about 40% of the solar disk. In summary, we found that regardless
  of the threshold level, only a small part of the solar disk area
  contributes to the SMMF. This means that the photospheric magnetic
  structure is an intermittent inherently porous medium, resembling a
  percolation cluster. These findings suggest that the long-standing
  concept that continuous vast unipolar areas on the solar surface are
  the source of the SMMF may need to be reconsidered.

---------------------------------------------------------
Title: Multi-wavelength Observation of M-class Flare associated with
    Filament eruption
Authors: Kim, Sujin; Yurchyshyn, Vasyl B.; Jiang, Chaowei; Cho,
   Kyung-Suk
2017SPD....4810822K    Altcode:
  We have investigated a M-class flare associated with filament eruption
  which developed into a Halo CME. The M-class flare occurred in 2011
  August 4. For this study, we used the Nobryama Radioheliograph (NoRH)
  17 and 34 GHz, RHESSI Hard X-ray satellite, and Atmo- spheric Imaging
  Assembly (AIA) and the Heliospheric Magentic Imager(HMI) onboard the
  Solar Dynamic Observatory (SDO). During the pre-eruption phase, clear
  nonthermal emission was detected in microwaves of NoRH and hard-X-ray
  of RHESSI. At the moment that the nonthermal emission start, the
  nonthermal sources appeared at the one edge of the filament structure on
  a polarity inversion line, and the slowing rising filament structure in
  AIA 94A underwent a sudden acceleration on its ascendance. Magnetograms
  showed converging motion of magnetic elements at the source position
  of HXR and MW. Based on the results, we conjecture that the plausible
  trigger of the filament eruption is magnetic reconnections at the HXR
  source position by converging motion of magnetic elements. In addition,
  we will discuss on the magnetic flux variation before and after the
  eruption based on the result of Nonlinear force-free field model.

---------------------------------------------------------
Title: The NST observation of a small loop eruption in He I D3 line
    on 2016 May 30
Authors: Kim, Yeon-Han; Xu, Yan; Bong, Su-Chan; Lim, Eunkyung; Yang,
   Heesu; Park, Young-Deuk; Yurchyshyn, Vasyl B.; Ahn, Kwangsu; Goode,
   Philip R.
2017SPD....4810505K    Altcode:
  Since the He I D3 line has a unique response to a flare impact on the
  low solar atmosphere, it can be a powerful diagnostic tool for energy
  transport processes. In order to obtain comprehensive data sets for
  studying solar flare activities in D3 spectral line, we performed
  observations for several days using the 1.6m New Solar Telescope of
  Big Bear Solar Observatory (BBSO) in 2015 and 2016, equipped with
  the He I D3 filter, the photospheric broadband filter, and Near IR
  imaging spectrograph (NIRIS). On 2016 May 30, we observed a small
  loop eruption in He I D3 images associated with a B class brightening,
  which is occurred around 17:10 UT in a small active region, and dynamic
  variations of photospheric features in G-band images. Accordingly,
  the cause of the loop eruption can be magnetic reconnection driven by
  photospheric plasma motions. In this presentation, we will give the
  observation results and the interpretation.

---------------------------------------------------------
Title: Multiwavelength observations of a flux rope formation by
    series of magnetic reconnection in the chromosphere
Authors: Kumar, Pankaj; Yurchyshyn, Vasyl; Cho, Kyung-Suk; Wang, Haimin
2017A&A...603A..36K    Altcode: 2017arXiv170309871K
  Using high-resolution observations from the 1.6 m New Solar Telescope
  (NST) operating at the Big Bear Solar Observatory (BBSO), we report
  direct evidence of merging and reconnection of cool Hα loops in the
  chromosphere during two homologous flares (B and C class) caused by a
  shear motion at the footpoints of two loops. The reconnection between
  these loops caused the formation of an unstable flux rope that showed
  counterclockwise rotation. The flux rope could not reach the height of
  torus instability and failed to form a coronal mass ejection. The HMI
  magnetograms revealed rotation of the negative and positive (N1/P2)
  polarity sunspots in the opposite directions, which increased the
  right- and left-handed twist in the magnetic structures rooted at
  N1/P2. Rapid photospheric flux cancellation (duration 20-30 min,
  rate ≈3.44 × 10<SUP>20</SUP> Mx h<SUP>-1</SUP>) was observed
  during and even after the first B6.0 flare and continued until
  the end of the second C2.3 flare. The RHESSI X-ray sources were
  located at the site of the loop coalescence. To the best of our
  knowledge, such a clear interaction of chromospheric loops along
  with rapid flux cancellation has not been reported before. These
  high-resolution observations suggest the formation of a small flux
  rope by a series of magnetic reconnections within chromospheric
  loops that are associated with very rapid flux cancellation. <P
  />Movies attached to Figs. 2, 7, 8, and 10 are available at <A
  href="http://www.aanda.org/10.1051/0004-6361/201629295/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: Analysis of the Flux Growth Rate in Emerging Active Regions
    on the Sun
Authors: Abramenko, V. I.; Kutsenko, A. S.; Tikhonova, O. I.;
   Yurchyshyn, V. B.
2017SoPh..292...48A    Altcode: 2017arXiv170300739A
  We studied the emergence process of 42 active regions (ARs) by analyzing
  the time derivative, R (t ), of the total unsigned flux. Line-of-sight
  magnetograms acquired by the Helioseismic and Magnetic Imager (HMI)
  onboard the Solar Dynamics Observatory (SDO) were used. A continuous
  piecewise linear fitting to the R (t )-profile was applied to detect
  an interval, Δ t<SUB>2</SUB>, of nearly constant R (t ) covering
  one or several local maxima. The magnitude of R (t ) averaged over Δ
  t<SUB>2</SUB> was accepted as an estimate of the maximum value of the
  flux growth rate, R<SUB>MAX</SUB>, which varies in a range of (0.5 -5
  )×10<SUP>20</SUP>Mxhour−<SUP>1</SUP> for ARs with a maximum total
  unsigned flux of (0.5 -3 )×10<SUP>22</SUP>Mx. The normalized flux
  growth rate, R<SUB>N</SUB>, was defined under the assumption that the
  saturated total unsigned flux, F<SUB>MAX</SUB>, equals unity. Out of 42
  ARs in our initial list, 36 events were successfully fitted, and they
  form two subsets (with a small overlap of eight events): the ARs with
  a short (&lt;13 hours) interval Δ t<SUB>2</SUB> and a high (&gt;0.024
  hour−<SUP>1</SUP>) normalized flux emergence rate, R<SUB>N</SUB>,
  form the "rapid" emergence event subset. The second subset consists of
  "gradual" emergence events, and it is characterized by a long (&gt;13
  hours) interval Δ t<SUB>2</SUB> and a low R<SUB>N</SUB> (&lt;0.024
  hour−<SUP>1</SUP>). In diagrams of R<SUB>MAX</SUB> plotted versus
  F<SUB>MAX</SUB>, the events from different subsets do not overlap,
  and each subset displays an individual power law. The power-law index
  derived from the entire ensemble of 36 events is 0.69 ±0.10 . The
  rapid emergence is consistent with a two-step emergence process of a
  single twisted flux tube. The gradual emergence is possibly related
  to a consecutive rising of several flux tubes emerging at nearly the
  same location in the photosphere.

---------------------------------------------------------
Title: Impact of the Icme-Earth Geometry on the Strength of the
Associated Geomagnetic Storm: The September 2014 and March 2015 Events
Authors: Cho, K. S.; Marubashi, K.; Kim, R. S.; Park, S. H.; Lim,
   E. K.; Kim, S. J.; Kumar, P.; Yurchyshyn, V.; Moon, Y. J.; Lee, J. O.
2017JKAS...50...29C    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: High-resolution Observations of a White-light Flare with NST
Authors: Yurchyshyn, V.; Kumar, P.; Abramenko, V.; Xu, Y.; Goode,
   P. R.; Cho, K. -S.; Lim, E. -K.
2017ApJ...838...32Y    Altcode:
  Using high-resolution data from the New Solar Telescope, we studied
  fine spatial and temporal details of an M1.3 white-light (WL) flare,
  which was one of three homologous solar flares (C6.8, M1.3, and M2.3)
  observed in close proximity to the west solar limb on 2014 October 29
  in NOAA active region 12192. We report that the TiO WL flare consists of
  compact and intense cores surrounded by less intense spatial halos. The
  strong and compact WL cores were measured to be ≈ 0.2 Mm across,
  with an area of about 10<SUP>14</SUP> cm<SUP>2</SUP>. Several TiO
  features were not cospatial with Hα flare ribbons and were displaced
  toward the disk center by about 500 km, which suggests that the TiO
  and Hα radiation probably did not originate in the same chromospheric
  volume. The observed TiO intensity enhancements are not normally
  distributed and are structured by the magnetic field of the penumbra.

---------------------------------------------------------
Title: Photospheric Origin of Three-minute Oscillations in a Sunspot
Authors: Chae, Jongchul; Lee, Jeongwoo; Cho, Kyuhyoun; Song, Donguk;
   Cho, Kyungsuk; Yurchyshyn, Vasyl
2017ApJ...836...18C    Altcode:
  The origin of the three-minute oscillations of intensity and velocity
  observed in the chromosphere of sunspot umbrae is still unclear. We
  investigated the spatio-spectral properties of the 3 minute oscillations
  of velocity in the photosphere of a sunspot umbra as well as those
  in the low chromosphere using the spectral data of the Ni I λ5436,
  Fe I λ5435, and Na I D<SUB>2</SUB> λ5890 lines taken by the Fast
  Imaging Solar Spectrograph of the 1.6 m New Solar Telescope at the Big
  Bear Solar Observatory. As a result, we found a local enhancement of
  the 3 minute oscillation power in the vicinities of a light bridge
  (LB) and numerous umbral dots (UDs) in the photosphere. These
  3 minute oscillations occurred independently of the 5 minute
  oscillations. Through wavelet analysis, we determined the amplitudes
  and phases of the 3 minute oscillations at the formation heights of the
  spectral lines, and they were found to be consistent with the upwardly
  propagating slow magnetoacoustic waves in the photosphere with energy
  flux large enough to explain the chromospheric oscillations. Our results
  suggest that the 3 minute chromospheric oscillations in this sunspot may
  have been generated by magnetoconvection occurring in the LB and UDs.

---------------------------------------------------------
Title: Flare-production potential associated with different sunspot
    groups
Authors: Eren, S.; Kilcik, A.; Atay, T.; Miteva, R.; Yurchyshyn, V.;
   Rozelot, J. P.; Ozguc, A.
2017MNRAS.465...68E    Altcode:
  In this study, we analysed different types (C, M, and X classes)
  of X-ray solar flares occurring in sunspot groups. The data cover
  1996-2014 time interval, and a total of 4262 active regions (ARs)
  were included in the data set. We defined the solar-flare-production
  potential as the ratio of the total number of flares observed in a
  sunspot group to the total number of the same-class sunspot groups. Our
  main findings are as follows: (1) large and complex sunspot groups
  (D+E+F) have the flare-production potential about eight times higher
  than the small and simple (A+B+C+H) ARs; (2) 79 per cent of all flares
  were produced by the large and complex sunspot groups, while only 21 per
  cent of flares were produced by the small groups; (3) the largest and
  the most complex F-class (very large and very complex) sunspot groups
  exhibit the highest flare-production potential (2.16 flare per sunspot
  group), while the smallest and the least complex A class sunspot groups
  show the lowest (0.05 flare per group) flare-production potential;
  (4) temporal variation of sunspot counts, sunspot group areas, and the
  total number of flares (including C flares) showed similar time profiles
  during both cycles with multiple peaks; (5) the mean area of ARs very
  well describes the flare-production potential of each group with the
  regression coefficient of &lt;italic&gt;R<SUP>2</SUP>&lt;/italic&gt;
  = 0.99. Most of these sunspot groups (&gt;70 per cent) are, according
  to the Zurich Classification, complex ARs.

---------------------------------------------------------
Title: Chromospheric Plasma Ejections in a Light Bridge of a Sunspot
Authors: Song, Donguk; Chae, Jongchul; Yurchyshyn, Vasyl; Lim,
   Eun-Kyung; Cho, Kyung-Suk; Yang, Heesu; Cho, Kyuhyoun; Kwak, Hannah
2017ApJ...835..240S    Altcode: 2017arXiv170106808S
  It is well-known that light bridges (LBs) inside a sunspot produce
  small-scale plasma ejections and transient brightenings in the
  chromosphere, but the nature and origin of such phenomena are still
  unclear. Utilizing the high-spatial and high-temporal resolution
  spectral data taken with the Fast Imaging Solar Spectrograph
  and the TiO 7057 Å broadband filter images installed at the 1.6
  m New Solar Telescope of Big Bear Solar Observatory, we report
  arcsecond-scale chromospheric plasma ejections (1.″7) inside a
  LB. Interestingly, the ejections are found to be a manifestation of
  upwardly propagating shock waves as evidenced by the sawtooth patterns
  seen in the temporal-spectral plots of the Ca II 8542 Å and Hα
  intensities. We also found a fine-scale photospheric pattern (1″)
  diverging with a speed of about 2 km s<SUP>-1</SUP> two minutes before
  the plasma ejections, which seems to be a manifestation of magnetic
  flux emergence. As a response to the plasma ejections, the corona
  displayed small-scale transient brightenings. Based on our findings,
  we suggest that the shock waves can be excited by the local disturbance
  caused by magnetic reconnection between the emerging flux inside the
  LB and the adjacent umbral magnetic field. The disturbance generates
  slow-mode waves, which soon develop into shock waves, and manifest
  themselves as the arcsecond-scale plasma ejections. It also appears
  that the dissipation of mechanical energy in the shock waves can heat
  the local corona.

---------------------------------------------------------
Title: Solar and Geomagnetic Activity Relation for the Last two
    Solar Cycles
Authors: Kilcik, A.; Yiǧit, E.; Yurchyshyn, V.; Ozguc, A.; Rozelot,
   J. P.
2017SunGe..12...31K    Altcode:
  The long-term relationship between solar (sunspot counts in different
  Zurich sunspot groups, International Sunspot Number (ISSN), solar wind,
  and X-Ray solar flare index and geomagnetic indices (Ap and Dst)
  is investigated. Data sets used in this study cover a time period
  from January 1996 to March 2014. Our main findings are as follows: 1)
  The best correlation between the sunspot counts and the Ap index are
  obtained for the large group time series, while the other categories
  exhibited lower (final and medium) or no correlation at all (small). It
  is interesting to note that Ap index is delayed by about 13 months
  relatively to all sunspot count series and ISSN data. 2) The best
  correlation between the sunspot counts and the Dst index was as well
  obtained for the large AR time series. The Dst index delays with respect
  to the large group by about 2 months. 3) The highest correlation between
  the solar and geomagnetic indices were obtained between the solar wind
  speed and Ap and Dst indices with zero time delays (r = 0.76, r = 0.52,
  respectively). 4) The correlation coefficients between the geomagnetic
  indices (Ap, Dst) and X-Ray solar flare index (r = 0.59, r = -0.48,
  respectively) are a little higher than the correlation coefficients
  between these geomagnetic indices and ISSN (r = 0.57, r = -0.43,
  respectively). 5) The magnitude of all solar and geomagnetic indices
  (except the solar wind speed) has significantly decreased during the
  current solar cycle as compared to the same phase of the previous cycle.

---------------------------------------------------------
Title: Pre-eruption Oscillations in Thin and Long Features in a
    Quiescent Filament
Authors: Joshi, Anand D.; Hanaoka, Yoichiro; Suematsu, Yoshinori;
   Morita, Satoshi; Yurchyshyn, Vasyl; Cho, Kyung-Suk
2016ApJ...833..243J    Altcode: 2016arXiv161204917J
  We investigate the eruption of a quiescent filament located close to
  an active region. Large-scale activation was observed in only half of
  the filament in the form of pre-eruption oscillations. Consequently
  only this half erupted nearly 30 hr after the oscillations
  commenced. Time-slice diagrams of 171 Å images from the Atmospheric
  Imaging Assembly were used to study the oscillations. These were
  observed in several thin and long features connecting the filament
  spine to the chromosphere below. This study traces the origin of
  such features and proposes their possible interpretation. Small-scale
  magnetic flux cancellation accompanied by a brightening was observed
  at the footpoint of the features shortly before their appearance, in
  images recorded by the Helioseismic and Magnetic Imager. A slow rise of
  the filament was detected in addition to the oscillations, indicating
  a gradual loss of equilibrium. Our analysis indicates that a change in
  magnetic field connectivity between two neighbouring active regions
  and the quiescent filament resulted in a weakening of the overlying
  arcade of the filament, leading to its eruption. It is also suggested
  that the oscillating features are filament barbs, and the oscillations
  are a manifestation during the pre-eruption phase of the filaments.

---------------------------------------------------------
Title: Sub-Pixel Magnetic Field Dynamics Derived from Photospheric
    Spectral Line Profiles
Authors: Rasca, A.; Chen, J.; Pevtsov, A. A.; Yurchyshyn, V.;
   Bertello, L.
2016AGUFMSH13C2308R    Altcode:
  Current high-resolution observations of the photosphere show
  small dynamic features at the resolving limit during emerging flux
  events. However, line-of-sight (LOS) magnetogram pixels only contain
  the net uncanceled magnetic flux, which is expected to increase
  for fixed regions as resolution limits improve. Using a new method
  with spectrographic images, we quantify distortions in photospheric
  absorption (or emission) lines caused by sub-pixel magnetic field and
  plasma dynamics in the vicinity of active regions and emerging flux
  events. Absorption lines—quantified by their displacement, width,
  asymmetry, and peakedness—have previously been used with Stokes
  I images from SOLIS/VSM to relate line distortions with sub-pixel
  plasma dynamics driven by solar flares or small-scale flux ropes. The
  method is extended to include the full Stokes parameters and relate
  inferred sub-pixel dynamics with small-scale magnetic fields. Our
  analysis is performed on several sets of spectrographic images taken
  by SOLIS/VSM and NST/NIRIS while observing eruptive and non-eruptive
  active regions. We discuss the results of this application and their
  relevance for understanding magnetic fields signatures and coupled
  plasma properties on sub-pixel scales.

---------------------------------------------------------
Title: How did a Major Confined Flare Occur in Super Solar Active
    Region 12192?
Authors: Jiang, C.; Wu, S. T.; Yurchyshyn, V.; Wang, H.; Feng, X. S.;
   Hu, Q.
2016AGUFMSH12B..04J    Altcode:
  We study the physical mechanism of a major X-class solar flare
  that occurred in the super NOAA active region (AR) 12192 using a
  data-driven numerical magnetohydrodynamic (MHD) modeling complemented
  with observations. With the evolving magnetic fields observed at the
  solar surface as bottom boundary input, we drive an MHD system to
  evolve self-consistently in correspondence with the realistic coronal
  evolution. During a two-day time interval, the modeled coronal field
  has been slowly stressed by the photospheric field evolution,which
  gradually created a large-scale coronal current sheet, i.e., a narrow
  layer with intense current, in the core of the AR. The current layer
  was successively enhanced until it became so thin that a tether-cutting
  reconnection between the sheared magnetic arcades was set in, which led
  to a flare. The modeled reconnecting field lines and their footpoints
  match well the observed hot flaring loops and the flare ribbons,
  respectively, suggesting that the model has successfully "reproduced"
  the macroscopic magnetic process of the flare. In particular, with
  simulation, we explained why this event is a confined eruption-the
  consequent of the reconnection is the shared arcade instead of a newly
  formed flux rope. We also found much weaker magnetic implosion effect
  comparing to many other X-class flares.

---------------------------------------------------------
Title: Pre-Eruption Oscillations in Quiescent Filament Observed in
    AIA 171 Å
Authors: Joshi, Anand D.; Yurchyshyn, Vasyl; Cho, Kyung-Suk
2016usc..confE..62J    Altcode:
  A large quiescent filament located near the south-west limb of the
  Sun underwent an eruption on 14 August 2013. Shortly before the
  eruption two flares occur in NOAA Active Region (AR) 11817, located
  near the filament. The temporal and spatial proximity suggests that
  the flares caused the filament to erupt. However, there is no extreme
  ultraviolet (EUV) wave or ejection which seemed to cause this. We use
  171 Å images for over two days before the eruption from Atmospheric
  Imaging Assembly (AIA) on board Solar Dynamics Observatory (SDO) to
  investigate this event. We observe oscillations in the western portion
  of the quiescent filament almost 40 hours prior to eruption, but not
  so much in the eastern portion. For several hours prior to eruption,
  the western portion is seen to undergo a slow rise. Subsequently, it
  is this western portion which erupts, while the eastern portion does
  not. We also use Helioseismic and Magnetic Imager (HMI) to study changes
  in the active region, and find that along with a continuous emergence
  of magnetic flux in the region, there was also a migration of polarity
  producing a large shear. We make use of the hmi.sharp to determine shear
  in the active region. We suggest that the oscillations are a result of
  natural perturbation, and the flares acted as a destabilising factor
  which resulted in the eruption.

---------------------------------------------------------
Title: Multi-wavelength Study of Transition Region Penumbral
    Subarcsecond Bright Dots Using IRIS and NST
Authors: Deng, Na; Yurchyshyn, Vasyl; Tian, Hui; Kleint, Lucia; Liu,
   Chang; Xu, Yan; Wang, Haimin
2016ApJ...829..103D    Altcode: 2016arXiv160700306D
  Using high-resolution transition region (TR) observations taken by
  the Interface Region Imaging Spectrograph (IRIS) mission, Tian et
  al. revealed numerous short-lived subarcsecond bright dots (BDs)
  above sunspots (mostly located in the penumbrae), which indicate yet
  unexplained small-scale energy releases. Moreover, whether or not
  these subarcsecond TR brightenings have any signature in the lower
  atmosphere and how they are formed are still not fully resolved. This
  paper presents a multi-wavelength study of the TR penumbral BDs using a
  coordinated observation of a near disk center sunspot with IRIS and the
  1.6 m New Solar Telescope (NST) at the Big Bear Solar Observatory. NST
  provides high-resolution chromospheric and photospheric observations
  with narrowband Hα imaging spectroscopy and broadband TiO images,
  respectively, complementary to IRIS TR observations. A total of 2692
  TR penumbral BDs are identified from a 37 minute time series of IRIS
  1400 Å slit-jaw images. Their locations tend to be associated more
  with downflowing and darker fibrils in the chromosphere, and weakly
  associated with bright penumbral features in the photosphere. However,
  temporal evolution analyses of the BDs show that there is no consistent
  and convincing brightening response in the chromosphere. These results
  are compatible with a formation mechanism of the TR penumbral BDs
  by falling plasma from coronal heights along more vertical and dense
  magnetic loops. The BDs may also be produced by small-scale impulsive
  magnetic reconnection taking place sufficiently high in the atmosphere
  that has no energy release in the chromosphere.

---------------------------------------------------------
Title: Fine-scale Photospheric Connections of Ellerman Bombs
Authors: Yang, Heesu; Chae, Jongchul; Lim, Eun-Kyung; Song, Donguk;
   Cho, Kyuhyoun; Kwak, Hannah; Yurchyshyn, Vasyl B.; Kim, Yeon-Han
2016ApJ...829..100Y    Altcode:
  We investigate the photospheric and magnetic field structures
  associated with Ellerman bombs (EBs) using the 1.6 m New Solar
  Telescope at Big Bear Solar Observatory. The nine observed EBs were
  accompanied by elongated granule-like features (EGFs) that showed
  transverse motions prior to the EBs with an average speed of about
  3.8 km s<SUP>-1</SUP>. Each EGF consisted of a sub-arcsecond bright
  core encircled by a dark lane around its moving front. The bright
  core appeared in the TiO broadband filter images and in the far wings
  of the Hα and Ca II 8542 Å lines. In four EBs, the bi-directional
  expanding motion of the EGFs was identified in the TiO images. In
  those cases, the EGFs were found to be accompanied by an emerging flux
  (EF). In four other EBs, the EGF developed at the edge of a penumbra and
  traveled in the sunspot’s radial direction. The EGFs in these cases
  were identified as a moving magnetic feature (MMF). Our results show a
  clear connection among the magnetic elements, photospheric features, and
  EBs. This result suggests that the EBs result from magnetic reconnection
  forced by EFs or MMFs that are frequently manifested by EGFs.

---------------------------------------------------------
Title: How Did a Major Confined Flare Occur in Super Solar Active
    Region 12192?
Authors: Jiang, Chaowei; Wu, S. T.; Yurchyshyn, Vasyl; Wang, Haiming;
   Feng, Xueshang; Hu, Qiang
2016ApJ...828...62J    Altcode: 2016arXiv160609334J
  We study the physical mechanism of a major X-class solar flare
  that occurred in the super NOAA active region (AR) 12192 using
  data-driven numerical magnetohydrodynamic (MHD) modeling complemented
  with observations. With the evolving magnetic fields observed at
  the solar surface as bottom boundary input, we drive an MHD system
  to evolve self-consistently in correspondence with the realistic
  coronal evolution. During a two-day time interval, the modeled coronal
  field has been slowly stressed by the photospheric field evolution,
  which gradually created a large-scale coronal current sheet, I.e.,
  a narrow layer with intense current, in the core of the AR. The
  current layer was successively enhanced until it became so thin that
  a tether-cutting reconnection between the sheared magnetic arcades
  was set in, which led to a flare. The modeled reconnecting field
  lines and their footpoints match well the observed hot flaring loops
  and the flare ribbons, respectively, suggesting that the model has
  successfully “reproduced” the macroscopic magnetic process of the
  flare. In particular, with simulation, we explained why this event is
  a confined eruption—the consequence of the reconnection is a shared
  arcade instead of a newly formed flux rope. We also found a much weaker
  magnetic implosion effect compared to many other X-class flares.

---------------------------------------------------------
Title: Ionospheric criticial frequencies and solar cycle effects
Authors: Kilcik, Ali; Ozguc, Atila; Rozelot, Jean Pierre; Yiǧit,
   Erdal; Elias, Ana; Donmez, Burcin; Yurchyshyn, Vasyl
2016cosp...41E.996K    Altcode:
  The long term solar activity dependencies of ionospheric F1 and
  F2 regions critical frequencies (foF1 and foF2) are investigated
  observationally for the last four solar cycles (1976-2015). We here
  show that the ionospheric F1 and F2 regions have different solar
  activity dependencies in terms of the sunspot group (SG) numbers:
  F1 region critical frequency (foF1) peaks at the same time with small
  SG numbers, while the foF2 reaches its maximum at the same time with
  the large SG numbers especially during the solar cycle 23. Thus, we
  may conclude that the sensitivities of ionospheric F1 and F2 region
  critical frequencies to sunspot group (SG) numbers are associated
  with different physical processes that are yet to be investigated
  in detail. Such new results provide further evidence that the two
  ionospheric regions have different responses to the solar activity. We
  also analyzed short term oscillatory behavior of ionospheric critical
  frequencies and found some solar signatures.

---------------------------------------------------------
Title: Temporal Variation of Different Categories Sunspot Groups
since 1996: Their Relation with Geomagnetic Ap and Dst Indices
Authors: Kilcik, Ali; Ozguc, Atila; Rozelot, Jean Pierre; Donmez,
   Burcin; Yurchyshyn, Vasyl
2016cosp...41E.995K    Altcode:
  We studied the temporal variation of the number of sunspot groups and
  sunspot counts in these groups in four categories as small (A, B),
  medium (C), large (D, E, F) and final (H modified Zurich classes)
  since 1996. Then we compared these data sets with geomagnetic Ap
  and Dst indices. In results of our analysis we found followings: 1)
  different categories sunspot groups and sunspot counts in these groups
  behave differently during a solar cycle. ii) Response of geomagnetic
  indices to these data sets are also different.

---------------------------------------------------------
Title: Multi-wavelength Study of Transition Region Penumbral
    Bright Dots Using Interface Region Imaging Spectrograph and New
    Solar Telescope
Authors: Deng, Na; Yurchyshyn, Vasyl B.; Tian, Hui; Kleint, Lucia;
   Liu, Chang; Xu, Yan; Wang, Haimin
2016SPD....47.0101D    Altcode:
  Using high-resolution transition region (TR) observations taken by
  the Interface Region Imaging Spectrograph (IRIS) mission, Tian et
  al. (2014b) revealed numerous short-lived sub-arcsecond bright dots
  above sunspots (mostly located in the penumbrae), which indicate yet
  unexplained small-scale energy releases. Moreover, whether these TR
  brightenings have any signature in the lower atmosphere and how they
  are formed are still not fully resolved. This paper presents a study of
  these bright dots using a coordinated observation of a near disk-center
  sunspot with IRIS and the 1.6 m New Solar Telescope (NST) at the Big
  Bear Solar Observatory. NST provides high-resolution chromospheric
  and photospheric observations with narrow-band H-alpha imaging
  spectroscopy and broad-band TiO images, respectively, complementary
  to IRIS TR observations. A total of 2692 TR penumbral bright dots
  are identified from a 37-minute time series of IRIS 1400 A slitjaw
  images. Their locations tend to be associated more with downflowing and
  darker fibrils in the chromosphere, and weakly associated with bright
  penumbral features in the photosphere. However, temporal evolution
  analyses of the dots show that there is no consistent and convincing
  brightening response in the chromosphere. These results are compatible
  with a formation mechanism of the TR penumbral bright dots by falling
  plasma from coronal heights along more vertical and dense magnetic
  loops. The dots may also be produced by small-scale impulsive magnetic
  reconnection taking place sufficiently high in the atmosphere that
  has no energy release in the chromosphere.Acknowledgement: This work
  is mainly supported by NASA grants NNX14AC12G, NNX13AF76G and by NSF
  grant AGS 1408703.

---------------------------------------------------------
Title: Active Latitude Oscillations Observed on the Sun
Authors: Kilcik, A.; Yurchyshyn, V.; Clette, F.; Ozguc, A.; Rozelot,
   J. -P.
2016SoPh..291.1077K    Altcode: 2016SoPh..tmp...62K; 2016arXiv160400831K
  We investigate periodicities in the mean heliographic latitudes of
  sunspot groups, called active latitudes, for the past six complete
  solar cycles (1945 - 2008). For this purpose, the multitaper method
  and Morlet wavelet analysis were used. We found that solar rotation
  periodicities (26 - 38 days) are present in active latitudes of both
  hemispheres for all the investigated cycles (18 to 23). Both in the
  northern and southern hemispheres, active latitudes drifted toward the
  equator from the beginning to the end of each cycle and followed an
  oscillating path. These motions are well described by a second-order
  polynomial. There are no meaningful periods of between 55 and about
  300 days in either hemisphere for all cycles. A periodicity of 300
  to 370 days appears in both hemispheres for Cycle 23, in the northern
  hemisphere for Cycle 20, and in the southern hemisphere for Cycle 18.

---------------------------------------------------------
Title: Observations of a Series of Flares and Associated Jet-like
    Eruptions Driven by the Emergence of Twisted Magnetic Fields
Authors: Lim, Eun-Kyung; Yurchyshyn, Vasyl; Park, Sung-Hong; Kim,
   Sujin; Cho, Kyung-Suk; Kumar, Pankaj; Chae, Jongchul; Yang, Heesu;
   Cho, Kyuhyoun; Song, Donguk; Kim, Yeon-Han
2016ApJ...817...39L    Altcode: 2015arXiv151201330L
  We studied temporal changes of morphological and magnetic properties
  of a succession of four confined flares followed by an eruptive flare
  using the high-resolution New Solar Telescope (NST) operating at the Big
  Bear Solar Observatory (BBSO) and Helioseismic and Magnetic Imager (HMI)
  magnetograms and Atmospheric Image Assembly (AIA) EUV images provided by
  the Solar Dynamics Observatory (SDO). From the NST/Hα and the SDO/AIA
  304 Å observations we found that each flare developed a jet structure
  that evolved in a manner similar to evolution of the blowout jet: (1)
  an inverted-Y-shaped jet appeared and drifted away from its initial
  position; (2) jets formed a curtain-like structure that consisted
  of many fine threads accompanied by subsequent brightenings near
  the footpoints of the fine threads; and finally, (3) the jet showed
  a twisted structure visible near the flare maximum. Analysis of the
  HMI data showed that both the negative magnetic flux and the magnetic
  helicity have been gradually increasing in the positive-polarity region,
  indicating the continuous injection of magnetic twist before and during
  the series of flares. Based on these results, we suggest that the
  continuous emergence of twisted magnetic flux played an important role
  in producing successive flares and developing a series of blowout jets.

---------------------------------------------------------
Title: Multiwavelength Observations of a Slow Raise, Multi-Step X1.6
    Flare and the Associated Eruption
Authors: Yurchyshyn, V.
2015AGUFMSH21C..04Y    Altcode:
  Using multi-wavelength observations we studied a slow rise, multi-step
  X1.6 flare that began on November 7, 2014 as a localized eruption of
  core fields inside a δ-sunspot and later engulfed the entire active
  region. This flare event was associated with formation of two systems
  of post eruption arcades (PEAs) and several J-shaped flare ribbons
  showing extremely fine details, irreversible changes in the photospheric
  magnetic fields, and it was accompanied by a fast and wide coronal mass
  ejection. Data from the Solar Dynamics Observatory, IRIS spacecraft
  along with the ground based data from the New Solar Telescope (NST)
  present evidence that i) the flare and the eruption were directly
  triggered by a flux emergence that occurred inside a δ--sunspot at
  the boundary between two umbrae; ii) this event represented an example
  of an in-situ formation of an unstable flux rope observed only in hot
  AIA channels (131 and 94Å) and LASCO C2 coronagraph images; iii)
  the global PEA system spanned the entire AR and was due to global
  scale reconnection occurring at heights of about one solar radii,
  indicating on the global spatial and temporal scale of the eruption.

---------------------------------------------------------
Title: Simultaneous observations of Ellerman bombs by NST and IRIS
Authors: Kim, Y. H.; Yurchyshyn, V.; Cho, I. H.; Lee, J.; Park, Y. D.;
   Yang, H.; Ahn, K.; Goode, P.
2015AGUFMSH31B2413K    Altcode:
  In this study, we present the simultaneous observations of Ellerman
  bombs made by New Solar Telescope (NST) of Big Bear Solar Observatory
  (BBSO) and Interface Region Imaging Spectrograph (IRIS) in space. The
  data obtained during joint NST-IRIS observations on 30 and 31 in July
  2014. We observed two representative events on both days. The first
  one was a relatively weak Ellerman bomb occurred around 19:20 UT on
  30 July 2014. IRIS observed this event by sit-and-stare mode thus we
  analyzed high cadence spectral data and slit-jaw data simultaneously. We
  found that this event was a hot explosion that occurred by magnetic
  reconnection in the lower atmosphere of the Sun. The second event
  was quite strong Ellerman bomb (20:20 UT on 31 July 2014) that is
  well observed by NST FISS (Fast Imaging Solar Spectrograph), while
  there was no IRIS spectral data. We had IRIS slit-jaw data only. The
  Ellerman bomb was clearly coincident with the IRIS brightening at the
  same location. Since the Ellerman bombs are usually believed to occur
  in the photosphere with no coronal emission, it should be explained its
  higher atmospheric emission in IRIS data. We will present the result
  of simultaneous observations by IRIS and NST instruments and discuss
  physical connection between Ellerman bombs and IRIS brightenings.

---------------------------------------------------------
Title: Multiwavelength Observations of a Slow-rise, Multistep X1.6
    Flare and the Associated Eruption
Authors: Yurchyshyn, V.; Kumar, P.; Cho, K. -S.; Lim, E. -K.;
   Abramenko, V. I.
2015ApJ...812..172Y    Altcode:
  Using multiwavelength observations, we studied a slow-rise, multistep
  X1.6 flare that began on 2014 November 7 as a localized eruption of core
  fields inside a δ-sunspot and later engulfed the entire active region
  (AR). This flare event was associated with formation of two systems
  of post-eruption arcades (PEAs) and several J-shaped flare ribbons
  showing extremely fine details, irreversible changes in the photospheric
  magnetic fields, and it was accompanied by a fast and wide coronal mass
  ejection. Data from the Solar Dynamics Observatory and IRIS spacecraft,
  along with the ground-based data from the New Solar Telescope, present
  evidence that (i) the flare and the eruption were directly triggered
  by a flux emergence that occurred inside a δ-sunspot at the boundary
  between two umbrae; (ii) this event represented an example of the
  formation of an unstable flux rope observed only in hot AIA channels
  (131 and 94 Å) and LASCO C2 coronagraph images; (iii) the global
  PEA spanned the entire AR and was due to global-scale reconnection
  occurring at heights of about one solar radius, indicating the global
  spatial and temporal scale of the eruption.

---------------------------------------------------------
Title: Simultaneous observation of a hot explosion by NST and IRIS
Authors: Kim, Yeon-Han; Yurchyshyn, Vasyl; Bong, Su-Chan; Cho, Il-Hyun;
   Cho, Kyung-Suk; Lee, Jaejin; Lim, Eun-Kyung; Park, Young-Deuk; Yang,
   Heesu; Ahn, Kwangsu; Goode, Philip R.; Jang, Bi-Ho
2015ApJ...810...38K    Altcode:
  We present the first simultaneous observations of so-called “hot
  explosions” in the cool atmosphere of the Sun made by the New Solar
  Telescope (NST) of Big Bear Solar Observatory and the Interface Region
  Imaging Spectrograph (IRIS) in space. The data were obtained during
  the joint IRIS-NST observations on 2014 July 30. The explosion of
  interest started around 19:20 UT and lasted for about 10 minutes. Our
  findings are as follows: (1) the IRIS brightening was observed in
  three channels of slit-jaw images, which cover the temperature range
  from 4000 to 80,000 K; (2) during the brightening, the Si iv emission
  profile showed a double-peaked shape with highly blue and redshifted
  components (-40 and 80 km s<SUP>-1</SUP>) (3) wing brightening occurred
  in Hα and Ca ii 8542 Å bands and related surges were observed in both
  bands of the NST Fast Imaging Solar Spectrograph (FISS) instrument;
  (4) the elongated granule, seen in NST TiO data, is clear evidence of
  the emergence of positive flux to trigger the hot explosion; (5) the
  brightening in Solar Dynamics Observatory/Atmospheric Imaging Assembly
  1600 Å images is quite consistent with the IRIS brightening. These
  observations suggest that our event is a hot explosion that occurred
  in the cool atmosphere of the Sun. In addition, our event appeared as
  an Ellerman bomb (EB) in the wing of Hα, although its intensity is
  weak and the vertical extent of the brightening seems to be relatively
  high compared with the typical EBs.

---------------------------------------------------------
Title: Statistical Comparison Between Pores and Sunspots by Using
    SDO/HMI
Authors: Cho, I. -H.; Cho, K. -S.; Bong, S. -C.; Lim, E. -K.; Kim,
   R. -S.; Choi, S.; Kim, Y. -H.; Yurchyshyn, V.
2015ApJ...811...49C    Altcode:
  We carried out an extensive statistical study of the properties of
  pores and sunspots, and investigated the relationship among their
  physical parameters such as size, intensity, magnetic field, and the
  line-of-sight (LOS) velocity in the umbrae. For this, we classified
  9881 samples into three groups of pores, transitional sunspots, and
  mature sunspots. As a result, (1) we find that the total magnetic
  flux inside the umbra of pores, transitional sunspots, and mature
  sunspots increases proportionally to the powers of the area and
  the power indices in the three groups significantly differ from each
  other. (2) The umbral area distribution of each group shows a Gaussian
  distribution and they are clearly separated, displaying three distinct
  peak values. All of the quantities significantly overlap among the three
  groups. (3) The umbral intensity shows a rapid decrease with increasing
  area, and their magnetic field strength shows a rapid increase with
  decreasing intensity. (4) The LOS velocity in pores is predominantly
  redshifted and its magnitude decreases with increasing magnetic field
  strength. The decreasing trend becomes nearly constant with marginal
  blueshift in the case of mature sunspots. The dispersion of LOS
  velocities in mature sunspots is significantly suppressed compared
  to pores. From our results, we conclude that the three groups have
  different characteristics in their area, intensity, magnetic field,
  and LOS velocity as well in their relationships.

---------------------------------------------------------
Title: Formation and Eruption of a Small Flux Rope in the Chromosphere
    Observed by NST, IRIS, and SDO
Authors: Kumar, Pankaj; Yurchyshyn, Vasyl; Wang, Haimin; Cho, Kyung-Suk
2015ApJ...809...83K    Altcode: 2015arXiv150701761K
  Using high-resolution images from the 1.6 m New Solar Telescope
  at Big Bear Solar Observatory, we report the direct evidence of
  chromospheric reconnection at the polarity inversion line between
  two small opposite polarity sunspots. Small jetlike structures
  (with velocities of ∼20-55 km s<SUP>-1</SUP>) were observed at the
  reconnection site before the onset of the first M1.0 flare. The slow
  rise of untwisting jets was followed by the onset of cool plasma inflow
  (∼10 km s<SUP>-1</SUP>) at the reconnection site, causing the onset
  of a two-ribbon flare. The reconnection between two sheared J-shaped
  cool Hα loops causes the formation of a small twisted (S-shaped) flux
  rope in the chromosphere. In addition, Helioseismic and Magnetic Imager
  magnetograms show the flux cancellation (both positive and negative)
  during the first M1.0 flare. The emergence of negative flux and the
  cancellation of positive flux (with shear flows) continue until the
  successful eruption of the flux rope. The newly formed chromospheric
  flux rope becomes unstable and rises slowly with a speed of ∼108 km
  s<SUP>-1</SUP> during a second C8.5 flare that occurred after ∼3
  hr of the first M1.0 flare. The flux rope was destroyed by repeated
  magnetic reconnection induced by its interaction with the ambient field
  (fan-spine topology) and looks like an untwisting surge (∼170 km
  s<SUP>-1</SUP>) in the coronal images recorded by the Solar Dynamics
  Observatory/Atmospheric Imaging Assembly. These observations suggest
  the formation of a chromospheric flux rope (by magnetic reconnection
  associated with flux cancellation) during the first M1.0 flare and
  its subsequent eruption/disruption during the second C8.5 flare.

---------------------------------------------------------
Title: An Ellerman bomb observed by NST and IRIS
Authors: Kim, Yeon-Han; Yurchyshyn, Vasyl; Ahn, Kwangsu; Cho, Il-Hyun;
   Lee, Jaejin; Park, Young-Deuk; Goode, Phillip
2015IAUGA..2257560K    Altcode:
  Recent observations by Interface Region Imaging Spectrograph (IRIS)
  instrument have shown a variety of brightenings around the large-scale
  active region in the solar atmosphere from the photosphere to the
  corona. Interestingly while some brightenings are clearly related to
  Ellerman bombs, some seem to have nothing to do with them. On 2014
  July 31, New Solar Telescope (NST) in Big Bear Solar Observatory (BBSO)
  performed a joint observation with IRIS instrument for the NOAA AR 12127
  from 20:00 UT to 22:00 UT. Around the sunspot several IRIS brightenings
  were observed in 3-channels of slit-jaw images (SJI_2796, SJI_1400,
  and SJI_1330), which can monitor the upper chromosphere and transition
  region. The NST’s Fast Imaging Solar Spectrograph (FISS) observed a
  well-developed Ellerman bomb in the upper right side of the sunspot. The
  Ellerman bomb is clearly coincident with the IRIS brightening at the
  same location. Since the Ellerman bombs are usually believed to occur
  in the photosphere with no coronal emission, it should be explained
  its higher atmospheric emission in IRIS data. We will present the
  result of simultaneous observations by IRIS and NST instruments.

---------------------------------------------------------
Title: Detection of Shock Merging in the Chromosphere of a Solar Pore
Authors: Chae, Jongchul; Song, Donguk; Seo, Minju; Cho, Kyung-Suk;
   Park, Young-Deuk; Yurchyshyn, Vasyl
2015ApJ...805L..21C    Altcode:
  It was theoretically demonstrated that a shock propagating in the solar
  atmosphere can overtake another and merge with it. We provide clear
  observational evidence that shock merging does occur quite often in
  the chromosphere of sunspots. Using Hα imaging spectral data taken by
  the Fast Imaging Solar Spectrograph of the 1.6 m New Solar Telescope
  at the Big Bear Soar Observatory, we construct time-distance maps
  of line-of-sight velocities along two appropriately chosen cuts in
  a pore. The maps show a number of alternating redshift and blueshift
  ridges, and we identify each interface between a preceding redshift
  ridge and the following blueshift ridge as a shock ridge. The important
  finding of ours is that two successive shock ridges often merge with
  each other. This finding can be theoretically explained by the merging
  of magneto-acoustic shock waves propagating with lower speeds of about
  10 km s<SUP>-1</SUP> and those propagating at higher speeds of about
  16-22 km s<SUP>-1</SUP>. The shock merging is an important nonlinear
  dynamical process of the solar chromosphere that can bridge the gap
  between higher-frequency chromospheric oscillations and lower-frequency
  dynamic phenomena such as fibrils.

---------------------------------------------------------
Title: The Chromosphere above the sunspot umbra as seen in the New
    Solar Telescope and Interface Region Imaging Spectrograph
Authors: Yurchyshyn, Vasyl; Goode, Phil; Abramenko, Valentyna;
   Kilcik, Ali
2015TESS....131202Y    Altcode:
  Recent observations of sunspot's umbra suggested that it may be finely
  structured at a sub-arcsecond scale representing a mix of hot and cool
  plasma elements. In this study we report observations from the New Solar
  Telescope (NST) of the umbral spikes, which are cool jet-like structures
  seen in the chromosphere of an umbra. Our analysis indicates that
  the spikes are not associated with photospheric umbral dots and they
  tend to occur above darkest parts of the umbra, where magnetic fields
  are strongest. The spikes exhibit up and down oscillatory motions and
  their spectral evolution suggests that they might be driven by upward
  propagating shocks generated by photospheric oscillations.We analyze
  sunspot oscillations using Interface Region Imaging Spectrograph
  (IRIS) data and narrow-band NST images and found long term variations
  in the intensity of chromospheric shocks. Also, sunspot umbral flashes
  (UFs) appear as narrow bright lanes running along the light bridges
  (LBs) and clusters of umbral dots (UDs). Time series suggested that
  UFs preferred to appear on the sunspot-center side of LBs, which may
  indicate the existence of a compact sub-photospheric driver of sunspot
  oscillations. We find that the sunspot's umbra appears bright in IRIS
  images above LBs and UDs. Co-spatial and co-temporal SDO/AIA data showed
  that these locations were associated with bright footpoints of umbral
  loops suggesting that LBs may play an important role in heating these
  loops. The power spectra analysis showed that the intensity of umbral
  oscillations significantly varies across the umbra and with height,
  suggesting that umbral non-uniformities and the structure of sunspot
  magnetic fields may play a role in wave propagation and heating of
  umbral loops.

---------------------------------------------------------
Title: Intensity and Doppler Velocity Oscillations in Pore Atmospheres
Authors: Cho, K. -S.; Bong, S. -C.; Nakariakov, V. M.; Lim, E. -K.;
   Park, Y. -D.; Chae, J. C.; Yang, H. -S.; Park, H. -M.; Yurchyshyn, V.
2015ApJ...802...45C    Altcode:
  We have investigated chromospheric traveling features running across two
  merged pores from their centers at speeds of about 55 km s<SUP>-1</SUP>,
  in the active region AR 11828. The pores were observed on 2013 August
  24 by using high-time, spatial, and spectral resolution data from the
  Fast Imaging Solar Spectrograph of the 1.6 m New Solar Telescope. We
  infer a line-of-sight (LOS) velocity by applying the lambdameter method
  to the Ca ii 8542 Å band and Hα band, and investigate intensity and
  LOS velocity changes at different wavelengths and different positions
  at the pores. We find that they have three-minute oscillations, and
  the intensity oscillation from the line center (0.0 \overset{\circ}A
  ) is preceded by that from the core (-0.3 \overset{\circ}A ) of the
  bands. There is no phase difference between the intensity and the
  LOS velocity oscillations at a given wavelength. The amplitude of LOS
  velocity from the near core spectra ({Δ }λ =0.10-0.21 \overset{\circ}A
  ) is greater than that from the far core spectra ({Δ }λ =0.24-0.36
  \overset{\circ}A ). These results support the interpretation of the
  observed wave as a slow magnetoacoustic wave propagating along the
  magnetic field lines in the pores. The apparent horizontal motion and
  a sudden decrease of its speed beyond the pores can be explained by
  the projection effect caused by inclination of the magnetic field with
  a canopy structure. We conclude that the observed wave properties of
  the pores are quite similar to those from the sunspot observations.

---------------------------------------------------------
Title: Dynamics in Sunspot Umbra as Seen in New Solar Telescope and
    Interface Region Imaging Spectrograph Data
Authors: Yurchyshyn, V.; Abramenko, V.; Kilcik, A.
2015ApJ...798..136Y    Altcode: 2014arXiv1411.0192Y
  We analyze sunspot oscillations using Interface Region Imaging
  Spectrograph (IRIS) slit-jaw and spectral data and narrow-band
  chromospheric images from the New Solar Telescope (NST) for the main
  sunspot in NOAA AR 11836. We report that the difference between the
  shock arrival times as measured by the Mg II k 2796.35 Å and Si IV
  1393.76 Å line formation levels changes during the observed period,
  and peak-to-peak delays may range from 40 s to zero. The intensity
  of chromospheric shocks also displays long-term (about 20 min)
  variations. NST's high spatial resolution Hα data allowed us to
  conclude that, in this sunspot, umbral flashes (UFs) appeared in the
  form of narrow bright lanes stretched along the light bridges and around
  clusters of umbral bright points. The time series also suggested that
  UFs preferred to appear on the sunspot-center side of light bridges,
  which may indicate the existence of a compact sub-photospheric
  driver of sunspot oscillations. The sunspot's umbra as seen in the
  IRIS chromospheric and transition region data appears bright above
  the locations of light bridges and the areas where the dark umbra
  is dotted with clusters of umbral dots. Co-spatial and co-temporal
  data from the Atmospheric Imaging Assembly on board the Solar Dynamics
  Observatory showed that the same locations were associated with bright
  footpoints of coronal loops suggesting that the light bridges may play
  an important role in heating the coronal sunspot loops. Finally, the
  power spectra analysis showed that the intensity of chromospheric and
  transition region oscillations significantly vary across the umbra and
  with height, suggesting that umbral non-uniformities and the structure
  of sunspot magnetic fields may play a role in wave propagation and
  heating of umbral loops.

---------------------------------------------------------
Title: Kinematics of Solar Chromospheric Surges of AR 10930
Authors: Bong, Su-Chan; Cho, Kyung-Suk; Yurchyshyn, Vasyl
2014JKAS...47..311B    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Sunspot Count Periodicities in Different Zurich Sunspot Group
    Classes Since 1986
Authors: Kilcik, A.; Ozguc, A.; Yurchyshyn, V.; Rozelot, J. P.
2014SoPh..289.4365K    Altcode: 2014arXiv1407.5895K; 2014SoPh..tmp..119K
  We used two methods to investigate the periodic behavior of sunspot
  counts in four categories for the time period January 1986 - October
  2013. These categories include the counts from simple (A and B),
  medium (C), large (D, E, and F), and final (final-stage; H) sunspot
  groups. We used i) the multitaper method with red noise approximation,
  and ii) the Morlet wavelet transform for periodicity analysis. Our
  main findings are that 1) the solar rotation periodicity of about 25
  to 37 days, which is of obvious significance, is found in all groups
  with at least a 95 % significance level; 2) the periodic behavior of
  a cycle is strongly related to its amplitude and group distribution
  during the cycle; 3) the appearance of periods follows the amplitude
  of the investigated solar cycles; and that 4) meaningful periods do
  not appear during the minimum phases of the investigated cycles.

---------------------------------------------------------
Title: Multi-wavelength High-resolution Observations of a Small-scale
    Emerging Magnetic Flux Event and the Chromospheric and Coronal
    Response
Authors: Vargas Domínguez, Santiago; Kosovichev, Alexander;
   Yurchyshyn, Vasyl
2014ApJ...794..140V    Altcode: 2014arXiv1405.3550V
  State-of-the-art solar instrumentation is now revealing magnetic
  activity of the Sun with unprecedented temporal and spatial
  resolutions. Observations with the 1.6 m aperture New Solar Telescope
  (NST) of the Big Bear Solar Observatory are making next steps in our
  understanding of the solar surface structure. Granular-scale magnetic
  flux emergence and the response of the solar atmosphere are among the
  key research topics of high-resolution solar physics. As part of a joint
  observing program with NASA's Interface Region Imaging Spectrograph
  (IRIS) mission on 2013 August 7, the NST observed active region
  NOAA 11,810 in the photospheric TiO 7057 Å band with a resolution
  of pixel size of 0.”034 and chromospheric He I 10830 Å and Hα
  6563 Å wavelengths. Complementary data are provided by the Solar
  Dynamics Observatory (SDO) and Hinode space-based telescopes. The
  region displayed a group of solar pores, in the vicinity of which we
  detect a small-scale buoyant horizontal magnetic flux tube causing
  granular alignments and interacting with the preexisting ambient field
  in the upper atmospheric layers. Following the expansion of distorted
  granules at the emergence site, we observed a sudden appearance of an
  extended surge in the He I 10830 Å data (bandpass of 0.05 Å). The
  IRIS transition region imaging caught ejection of a hot plasma jet
  associated with the He I surge. The SDO/HMI data used to study the
  evolution of the magnetic and Doppler velocity fields reveal emerging
  magnetic loop-like structures. Hinode/Ca II H and IRIS filtergrams
  detail the connectivities of the newly emerged magnetic field in the
  lower solar chromosphere. From these data, we find that the orientation
  of the emerging magnetic field lines from a twisted flux tube formed
  an angle of ~45° with the overlying ambient field. Nevertheless,
  the interaction of emerging magnetic field lines with the pre-existing
  overlying field generates high-temperature emission regions and boosts
  the surge/jet production. The localized heating is detected before
  and after the first signs of the surge/jet ejection. We compare the
  results with previous observations and theoretical models and propose a
  scenario for the activation of plasma jet/surges and confined heating
  triggered by buoyant magnetic flux tubes rising up into a magnetized
  upper environment. Such process may play a significant role in the
  mass and energy flow from the interior to the corona.

---------------------------------------------------------
Title: Solar Cycle 24: Curious Changes in the Relative Numbers of
    Sunspot Group Types
Authors: Kilcik, A.; Yurchyshyn, V. B.; Ozguc, A.; Rozelot, J. P.
2014ApJ...794L...2K    Altcode:
  Here, we analyze different sunspot group (SG) behaviors from the points
  of view of both the sunspot counts (SSCs) and the number of SGs, in
  four categories, for the time period of 1982 January-2014 May. These
  categories include data from simple (A and B), medium (C), large (D,
  E, and F), and decaying (H) SGs. We investigate temporal variations of
  all data sets used in this study and find the following results. (1)
  There is a very significant decrease in the large groups' SSCs and
  the number of SGs in solar cycle 24 (cycle 24) compared to cycles
  21-23. (2) There is no strong variation in the decaying groups' data
  sets for the entire investigated time interval. (3) Medium group data
  show a gradual decrease for the last three cycles. (4) A significant
  decrease occurred in the small groups during solar cycle 23, while no
  strong changes show in the current cycle (cycle 24) compared to the
  previous ones. We confirm that the temporal behavior of all categories
  is quite different from cycle to cycle and it is especially flagrant
  in solar cycle 24. Thus, we argue that the reduced absolute number
  of the large SGs is largely, if not solely, responsible for the weak
  cycle 24. These results might be important for long-term space weather
  predictions to understand the rate of formation of different groups
  of sunspots during a solar cycle and the possible consequences for
  the long-term geomagnetic activity.

---------------------------------------------------------
Title: Sunspot activity for last cycles
Authors: Kilcik, A.; Ozguc, A.; Yurchyshyn, V.; Rozelot, J. P.
2014simi.conf....3K    Altcode:
  Here we analyzed the behavior of different class sunspot groups by
  separating them in different categories for last cycles. In result of
  our analysis, we found that observed sunspot groups behave differently
  for different solar cycles, and each class sunspots have different
  relation with geomagnetic indices. Our main findings are as follows:
  1) All groups behave similarly during the solar cycle 22, while the
  situation is quite different for other cycles (cycle 23 and 24). 2)
  Complex sunspot groups describe the geomagnetic activity better than
  simple groups. 3) The periodic behavior of different group sunspot
  counts show remarkable differences that it may explain the unusual
  behavior of solar cycle 23, and may be the behavior of current cycle.

---------------------------------------------------------
Title: High Resolution Observations of Chromospheric Jets in
    Sunspot Umbra
Authors: Yurchyshyn, Vasyl B.; Abramenko, Valentyna; Kosovichev,
   Alexander G.; Goode, Philip R.
2014AAS...22432301Y    Altcode:
  Recent observations of sunspot's umbra suggested that it may be finely
  structured at a sub-arcsecond scale representing a mix of hot and cool
  plasma elements. In this study we report the first detailed observations
  of the umbral spikes, which are cool jet-like structures seen in the
  chromosphere of an umbra. The spikes are cone-shaped features with
  a typical height of 0.5-1. Mm and a width of about 0. Mm. Their life
  time ranges from 2 to 3 ~min and they tend to re-appear at the same
  location. The preliminary analysis indicates that the spikes are not
  associated with photospheric umbral dots and they rather tend to
  occur above darkest parts of the umbra, where magnetic fields are
  strongest. The spikes exhibit up and down oscillatory motions and
  their spectral evolution suggests that they might be driven by upward
  propagating shocks generated by photospheric oscillations. It is worth
  noting that triggering of the running penumbral waves seems to occur
  during the interval when the spikes reach their maximum height.

---------------------------------------------------------
Title: Photospheric and Chromospheric Dynamics of Sunspots Observed
    with New Solar Telescope
Authors: Kosovichev, Alexander G.; Yurchyshyn, Vasyl B.
2014AAS...22421811K    Altcode:
  The 1.6m New Solar Telescope (NST) of Big Bear Solar Observatory
  allows us to investigate the structure and dynamics of sunspots with
  unprecedented spatial and temporal resolutions. We present results
  of simultaneous observations of a sunspot in the photosphere with a
  broad-band TiO-line filter and in the chromospheric H-alpha line with
  Visible Imaging Spectrometer, and compare the observational results with
  MHD models of sunspots. The observations reveal previously unresolved
  features of the sunspot umbra and penumbra. In particular, the TiO data
  clearly demonstrate highly twisted dynamics of penumbral filaments and
  umbral dots and reveal strong shearing plasma flows in sunspot bridges,
  not explained by the MHD simulations. The high-resolution H-alpha
  spectroscopic data provide new views of the sunspot chromospheric
  dynamics, including the fine structure of oscillations and waves,
  penumbral jets, ubiquitous small-scale eruptions, and accretion
  flows in a form of dense plasma sheets. The diffraction-limited NST
  observations show that the sunspot dynamics is more complicated and
  much richer than it is described by the current sunspot models.

---------------------------------------------------------
Title: High Resolution Observations of Chromospheric Jets in
    Sunspot Umbra
Authors: Yurchyshyn, V.; Abramenko, V.; Kosovichev, A.; Goode, P.
2014ApJ...787...58Y    Altcode: 2014arXiv1404.7444Y
  Recent observations of a sunspot's umbra have suggested that it may
  be finely structured on a subarcsecond scale representing a mix of hot
  and cool plasma elements. In this study, we report the first detailed
  observations of umbral spikes, which are cool jet-like structures seen
  in the chromosphere of an umbra. The spikes are cone-shaped features
  with a typical height of 0.5-1.0 Mm and a width of about 0.1 Mm. Their
  lifetime ranges from 2 to 3 minutes and they tend to re-appear at
  the same location. The spikes are not associated with photospheric
  umbral dots and they instead tend to occur above the darkest parts of
  the umbra where magnetic fields are strongest. The spikes exhibit up
  and down oscillatory motions and their spectral evolution suggests
  that they might be driven by upward propagating shocks generated by
  photospheric oscillations. It is worth noting that triggering of the
  running penumbral waves seems to occur during the interval when the
  spikes reach their maximum height.

---------------------------------------------------------
Title: Emergence of a small-scale magnetic flux tube and the response
    of the solar atmosphere
Authors: Vargas Dominguez, S.; Kosovichev, A. G.; Yurchyshyn, V.
2014CEAB...38...25V    Altcode:
  Cutting-edge observations with the 1.6-meter telescope at Big Bear
  Solar Observatory (BBSO) in California have taken research into the
  activity of the Sun to new levels of understanding of the structure
  and evolution of the solar atmosphere at high-resolution spatial and
  temporal scales. On August 7, 2013 the NST observed active region NOAA
  11810 in photospheric and chromospheric wavelengths. The observations
  were performed as part of a program conducted jointly with NASA's
  Interface Region Imaging Spectrograph (IRIS) mission, Solar Dynamics
  Observatory (SDO) and Hinode satellite. These observations provided a
  unique view on the emergence of a buoyant small-scale magnetic-flux
  rope in the solar photosphere. The event is accompanied by response
  of the solar atmosphere once the newly emerged field interacts with
  the pre-existing overlying one. The reconnection process that takes
  place in the region produces jet emission and high-temperature points
  in the chromosphere and corona.

---------------------------------------------------------
Title: Characteristic Length of Energy-containing Structures at the
    Base of a Coronal Hole
Authors: Abramenko, V. I.; Zank, G. P.; Dosch, A.; Yurchyshyn, V. B.;
   Goode, P. R.; Ahn, K.; Cao, W.
2013ApJ...773..167A    Altcode: 2013arXiv1307.4421A
  An essential parameter for models of coronal heating and fast solar
  wind acceleration that rely on the dissipation of MHD turbulence is
  the characteristic energy-containing length λ<SUB></SUB> of the
  squared velocity and magnetic field fluctuations (u <SUP>2</SUP>
  and b <SUP>2</SUP>) transverse to the mean magnetic field inside a
  coronal hole (CH) at the base of the corona. The characteristic length
  scale directly defines the heating rate. We use a time series analysis
  of solar granulation and magnetic field measurements inside two CHs
  obtained with the New Solar Telescope at Big Bear Solar Observatory. A
  data set for transverse magnetic fields obtained with the Solar Optical
  Telescope/Spectro-Polarimeter on board the Hinode spacecraft was
  utilized to analyze the squared transverse magnetic field fluctuations
  b_t^2. Local correlation tracking was applied to derive the squared
  transverse velocity fluctuations u <SUP>2</SUP>. We find that for u
  <SUP>2</SUP> structures, the Batchelor integral scale λ varies in
  a range of 1800-2100 km, whereas the correlation length sigmav and
  the e-folding length L vary between 660 and 1460 km. Structures for
  b_t^2 yield λ ≈ 1600 km, sigmav ≈ 640 km, and L ≈ 620 km. An
  averaged (over λ, sigmav, and L) value of the characteristic length
  of u <SUP>2</SUP> fluctuations is 1260 ± 500 km, and that of b_t^2
  is 950 ± 560 km. The characteristic length scale in the photosphere
  is approximately 1.5-50 times smaller than that adopted in previous
  models (3-30 × 10<SUP>3</SUP> km). Our results provide a critical
  input parameter for current models of coronal heating and should yield
  an improved understanding of fast solar wind acceleration.

---------------------------------------------------------
Title: Observation of a Non-radial Penumbra in a Flux Emerging Region
    under Chromospheric Canopy Fields
Authors: Lim, Eun-Kyung; Yurchyshyn, Vasyl; Goode, Philip; Cho,
   Kyung-Suk
2013ApJ...769L..18L    Altcode:
  The presence of a penumbra is one of the main properties of a mature
  sunspot, but its formation mechanism has been elusive due to a lack
  of observations that fully cover the formation process. Utilizing the
  New Solar Telescope at the Big Bear Solar Observatory, we observed
  the formation of a partial penumbra for about 7 hr simultaneously at
  the photospheric (TiO; 7057 Å) and the chromospheric (Hα - 1 Å)
  spectral lines with high spatial and temporal resolution. From this
  uninterrupted, long observing sequence, we found that the formation of
  the observed penumbra was closely associated with flux emergence under
  the pre-existing chromospheric canopy fields. Based on this finding,
  we suggest a possible scenario for penumbra formation in which a
  penumbra forms when the emerging flux is constrained from continuing
  to emerge, but rather is trapped at the photospheric level by the
  overlying chromospheric canopy fields.

---------------------------------------------------------
Title: Dynamics of Chromospheric Upflows and Underlying Magnetic
    Fields
Authors: Yurchyshyn, V.; Abramenko, V.; Goode, P.
2013ApJ...767...17Y    Altcode: 2013arXiv1303.4766Y
  We used Hα-0.1 nm and magnetic field (at 1.56μ) data obtained with
  the New Solar Telescope to study the origin of the disk counterparts to
  type II spicules, so-called rapid blueshifted excursions (RBEs). The
  high time cadence of our chromospheric (10 s) and magnetic field
  (45 s) data allowed us to generate x-t plots using slits parallel
  to the spines of the RBEs. These plots, along with potential field
  extrapolation, led us to suggest that the occurrence of RBEs is
  generally correlated with the appearance of new, mixed, or unipolar
  fields in close proximity to network fields. RBEs show a tendency
  to occur at the interface between large-scale fields and small-scale
  dynamic magnetic loops and thus are likely to be associated with the
  existence of a magnetic canopy. Detection of kinked and/or inverse
  "Y"-shaped RBEs further confirm this conclusion.

---------------------------------------------------------
Title: Three 2012 Transits of Venus: From Earth, Jupiter, and Saturn
Authors: Pasachoff, Jay M.; Schneider, G.; Babcock, B. A.; Lu, M.;
   Edelman, E.; Reardon, K.; Widemann, T.; Tanga, P.; Dantowitz, R.;
   Silverstone, M. D.; Ehrenreich, D.; Vidal-Madjar, A.; Nicholson,
   P. D.; Willson, R. C.; Kopp, G. A.; Yurchyshyn, V. B.; Sterling,
   A. C.; Scherrer, P. H.; Schou, J.; Golub, L.; McCauley, P.; Reeves, K.
2013AAS...22131506P    Altcode:
  We observed the 2012 June 6/5 transit seen from Earth (E/ToV),
  simultaneously with Venus Express and several other spacecraft
  not only to study the Cytherean atmosphere but also to provide an
  exoplanet-transit analog. From Haleakala, the whole transit was visible
  in coronal skies; among our instruments was one of the world-wide Venus
  Twilight Experiment's nine coronagraphs. Venus's atmosphere became
  visible before first contact. SacPeak/IBIS provided high-resolution
  images at Hα/carbon-dioxide. Big Bear's NST also provided
  high-resolution observations of the Cytherean atmosphere and black-drop
  evolution. Our liaison with UH's Mees Solar Observatory scientists
  provided magneto-optical imaging at calcium and potassium. Solar
  Dynamics Observatory's AIA and HMI, and the Solar Optical Telescope
  (SOT) and X-ray Telescope (XRT) on Hinode, and total-solar-irradiance
  measurements with ACRIMSAT and SORCE/TIM, were used to observe the
  event as an exoplanet-transit analog. On September 20, we imaged
  Jupiter for 14 Hubble Space Telescope orbits, centered on a 10-hour
  ToV visible from Jupiter (J/ToV), as an exoplanet-transit analog in
  our own solar system, using Jupiter as an integrating sphere. Imaging
  was good, although much work remains to determine if we can detect
  the expected 0.01% solar irradiance decrease at Jupiter and the even
  slighter differential effect between our violet and near-infrared
  filters caused by Venus's atmosphere. We also give a first report on our
  currently planned December 21 Cassini UVIS observations of a transit of
  Venus from Saturn (S/ToV). Our E/ToV expedition was sponsored by the
  Committee for Research and Exploration/National Geographic Society;
  supplemented: NASA/AAS's Small Research Grant Program. We thank Rob
  Ratkowski, Stan Truitt, Rob Lucas, Aram Friedman, and Eric Pilger
  '82 at Haleakala, and Joseph Gangestad '06 at Big Bear for assistance,
  and Lockheed Martin Solar and Astrophysics Lab and Hinode science and
  operations teams for support for coordinated observations with NASA
  satellites. Our J/ToV observations were based on observations made
  with HST, operated by AURA, Inc., under NASA contract NAS 5-26555;
  these observations are associated with program #13067.

---------------------------------------------------------
Title: Investigation of Small-Scale Turbulent MHD Phenomena Using
    Numerical Simulations and NST Observations
Authors: Kitiashvili, I.; Abramenko, V.; Goode, P. R.; Kosovichev,
   A.; Mansour, N.; Wray, A.; Yurchyshyn, V.
2012IAUSS...6E.104K    Altcode:
  Recent progress in observational capabilities and numerical modeling
  have provided unique high-resolution information demonstrating
  complicated dynamics and structures of turbulent flows and magnetic
  field on the Sun. The realistic approach to numerical simulations is
  based on physical first principles and takes into account compressible
  fluid flow in a highly stratified magnetized medium, 3D multi-bin
  radiative energy transfer between fluid elements, a real-gas equation
  of state, ionization, and excitation of all abundant species, magnetic
  effects and sub-grid turbulence. We present new results of 3D radiative
  MHD simulations of the upper solar convection zone and chromosphere
  that reveal a fundamental role of small-scale vortex dynamics, and
  compare the numerical results and predictions with observational
  results from the 1.6 m clear aperture New Solar Telescope (NST) at
  Big Bear Observatory. In particular, we investigate formation and
  dynamics of ubiquitous small-scale vortex tubes mostly concentrated
  in the intergranular lanes and their role in magnetic structuring
  and acoustic emission of the Sun. These whirlpool-like flows are
  characterized by very strong horizontal shear velocities (7 - 11 km/s)
  and downflows (~7 km/s), and are accompanied by sharp decreases in
  temperature, density and pressure at the surface. High-speed whirlpool
  flows can attract and capture other vortices, penetrate into the low
  chromosphere, and form stable magnetic flux tubes. The simulations also
  reveal a strong connection between acoustic wave excitation events and
  the dynamics of vortex tubes. In this talk, we will discuss different
  aspects of small-scale turbulent dynamics of the low atmosphere from the
  high-resolution simulations in comparison with recent NST observations,
  and the strategy for future synergies of numerical simulations and
  observations with large aperture solar telescopes.

---------------------------------------------------------
Title: Energy-Containing Length Scale at the Base of a Coronal Hole:
    New Observational Findings
Authors: Abramenko, V.; Dosch, A.; Zank, G. P.; Yurchyshyn, V.; Goode,
   P. R.
2012AGUFMSH33D2253A    Altcode:
  Dynamics of the photospheric flux tubes is thought to be a key
  factor for generation and propagation of MHD waves and magnetic
  stress into the corona. Recently, New Solar Telescope (NST, Big
  Bear Solar Observatory) imaging observations in helium I 10830 Å
  revealed ultrafine, hot magnetic loops reaching from the photosphere
  to the corona and originating from intense, compact magnetic field
  elements. One of the essential input parameters to run the models of
  the fast solar wind is a characteristic energy-containing length scale,
  lambda, of the dynamical structures transverse to the mean magnetic
  field in a coronal hole (CH) in the base of the corona. We used NST
  time series of solar granulation motions to estimate the velocity
  fluctuations, as well as NST near-infrared magnetograms to derive
  the magnetic field fluctuations. The NST adaptive optics corrected
  speckle-reconstructed images of 10 seconds cadence were an input for the
  local correlation tracking (LCT) code to derive the squared transverse
  velocity patterns. We found that the characteristic length scale for
  the energy-carrying structures in the photosphere is about 300 km,
  which is two orders of magnitude lower than it was adopted in previous
  models. The influence of the result on the coronal heating and fast
  solar wind modeling will be discussed.; Correlation functions calculated
  from the squared velocities for the three data sets: a coronal hole,
  quiet sun and active region plage area.

---------------------------------------------------------
Title: The relationship between the occurrence of type II spicules
    and the dynamics of underlying magnetic fields
Authors: Yurchyshyn, V.; Abramenko, V.; Goode, P. R.
2012AGUFMSH32A..05Y    Altcode:
  Type II spicules are thought to be small-scale chromospheric
  up-flows. When observed against the solar disk they can be identified
  as rapid blue shifted events (or excursions, RBE, Rouppe van der
  Voort et al.). While their nature is being questioned and their
  associated driving mechanism remains elusive, these up-flows may be
  instrumental in the processes of coronal heating and solar wind. We use
  high resolution photospheric, chromospheric and magnetic field data
  from the New Solar Telescope operating at Big Bear Solar Observatory
  to further determine the properties of these events and refine the
  role that they may play. We find that the majority of RBEs, occurring
  around network clusters of bright points, can be linked to episodes
  of small flux emergence, in particular appearance of opposite polarity
  fields. Case studies further indicate that some of the RBEs appear to
  have kink and inverted "Y" shaped roots. The data thus suggest that
  magnetic reconnection may be responsible for at least some fraction
  of observed RBEs. We will present these observations in details and
  discuss possible implications.Sequence of H-alpha-0.075nm images
  spanning 7 min showing evolution of RBE activity near a cluster
  of network fields. The two yellow circles enclose the area where
  multipolar fields rapidly appeared. Comparing panels 19:05:11 UT and
  19:05:55 UT one may notice that a new magnetic dipole and a dark jet
  appeared in the encircled area. The same is true about the encircled
  area in 19:07:26UT panel. The RBE activity ceased as soon as the the
  field of view was cleared from small-scale magnetic elements.

---------------------------------------------------------
Title: Coronal Mass Ejections and the Index of Effective Solar
    Multipole
Authors: Obridko, V. N.; Ivanov, E. V.; Özgüç, A.; Kilcik, A.;
   Yurchyshyn, V. B.
2012SoPh..281..779O    Altcode: 2012SoPh..tmp..199O
  The paper considers the relationship between the cyclic variations
  in the velocity of coronal mass ejections (CME) and the large-scale
  magnetic field structure (LSMF) in cycles 21 - 23. To characterize
  a typical size of the LSMF structure, we have used the index of
  the effective solar multipole (ESMI). The cyclic behavior of the CME
  occurrence rate and velocity proved to be similar to that of ESMI. The
  hysteresis observed in variations of the CME maximum velocity is
  interpreted as a manifestation of different contributions from the
  two field structures (local and global magnetic fields) in different
  phases of the 11-year activity cycle. It is suggested that cyclic
  variations in the maximum velocity of coronal mass ejections are due
  to different conditions for the formation of the complexes of active
  regions connected by coronal arch systems, which are the main source
  of high-velocity CMEs.

---------------------------------------------------------
Title: Turbulent Pair Dispersion of Photospheric Bright Points
Authors: Lepreti, F.; Carbone, V.; Abramenko, V. I.; Yurchyshyn, V.;
   Goode, P. R.; Capparelli, V.; Vecchio, A.
2012ApJ...759L..17L    Altcode:
  Observations of solar granulation obtained with the New Solar Telescope
  of Big Bear Solar Observatory are used to study the turbulent pair
  dispersion of photospheric bright points in a quiet-Sun area, a
  coronal hole, and an active region plage. In all the three magnetic
  environments, it is found that the pair mean-squared separation
  Δ<SUP>2</SUP>(t) follows a power-law timescaling Δ<SUP>2</SUP>(t) ~ t
  <SUP>η</SUP> in the range 10 s &lt;~ t &lt;~ 400 s. The power-law index
  is found to be η ~= 1.5 for all the three investigated regions. It
  is shown that these results can be explained in the same framework as
  the classical Batchelor theory, under the hypothesis that the observed
  range of timescales corresponds to a non-asymptotic regime in which the
  photospheric bright points keep the memory of their initial separations.

---------------------------------------------------------
Title: The 2012 Transit of Venus for Cytherean Atmospheric Studies
    and as an Exoplanet Analog
Authors: Pasachoff, Jay M.; Schneider, G.; Babcock, B. A.; Lu, M.;
   Reardon, K. P.; Widemann, T.; Tanga, P.; Dantowitz, R.; Willson,
   R.; Kopp, G.; Yurchyshyn, V.; Sterling, A.; Scherrer, P.; Schou, J.;
   Golub, L.; Reeves, K.
2012DPS....4450806P    Altcode:
  We worked to assemble as complete a dataset as possible for the
  Cytherean atmosphere in collaboration with Venus Express in situ
  and to provide an analog of spectral and total irradiance exoplanet
  measurements. From Haleakala, the whole transit was visible in
  coronal skies; our B images showed the evolution of the visibility
  of Venus's atmosphere and of the black-drop effect, as part of the
  Venus Twilight Experiment's 9 coronagraphs distributed worldwide
  with BVRI. We imaged the Cytherean atmosphere over two minutes before
  first contact, with subarcsecond resolution, with the coronagraph and
  a separate refractor. The IBIS imaging spectrometer at Sacramento
  Peak Observatory at H-alpha and carbon-dioxide also provided us
  high-resolution imaging. The NST of Big Bear Solar Observatory
  also provided high-resolution vacuum observations of the Cytherean
  atmosphere and black drop evolution. Our liaison with UH's Mees Solar
  Observatory scientists provided magneto-optical imaging at calcium
  and potassium. Spaceborne observations included the Solar Dynamics
  Observatory's AIA and HMI, and the Solar Optical Telescope (SOT)
  and X-ray Telescope (XRT) on Hinode, and total-solar-irradiance
  measurements with ACRIMSAT and SORCE/TIM, to characterize the
  event as an exoplanet-transit analog. Our expedition was sponsored
  by the Committee for Research and Exploration/National Geographic
  Society. Some of the funds for the carbon-dioxide filter for IBIS were
  provided by NASA through AAS's Small Research Grant Program. We thank
  Rob Lucas, Aram Friedman, and Eric Pilger '82 for assistance with
  Haleakala observing, Rob Ratkowski of Haleakala Amateur Astronomers
  for assistance with equipment and with the site, Stan Truitt for the
  loan of his Paramount ME, and Steve Bisque/Software Bisque for TheSky
  X controller. We thank Joseph Gangestad '06 of Aerospace Corp., a
  veteran of our 2004 expedition, for assistance at Big Bear. We thank
  the Lockheed Martin Solar and Astrophysics Laboratory and Hinode
  science and operations teams for planning and support.

---------------------------------------------------------
Title: Detection of Small-scale Granular Structures in the Quiet
    Sun with the New Solar Telescope
Authors: Abramenko, V. I.; Yurchyshyn, V. B.; Goode, P. R.;
   Kitiashvili, I. N.; Kosovichev, A. G.
2012ApJ...756L..27A    Altcode: 2012arXiv1208.4337A
  Results of a statistical analysis of solar granulation are presented. A
  data set of 36 images of a quiet-Sun area on the solar disk center was
  used. The data were obtained with the 1.6 m clear aperture New Solar
  Telescope at Big Bear Solar Observatory and with a broadband filter
  centered at the TiO (705.7 nm) spectral line. The very high spatial
  resolution of the data (diffraction limit of 77 km and pixel scale of
  0farcs0375) augmented by the very high image contrast (15.5% ± 0.6%)
  allowed us to detect for the first time a distinct subpopulation of
  mini-granular structures. These structures are dominant on spatial
  scales below 600 km. Their size is distributed as a power law with an
  index of -1.8 (which is close to the Kolmogorov's -5/3 law) and no
  predominant scale. The regular granules display a Gaussian (normal)
  size distribution with a mean diameter of 1050 km. Mini-granular
  structures contribute significantly to the total granular area. They are
  predominantly confined to the wide dark lanes between regular granules
  and often form chains and clusters, but different from magnetic bright
  points. A multi-fractality test reveals that the structures smaller
  than 600 km represent a multi-fractal, whereas on larger scales the
  granulation pattern shows no multi-fractality and can be considered
  as a Gaussian random field. The origin, properties, and role of the
  population of mini-granular structures in the solar magnetoconvection
  are yet to be explored.

---------------------------------------------------------
Title: Variations of Current Helicity in Active Region 10930 as
    Inferred from Hinode Spectropolarimeter Data and Cancellation Exponent
Authors: Yurchyshyn, V.; Abramenko, V.; Watanabe, H.
2012ASPC..454..311Y    Altcode:
  Current helicity derived from vector magnetograms possesses a
  well-pronounced scaling behavior, which can be studied by introducing
  a signed measure and calculating the power-law exponent (cancellation
  exponent). The time variations of this exponent seem to be related
  to flare activity of an active region. Here we focus on changes
  of current helicity in active region NOAA 10930 as derived from
  a set of Hinode spectropolarimeter data. Our findings are that the
  cancellation exponent first strongly increased on Dec 11 then rapidly
  decreased after a small sunspot-satellite developed. Afterward, the
  cancellation exponent began its gradual increase without significant
  new magnetic flux emergence. These two different modes of behavior
  may indicate different processes that ultimately led to an eruption:
  the first process is rapid injection of current helicity, while the
  second process is gradual redistribution of injected helicity over
  all spatial scales in the active region.

---------------------------------------------------------
Title: First Simultaneous Detection of Moving Magnetic Features in
    Photospheric Intensity and Magnetic Field Data
Authors: Lim, Eun-Kyung; Yurchyshyn, Vasyl; Goode, Philip
2012ApJ...753...89L    Altcode: 2012arXiv1205.0574L
  The formation and the temporal evolution of a bipolar moving magnetic
  feature (MMF) was studied with high-spatial and temporal resolution. The
  photometric properties were observed with the New Solar Telescope at
  Big Bear Solar Observatory using a broadband TiO filter (705.7 nm),
  while the magnetic field was analyzed using the spectropolarimetric
  data obtained by Hinode. For the first time, we observed a bipolar
  MMF simultaneously in intensity images and magnetic field data, and
  studied the details of its structure. The vector magnetic field and the
  Doppler velocity of the MMF were also studied. A bipolar MMF with its
  positive polarity closer to the negative penumbra formed, accompanied by
  a bright, filamentary structure in the TiO data connecting the MMF and
  a dark penumbral filament. A fast downflow (&lt;=2 km s<SUP>-1</SUP>)
  was detected at the positive polarity. The vector magnetic field
  obtained from the full Stokes inversion revealed that a bipolar MMF
  has a U-shaped magnetic field configuration. Our observations provide
  a clear intensity counterpart of the observed MMF in the photosphere,
  and strong evidence of the connection between the MMF and the penumbral
  filament as a serpentine field.

---------------------------------------------------------
Title: Transverse Motions of Chromospheric Type II Spicules Observed
    by the New Solar Telescope
Authors: Yurchyshyn, V.; Kilcik, A.; Abramenko, V.
2012arXiv1207.6417Y    Altcode:
  Using high resolution off-band \ha\ data from the New Solar Telescope
  and Morlet wavelet analysis technique, we analyzed transverse motions
  of type II spicules observed near the North Pole of the Sun. Our new
  findings are that i) some of the observed type II spicules display
  kink or an inverse "Y" features, suggesting that their origin may be
  due to magnetic reconnection, and ii) type II spicules tend to display
  coherent transverse motions/oscillations. Also, the wavelet analysis
  detected significant presence of high frequency oscillations in type
  II spicules, ranging from 30 to 180 s with the the average period of 90
  s. We conclude that at least some of type II spicules and their coherent
  transverse motions may be caused by reconnection between large scale
  fields rooted in the intergranular lanes and and small-scale emerging
  dipoles, a process that is know to generate high frequency kink mode
  MHD waves propagating along the magnetic field lines.

---------------------------------------------------------
Title: Small Scale Field Emergence and Its Impact on Photospheric
    Granulation
Authors: Yurchyshyn, V.; Ahn, K.; Abramenko, V.; Goode, P.; Cao, W.
2012arXiv1207.6418Y    Altcode:
  We used photospheric intensity images and magnetic field measurements
  from the New Solar Telescope in Big Bear and Helioseismic Magnetic
  Imager on board Solar Dynamics Observatory (SDO) to study the the effect
  that the new small-scale emerging flux induces on solar granulation. We
  report that emerging flux appears to leave different types of footprint
  on solar granulation: i) diffuse irregular patches of increased
  brightness, ii) well defined filament-like structures and accompanied
  bright points, and iii) bright point-like features that appear inside
  granules. We suggest that the type of the footprint depends on the
  intensity of emerging fields. Stronger fields, emerging as a part of
  large magnetic structure, create on the solar surface a well defined
  filamentary pattern with bright points at the ends of the filaments,
  while weak turbulent fields are associated with bright patches inside
  the host granule.

---------------------------------------------------------
Title: New solar telescope in Big Bear: evidence for super-diffusivity
    and small-scale solar dynamos?
Authors: Goode, Philip R.; Abramenko, Valentyna; Yurchyshyn, Vasyl
2012PhyS...86a8402G    Altcode:
  The 1.6 m clear aperture New Solar Telescope (NST) in Big Bear Solar
  Observatory (BBSO) is now providing the highest resolution solar data
  ever. These data have revealed surprises about the Sun on small-scales
  including the observation that bright points (BPs), which can be
  used as proxies for the intense, compact magnetic elements that are
  apparent in photospheric intergranular lanes. The BPs are ever more
  numerous on ever smaller spatial scales as though there were no limit
  to how small the BPs can be. Here we discuss high resolution NST data
  on BPs that provide support for the ideas that a turbulent regime
  of super-diffusivity dominates in the quiet Sun, and there are local
  dynamos operating near the solar surface.

---------------------------------------------------------
Title: Turbulent Kinetic Energy Spectra of Solar Convection from
    NST Observations and Realistic MHD Simulations
Authors: Kitiashvili, I. N.; Abramenko, V. I.; Goode, P. R.;
   Kosovichev, A. G.; Lele, S. K.; Mansour, N. N.; Wray, A. A.;
   Yurchyshyn, V. B.
2012arXiv1206.5300K    Altcode:
  Turbulent properties of the quiet Sun represent the basic state of
  surface conditions, and a background for various processes of solar
  activity. Therefore understanding of properties and dynamics of this
  `basic' state is important for investigation of more complex phenomena,
  formation and development of observed phenomena in the photosphere and
  atmosphere. For characterization of the turbulent properties we compare
  kinetic energy spectra on granular and sub-granular scales obtained
  from infrared TiO observations with the New Solar Telescope (Big Bear
  Solar Observatory) and from 3D radiative MHD numerical simulations
  ('SolarBox' code). We find that the numerical simulations require a high
  spatial resolution with 10 - 25 km grid-step in order to reproduce the
  inertial (Kolmogorov) turbulence range. The observational data require
  an averaging procedure to remove noise and potential instrumental
  artifacts. The resulting kinetic energy spectra show a good agreement
  between the simulations and observations, opening new perspectives for
  detailed joint analysis of more complex turbulent phenomena on the Sun,
  and possibly on other stars. In addition, using the simulations and
  observations we investigate effects of background magnetic field,
  which is concentrated in self-organized complicated structures in
  intergranular lanes, and find an increase of the small-scale turbulence
  energy and its decrease at larger scales due to magnetic field effects.

---------------------------------------------------------
Title: High spatial resolution VAULT H-Lyα observations and
    multiwavelength analysis of an active region filament
Authors: Vial, J. -C.; Olivier, K.; Philippon, A. A.; Vourlidas, A.;
   Yurchyshyn, V.
2012A&A...541A.108V    Altcode:
  Context. The search for the fine structure of prominences has
  received considerable new attention thanks to the Swedish Solar
  Telescope (SST) Hα pictures that provide an unsurpassed spatial
  resolution. Recently, it has been shown that the filaments' coronal
  environment, at least for quiescent filaments, is perturbed by either
  cool absorbing material (in the EUV) or an "emissivity blocking"
  (actually a lack of transition region and coronal material). <BR />
  Aims: The aim is to assess the fine structure in an active region
  filament and to determine the nature of the EUV absorption or lack
  of emission phenomena, using the very optically thick line H-Lyα,
  formed at a temperature higher than Hα. <BR /> Methods: We performed
  a multiwavelength study where high-resolution imaging in the H-Lyα
  line (VAULT) was analysed and compared with observations of an active
  region filament in Hα (BBSO) and EUV lines (EIT and TRACE). <BR />
  Results: As for the SST data, small-scale structures were detected at
  a typical scale of about one to two arcseconds with, for some cuts,
  an indication of fine scales down to 0.4 arcsec in the optically thick
  H-Lyα line. The filament intensity relative to the intensity of the
  (active) region it is embedded in is about 0.2 in H-Lyα. This ratio
  (Lymanα ratio intensity or "LRI") is the lowest value compared to
  other lines, e.g. Hα. The filament environment was also investigated
  and evidence of an UV extension was found. The comparison of spatial
  cuts in different lines across the filament shows evidence of strong
  absorption, and consequently of cool plasma on one side of the filament,
  but not on the other (that side is obscured by the filament itself). <BR
  /> Conclusions: The absence of very fine structure in H-Lyα compared
  to Hα is explained by the formation temperature of the H-Lyα line
  (~20 000 K), where the transition regions of the thin threads begin to
  merge. From the detection of H-Lyα absorption on the observable side of
  the filament side, we derive the presence of absorbing (cool) material
  and possibly also of emissivity blocking (or coronal void). This poses
  the question whether these absorption effects are typical of active
  region filaments. <P />Appendix A is available in electronic form at
  <A href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: Direct Observation of the Intensity Counterpart of Moving
    Magnetic Features on the Photosphere and the Corresponding Vector
    Magnetic Fields
Authors: Lim, Eunkyung; Yurchyshyn, V.; Goode, P.
2012AAS...22020622L    Altcode:
  The formation and the temporal evolution of a bipolar moving magnetic
  feature (MMF) was studied with high spatio-temporal resolution. The
  photometric properties were observed with the New Solar Telescope at
  Big Bear Solar Observatory using a broadband TiO filter at 705.7nm,
  while the magnetic field was analyzed using the Spectropolarimetric
  data obtained by Hinode/SOT. From our high resolution, multi-wavelength
  observation, we studied 1) the detailed structure of the intensity
  counterpart in the photosphere of a bipolar MMF, 2) the vector magnetic
  field and the Doppler velocity of the MMF in time. A bipolar MMF
  having its positive polarity closer to the negative penumbra formed
  being accompanied by a bright, filamentary structure in the TiO line
  connecting the MMF and a dark penumbral filament. A fast downflow
  was detected in the positive polarity region, where the filamentary
  structure is seen to be brighter than its surroundings. The vector
  magnetic field obtained from the full Stokes inversion reveals a
  developing U-shaped magnetic dip between the poles of the bipolar
  MMF. Our observations provide the most clear intensity counterpart
  in the photosphere to the observed MMF, and strong evidence of the
  connection between the MMF and the local penumbral filament as a
  serpentine field.

---------------------------------------------------------
Title: Observational Signatures of the Small-Scale Dynamo in the
    Quiet Sun
Authors: Abramenko, V.; Yurchyshyn, V.; Goode, P. R.
2012ASPC..455...17A    Altcode:
  The generation and diffusion of the magnetic field on the Sun is a key
  mechanism responsible for solar activity on all spatial and temporal
  scales—from the solar cycle down to the evolution of small-scale
  magnetic elements in the quiet Sun. The solar dynamo operates as
  a non-linear dynamical process and is thought to be manifest in two
  types: as a global dynamo responsible for the solar cycle periodicity,
  and as a small-scale turbulent dynamo responsible for the formation
  of the magnetic carpet in the quiet Sun. Numerous MHD simulations of
  solar turbulence did not yet reach a consensus as to the existence
  of a turbulent dynamo on the Sun. At the same time, high-resolution
  observations of the quiet Sun from Hinode instruments suggest
  possibilities for the turbulent dynamo. Analysis of characteristics of
  turbulence derived from observations would be beneficial in tackling
  the problem. We analyze magnetic and velocity energy spectra as derived
  from Hinode/SOT, SOHO/MDI, SDO/HMI and the New Solar Telescope (NST)
  of Big Bear Solar Observatory (BBSO) to explore the possibilities for
  the small-scale turbulent dynamo in the quiet Sun.

---------------------------------------------------------
Title: Oscillations of Rapid Blueshifted Events as Derived from
    NST Data
Authors: Yurchyshyn, Vasyl B.; Kilcik, A.; Abramenko, V.
2012AAS...22020304Y    Altcode:
  We studied oscillations of type II spicules observed near the north
  pole of the sun. The study is based on high-resolution data recorded by
  the New Solar Telescope at the Big Bear Solar Observatory. The spicule
  oscillations were probed by applying the global wavelet method to a 34
  min continuous time series of off-band Halpha images. The main findings
  are: i) Type II spicules are oscillating with about 1 min period,
  while the outside quiet regions show dominance of 3 min periods. ii)
  Spicules belonging to a cluster, tend to oscillate as a group. We will
  present details of these findings and discuss possible implications.

---------------------------------------------------------
Title: Origin of Rapid Blueshifted Events in Coronal Holes
Authors: Yurchyshyn, Vasyl B.; Ahn, K.; Abramenko, V.; Goode, P.;
   Cao, W.
2012AAS...22042304Y    Altcode:
  Clusters of photospheric bright points are surrounded by chromospheric
  rosette-like structures. These rosettes, when observed in the far
  off-band (-0.1nm) Halpha images often appear to consist of short living,
  narrow rapid blueshifted events (RBEs). RBEs, in turn, are thought to
  be disk counterparts of type II spicules (spicules II), detected in
  Hinode data, which may be playing play an important role in coronal
  heating since they are thought to supply mass to the solar corona. The
  search for the origin of type II spicules was one of the main focus of
  solar physics research in the recent years. <P />Here we present our
  findings on the possible driving mechanism of spicules II, which are
  based on high resolution photospheric, chromospheric and magnetic field
  data from the New Solar Telescope (NST) collected in a coronal hole. We
  report that the majority of RBEs, occurring around a network cluster,
  are associated with appearance of opposite polarity features within
  the unipolar cluster fields, suggesting that magnetic reconnection
  may be the driving mechanism. We will present these observations in
  details and discuss possible implications.

---------------------------------------------------------
Title: Observational Criteria For Small-scale Turbulent Dynamo In
    The Solar Photosphere
Authors: Abramenko, Valentyna; Goode, P.; Yurchyshyn, V.
2012AAS...22011002A    Altcode:
  Generation and dispersal of the magnetic field on the Sun is a key
  mechanism responsible for solar activity on all spatial and temporal
  scales - from the solar cycle down to the evolution of small-scale
  magnetic elements in the quiet Sun. The solar dynamo operates as
  a non-linear dynamical process and is thought to be manifested
  in two types: as a global dynamo responsible for the solar cycle
  periodicity, and as a small-scale turbulent dynamo (SSTD) responsible
  for the formation of magnetic carpet in the quiet Sun. Numerous MHD
  simulations of the solar turbulence did not yet reach a consensus
  as to the existence and role of SSTD on the Sun. At the same time,
  high-resolution observations of the quiet Sun are capable to provide
  certain criteria to prove or rule out SSTD. We suggest to probe four
  possible criteria: i) mutual behaviour of the kinetic and magnetic power
  spectra; ii) intermittency/multifractality of the magnetic field; iii)
  smallest observed scale of magnetic flux tubes; iv) regime of magnetic
  diffusivity on smallest observable scales. We analyse magnetic, velocity
  and solar granulation data as derived from Hinode/SOT, SOHO/MDI, SDO/HMI
  and the New Solar Telescope (NST) of Big Bear Solar Observatory (BBSO)
  to explore the possibilities for SSTD in the quiet Sun.

---------------------------------------------------------
Title: Properties of Umbral Dots as Measured from the New Solar
    Telescope Data and MHD Simulations
Authors: Kilcik, A.; Yurchyshyn, V. B.; Rempel, M.; Abramenko, V.;
   Kitai, R.; Goode, P. R.; Cao, W.; Watanabe, H.
2012ApJ...745..163K    Altcode: 2011arXiv1111.3997K
  We studied bright umbral dots (UDs) detected in a moderate size sunspot
  and compared their statistical properties to recent MHD models. The
  study is based on high-resolution data recorded by the New Solar
  Telescope at the Big Bear Solar Observatory and three-dimensional (3D)
  MHD simulations of sunspots. Observed UDs, living longer than 150 s,
  were detected and tracked in a 46 minute long data set, using an
  automatic detection code. A total of 1553 (620) UDs were detected
  in the photospheric (low chromospheric) data. Our main findings
  are (1) none of the analyzed UDs is precisely circular, (2) the
  diameter-intensity relationship only holds in bright umbral areas, and
  (3) UD velocities are inversely related to their lifetime. While nearly
  all photospheric UDs can be identified in the low chromospheric images,
  some small closely spaced UDs appear in the low chromosphere as a single
  cluster. Slow-moving and long-living UDs seem to exist in both the low
  chromosphere and photosphere, while fast-moving and short-living UDs
  are mainly detected in the photospheric images. Comparison to the 3D
  MHD simulations showed that both types of UDs display, on average, very
  similar statistical characteristics. However, (1) the average number
  of observed UDs per unit area is smaller than that of the model UDs,
  and (2) on average, the diameter of model UDs is slightly larger than
  that of observed ones.

---------------------------------------------------------
Title: Magnetic and Kinetic Power Spectra as a Tool to Probe the
    Turbulent Dynamo
Authors: Abramenko, V. I.; Yurchyshyn, V. B.; Goode, P. R.
2011arXiv1112.2750A    Altcode:
  Generation and diffusion of the magnetic field on the Sun is a key
  mechanism responsible for solar activity on all spatial and temporal
  scales - from the solar cycle down to the evolution of small-scale
  magnetic elements in the quiet Sun. The solar dynamo operates as
  a non-linear dynamical process and is thought to be manifest in two
  types: as a global dynamo responsible for the solar cycle periodicity,
  and as a small-scale turbulent dynamo responsible for the formation
  of magnetic carpet in the quiet Sun. Numerous MHD simulations of the
  solar turbulence did not yet reach a consensus as to the existence
  of a turbulent dynamo on the Sun. At the same time, high-resolution
  observations of the quiet Sun from Hinode instruments suggest
  possibilities for the turbulent dynamo. Analysis of characteristics of
  turbulence derived from observations would be beneficial in tackling
  the problem. We analyse magnetic and velocity energy spectra as derived
  from Hinode/SOT, SOHO/MDI, SDO/HMI and the New Solar Telescope (NST)
  of Big Bear Solar Observatory (BBSO) to explore the possibilities for
  the small-scale turbulent dynamo in the quiet Sun.

---------------------------------------------------------
Title: Signatures of Small-Scale Magnetic Field Emergence as Seen
    from the New Solar Telescope in Big Bear
Authors: Yurchyshyn, V.
2011AGUFMSH33C..06Y    Altcode:
  Increased resolution of solar telescopes allow us to study emerging
  small-scale magnetic fields in unprecedented detail. First light Hinode
  magnetograms showed evidence of both horizontal and line-of-sight field
  being constantly brought to the solar surface by solar convection
  motion. What are the signatures of these fields in the photosphere,
  if any? The largest aperture ground-based solar telescope, the New
  Solar Telescope (NST) of Big Bear Solar Observatory now allows us to
  address many important issues of coupling between the photosphere and
  chromosphere by means of simultaneous observations of photospheric
  granulation with well-resolved bright points (BPs) and associated
  dynamics in the low chromosphere, as seen in the H-alpha spectral
  line. Excellent seeing conditions, augmented with an adaptive optics
  system and speckle-reconstruction applications produce diffraction
  limited images. We examine NST granulation and Halpha images co-temporal
  with SDO, Hinode and BBSO/IRIM vector magnetograms. Our main finding
  is that emerging magnetic flux leaves clear footprint in solar
  granulation. Moreover, the granulation responds to the emerging flux
  much earlier that it appears in magnetograms. NST granulation images
  also reveal that various bright points as well as bright granular lanes
  may form and evolve within a granule. These newly detected features
  are believed to be associated with small-scale magnetic fields.

---------------------------------------------------------
Title: Turbulent Diffusion in the Photosphere as Derived from
    Photospheric Bright Point Motion
Authors: Abramenko, V. I.; Carbone, V.; Yurchyshyn, V.; Goode, P. R.;
   Stein, R. F.; Lepreti, F.; Capparelli, V.; Vecchio, A.
2011ApJ...743..133A    Altcode: 2011arXiv1111.4456A
  On the basis of observations of solar granulation obtained with the
  New Solar Telescope of Big Bear Solar Observatory, we explored proper
  motion of bright points (BPs) in a quiet-sun area, a coronal hole, and
  an active region plage. We automatically detected and traced BPs and
  derived their mean-squared displacements as a function of time (starting
  from the appearance of each BP) for all available time intervals. In all
  three magnetic environments, we found the presence of a super-diffusion
  regime, which is the most pronounced inside the time interval of 10-300
  s. Super-diffusion, measured via the spectral index, γ, which is the
  slope of the mean-squared displacement spectrum, increases from the
  plage area (γ = 1.48) to the quiet-sun area (γ = 1.53) to the coronal
  hole (γ = 1.67). We also found that the coefficient of turbulent
  diffusion changes in direct proportion to both temporal and spatial
  scales. For the minimum spatial scale (22 km) and minimum time scale
  (10 s), it is 22 and 19 km<SUP>2</SUP> s<SUP>-1</SUP> for the coronal
  hole and the quiet-sun area, respectively, whereas for the plage area
  it is about 12 km<SUP>2</SUP> s<SUP>-1</SUP> for the minimum time
  scale of 15 s. We applied our BP tracking code to three-dimensional
  MHD model data of solar convection and found the super-diffusion with
  γ = 1.45. An expression for the turbulent diffusion coefficient as
  a function of scales and γ is obtained.

---------------------------------------------------------
Title: Properties of Umbral Dots as Measured from the New Solar
    Telescope Data and MHD Simulations
Authors: Yurchyshyn, V.; Kilcik, A.; Rempel, M.; Abramenko, V.; Kitai,
   R.; Goode, P. R.; Cao, W.; Watanabe, H.
2011sdmi.confE..86Y    Altcode:
  We studied bright umbral dots (UDs) detected in the main sunspot
  of AR NOAA 11108 and compare their statistical properties to a
  state-of-the-art MHD model of a sunspot. The study is based on
  high resolution data recorded on September 20, 2010 by the New Solar
  Telescope (NST) at Big Bear Solar Observatory and 3D MHD simulations of
  sunspots. The 46 min data set included photospheric (0.3nm TiO filter
  centered at 705.7 nm) and chromospheric (0.025nm Hα Lyot filter)
  adaptive optics corrected and speckle reconstructed images. Bright
  UDs, living longer than 150 s, were detected and tracked using an
  automatic UD detection code. Total 1553 (620) UDs were detected
  in the photospheric (chromospheric) data. Our main findings are:
  i) none of the analyzed UDs is of an exact circular shape, ii) the
  diameter-intensity relationship only works for bright umbral areas, and
  iii) UD velocities inversely related to their life time. Comparison of
  photospheric and chromospheric data showed that nearly all photospheric
  UDs can be identified in the chromospheric images. However, it appears
  that some small closely spaced UDs appear in the chromospheric images
  as a single cluster, which may lead to the underestimation of the total
  number of detected chromospheric UDs. Also, while slow moving and long
  living UDs seem to exist in both chromosphere and photosphere, fast
  moving and short living ones are detected mainly in the photospheric
  images. Comparison of model and observed data shows that both types
  of UDs display very similar statistical characteristics. The main
  difference between parameters of model and observed UDs is that i)
  the average number of observed UDs per unit area is smaller than that
  of the model UDs, and ii) on average, the diameter of model UDs is
  slightly larger than that of observed ones.

---------------------------------------------------------
Title: High-resolution observations of the solar dynamics and
    magnetism
Authors: Goode, Phil; Cao, Wenda; Yurchyshyn, Vasyl
2011sdmi.confE..28G    Altcode:
  The NST is the first facility-class solar telescope built in the US
  in a generation. Images and movies illustrating the high resolution
  capabilities of the NST will be shown. In particular, high resolution
  NST observations reveal vortices in the granular field that are
  associated with newly discovered, but ubiquitous small-scale jets,
  which are much smaller-scale than Hinode type-II jets. NST observations
  have been used to probe the nature of the diffusion of magnetic bright
  points, which seems consistent with the operation of small-scale
  dynamos, while seeming to be sufficient on large-scales to support the
  Wang-Sheeley dynamo picture. Other recent NST results correlated with
  satellite observations will be shown and discussed.

---------------------------------------------------------
Title: Photospheric Signatures of Granular-scale Flux Emergence and
    Cancellation at the Penumbral Boundary
Authors: Lim, Eun-Kyung; Yurchyshyn, Vasyl; Abramenko, Valentyna;
   Ahn, Kwangsu; Cao, Wenda; Goode, Philip
2011ApJ...740...82L    Altcode: 2011arXiv1107.5254L
  We studied flux emergence events of sub-granular scale in a solar
  active region. The New Solar Telescope (NST) of the Big Bear Solar
  Observatory made it possible to clearly observe the photospheric
  signature of flux emergence with very high spatial (0farcs11 at 7057
  Å) and temporal (15 s) resolution. From TiO observations with the
  pixel scale of 0farcs0375, we found several elongated granule-like
  features (GLFs) stretching from the penumbral filaments of a sunspot
  at a relatively high speed of over 4 km s<SUP>-1</SUP>. After a
  slender arched darkening appeared at the tip of a penumbral filament,
  a bright point (BP) developed and quickly moved away from the filament,
  forming and stretching a GLF. The size of a GLF was approximately
  0farcs5 wide and 3” long. The moving BP encountered nearby structures
  after several minutes of stretching, and the well-defined elongated
  shape of the GLF faded away. Magnetograms from the Solar Dynamics
  Observatory/Helioseismic and Magnetic Imager and NST/InfraRed Imaging
  Magnetograph revealed that those GLFs are photospheric indicators of
  small-scale flux emergence, and their disappearance is related to
  magnetic cancellation. From two well-observed events, we describe
  detailed development of the sub-structures of GLFs and different
  cancellation processes that each of the two GLFs underwent.

---------------------------------------------------------
Title: On the Origin of Intergranular Jets
Authors: Yurchyshyn, V. B.; Goode, P. R.; Abramenko, V. I.; Steiner, O.
2011ApJ...736L..35Y    Altcode: 2011arXiv1106.5535Y
  We observe that intergranular jets, originating in the intergranular
  space surrounding individual granules, tend to be associated with
  granular fragmentation, in particular, with the formation and evolution
  of a bright granular lane (BGL) within individual granules. The BGLs
  have recently been identified as vortex tubes by Steiner et al. We
  further discover the development of a well-defined bright grain
  located between the BGL and the dark intergranular lane to which it
  is connected. Signatures of a BGL may reach the lower chromosphere
  and can be detected in off-band Hα images. Simulations also indicate
  that vortex tubes are frequently associated with small-scale magnetic
  fields. We speculate that the intergranular jets detected in the New
  Solar Telescope (NST) data may result from the interaction between
  the turbulent small-scale fields associated with the vortex tube
  and the larger-scale fields existing in the intergranular lanes. The
  intergranular jets are much smaller and weaker than all previously known
  jet-like events. At the same time, they appear much more numerous than
  the larger events, leading us to the speculation that the total energy
  release and mass transport by these tiny events may not be negligible in
  the energy and mass-flux balance near the temperature minimum atop the
  photosphere. The study is based on the photospheric TiO broadband (1.0
  nm) filter data acquired with the 1.6 m NST operating at the Big Bear
  Solar Observatory. The data set also includes NST off-band Hα images
  collected through a Zeiss Lyot filter with a passband of 0.025 nm.

---------------------------------------------------------
Title: Dynamics of Photospheric Bright Points in a Transient
    Coronal Hole
Authors: Yurchyshyn, Vasyl; BBSO Team
2011shin.confE.165Y    Altcode:
  We use data from the New Solar Telescope (NST) in Big Bear to search
  for connection between typical dynamics of bright points (collision,
  clustering and rapid motions) and chromospheric activity, such as
  jets that are visible on all scales down to the smallest resolved
  features. In this presentation we will highlight the most important
  findings, which include the following. 1) In mostly unipolar coronal
  holes, the majority of colliding/interacting BPs are not associated with
  any detectable chromospheric activity. This means that the component
  reconnection, presumably occurring when the same polarity BPs interact,
  may not be very effective in producing chromospheric flows. 2) NST/TiO
  images further reveal the hidden structure of plasma vortex tubes
  abundant in coronal holes. Some vortex-tube events are co-spatial
  with small-scale chromospheric jets, which suggests that the tubes
  may be associated with new magnetic flux emerging within a granule. 3)
  On large spatial scales of a CH we observe that displacements of BPs
  display a well pronounced dominant direction of motion that corresponds
  to the direction of migration of the CH.

---------------------------------------------------------
Title: Effects of Hysteresis Between Maximum CME Speed Index and
    Some Solar Activity Indicators during Cycle 23
Authors: Kilcik, A.; Ozguc, A.; Yurchyshyn, V. B.; Rozelot, J. P.
2011simi.conf....6K    Altcode:
  Using the smoothed time series of maximum CME speed index data set
  for solar cycle 23 we find that maximum CME speed index and some solar
  activity indicators show a hysteresis phenomenon. It is observed that
  total sunspot number, total sunspot area, solar radio flux (10.7 cm)
  and flare index follow different paths for the ascending and descending
  phases of solar cycle 23 while saturation effect exists at the maximum
  phase of the cycle. However we notice that the separations between
  the paths are not the same for the solar activity indicators we used.

---------------------------------------------------------
Title: Sunspot Umbral Dots Detected with the New Solar Telescope
Authors: Kilcik, Ali; Yurchyshyn, V.; Abramenko, V.; Goode, P.; Cao, W.
2011SPD....42.1901K    Altcode: 2011BAAS..43S.1901K
  We present a study of bright umbral dots detected inside a large sunspot
  of NOAA AR 11108. This study is based on high resolution data recorded
  on September 20, 2010 with the New Solar Telescope (NST) at Big Bear
  Solar Observatory. The data set, spanning 46 min, consists of a total
  of 184 adaptive optics corrected and speckle reconstructed images
  obtained with a 0.3 nm passband TiO filter centered on the 705.7 nm
  spectral line. The image cadence is 15 s and the pixel size of 0.0375
  arcsec. <P />Bright umbral dots (UDs) were detected and tracked using
  an automatic routine. Here we only focus on long living UDs (&gt;150
  s in life time) and a total of 513 such features were detected during
  the observed period. We found that the average lifetime of a UD is 7.4
  min and an average size is 0.34 arcsec. There is a tendency for larger
  UDs to be brighter (and more circular). Many UDs are not of circular
  shape. We will also present probability distribution of various physical
  parameters and compare the results to similar earlier studies.

---------------------------------------------------------
Title: NST and Photospheric Fine -scale Structures Indicating the
    Small Scale Flux Emergence in an Active Region
Authors: Lim, Eunkyung; Yurchyshyn, V.; Abramenko, V.; Goode, P.;
   Ahn, K.
2011SPD....42.0604L    Altcode: 2011BAAS..43S.0604L
  We have studied very small-scale flux emergence events on granular
  scales in a solar active region. The New Solar Telescope of Big Bear
  Solar Observatory made it possible to clearly observe the photospheric
  signature of flux emergence with a very high spatial (0".034/pixel) and
  temporal (15s) resolution. From the TiO observations, we found several
  elongated thread-like granules protruding from the penumbral filaments
  of a sunspot at a relatively high speed of over 4km s-1. A slender
  arched darkening protrudes from the tip of the penumbral filament, then
  quickly stretches its length along the intergranular lane with a slight
  bright point developing at the previously shaded leading edge. The size
  of such granules is approximately 0".5 wide and 3” long, and their
  stretching lasts for several minutes before contacting other magnetic
  structures nearby. Magnetograms from HMI/SDO and IRIM/BBSO show that
  such elongated granules are photospheric indicators of small-scale
  flux emergence. The cancellation process is also described in detail
  for two events that show different chromospheric signatures, such
  as brightenings and jets during the cancellation. We speculate that
  subsurface connectivity and the depth of the roots of magnetic field
  are the main keys to determining different cancellation phenomena.

---------------------------------------------------------
Title: Utilizing Nst Data To Look For Connection Between Photospheric
    Dynamics And Small-scale Chromospheric Activity
Authors: Yurchyshyn, Vasyl B.
2011SPD....42.0602Y    Altcode: 2011BAAS..43S.0602Y
  The largest ground-based solar telescope, the new solar telescope (NST)
  of Big Bear Solar Observatory now allows us to address many important
  issues of coupling between the photosphere and chromosphere by means of
  simultaneous observations of photospheric granulation with well resolved
  bright points (BPs) and associated dynamics in the low chromosphere,
  as seen in H-alpha spectral line. Excellent seeing conditions,
  augmented with an adaptive optics system and speckle-reconstruction
  applications produce diffraction limited images. We use these data to
  search for any possible connection between typical dynamics of bright
  points (collision, clustering and rapid motions) and chromospheric
  activity, such as jets that are visible on all scales down to the
  smallest resolved features. In this presentation we will highlight the
  most important findings, which include the following. 1) In mostly
  unipolar coronal holes, the majority of colliding/interacting BPs
  are not associated with any detectable chromospheric activity. This
  means that the component reconnection, presumably occurring when the
  same polarity BPs interact, may not be very effective in producing
  chromospheric flows. We speculate that interaction of opposite polarity
  BPs may be more effective in generating up-flows. 2) NST/TiO images
  further reveal the hidden structure of plasma vortex tubes, previously
  predicted by Steiner et al. Besides the bright granular lane, a vortex
  tube structure also includes rapidly developing bright grain co-spatial
  with the tube's axis. Finally, some vortex tube events, detected in
  a CH data set, are co-spatial with small-scale chromospheric jets,
  which suggests that they may be associated with new magnetic flux
  emerging within a granule.

---------------------------------------------------------
Title: New View on Quiet-Sun Photospheric Dynamics Offered by NST Data
Authors: Abramenko, Valentyna; Yurchyshyn, V.; Goode, P. R.
2011SPD....42.0603A    Altcode: 2011BAAS..43S.0603A
  Recent observations of the quiet sun photosphere obtained with the
  1.6 meter New Solar telescope (NST) of Big Bear Solar observatory
  (BBSO) delivered new information about photospheric fine structures
  and their dynamics, as well as posing new questions. The 2-hour
  uninterrupted data set of solar granulation obtained under excellent
  seeing conditions on August 3, 2010 (with cadence of 10 sec) was the
  basis for the study. Statistical analysis of automatically detected and
  tracked magnetic bright points (MBPs) showed that the MBPs population
  monotonically increases as their size decreases, down to 60-70 km. Our
  analysis shows that if the smallest magnetic flux tubes exist, their
  size is still smaller that 60-70 km, which impose strong restrictions on
  the modeling of these structures. We also found that the distributions
  of the MBP's size and lifetime do not follow a traditional Gaussian
  distribution, typical for random processes. Instead, it follows a
  log-normal distribution, typical for avalanches, catastrophes, stock
  market data, etc. Our data set also demonstrated that a majority (98.6
  %) of MBPs are short live (&lt;2 min). This remarkable fact was not
  obvious from previous studies because an extremely high time cadence
  was required. The fact indicates that the majority of MBPs appear for a
  very short time (tens of seconds), similar to other transient features,
  for example, chromospheric jets. The most important point here is that
  these small and short living MBPs significantly increase dynamics
  (flux emergence, collapse into MBPs, and magnetic flux recycling)
  of the solar surface magnetic fields.

---------------------------------------------------------
Title: Response of Granulation to Small-scale Bright Features in
    the Quiet Sun
Authors: Anđić, A.; Chae, J.; Goode, P. R.; Cao, W.; Ahn, K.;
   Yurchyshyn, V.; Abramenko, V.
2011ApJ...731...29A    Altcode: 2011arXiv1102.3404A
  We detected 2.8 bright points (BPs) per Mm<SUP>2</SUP> in the quiet
  Sun with the New Solar Telescope at Big Bear Solar Observatory, using
  the TiO 705.68 nm spectral line at an angular resolution ~0farcs1 to
  obtain a 30 minute data sequence. Some BPs formed knots that were
  stable in time and influenced the properties of the granulation
  pattern around them. The observed granulation pattern within ~3”
  of knots presents smaller granules than those observed in a normal
  granulation pattern, i.e., around the knots a suppressed convection
  is detected. Observed BPs covered ~5% of the solar surface and were
  not homogeneously distributed. BPs had an average size of 0farcs22,
  they were detectable for 4.28 minutes on average, and had an averaged
  contrast of 0.1% in the deep red TiO spectral line.

---------------------------------------------------------
Title: Time Distributions of Large and Small Sunspot Groups Over
    Four Solar Cycles
Authors: Kilcik, A.; Yurchyshyn, V. B.; Abramenko, V.; Goode, P. R.;
   Ozguc, A.; Rozelot, J. P.; Cao, W.
2011ApJ...731...30K    Altcode: 2011arXiv1111.3999K
  Here we analyze solar activity by focusing on time variations of
  the number of sunspot groups (SGs) as a function of their modified
  Zurich class. We analyzed data for solar cycles 20-23 by using Rome
  (cycles 20 and 21) and Learmonth Solar Observatory (cycles 22 and 23)
  SG numbers. All SGs recorded during these time intervals were separated
  into two groups. The first group includes small SGs (A, B, C, H, and
  J classes by Zurich classification), and the second group consists
  of large SGs (D, E, F, and G classes). We then calculated small and
  large SG numbers from their daily mean numbers as observed on the
  solar disk during a given month. We report that the time variations
  of small and large SG numbers are asymmetric except for solar cycle
  22. In general, large SG numbers appear to reach their maximum in the
  middle of the solar cycle (phases 0.45-0.5), while the international
  sunspot numbers and the small SG numbers generally peak much earlier
  (solar cycle phases 0.29-0.35). Moreover, the 10.7 cm solar radio
  flux, the facular area, and the maximum coronal mass ejection speed
  show better agreement with the large SG numbers than they do with
  the small SG numbers. Our results suggest that the large SG numbers
  are more likely to shed light on solar activity and its geophysical
  implications. Our findings may also influence our understanding of
  long-term variations of the total solar irradiance, which is thought
  to be an important factor in the Sun-Earth climate relationship.

---------------------------------------------------------
Title: Maximum Coronal Mass Ejection Speed as an Indicator of Solar
    and Geomagnetic Activities
Authors: Kilcik, A.; Yurchyshyn, V. B.; Abramenko, V.; Goode, P. R.;
   Gopalswamy, N.; Ozguc, A.; Rozelot, J. P.
2011ApJ...727...44K    Altcode: 2011arXiv1111.4000K
  We investigate the relationship between the monthly averaged maximal
  speeds of coronal mass ejections (CMEs), international sunspot number
  (ISSN), and the geomagnetic Dst and Ap indices covering the 1996-2008
  time interval (solar cycle 23). Our new findings are as follows. (1)
  There is a noteworthy relationship between monthly averaged maximum CME
  speeds and sunspot numbers, Ap and Dst indices. Various peculiarities
  in the monthly Dst index are correlated better with the fine structures
  in the CME speed profile than that in the ISSN data. (2) Unlike the
  sunspot numbers, the CME speed index does not exhibit a double peak
  maximum. Instead, the CME speed profile peaks during the declining
  phase of solar cycle 23. Similar to the Ap index, both CME speed and
  the Dst indices lag behind the sunspot numbers by several months. (3)
  The CME number shows a double peak similar to that seen in the sunspot
  numbers. The CME occurrence rate remained very high even near the
  minimum of the solar cycle 23, when both the sunspot number and the
  CME average maximum speed were reaching their minimum values. (4) A
  well-defined peak of the Ap index between 2002 May and 2004 August was
  co-temporal with the excess of the mid-latitude coronal holes during
  solar cycle 23. The above findings suggest that the CME speed index may
  be a useful indicator of both solar and geomagnetic activities. It may
  have advantages over the sunspot numbers, because it better reflects
  the intensity of Earth-directed solar eruptions.

---------------------------------------------------------
Title: Relationship Between Earth Directed Solar Eruptions and
    Magnetic Clouds at 1AU (Invited)
Authors: Yurchyshyn, V.
2010AGUFMSH43C..03Y    Altcode:
  Understanding the connection between the magnetic configurations of a
  coronal mass ejection (CME) and their counterpart in the interplanetary
  medium is very important in terms of space weather predictions. Recent
  data convincingly demonstrate that fast CME originating from near
  the solar disk center are the major cause of extreme space weather
  events. There also appears to be a link between the CME orientation and
  the direction of the magnetic fields in the underlying flux rope. Many
  CMEs rotate as they propagate in the interplanetary medium so that the
  probability of a strong geomagnetic storm depends on both the initial
  properties of the erupted structure and the interaction between the
  ejecta and heliospheric magnetic fields. Detailed understanding of
  this interaction may shed light on the problems related to connecting
  solar surface phenomena to their interplanetary counterparts. In
  this presentation I will briefly review current progress on the CME
  evolution in the heliosphere.

---------------------------------------------------------
Title: Photosphere-Chromosphere Connection as Derived from Nst
    Observations
Authors: Yurchyshyn, V.; Abramenko, V.; Goode, P. R.
2010AGUFMSH31C1807Y    Altcode:
  Largest ground-based new solar telescope (NST) of Big Bear Solar
  Observatory allows us to simultaneously observe photospheric
  granulation with luxurious filigree of bright points (BPs) and
  low/middle chromosphere in H- alpha spectral line. Excellent climate
  conditions of Big Bear Valley, augmented with an adaptive optics system
  and speckle-reconstruction applications produce diffraction limited
  images. Recent observations (July- August 2010) showed that BPs visible
  in the photosphere with the TiO filter (centered at a wavelength of
  705.7 nm) are co-spatial with the BPs visible in the blue wind of
  H-alpha line. As evidenced from these data, the H-alpha BPs, in turn,
  are frequently at origin of small-scale chromospheric jets. These jets
  are visible at all scales down to the smallest resolved features. As
  long as photospheric BPs are co-spatial with the magnetic elements,
  one might conclude that photospheric magnetic fields are relevant
  to the chromospheric jet formation. NST Ha-0.13nm image acquired on
  June 28, 2010. The dark features are upward directed flows that have
  velocities up to 60km/sec seen against the background of photospheric
  granulation with inclusions of BPs. The corresponding movie shows
  reveals significant dynamics associated with these rosette like
  structures stemming from clusters of BPs.

---------------------------------------------------------
Title: Relationship between orientations of halo CMEs and the
    underlying filament / active regions
Authors: Kilcik, A.; Yurchyshyn, V.; Abramenko, V.; Goode, P. R.
2010AGUFMSH51C1684K    Altcode:
  Coronal mass ejections (CMEs) are the most important objects of space
  weather studies. Although they have been at focus of many studies for
  a long time now, there are still many unanswered questions. Here we
  focus on the possible relationship between the direction of CME rotation
  and the prevailing magnetic twist of the CME's source region. We could
  determine the predominant helicity for 45 filaments and active regions
  that appeared on both hemispheres of the Sun. We thus further confirm
  that 76% of all source regions in the southern hemisphere were “S”
  shaped, while 79% of northern hemisphere events were reverse “S”
  (“Z”) shaped. These ratios agree with the well known hemispheric
  segregation rule. According to theoretical considerations, (Green,
  et al. 2007; Lynch, et al. 2009) CMEs, associated with eruption of
  “S” (“Z') shaped structures are expected to rotate clockwise
  (counterclockwise). Here we report that 67% of all source regions in
  the southern hemisphere showed a predominant twist that agreed with
  the direction of rotation of the corresponding CMEs. In the northern
  hemisphere this ration was 63%. These findings may significantly
  improve our understanding of CME evolution and their connection to
  magnetic clouds. They may are affect our ability to predict severity
  of geomagnetic storms.

---------------------------------------------------------
Title: Size and Life Time Distributions of Bright Points in the
    Quiet Sun Photosphere
Authors: Abramenko, V.; Yurchyshyn, V.; Goode, P. R.
2010AGUFMSH31C1806A    Altcode:
  We present results of two-hour uninterrupted observations of solar
  granulation obtained at excellent seeing conditions on August 3, 2010
  with the largest ground-based new solar telescope (NST) operating
  at Big Bear Solar observatory. Adaptive optics corrected data were
  acquired with a broad-band TiO filter (centered at a wavelength of
  705.7 nm). The time cadence was 10s and the pixel size was 0.0375
  arcsec. Photospheric bright points (BPs) were automatically detected
  and traced. We find that NST TiO BPs are co-spatial with those visible
  in Hinode/SOT G-band images. In cases where Hinode/SOT detects one
  large BP, NST shows several fully resolved BPs. Extended filigree
  features running along intergranular lanes appear in NST images clearly
  fragmented into separate BPs. The distribution function of the NST
  BPs size is exponential and extends to the diffraction limit of NST
  (77 km) without any saturation. The life time distribution function
  follows a power law with an index of -1.9. About 98.6% of all detected
  BPs live shorter than 120 s, and the most persistent BP lasted for
  44 minutes. The size and the maximum intensity of BPs were found to
  be proportional to the life time. Results are discussed in framework
  of coronal heating and turbulent dynamo. Left - Hinode G-band image
  obtained on 2010 August 3 at 12:22:11 UT (pixel size 0.109"). Right -
  NST TiO image obtained on 2010 August 3 at 12:22:10 UT. Both images
  cover the same area of 18.8" x 18.8" on the Sun. <P />PDFs of the BPs
  diameter calculated from NST TiO images (black) and from Hinode/SOT
  G-band images (by Utz et al. 2009, blue).

---------------------------------------------------------
Title: Statistical Distribution of Size and Lifetime of Bright Points
    Observed with the New Solar Telescope
Authors: Abramenko, Valentyna; Yurchyshyn, Vasyl; Goode, Philip;
   Kilcik, Ali
2010ApJ...725L.101A    Altcode: 2010arXiv1012.1584A
  We present results of 2 hr non-interrupted observations of solar
  granulation obtained under excellent seeing conditions with the largest
  aperture ground-based solar telescope—the New Solar Telescope
  (NST)—of Big Bear Solar Observatory. Observations were performed
  with adaptive optics correction using a broadband TiO filter in the
  705.7 nm spectral line with a time cadence of 10 s and a pixel size
  of 0farcs0375. Photospheric bright points (BPs) were detected and
  tracked. We find that the BPs detected in NST images are cospatial with
  those visible in Hinode/SOT G-band images. In cases where Hinode/SOT
  detects one large BP, NST detects several separated BPs. Extended
  filigree features are clearly fragmented into separate BPs in NST
  images. The distribution function of BP sizes extends to the diffraction
  limit of NST (77 km) without saturation and corresponds to a log-normal
  distribution. The lifetime distribution function follows a log-normal
  approximation for all BPs with lifetime exceeding 100 s. A majority
  of BPs are transient events reflecting the strong dynamics of the
  quiet Sun: 98.6% of BPs live less than 120 s. The longest registered
  lifetime was 44 minutes. The size and maximum intensity of BPs were
  found to be proportional to their lifetimes.

---------------------------------------------------------
Title: Chromospheric Signatures of Small-scale Flux Emergence as
    Observed with New Solar Telescope and Hinode Instruments
Authors: Yurchyshyn, V. B.; Goode, P. R.; Abramenko, V. I.; Chae,
   J.; Cao, W.; Andic, A.; Ahn, K.
2010ApJ...722.1970Y    Altcode: 2011arXiv1102.1034Y
  With the ever-increasing influx of high-resolution images of the solar
  surface obtained at a multitude of wavelengths, various processes
  occurring at small spatial scales have become a greater focus of our
  attention. Complex small-scale magnetic fields have been reported that
  appear to have enough stored energy to heat the chromosphere. While
  significant progress has been made in understanding small-scale
  phenomena, many specifics remain elusive. We present here a detailed
  study of a single event of disappearance of a magnetic dipole and
  associated chromospheric activity. Based on New Solar Telescope Hα
  data and Hinode photospheric line-of-sight magnetograms and Ca II
  H images, we report the following. (1) Our analysis indicates that
  even very small dipoles (elements separated by about 0farcs5 or less)
  may reach the chromosphere and trigger non-negligible chromospheric
  activity. (2) Careful consideration of the magnetic environment where
  the new flux is deposited may shed light on the details of magnetic
  flux removal from the solar surface. We argue that the apparent
  collision and disappearance of two opposite polarity elements may
  not necessarily indicate their cancellation (i.e., reconnection,
  emergence of a "U" tube, or submergence of Ω loops). In our case, the
  magnetic dipole disappeared by reconnecting with overlying large-scale
  inclined plage fields. (3) Bright points (BPs) seen in off-band Hα
  images are very well correlated with the Ca II H BPs, which in turn
  are cospatial with G-band BPs. We further speculate that, in general,
  Hα BPs are expected to be cospatial with photospheric BPs; however,
  a direct comparison is needed to refine their relationship.

---------------------------------------------------------
Title: Intermittency and Multifractality Spectra of the Magnetic
    Field in Solar Active Regions
Authors: Abramenko, Valentyna; Yurchyshyn, Vasyl
2010ApJ...722..122A    Altcode: 2010arXiv1012.1586A
  We present the results of a study of intermittency and multifractality
  of magnetic structures in solar active regions (ARs). Line-of-sight
  magnetograms for 214 ARs of different flare productivity observed at
  the center of the solar disk from 1997 January until 2006 December
  are utilized. Data from the Michelson Doppler Imager (MDI) instrument
  on board the Solar and Heliospheric Observatory operating in the high
  resolution mode, the Big Bear Solar Observatory digital magnetograph,
  and the Hinode SOT/SP instrument were used. Intermittency spectra
  were derived from high-order structure functions and flatness
  functions. The flatness function exponent is a measure of the degree
  of intermittency. We found that the flatness function exponent at
  scales below approximately 10 Mm is correlated with flare productivity
  (the correlation coefficient is -0.63). The Hinode data show that the
  intermittency regime is extended toward small scales (below 2 Mm) as
  compared to the MDI data. The spectra of multifractality, derived from
  the structure functions and flatness functions, are found to be broader
  for ARs of higher flare productivity as compared to those of low flare
  productivity. The magnetic structure of high-flaring ARs consists of
  a voluminous set of monofractals, and this set is much richer than
  that for low-flaring ARs. The results indicate the relevance of the
  multifractal organization of the photospheric magnetic fields to the
  flaring activity. The strong intermittency observed in complex and
  high-flaring ARs is a hint that we observe a photospheric imprint of
  enhanced sub-photospheric dynamics.

---------------------------------------------------------
Title: Magnetic Energy Spectra in Solar Active Regions
Authors: Abramenko, Valentyna; Yurchyshyn, Vasyl
2010ApJ...720..717A    Altcode: 2010arXiv1007.3702A
  Line-of-sight magnetograms for 217 active regions (ARs) with different
  flare rates observed at the solar disk center from 1997 January until
  2006 December are utilized to study the turbulence regime and its
  relationship to flare productivity. Data from the SOHO/MDI instrument
  recorded in the high-resolution mode and data from the BBSO magnetograph
  were used. The turbulence regime was probed via magnetic energy spectra
  and magnetic dissipation spectra. We found steeper energy spectra for
  ARs with higher flare productivity. We also report that both the power
  index, α, of the energy spectrum, E(k) ~ k <SUP>-α</SUP>, and the
  total spectral energy, W = ∫E(k)dk, are comparably correlated with the
  flare index, A, of an AR. The correlations are found to be stronger than
  those found between the flare index and the total unsigned flux. The
  flare index for an AR can be estimated based on measurements of α and
  W as A = 10<SUP> b </SUP>(αW)<SUP> c </SUP>, with b = -7.92 ± 0.58
  and c = 1.85 ± 0.13. We found that the regime of the fully developed
  turbulence occurs in decaying ARs and in emerging ARs (at the very
  early stage of emergence). Well-developed ARs display underdeveloped
  turbulence with strong magnetic dissipation at all scales.

---------------------------------------------------------
Title: Evidence of Filament Upflows Originating from Intensity
    Oscillations on the Solar Surface
Authors: Cao, Wenda; Ning, Zongjun; Goode, Philip R.; Yurchyshyn,
   Vasyl; Ji, Haisheng
2010ApJ...719L..95C    Altcode:
  A filament footpoint rooted in an active region (NOAA 11032) was well
  observed for about 78 minutes with the 1.6 m New Solar Telescope at the
  Big Bear Solar Observatory on 2009 November 18 in Hα ±0.75 Å. This
  data set had high cadence (~15 s) and high spatial resolution (~0farcs1)
  and offered a unique opportunity to study filament dynamics. As in
  previous findings from space observations, several dark intermittent
  upflows were identified, and they behave in groups at isolated locations
  along the filament. However, we have two new findings. First, we
  find that the dark upflows propagating along the filament channel are
  strongly associated with the intensity oscillations on the solar surface
  around the filament footpoints. The upflows start at the same time as
  the peak in the oscillations, illustrating that the upflow velocities
  are well correlated with the oscillations. Second, the intensity of
  one of the seven upflows detected in our data set exhibits a clear
  periodicity when the upflow propagates along the filament. The periods
  gradually vary from ~10 to ~5 minutes. Our results give observational
  clues on the driving mechanism of the upflows in the filament.

---------------------------------------------------------
Title: Oscillatory Behavior in the Quiet Sun Observed with the New
    Solar Telescope
Authors: Anđić, A.; Goode, P. R.; Chae, J.; Cao, W.; Ahn, K.;
   Yurchyshyn, V.; Abramenko, V.
2010ApJ...717L..79A    Altcode: 2010arXiv1007.0272A
  Surface photometry of the quiet Sun has achieved an angular resolution
  of 0farcs1 with the New Solar Telescope at Big Bear Solar Observatory,
  revealing that a disproportionate fraction of the oscillatory events
  appear above observed bright point-like structures. During the tracking
  of these structures, we noted that the more powerful oscillatory events
  are cospatial with them, indicating that observed flux tubes may be
  the source of many observed oscillatory events.

---------------------------------------------------------
Title: Flare Productivity Forecast Based on the Magnetic Energy
    Spectrum of Active Regions
Authors: Abramenko, Valentyna; Yurchyshyn, Vasyl
2010shin.confE.104A    Altcode:
  Line-of-sight magnetograms for 217 active regions (ARs) of different
  flare rate observed at the solar disk center from January 1997 until
  December 2006 are utilized to study the turbulence regime and its
  relationship to the flare productivity. Data from SOHO/MDI instrument
  recorded in the high resolution mode were used. The turbulence regime
  was probed via magnetic energy spectra and magnetic dissipation
  spectra. We found steeper energy spectra for ARs of higher flare
  productivity. We also report that both the power index, α, of the
  energy spectrum, E(k)= const k^{-α}, and the total spectral energy,
  W=\int E(k)dk, are comparably correlated with the flare index, A,
  of an active region. The flare index for an AR can be forecasted
  based on measurements of α and W as A=10^b (α W)^c, with b=-7.92
  ± 0.58 and c=1.85 ± 0.13. We find that regime of the classical
  fully-developed turbulence occurs in decaying ARs and in emerging
  ARs only at the very early stage of emergence. Well-developed ARs
  display under-developed turbulence with strong magnetic dissipation
  at all scales. The signature of under-developed turbulence indicates
  that free cascading of energy from large to small scales is no longer
  possible in mature active regions, and active region can no longer
  evolve through series of quasi-stable states. Fraction of energy now
  dissipates "along the way" via burst like energy release, a process
  know as flaring in an active region.

---------------------------------------------------------
Title: The NST: First results and some lessons for ATST and EST
Authors: Goode, P. R.; Coulter, R.; Gorceix, N.; Yurchyshyn, V.;
   Cao, W.
2010AN....331..620G    Altcode:
  In January 2009, first light observations with the NST (New Solar
  Telescope) in Big Bear Solar Observatory (BBSO) were made. NST has a
  1.7 m primary with a 1.6 m clear aperture. First observational results
  in TiO and Hα are shown and discussed. The NST primary mirror is the
  most aspheric telescope mirror deployed to date. The NST is early in its
  commissioning, and the plans for this phase will be sketched. Lessons
  learned in building and implementing the NST are germane for the ATST
  and EST telescopes and will be discussed. The NST has an off-axis
  Gregorian configuration consisting of a parabolic primary, heat-stop,
  elliptical secondary and diagonal flats. The focal ratio of the
  primary mirror is f/2.4. The working wavelength range covers from 0.4
  to 1.7 μm in the Coudé Lab beneath the telescope and all wavelengths
  including the far infrared at the Nasmyth focus on the dome floor.

---------------------------------------------------------
Title: Small Scale Chromospheric Dynamics Detected With The New
    Solar Telescope In Big Bear
Authors: Yurchyshyn, Vasyl B.
2010AAS...21630504Y    Altcode:
  High resolution observations of quiet Sun areas obtained with the
  New Solar Telescope (NST) in Big Bear Solar Observatory revealed
  surprisingly storming small-scale chromospheric dynamics. We thus
  discovered tiny chromospheric jets originating in the ubiquitous
  lanes that surround individual granules characterizing the solar
  surface. These jets do not appear to be exclusively associated with
  photospheric bright points and/or vertices of the intergranular
  lanes. They seem to have sufficient energy to resolve the mystery
  of why the overlying chromosphere is hotter than the photosphere. We
  will further address the nature of these chromospheric jets and their
  relationship to ambient magnetic fields by combining high resolution
  data from NST instruments and Hinode observatory.

---------------------------------------------------------
Title: Relationship Between Earth-Directed Solar Eruptions and
Magnetic Clouds at 1 AU: A Brief Review
Authors: Yurchyshyn, Vasyl; Tripathi, Durgesh
2010aogs...21...51Y    Altcode: 2009arXiv0904.2366Y
  We review relationships between coronal mass ejections (CMEs), EIT
  post eruption arcades, and the coronal neutral line associated with
  global magnetic field and magnetic clouds near the Earth. Our previous
  findings indicate that the orientation of a halo CME elongation may
  correspond to the orientation of the underlying flux rope. Here we
  revisit these preliminary reports by comparing orientation angles
  of elongated LASCO CMEs, both full and partial halos, to the post
  eruption arcades. Based on 100 analysed events, it was found that the
  overwhelming majority of halo CMEs are elongated in the direction of
  the axial field of the post eruption arcades. Moreover, this conclusion
  also holds for partial halo CMEs as well as for events that originate
  further from the disk center. This suggests that the projection effect
  does not drastically change the appearance of full and partial halos
  and their images still bear reliable information about the underlying
  magnetic fields. We also compared orientations of the erupted fields
  near the Sun and in the interplanetary space and found that the local
  tilt of the coronal neutral line at 2.5 solar radii is well correlated
  with the magnetic cloud axis measured near the Earth. We suggest that
  the heliospheric magnetic fields significantly affect the propagating
  ejecta. Sometimes, the ejecta may even rotate so that its axis locally
  aligns itself with the heliospheric current sheet.

---------------------------------------------------------
Title: Highest Resolution Observations of the Quietest Sun
Authors: Goode, Philip R.; Yurchyshyn, Vasyl; Cao, Wenda; Abramenko,
   Valentyna; Andic, Aleksandra; Ahn, Kwangsu; Chae, Jongchul
2010ApJ...714L..31G    Altcode:
  Highest resolution observations made with the new 1.6 m aperture solar
  telescope in Big Bear Solar Observatory during this time of historic
  inactivity on the Sun reveal new insights into the small-scale dynamics
  of the Sun's photosphere. The telescope's unprecedented resolution
  enabled us to observe that the smallest scale photospheric magnetic
  field seems to come in isolated points in the dark intergranular lanes,
  rather than the predicted continuous sheets confined to the lanes, and
  the unexpected longevity of the bright points implies a deeper anchoring
  than predicted. Further, we demonstrated for the first time that the
  photospheric plasma motion and magnetic fields are in equipartition
  over a wide dynamic range, and both cascade energy to ever-smaller
  scales according to classical Kolmogorov turbulence theory. Finally,
  we discovered tiny jet-like features originating in the dark lanes that
  surround the ubiquitous granules that characterize the solar surface.

---------------------------------------------------------
Title: Low-Latitude Coronal Holes at the Minimum of the 23rd Solar
    Cycle
Authors: Abramenko, Valentyna; Yurchyshyn, Vasyl; Linker, Jon; Mikić,
   Zoran; Luhmann, Janet; Lee, Christina O.
2010ApJ...712..813A    Altcode: 2010arXiv1002.1685A
  Low- and mid-latitude coronal holes (CHs) observed on the Sun during
  the current solar activity minimum (from 2006 September 21, Carrington
  rotation (CR) 2048, to 2009 June 26, CR 2084) were analyzed using Solar
  and Heliospheric Observatory/Extreme ultraviolet Imaging Telescope and
  STEREO-A SECCHI EUVI data. From both the observations and Potential
  Field Source Surface modeling, we find that the area occupied by
  CHs inside a belt of ±40° around the solar equator is larger in
  the current 2007 solar minimum relative to the similar phase of the
  previous 1996 solar minimum. The enhanced CH area is related to a
  recurrent appearance of five persistent CHs, which survived during 7-27
  solar rotations. Three of the CHs are of positive magnetic polarity
  and two are negative. The most long-lived CH was being formed during
  2 days and existed for 27 rotations. This CH was associated with fast
  solar wind at 1 AU of approximately 620 ± 40 km s<SUP>-1</SUP>. The
  three-dimensional magnetohydrodynamic modeling for this time period
  shows an open field structure above this CH. We conclude that the global
  magnetic field of the Sun possessed a multi-pole structure during
  this time period. Calculation of the harmonic power spectrum of the
  solar magnetic field demonstrates a greater prevalence of multi-pole
  components over the dipole component in the 2007 solar minimum compared
  to the 1996 solar minimum. The unusual large separation between the
  dipole and multi-pole components is due to the very low magnitude
  of the dipole component, which is three times lower than that in the
  previous 1996 solar minimum.

---------------------------------------------------------
Title: Vorticity of Granular Flows from NST Observations
Authors: Pevtsov, A. A.; Abramenko, V.; Yurchyshyn, V.; Goode, P. R.
2009AGUFMSH53B..04P    Altcode:
  We use observations taken with the New Solar Telescope (NST) at Big
  Bear Solar Observatory, the world largest solar optical telescope with
  diffraction limited spatial resolution of 0.06 arc seconds, to study
  vorticity of granular flows in quiet Sun areas. We employ sequence
  of images observed with TiO (705.7 nm) filter with time cadence
  of 30 seconds. The atmospheric seeing effects were removed using
  speckle-reconstruction technique. We compare vorticity of granular
  flows and intergranular vortices, and discuss our findings in the
  framework of surface (turbulent) dynamo.

---------------------------------------------------------
Title: SMALL SCALE DYNAMICS IN THE QUIESCENT CHROMOSPHERE AS SEEN
    IN NST DATA
Authors: Yurchyshyn, V.
2009AGUFMSH53B..03Y    Altcode:
  High resolution NST data obtained in the blue wing (-0.75Å) of the
  H-alpha spectral line show the presence of surprisingly numerous
  small-scale bright emission features nearly evenly distributed over
  the field of view. While larger features often exhibit association
  with H-alpha jets, smaller events (size &lt; 0.5 arcsec) are not
  accompanied by any detectable plasma flows. We will present results
  from a statistical study of these emission features and discuss life
  time of these events, size, their distribution relative to the magnetic
  field and the association with the plasma jets.

---------------------------------------------------------
Title: Parameters of the Magnetic Flux inside Coronal Holes
Authors: Abramenko, Valentyna; Yurchyshyn, Vasyl; Watanabe, Hiroko
2009SoPh..260...43A    Altcode: 2009arXiv0908.2460A
  The parameters of the magnetic flux distribution inside low-latitude
  coronal holes (CHs) were analyzed. A statistical study of 44 CHs
  based on Solar and Heliospheric Observatory (SOHO)/MDI full disk
  magnetograms and SOHO/EIT 284 Å images showed that the density of
  the net magnetic flux, B<SUB>net</SUB>, does not correlate with the
  associated solar wind speeds, V<SUB>x</SUB>. Both the area and net flux
  of CHs correlate with the solar wind speed and the corresponding spatial
  Pearson correlation coefficients are 0.75 and 0.71, respectively. A
  possible explanation for the low correlation between B<SUB>net</SUB>
  and V<SUB>x</SUB> is proposed. The observed non-correlation might
  be rooted in the structural complexity of the magnetic field. As a
  measure of the complexity of the magnetic field, the filling factor,
  f(r), was calculated as a function of spatial scales. In CHs, f(r)
  was found to be nearly constant at scales above 2 Mm, which indicates a
  monofractal structural organization and smooth temporal evolution. The
  magnitude of the filling factor is 0.04 from the Hinode SOT/SP data
  and 0.07 from the MDI/HR data. The Hinode data show that at scales
  smaller than 2 Mm, the filling factor decreases rapidly, which means
  a multifractal structure and highly intermittent, burst-like energy
  release regime. The absence of the necessary complexity in CH magnetic
  fields at scales above 2 Mm seems to be the most plausible reason
  why the net magnetic flux density does not seem to be related to the
  solar wind speed: the energy release dynamics, needed for solar wind
  acceleration, appears to occur at small scales below 1 Mm.

---------------------------------------------------------
Title: Rotation of White-light Coronal Mass Ejection Structures as
    Inferred from LASCO Coronagraph
Authors: Yurchyshyn, Vasyl; Abramenko, Valentyna; Tripathi, Durgesh
2009ApJ...705..426Y    Altcode:
  Understanding the connection between the magnetic configurations of a
  coronal mass ejection (CME) and their counterpart in the interplanetary
  medium is very important in terms of space weather predictions. Our
  previous findings indicate that the orientation of a halo CME elongation
  may correspond to the orientation of the underlying flux rope. Here
  we further explore these preliminary results by comparing orientation
  angles of elongated LASCO CMEs, both full and partial halos, to the
  EUV Imaging Telescope post-eruption arcades (PEAs). By analyzing a
  sample of 100 events, we found that the overwhelming majority of CMEs
  are elongated in the direction of the axial field of PEAs. During their
  evolution, CMEs appear to rotate by about 10° for most of the events
  (70%) with about 30°-50° for some events, and the corresponding time
  profiles display regular and gradual changes. It seems that there is
  a slight preference for the CMEs to rotate toward the solar equator
  and heliospheric current sheet (59% of the cases). We suggest that the
  rotation of the ejecta may be due to the presence of a heliospheric
  magnetic field, and it could shed light on the problems related to
  connecting solar surface phenomena to their interplanetary counterparts.

---------------------------------------------------------
Title: Analyses of magnetic field structures for active region 10720
    using a data-driven 3D MHD model
Authors: Wu, S. T.; Wang, A. H.; Gary, G. Allen; Kucera, Ales; Rybak,
   Jan; Liu, Yang; Vrśnak, Bojan; Yurchyshyn, Vasyl
2009AdSpR..44...46W    Altcode:
  In order to understand solar eruptive events (flares and CMEs) we
  need to investigate the changes at the solar surface. Thus, we use
  a data-driven, three-dimensional magnetohydrodynamic (MHD) model to
  analyze a flare and coronal mass ejection productive active region,
  AR 10720 on January 15, 2005. The measured magnetic field from Big
  Bear Solar Observatory (BBSO) digital vector magnetograph (DGVM) was
  used to model the non-potential coronal magnetic field changes and the
  evolution of electric current before and after the event occurred. The
  numerical results include the change of magnetic flux ( Φ), the net
  electric current ( I<SUB>N</SUB>), the length of magnetic shear of the
  main neutral line ( L<SUB>ss</SUB>), the flux normalized measure of
  the field twist (α={μI<SUB>N</SUB>}/{Φ}) with μ being the magnetic
  permeability. The current helicity ( H<SUB>c</SUB>) injected into the
  corona and the photospheric surface velocity are also computed. The
  characteristic parameters of the buildup process before the event and
  the decay process after the event are investigated and the amount of
  magnetic energy converted to drive the event is estimated.

---------------------------------------------------------
Title: Properties of Solar Active Regions and Their Relationship
with Solar Eruption: a Statistical Study
Authors: Liu, Yang; Akiyama, S.; Gopalswamy, N.; Mason, J.; Nitta,
   N.; Tylka, A.; Yashiro, S.; Yurchyshyn, V.
2009SPD....40.0920L    Altcode:
  Using magnetograms taken by SOHO/MDI, we have calculated some parameters
  for solar active regions, and explored possible relationships between
  them and solar eruptions. The parameters of active regions we studied
  are magnetic flux, net flux, potential field energy, orientation
  and separation. We also estimated decay index of magnetic field
  overlying the neutral line, and the configuration of ambient field
  under which the active region sits. The data used were taken from
  1996 to 2005. With these results as a reference, we studied the active
  regions that produced the large solar energetic particle (SEP) events,
  or produced ground level enhancement (GLE) events. Comparison is also
  made between the active regions that produced full eruption and confine
  eruption (based on an event list published by Yashiro et al 2005, JGR,
  11012S05Y). We present our results here, together with a discussion.

---------------------------------------------------------
Title: Statistical Assessment of Photospheric Magnetic Features in
    Imminent Solar Flare Predictions
Authors: Song, Hui; Tan, Changyi; Jing, Ju; Wang, Haimin; Yurchyshyn,
   Vasyl; Abramenko, Valentyna
2009SoPh..254..101S    Altcode:
  In this study we use the ordinal logistic regression method to establish
  a prediction model, which estimates the probability for each solar
  active region to produce X-, M-, or C-class flares during the next
  1-day time period. The three predictive parameters are (1) the total
  unsigned magnetic flux T<SUB>flux</SUB>, which is a measure of an
  active region's size, (2) the length of the strong-gradient neutral
  line L<SUB>gnl</SUB>, which describes the global nonpotentiality of an
  active region, and (3) the total magnetic dissipation E<SUB>diss</SUB>,
  which is another proxy of an active region's nonpotentiality. These
  parameters are all derived from SOHO MDI magnetograms. The ordinal
  response variable is the different level of solar flare magnitude. By
  analyzing 174 active regions, L<SUB>gnl</SUB> is proven to be the
  most powerful predictor, if only one predictor is chosen. Compared
  with the current prediction methods used by the Solar Monitor at the
  Solar Data Analysis Center (SDAC) and NOAA's Space Weather Prediction
  Center (SWPC), the ordinal logistic model using L<SUB>gnl</SUB>,
  T<SUB>flux</SUB>, and E<SUB>diss</SUB> as predictors demonstrated
  its automatic functionality, simplicity, and fairly high prediction
  accuracy. To our knowledge, this is the first time the ordinal logistic
  regression model has been used in solar physics to predict solar flares.

---------------------------------------------------------
Title: Relationship betwwen of Coronal Mass Ejections and EIT Post
    Flare Arcades
Authors: Yurchyshyn, V.
2008AGUFMSH13B1551Y    Altcode:
  Our recent study indicates the orientation of a halo CME elongation
  may correspond to the orientation of the underlying flux rope. This is
  a continuation of the research and here we compare orientation angles
  of elongated LASCO CMEs, both halo and partial to the EIT post eruption
  arcades (PEA). Data for 100 events had been analyzed and er report the
  following: i) it is further supported that majority of halo CMEs are
  elongated in the direction of the axial field of PEA arcades; ii) this
  relationship holds true for partial CME and those events that originate
  further from the disk center. There is also an indication that events
  in the northern hemisphere generally exhibit better correlation that
  those in the southern hemisphere.

---------------------------------------------------------
Title: Intermittency in the Photosphere and Corona above an Active
    Region
Authors: Abramenko, Valentyna; Yurchyshyn, Vasyl; Wang, Haimin
2008ApJ...681.1669A    Altcode: 2009arXiv0903.2882A
  Recent studies have demonstrated without doubt that the magnetic field
  in the photosphere and corona is an intermittent structure, opening
  new views of the underlying physics. In particular, such problems
  as the existence in the corona of localized areas with extremely
  strong resistivity (required to explain magnetic reconnection at all
  scales) and the interchange between small and large scales (required
  in the study of photospheric-coronal coupling), to name a few, can be
  easily captured by the concept of intermittency. This study focuses
  on simultaneous time variations of intermittency properties derived
  in the photosphere, chromosphere, and corona. We analyze data for
  NOAA Active Region 10930 acquired between 2006 December 8, 12:00 UT,
  and December 13, 18:45 UT. Photospheric intermittency is inferred
  from Hinode magnetic field measurements, while intermittency in the
  transition region and corona is derived from Nobeyama 9 GHz radio
  polarization measurements and high-cadence Hinode XRT (thin-Be) data,
  as well as GOES 1-8 Å flux. The photospheric dynamics and its possible
  relationship with the intermittency variations are also analyzed
  by calculating the kinetic vorticity. In this case study, we find
  the following chain of events: The intermittency of the photospheric
  magnetic field peaked after the specific kinetic vorticity of plasma
  flows in the active region reached its maximum (4 hr time delay). In
  turn, a gradual increase of coronal intermittency occurred after the
  peak of the photospheric intermittency. The time delay between the peak
  of photospheric intermittency and the occurrence of the first strong
  (X3.4) flare was approximately 1.3 days. Our analysis seems to suggest
  that the enhancement of intermittency/complexity first occurs in the
  photosphere and is later transported toward the corona.

---------------------------------------------------------
Title: Statistical Study of Orientations of Coronal Mass Ejections
    and EIT Flare Arcades
Authors: Yurchyshyn, V.; Tripathi, D.
2008AGUSMSH43A..01Y    Altcode:
  Coronal mass ejections (CMEs) and their interplanetary counterparts,
  interplanetary CMEs (ICMEs) usually exhibit a complex structure that
  very often includes a magnetic cloud (MC), which is thought to be
  a magnetic fluxrope. Our recent study indicates the orientation of a
  halo CME elongation may correspond to the orientation of the underlying
  flux rope. This is a continuation of the research and here we compare
  orientation angles of elongated LASCO CMEs, both halo and partial to the
  EIT post eruption arcades (PEA). Data for 100 events had been analyzed
  and er report the following: i) it is further supported that majority
  of halo CMEs are elongated in the direction of the aixial field of
  PEA arcades. This relationship is found to be weeker for partial CME
  and those events that originate further from the disk center. There
  also is an indication that events in the northern hemisphere generally
  exhibit better correlation that those in the southern hemisphere.

---------------------------------------------------------
Title: Intermittency in the photosphere and corona as derived from
    the Hinode data
Authors: Abramenko, V.; Yurchyshyn, V.; Wang, H.
2008AGUSMSP21B..01A    Altcode:
  Recent studies undoubtedly demonstrate that the magnetic fields in the
  photosphere and corona are strongly non-Gaussian and can be represented
  as intermittent structures, which offers new views on the underlying
  physics. In particular, such problems as the existence in the corona of
  localized areas with extremely strong resistivity (required to explain
  magnetic reconnection of all scales) and the interchange between
  small and large scales (required in study of the photosphere/corona
  coupling), to name a few, can be easily captured by the concept of
  intermittency. This study is focused on simultaneous time variations
  of intermittency properties derived in the photosphere, chromosphere
  and corona. We analyzed data for NOAA AR 10930 acquired between Dec 08,
  2006 12:00 UT and Dec 13, 2006 18:45 UT. Photospheric intermittency was
  inferred from Hinode magnetic field measurements, while intermittency
  in the transition region and corona was derived from Nobeyama 9 GHz
  radio polarization measurements, high cadence Hinode/XRT/Be-thin data
  as well as GOES 1-8Å~ flux. Photospheric dynamics and its possible
  relationship with the intermittency variations were also analyzed by
  calculating the kinetic vorticity. For this case study we found the
  following chain of events. Intermittency of the photospheric magnetic
  field peaked after the specific kinetic vorticity of plasma flows
  in the AR reached its maximum level (4 hour time delay). In turn,
  gradual increase of coronal intermittency occurred after the peak
  of the photospheric intermittency. The time delay between the peak
  of photospheric intermittency and the occurrence of the first strong
  (X3.4) flare was approximately 1.3 days. Our analysis seems to suggest
  that the enhancement of intermittency/complexity first occurs in the
  photosphere and is later transported toward the corona.

---------------------------------------------------------
Title: Global High Resolution Halpha Network Observations During
    the Whole Heliosphere Interval Campaign.
Authors: Yurchyshyn, V.
2008AGUSMSH51A..03Y    Altcode:
  We will present the full disk Halpha data acquired by the Global
  High Resolution Halpha Network during the Whole Heliosphere Interval
  Campaign. The network includes seven stations located in China (2),
  Europe (4) and USA (1). We will also briefly describe the layout and
  data from the new BBSO full disk halpha telescope.

---------------------------------------------------------
Title: The evolution of vector magnetic field associated with major
    flares in NOAA AR10656
Authors: Wang, Shuo; Deng, Yuanyong; Jain, Rajmal; Yurchyshyn, Vasyl;
   Wang, Haimin; Liu, Yuanyuan; Yang, Zhiliang
2008JApA...29...57W    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Relationship between EIT Posteruption Arcades, Coronal Mass
    Ejections, the Coronal Neutral Line, and Magnetic Clouds
Authors: Yurchyshyn, Vasyl
2008ApJ...675L..49Y    Altcode: 2007arXiv0710.1292Y
  There is observational evidence that the elongation of an Earth-directed
  coronal mass ejection (CME) may indicate the orientation of the
  underlying erupting flux rope. In this study, we compare orientations of
  CMEs, magnetic clouds (MCs), EIT (EUV Imaging Telescope) posteruption
  arcades, and the coronal neutral line (CNL). We report on good
  correlations between (1) the directions of the axial field in the
  EIT arcades and the elongations of halo CMEs, and (2) the tilt of the
  CNL and MC axis orientations. We found that majority of the eruptions
  that had EIT arcades, CMEs, and MCs similarly oriented also had the
  CNL co-aligned with them. On the other hand, those events that showed
  no agreement between orientations of the EIT arcades, CMEs, and MCs
  had their MCs aligned with the CNL. We speculate that the axis of the
  ejecta may be rotated in such a way that it is locally aligns itself
  with the heliospheric current sheet.

---------------------------------------------------------
Title: Successive Flaring during the 2005 September 13 Eruption
Authors: Wang, Haimin; Liu, Chang; Jing, Ju; Yurchyshyn, Vasyl
2007ApJ...671..973W    Altcode:
  We report a detailed analysis of successive flaring during the
  X1.5 event in the NOAA AR 0808 on 2005 September 13. We identify a
  filament lying at the southeast boundary of the active region as the
  physical linkage between the two flares in close succession. It is
  noticeable that the filament erupted ~13 minutes after the initial
  flare onset at ~19:22 UT near the central magnetic polarity inversion
  line (PIL). During this time period, the filament only showed a slow
  rising; meanwhile, a spatially associated large magnetic loop with one
  leg connecting to the initial flaring site began to brighten in the
  TRACE 195 Å channel. After ~19:35 UT, the filament abruptly erupted
  together with the bright TRACE loop. Besides the moving ribbons at
  the first flaring site, the filament eruption caused a secondary flare
  identified with another set of moving ribbons. This event thus provides
  a clear evidence for the successive flaring where the initial flare
  destabilizes the nearby flux loop system, leading to the filament
  eruption with the second flare. We also identify the initial flare
  core by finding rapid, irreversible enhancements of the photospheric
  transverse magnetic fields at a section of the PIL.

---------------------------------------------------------
Title: Calculation of Intermittency in the Photosphere and Corona
    From Hinode Data
Authors: Abramenko, V.; Yurchyshyn, V.
2007AGUFMSH34A..05A    Altcode:
  High spatial and temporal resolution observations of the photospheric
  magnetic field and solar corona, offered recently by Hinode instrument,
  provide us a unique opportunity to simultaneously estimate degree of
  intermittency in the photosphere and the corona and to track their
  variations in time. To do this, we adopted a flatness-function
  technique, where the slope of the function defines degree of
  intermittency. The function itself is calculated as the ratio of
  the sixth-order structure function to the cube of the second-order
  structure function. Three independent data sets, that were utilized
  to calculate the intermittency in the corona (XRT/Hinode, GOES, and
  Nobeyama 9.4 Hz polarization flux), showed a synchronous increase of
  intermittency during a 5-day time interval that ends with the occurrence
  of the X3.4 flare in the NOAA 10930. Photospheric intermittency,
  calculated from SOT-FG/Hinode magnetograms, peaked approximately 1.5
  days before the flare onset. The result allows to suggest a preceding
  gain of intermittency in the photosphere with a following transport
  of intermittency into the corona.

---------------------------------------------------------
Title: Relationship between Halo Coronal Mass Ejections, EIT Flare
    Arcades, Coronal Neutral Line and Magnetic Clouds
Authors: Yurchyshyn, V.
2007AGUFMSH23B..04Y    Altcode:
  Coronal mass ejections (CMEs) are the most important solar drivers of
  geomagnetic storms. Their interplanetary counterparts, interplanetary
  CMEs (ICMEs), can be detected in-situ, for example, by ACE and
  Wind spacecraft. An ICME usually exhibits a complex structure that
  very often includes a magnetic cloud (MC), which is thought to be a
  magnetic flux rope, capable of providing prolonged periods of southward
  interplanetary magnetic field at 1 AU. The magnitude of the storm
  depends, in general, on the orientation and intensity of the magnetic
  field in the ejecta. In this presentation we will discuss how the size
  of the geomagnetic storm can be predicted from coronagraph images. There
  is observational evidence that the orientation of a halo CME elongation
  corresponds to the orientation of the underlying flux rope, while the
  intensity of the magnetic field in an ejecta seems to be related to
  the CME speed. Here we compare orientation angles of elongated LASCO
  halo CMEs, EIT flare arcades (post flare loop system), the local tilt
  of the heliospheric current sheet and the corresponding MCs. We report
  that i) for about 64% of CME-ICME events, a good correspondence was
  found between the orientation angles of CMEs and MC; ii) 20 out of 25
  CMEs (80%) were oriented along the axis of the corresponding EIT flare
  arcade; and iii) 19 out of 25 (76%) of CMEs are co- aligned with the
  heliospheric current sheet at 2.5 solar radii. In the final part of
  the presentation we will discuss the applications of our findings to
  CME modeling, space weather forecast and possible future studies.

---------------------------------------------------------
Title: The Eruption from a Sigmoidal Solar Active Region on 2005
    May 13
Authors: Liu, Chang; Lee, Jeongwoo; Yurchyshyn, Vasyl; Deng, Na; Cho,
   Kyung-suk; Karlický, Marian; Wang, Haimin
2007ApJ...669.1372L    Altcode: 2007arXiv0707.2240L
  This paper presents a multiwavelength study of the M8.0 flare and
  its associated fast halo CME that originated from a bipolar NOAA
  AR 10759 on 2005 May 13. The source active region has a conspicuous
  sigmoid structure at the TRACE 171 Å channel as well as in the SXI
  soft X-ray images, and we mainly concern ourselves with the detailed
  process of the sigmoid eruption, as evidenced by the multiwavelength
  data ranging from Hα, WL, EUV/UV, radio, and hard X-rays (HXRs). The
  most important finding is that the flare brightening starts in the
  core of the active region earlier than that of the rising motion of
  the flux rope. This timing clearly addresses one of the main issues in
  the magnetic eruption onset of sigmoid, namely, whether the eruption
  is initiated by an internal tether cutting to allow the flux rope
  to rise upward, or a flux rope rises due to a loss of equilibrium to
  later induce tether cutting below it. Our high time cadence SXI and Hα
  data show that the first scenario is relevant to this eruption. As in
  other major findings, we have the RHESSI HXR images showing a change
  of the HXR source from a confined footpoint structure to an elongated
  ribbon-like structure after the flare maximum, which we relate to the
  sigmoid-to-arcade evolution. The radio dynamic spectrum shows a type II
  precursor that occurred at the time of expansion of the sigmoid and a
  drifting pulsating structure in the flare rising phase in HXRs. Finally,
  type II and III bursts are seen at the time of maximum HXR emission,
  simultaneous with the maximum reconnection rate derived from the flare
  ribbon motion in UV. We interpret these various observed properties
  with the runaway tether-cutting model proposed by Moore et al. in 2001.

---------------------------------------------------------
Title: Two-Dimensional Spectroscopy of Photospheric Shear Flows in
    a Small δ Spot
Authors: Denker, C.; Deng, N.; Tritschler, A.; Yurchyshyn, V.
2007SoPh..245..219D    Altcode: 2007arXiv0708.3490D
  In recent high-resolution observations of complex active regions,
  long-lasting and well-defined regions of strong flows were identified
  in major flares and associated with bright kernels of visible,
  near-infrared, and X-ray radiation. These flows, which occurred in the
  proximity of the magnetic neutral line, significantly contributed to
  the generation of magnetic shear. Signatures of these shear flows are
  strongly curved penumbral filaments, which are almost tangential to
  sunspot umbrae rather than exhibiting the typical radial filamentary
  structure. Solar active region NOAA 10756 was a moderately complex
  βδ sunspot group, which provided an opportunity to extend previous
  studies of such shear flows to quieter settings. We conclude that
  shear flows are a common phenomenon in complex active regions and δ
  spots. However, they are not necessarily a prerequisite condition for
  flaring. Indeed, in the present observations, the photospheric shear
  flows along the magnetic neutral line are not related to any change of
  the local magnetic shear. We present high-resolution observations of
  NOAA 10756 obtained with the 65-cm vacuum reflector at Big Bear Solar
  Observatory (BBSO). Time series of speckle-reconstructed white-light
  images and two-dimensional spectroscopic data were combined to study
  the temporal evolution of the three-dimensional vector flow field
  in the βδ sunspot group. An hour-long data set of consistent high
  quality was obtained, which had a cadence of better than 30 seconds
  and subarcsecond spatial resolution.

---------------------------------------------------------
Title: Relationship Between Orientations of Halo Coronal Mass
    Ejections, EIT Flare Arcades, Heliospheric Current Sheet and
    Magnetic Clouds
Authors: Yurchyshyn, Vasyl B.
2007AAS...210.2928Y    Altcode: 2007BAAS...39..325Y
  Coronal mass ejections (CMEs) are the most important solar drivers of
  geomagnetic storms. Their interplanetary counterparts, interplanetary
  CMEs (ICMEs), can be detected in-situ, for example, by ACE and
  Wind spacecraft. An ICME usually exhibits a complex structure that
  very often includes a magnetic cloud (MC), which is thought to be a
  magnetic flux rope, capable of providing prolonged periods of southward
  interplanetary magnetic field at 1 AU. In our recent study we found that
  the orientation of a halo CME elongation corresponds to the orientation
  of the underlying flux rope. This is a continuation of this recent
  research and here we compare orientation angles of elongated LASCO
  halo CMEs, EIT flare arcades (post flare loop system), the local tilt
  of the heliospheric current sheet and the corresponding MCs. We report
  that i) for about 64% of CME-ICME events, a good correspondence was
  found between the orientation angles of CMEs and MC; ii) 20 out of
  25 CMEs (80%) were oriented along the axis of the corresponding EIT
  flare arcade; and iii) 17 out of 25 (68%) of MCs are co-aligned with
  the heliospheric current sheet at 2.5 solar radii. In the final part
  of the presentation we will discuss the applications of our findings
  to CME modeling, space weather forecast and possible future studies.

---------------------------------------------------------
Title: Automatic Prediction of Super Geomagnetic Storms and Solar
    Flares
Authors: Song, Hui; Yurchyshyn, V.; Tan, C.; Jing, J.; Wang, H.
2007AAS...21010501S    Altcode: 2007BAAS...39..230S
  In this study we first investigated the relationship between magnetic
  structures of coronal mass ejection (CME) source regions and geomagnetic
  storms, in particular, the super storms when the D<SUB>st</SUB> index
  decreases below -200 nT. By examining all full halo CMEs that erupted
  between 1996 and 2004, we selected 73 events associated with M-class
  and X-class solar flares, which have a clearly identifiable source
  region. By analyzing daily full-disk MDI magnetograms, we found that
  the horizontal gradient of the line-of-sight magnetic field is a viable
  parameter to identify a flaring magnetic neutral line and thus can be
  used to predict the possible source region of CMEs. We report that
  for about 92% of super storms the orientation angle of the magnetic
  structures of source regions was found to be southward. Our findings
  demonstrate that this approach can be used to perform an automatic
  prediction of the occurrence of large X-class flares and super
  geomagnetic storms. <P />In order to further extend our prediction
  of flares, we next used the ordinal logistic regression method to
  establish a prediction model, which estimates the probability for each
  active region to produce X-, M- or C-class flares during the next 1-day
  time period. Three predictive parameters are: total unsigned magnetic
  flux T<SUB>flux</SUB>, the length of strong gradient neutral line
  L<SUB>gnl</SUB>, and total magnetic dissipation E<SUB>diss</SUB>. The
  ordinal response variable is the different level of solar flares
  magnitude. Compared the results with the current predictions methods
  used by NASA SDAC and NOAA SEC, the ordinal logistic model using
  L<SUB>gnl</SUB> and T<SUB>flux</SUB> as predictors demonstrated its
  automaticity, simpleness and fairly high prediction accuracy. To our
  knowledge, this is the first time the ordinal logistic regression
  model was used in solar physics to predict solar flares.

---------------------------------------------------------
Title: Filament Eruption after the Onset of the X1.5 Flare on 2005
    September 13
Authors: Wang, Haimin; Liu, C.; Jing, J.; Yurchyshyn, V.
2007AAS...210.9321W    Altcode: 2007BAAS...39..214W
  Erupting filaments usually play the role as the initial driver of
  flaring process preceding the subsequent flare emissions. In this
  Letter, we report a rare case that during the X1.5 flare on 2005
  September 13, a filament at the boundary of the NOAA AR 0808 erupted
  about 13 minutes after the flare onset at 19:22 UT near the central AR
  neutral line. During this time period, the filament only showed a slow
  rising; meanwhile, a spatially associated large magnetic loop with
  one leg connecting to the initial flaring site began to brighten in
  the TRACE 195A channel. After 19:35 UT, the filament abruptly erupted
  together with the bright TRACE loop. Besides the moving ribbons at the
  first flaring site, the filament eruption caused a secondary flare
  identified with another set of moving ribbons. We suggest possible
  triggering mechanisms for the initial flare and the eruption of the
  peripheral flux loop system, which leads to the sympathetic flaring.

---------------------------------------------------------
Title: On The Magnetic Flux Budget In Low-corona Magnetic Reconnection
    And Interplanetary Magnetic Flux Ropes
Authors: Qiu, Jiong; Hu, Q.; Howard, T. A.; Yurchyshyn, V. B.
2007AAS...210.2927Q    Altcode: 2007BAAS...39..142Q
  We present the first quantitative comparison between the total
  magnetic reconnection flux in the low-corona in the wake of coronal
  mass ejections (CMEs) and the magnetic flux in magnetic clouds
  (MCs) that reach 1AU 2 - 3 days after the CME onset. The total
  reconnection flux is measured from flare ribbons, and the MC flux
  is computed using in-situ observations at 1 AU, all ranging from
  10<SUP>20 </SUP>to 10<SUP>22</SUP> Mx. It is found that for the
  nine studied events in which the association between flares, CMEs,
  and MCs is identified, the MC flux is correlated with the total
  reconnection flux Φ<SUB>r</SUB>. Further, the poloidal (azimuthal)
  MC flux Φ<SUB>p</SUB> is comparable with the reconnection flux
  Φ<SUB>r</SUB> and the toroidal (axial) MC flux Φ<SUB>t</SUB> is a
  fraction of Φ<SUB>r</SUB>. Events associated with filament eruption
  do not exhibit a different Φ<SUB>r</SUB> - Φ<SUB>p</SUB> relation
  from events not accompanied by erupting filaments. The relations
  revealed between these independently measured physical quantities
  suggest that, for the studied samples, the magnetic flux and twist
  of interplanetary magnetic flux ropes, reflected by MCs, are highly
  relevant to low-corona magnetic reconnection during the eruption. We
  discuss the implications of this result for the formation mechanism
  of twisted magnetic flux ropes, namely, whether the helical structure
  of the magnetic flux rope is largely pre-existing or formed in-situ
  by low-corona magnetic reconnection. We also measure magnetic flux
  encompassed in coronal dimming regions (Φ<SUB>d</SUB>) and discuss its
  relation to the reconnection flux inferred from flare ribbons and MC
  flux. This work is supported by NSF grant ATM-0603789 and NASA grants
  NNG04GF47G, NNG06GA37G, and NNG06GD41G.

---------------------------------------------------------
Title: On the Magnetic Flux Budget in Low-Corona Magnetic Reconnection
    and Interplanetary Coronal Mass Ejections
Authors: Qiu, Jiong; Hu, Qiang; Howard, Timothy A.; Yurchyshyn,
   Vasyl B.
2007ApJ...659..758Q    Altcode:
  We present the first quantitative comparison between the total
  magnetic reconnection flux in the low corona in the wake of
  coronal mass ejections (CMEs) and the magnetic flux in magnetic
  clouds (MCs) that reach 1 AU 2-3 days after CME onset. The total
  reconnection flux is measured from flare ribbons, and the MC flux
  is computed using in situ observations at 1 AU, all ranging from
  10<SUP>20</SUP> to 10<SUP>22</SUP> Mx. It is found that for the
  nine studied events in which the association between flares, CMEs,
  and MCs is identified, the MC flux is correlated with the total
  reconnection flux Φ<SUB>r</SUB>. Further, the poloidal (azimuthal)
  MC flux Φ<SUB>p</SUB> is comparable with the reconnection flux
  Φ<SUB>r</SUB>, and the toroidal (axial) MC flux Φ<SUB>t</SUB> is a
  fraction of Φ<SUB>r</SUB>. Events associated with filament eruption do
  not exhibit a different Φ<SUB>t,p</SUB>-Φ<SUB>r</SUB> relation from
  events not accompanied by erupting filaments. The relations revealed
  between these independently measured physical quantities suggest that
  for the studied samples, the magnetic flux and twist of interplanetary
  magnetic flux ropes, reflected by MCs, are highly relevant to low-corona
  magnetic reconnection during the eruption. We discuss the implications
  of this result for the formation mechanism of twisted magnetic flux
  ropes, namely, whether the helical structure of the magnetic flux
  rope is largely pre-existing or formed in situ by low-corona magnetic
  reconnection. We also measure magnetic flux encompassed in coronal
  dimming regions (Φ<SUB>d</SUB>) and discuss its relation to the
  reconnection flux inferred from flare ribbons and MC flux.

---------------------------------------------------------
Title: Orientations of LASCO Halo CMEs and their connection to the
    flux rope structure of interplanetary CMEs
Authors: Yurchyshyn, V.; Hu, Q.; Lepping, R. P.; Lynch, B. J.;
   Krall, J.
2007AdSpR..40.1821Y    Altcode: 2007astro.ph..3627Y
  Coronal mass ejections (CMEs) observed near the Sun via LASCO
  coronographic imaging are the most important solar drivers
  of geomagnetic storms. ICMEs, their interplanetary, near-Earth
  counterparts, can be detected in situ, for example, by the Wind and
  ACE spacecraft. An ICME usually exhibits a complex structure that very
  often includes a magnetic cloud (MC). They can be commonly modelled
  as magnetic flux ropes and there is observational evidence to expect
  that the orientation of a halo CME elongation corresponds to the
  orientation of the flux rope. In this study, we compare orientations
  of elongated CME halos and the corresponding MCs, measured by Wind
  and ACE spacecraft. We characterize the MC structures by using the
  Grad-Shafranov reconstruction technique and three MC fitting methods
  to obtain their axis directions. The CME tilt angles and MC fitted
  axis angles were compared without taking into account handedness
  of the underlying flux rope field and the polarity of its axial
  field. We report that for about 64% of CME-MC events, we found a good
  correspondence between the orientation angles implying that for the
  majority of interplanetary ejecta their orientations do not change
  significantly (less than 45 deg rotation) while travelling from the
  Sun to the near-Earth environment.

---------------------------------------------------------
Title: The May 13, 2005 Eruption: Observations, Data Analysis and
    Interpretation
Authors: Yurchyshyn, V.; Liu, C.; Abramenko, V.; Krall, J.
2006SoPh..239..317Y    Altcode: 2006SoPh..tmp...72Y
  In this study, we present detailed description and analysis of the May
  13, 2005 eruption, the corresponding coronal mass ejection (CME) and
  intense geomagnetic storm observed near the Earth on May 15, 2005. This
  isolated two-ribbon M8.0 flare and the very fast CME occurred in a
  relatively simple magnetic configuration during a quiet period of solar
  activity, which enabled us to reliably associate the solar surface event
  with its counterpart observed in the Earth magnetosphere. In our study,
  we utilized (i) various tools to analyze a multi-wavelength data set
  that includes ground (BBSO vector magnetograms, Hα) and space (SOHO,
  TRACE, RHESSI and ACE) based data; (ii) linear force-free modeling
  to reconstruct the coronal field above the active region and (iii)
  erupting flux rope (EFR) model to simulate a near-Sun halo CME and
  a near-Earth interplanetary CME (ICME). Our findings indicate that
  persisting converging and shearing motions near the main neutral line
  could lead to the formation of twisted core fields and eventually
  their eruption via reconnection. In the discussed scenario, the in
  situ formed erupting loop can be observed as a magnetic cloud (MC)
  when it reaches the Earth. The EFR model was able to produce both a
  model halo CME and ICME providing a good global match to the overall
  timing and components of the magnetic field in the observed MC. The
  orientation of the model ICME and the sense of the twist, inferred
  from the EFR model, agree well with the orientation and the magnetic
  helicity found in the source active region.

---------------------------------------------------------
Title: On Magnetic Flux Budget in Low-corona Magnetic Reconnection
    and Interplanetary Coronal Mass Ejections
Authors: Qiu, J.; Hu, Q.; Howard, T.; Yurchyshyn, V.
2006AGUFMSH33B0406Q    Altcode:
  We present the first quantitative comparison between the total
  magnetic reconnection flux in low-corona at the wake of coronal mass
  ejections (CMEs) and the magnetic flux in magnetic clouds (MCs) that
  reach 1~AU 2 - 3 days after CME onset. The total reconnection flux
  is measured from flare ribbons, and the MC flux is computed using
  in-situ observations at 1~AU, all ranging from 10^{20-22} Mx. It is
  found that for the studied 9 events, in which the association between
  flares, CMEs, and MCs is identified, the MC flux is correlated with
  the total reconnection flux Φ_r. Further, the poloidal (azimuthal) MC
  flux Φ_p is comparable with reconnection flux Φr, and the toroidal
  (axial) MC flux Φ_t is a fraction of Φr. Events associated with
  filament eruption do not exhibit a different Φt, p - Φ_r relation
  from events not accompanied by erupting filaments. The revealed
  relations between these independently measured physical quantities
  suggest that, for the studied samples, the magnetic flux and twist of
  the interplanetary magnetic flux rope, reflected by MCs, are highly
  relevant to low-corona magnetic reconnection during the eruption. %which
  contributes significantly to the formation of the helical structure of
  the flux ropes. We discuss the implication on the formation mechanism
  of twisted magnetic flux ropes, namely, whether the helical structure
  of the magnetic flux rope is largely pre-existing or formed in-situ
  by low-corona magnetic reconnection. We also measure magnetic flux
  encompassed in coronal dimming regions (Φ_d) and discuss its relation
  with reconnection flux inferred from flare ribbons and MC flux.

---------------------------------------------------------
Title: The Automatic Predictability of Super Geomagnetic Storms from
    halo CMEs associated with Large Solar Flares
Authors: Song, Hui; Yurchyshyn, Vasyl; Yang, Guo; Tan, Changyi; Chen,
   Weizhong; Wang, Haimin
2006SoPh..238..141S    Altcode: 2006SoPh..tmp...30S
  We investigate the relationship between magnetic structures of
  coronal mass ejection (CME) source regions and geomagnetic storms, in
  particular, the super storms when the D<SUB>st</SUB> index decreases
  below −200 nT. By examining all full halo CMEs that erupted
  between 1996 and 2004, we selected 73 events associated with M-class
  and X-class solar flares, which have a clearly identifiable source
  region. By analyzing daily full-disk MDI magnetograms, we found that
  the horizontal gradient of the line-of-sight magnetic field is a viable
  parameter to identify a flaring magnetic neutral line and thus can be
  used to predict the possible source region of CMEs. The accuracy of
  this prediction is about 75%, especially for those associated with
  X-class flares (up to 89%). The mean orientation of the magnetic
  structures of source regions was derived and characterized by the
  orientation angle θ, which is defined to be ≤ 90<SUP>∘</SUP>
  in the case of the southward orientation and ≥ 90<SUP>∘</SUP>,
  when the magnetic structure is northwardly oriented. The orientation
  angle was calculated as the median orientation angle of extrapolated
  field lines relative to the flaring neutral line. We report that for
  about 92% of super storms (12 out of 13 events) the orientation angle
  was found to be southward. In the case of intense and moderate storms
  (D<SUB>st</SUB>≥ −200 nT), the relationship is less pronounced
  (70%, 21 out of 30 events). Our findings demonstrate that the approach
  presented in this paper can be used to perform an automatic prediction
  of the occurrence of large X-class flares and super geomagnetic storms.

---------------------------------------------------------
Title: An Overview of Existing Algorithms for Resolving the
180<SUP>°</SUP> Ambiguity in Vector Magnetic Fields: Quantitative
    Tests with Synthetic Data
Authors: Metcalf, Thomas R.; Leka, K. D.; Barnes, Graham; Lites,
   Bruce W.; Georgoulis, Manolis K.; Pevtsov, A. A.; Balasubramaniam,
   K. S.; Gary, G. Allen; Jing, Ju; Li, Jing; Liu, Y.; Wang, H. N.;
   Abramenko, Valentyna; Yurchyshyn, Vasyl; Moon, Y. -J.
2006SoPh..237..267M    Altcode: 2006SoPh..tmp...14M
  We report here on the present state-of-the-art in algorithms used
  for resolving the 180° ambiguity in solar vector magnetic field
  measurements. With present observations and techniques, some assumption
  must be made about the solar magnetic field in order to resolve
  this ambiguity. Our focus is the application of numerous existing
  algorithms to test data for which the correct answer is known. In
  this context, we compare the algorithms quantitatively and seek to
  understand where each succeeds, where it fails, and why. We have
  considered five basic approaches: comparing the observed field to a
  reference field or direction, minimizing the vertical gradient of the
  magnetic pressure, minimizing the vertical current density, minimizing
  some approximation to the total current density, and minimizing some
  approximation to the field's divergence. Of the automated methods
  requiring no human intervention, those which minimize the square of
  the vertical current density in conjunction with an approximation for
  the vanishing divergence of the magnetic field show the most promise.

---------------------------------------------------------
Title: The Relationship between Magnetic Gradient and Magnetic Shear
    in Five Super Active Regions Producing Great Flares
Authors: Wang, Hai-Min; Song, Hui; Jing, Ju; Yurchyshyn, Vasyl; Deng,
   Yuan-Yong; Zhang, Hong-Qi; Falconer, David; Li, Jing
2006ChJAA...6..477W    Altcode:
  We study the magnetic structure of five well-known active regions that
  produced great flares (X5 or larger). The six flares under investigation
  are the X12 flare on 1991 June 9 in AR 6659, the X5.7 flare on 2000 July
  14 in AR 9077, the X5.6 flare on 2001 April 6 in AR 9415, the X5.3 flare
  on 2001 August 25 in AR 9591, the X17 flare on 2003 October 28 and the
  X10 flare on 2003 October 29, both in AR 10486. The last five events
  had corresponding LASCO observations and were all associated with Halo
  CMEs. We analyzed vector magnetograms from Big Bear Solar Observatory,
  Huairou Solar Observing Station, Marshall Space Flight Center and Mees
  Solar Observatory. In particular, we studied the magnetic gradient
  derived from line-of-sight magnetograms and magnetic shear derived from
  vector magnetograms, and found an apparent correlation between these
  two parameters at a level of about 90%. We found that the magnetic
  gradient could be a better proxy than the shear for predicting where a
  major flare might occur: all six flares occurred in neutral lines with
  maximum gradient. The mean gradient of the flaring neutral lines ranges
  from 0.14 to 0.50 G km<SUP>-1</SUP>, 2.3 to 8 times the average value
  for all the neutral lines in the active regions. If we use magnetic
  shear as the proxy, the flaring neutral line in at least one, possibly
  two, of the six events would be mis-identified.

---------------------------------------------------------
Title: Orientations Of Lasco Halo Cmes And Their Connection To The
    Flux Rope Structure Of Icmes
Authors: Yurchyshyn, Vasyl B.; Hu, Q.; Lepping, R. P.; Lynch, B. J.;
   Krall, J.
2006SPD....37.2402Y    Altcode: 2006BAAS...38..250Y
  Coronal mass ejections (CMEs) are the most important solar drivers of
  geomagnetic storms. They are observed by remote sensing, such as LASCO
  coronographic imaging on board SOHO spacecraft. Their interplanetary
  counterparts, ICMEs, can be detected in-situ, for example, by ACE
  and Wind spacecraft. An ICME usually exhibits a complex structure
  that very often includes a magnetic cloud (MC). MCs are distinctive
  magnetic features that can be commonly modeled as magnetic flux
  ropes which are capable of providing prolonged periods of southward
  interplanetary magnetic field at 1 AU, due to the poloidal and/or
  toroidal component of their internal magnetic field. It is thought that
  the orientation of a halo CME elongation corresponds to the orientation
  of the flux rope. Therefore, in this study we compare orientation
  angles of elongated halo CMEs observed by the LASCO instrument and the
  corresponding MCs, measured by Wind and ACE spacecraft. We characterize
  the ICME structures by using the Grad-Shafranov reconstruction
  technique and several ICME/MC fitting methods to obtain their axis
  orientations. The CME and MC angles are compared without taking into
  account handedness of the underlying flux rope field and the polarity
  of its axial field. We report that for about 64\% of CME-ICME events,
  we found a good correspondence between the orientation angles implying
  that for two thirds of interplanetary ejecta their orientations do not
  change more significantly (less than 45 deg rotation) while traveling
  from the sun to the near earth environment. We also briefly discuss
  the applications of our results to space weather forecast and possible
  future studies.

---------------------------------------------------------
Title: Sigmoid, Type II Precursor, and Coronal Mass Ejection
Authors: Lee, Jeongwoo; Liu, C.; Cho, K.; Gary, D. E.; Yurchyshyn,
   V.; Deng, N.; Wang, H.
2006SPD....37.0907L    Altcode: 2006BAAS...38..236L
  The 2005 May 13 flare occurred in the sigmoidal active region, NOAA
  10759, and its time dependent change on the TRACE, EIT, and SXI images
  suggests an eruption process as envisioned by the runaway tether-cutting
  model. However, the onset of the eruption in the low corona and the
  final explosion of the magnetic field in the high corona are not
  directly observable at these wavelengths and we infer them indirectly
  from the radio data obtained with the Owens Valley Solar Array (OVSA),
  Green Bank Solar Radio Burst Spectrometer (GBSRBS), PHOENIX-spectrograph
  of ETH Zurich, and the Potsdam-Tremsdorf Spectrograph. The Potsdam
  spectrograph shows a so-called Type II Precursor in the early phase
  of loop expansion, indicating a coronal shock formed near the flare
  site. The GBSRBS spectra show a type III burst followed by type II
  bursts in the maximum phase, which implies opening of field lines
  and strong shock formation in the high corona. Finally, the radio
  pulsations are detected on the OVSA and PHOENIX spectrographs, which
  we interpret as due to the magnetic loop oscillation as a dynamic
  response to the mass ejection. These radio data along with the EUV
  and X-ray images are used to infer the runaway tether-cutting process
  during this event in all coronal heights.This work is supported by
  NSF/SHINE grant ATM-0548952 and NSF grant AST-0307670 to NJIT.

---------------------------------------------------------
Title: Flux Emergence Rate In Coronal Holes And In Adjacent Quiet-sun
    Regions
Authors: Abramenko, Valentyna; Fisk, L.; Yurchyshyn, V.
2006SPD....37.1403A    Altcode: 2006BAAS...38..243A
  The rate of emergence of new magnetic flux in coronal holes, and in
  surroundingregions on the quiet Sun was analyzed from observations
  from the MichelsonDoppler Imager and the EUV Imager Telescope on the
  Solar and HeliosphericObservatory (SOHO). Coronal holes are regions
  where the open magnetic flux ofthe Sun, the component that forms the
  heliospheric magnetic field, isconcentrated. It is determined that
  the rate of emergence of new magnetic fluxis systematically lower,
  by a factor of 2, in coronal holes relative to thesurrounding quiet
  Sun. This result is consistent with a prediction in a recentmodel for
  the transport of open magnetic flux on the Sun, which demonstratedthat
  open flux tends to accumulate and concentrate in regions where the
  rate ofemergence of new magnetic flux is a local minimum.

---------------------------------------------------------
Title: The Eruption from a Sigmoid Active Region on 2005 May 13
Authors: Liu, Chang; Lee, J.; Yurchyshyn, V.; Cho, K.; Deng, N.;
   Gary, D. E.; Wang, H.
2006SPD....37.0821L    Altcode: 2006BAAS...38..234L
  A sigmoidal structure of active regions has been of interest as is
  believed to lead to magnetic eruption. We found from TRACE EUV images
  that NOAA AR 10759 exhibited a typical sigmoid shape just before the
  M8.0 flare and a fast halo CME on 2005 May 13, and reduced to a more
  confined arcade after the eruption. We have thus examined these time
  dependent changes during the flare by utilizing a multiwavelength
  data set: EUV (TRACE, EIT), soft X-rays (SXI), H-alpha (BBSO,ISOON),
  radio spectra (OVSA, Potsdam-Tremsdorf, GBSRBS, Phoenix, RSTN),
  and CME (LASCO). Several similarities of this event with the runaway
  tether-cutting scenario elaborated by Moore et al. (2001) has been
  found. Before the maximum phase, the flare brightening first occurred in
  the core of the active region, and then two elbows in the outer region
  gradually expanded, which we compare to the tether-cutting in the
  sigmoid center and the ejective eruption, respectively. At the flare
  maximum, the large-scale disturbances such as Moreton waves, type II,
  and III radio bursts were observed, which we suggest as evidence for
  the blow-out of the envelope field and particle acceleration. Finally
  the flare arcade formed along the neutral line as the opened legs of
  the envelop field reconnect with each other. This dataset therefore
  supports the idea that the eruption may start in the sheared core
  field and proceeds outward with the rising plasmoid via the runaway
  tether-cutting reconnection and finally becomes a CME.This work is
  supported by NSF/SHINE grant ATM-0548952, NSF grant ATM-0536921,
  and NASA grant NNG0-4GJ51G.

---------------------------------------------------------
Title: Evidence for Tether-Cutting Reconnection in a Quadrupole
    Magnetic Configuration in the April 9, 2001, M7.9 Flare
Authors: Yurchyshyn, V.; Karlický, M.; Hu, Q.; Wang, H.
2006SoPh..235..147Y    Altcode:
  We studied the M7.9 flare on April 9, 2001 that occurred within a
  δ-sunspot of active region NOAA 9415. We used a multi-wavelength
  data set, which includes Yohkoh, TRACE, SOHO, and ACE spacecraft
  observations, Potsdam and Ondřejov radio data and Big Bear Solar
  Observatory (BBSO) images in order to study the large-scale structure
  of this two-ribbon flare that was accompanied by a very fast coronal
  mass ejection (CME). We analyzed light curves of the flare emission as
  well as the structure of the radio emission and report the following:
  the timing of the event, i.e., the fact that the initial brightenings,
  associated with the core magnetic field, occurred earlier than the
  remote brightening (RB), argue against the break-out model in the
  early phase of this event. We thus conclude that the M7.9 flare and
  the CME were triggered by a tether-cutting reconnection deep in the
  core field connecting the δ-spot and this reconnection formed an
  unstable flux rope. Further evolution of the erupted flux rope could
  be described either by the "standard" flare model or a break-out
  type of the reconnection. The complex structure of flare emission
  in visible, X-ray, and radio spectral ranges point toward a scenario
  which involves multiple reconnection processes between extended closed
  magnetic structures.

---------------------------------------------------------
Title: Flux Rope Model of the 2003 October 28-30 Coronal Mass Ejection
    and Interplanetary Coronal Mass Ejection
Authors: Krall, J.; Yurchyshyn, V. B.; Slinker, S.; Skoug, R. M.;
   Chen, J.
2006ApJ...642..541K    Altcode:
  A numerical model of an erupting solar flux rope is shown to reproduce
  both quantitative near-Sun properties of the 2003 October 28 coronal
  mass ejection and the timing, strength, and orientation of the fields
  measured in situ at 1 AU. Using a simple erupting flux rope model, we
  determine the best-fit parameters for this event. Our analysis shows
  that the orientation of the magnetic axis of the flux rope in this
  case rotates smoothly through approximately 50° as the flux rope apex
  expands from the solar surface to 1 AU. Using a global magnetospheric
  simulation code, we further show that the resulting model solar wind
  properties at 1 AU produce a magnetospheric response comparable to
  that computed using the actual solar wind data.

---------------------------------------------------------
Title: The Rate of Emergence of Magnetic Dipoles in Coronal Holes
    and Adjacent Quiet-Sun Regions
Authors: Abramenko, V. I.; Fisk, L. A.; Yurchyshyn, V. B.
2006ApJ...641L..65A    Altcode:
  Observations from the Michelson Doppler Imager and the EUV Imaging
  Telescope on the Solar and Heliospheric Observatory are analyzed to
  determine the rate of emergence of new magnetic flux in coronal holes
  and in surrounding regions on the quiet Sun. Coronal holes are regions
  where the open magnetic flux of the Sun, the component that forms the
  heliospheric magnetic field, is concentrated. It is determined that
  the rate of emergence of new magnetic flux is systematically lower,
  by a factor of ~2, in coronal holes relative to the surrounding quiet
  Sun. This result is consistent with a prediction in a recent model for
  the transport of open magnetic flux on the Sun, which demonstrated
  that open flux tends to accumulate and concentrate in regions where
  the rate of emergence of new magnetic flux is a local minimum.

---------------------------------------------------------
Title: Relationship between the magnetic field of interplanetary
    ejecta and their solar sources
Authors: Yurchyshyn, V.
2006cosp...36..677Y    Altcode: 2006cosp.meet..677Y
  Solar coronal mass ejections CMEs are a principal link that connects
  the chain of events in the solar atmosphere interplanetary space and
  the earth s magnetic environment The occurrence of earth-directed
  CMEs is well associated with geomagnetic disturbances that can impose
  large negative interplanetary magnetic fields IMF across the dayside
  magnetosphere at 1 AU and large pressure-produced compressions of the
  dayside magnetopause Such geomagnetic storms can be the sources of
  impaired and even disrupted technological systems flying in space and
  operating on the earth s surface Recent research from our group has
  demonstrated that the size of a geomagnetic storm as measured by the
  geomagnetic index Dst appears to be well associated with the expansion
  speed of the halo CME that triggered the storm The relationship was
  found to be more pronounced for very fast ejecta v 1000 km s In addition
  we obtained new and original results that demonstrate the relationship
  between magnetic fields of the solar source of a coronal eruption and
  magnetic fields of the interplanetary ejecta In this presentation
  we will investigate the very real possibility that the polarity of
  IMF near 1 AU can be deduced from key solar data -- photospheric
  magnetograms coronal images and the observed configurations of CMEs
  near the Sun This information is critical together with data on the
  CME arrival time velocity and plasma density for assessing geospace
  disturbances that might result from the solar eruption This research
  also contributes to deeper understandings of the

---------------------------------------------------------
Title: Observed pre flare characteristics of active region magnetic
    fields
Authors: Yurchyshyn, V.
2006cosp...36..676Y    Altcode: 2006cosp.meet..676Y
  I will present data and results on observations of flare-related
  magnetic conditions in solar active regions The following topics will
  be discussed Static non-potential magnetic characteristics before
  flares such as magnetic gradients shear and twist 2 spatio-temporal
  dynamics of the photospheric magnetic flux such as flows and flux
  emergence 3 evolution of magnetic structures leading to and following
  flares A special attention will be payed to new approaches to quantify
  complexity of the photospheric magnetic fields in terms of intermittency
  magnetic power spectra and probability distribution functions Discovered
  correlation between the parameters and the flare activity in active
  regions provides new insights into understanding of the nature
  of magnetic coupling between the sub-photospheric layers where the
  magnetic field is generated and the corona where eruptions occur

---------------------------------------------------------
Title: Magnetic Structure of Halo CMEs and Corresponding ICMEs
Authors: Krall, J.; Yurchyshyn, V. B.; Chen, J.
2005AGUFMSH13A0300K    Altcode:
  The detailed connection between a halo coronal mass ejection (CME)
  and its corresponding “interplanetary CME” (ICME) is an area of
  active study. Using the erupting flux rope model [1-2], we present
  model/data comparisons for multiple CME/ICME events near the sun
  (using coronagraph image data) and in the heliosphere (using in situ
  measurements). We find that the near-Sun magnetic configuration, as
  obtained from a match of the model to the observed halo-CME morphology,
  is closely related to the ICME magnetic configuration, as determined
  by matching the model ICME to the in situ magnetic field and plasma
  measurements. The differences between the near-Sun flux-rope orientation
  parameters and the near-Earth orientation parameters are noted in each
  case. These indicate that, typically, the apex of the flux rope is
  deflected by 5-10 degrees as the flux rope expands outwards to 1 AU. [1]
  Chen, J. 1996, JGR, 101, 27499 [2] Krall, J. et al., 2000, ApJ, 539, 964

---------------------------------------------------------
Title: Continuation of the SHINE Campaign Studies: Eruption on May
    13, 2005
Authors: Yurchyshyn, V.; Liu, C.
2005AGUFMSH13A0274Y    Altcode:
  We will present data on a well observed eruptive flare that occurred
  on May 13, 2005 in NOAA AR 0759. This typical two-ribbon flare was
  associated with a fast CME and caused an intense geomagnetic storm
  (Dst &lt; -259nT) on early May 15th. The magnetic structure of this
  flare, the position of the AR, flare duration, filament activation,
  sigmoidal appearance in Halpha and coronal images, association with
  a CME and coronal dimming as well as interplanetary characteristics
  are strikingly similar to those of the 1997 May 12 SHINE campaign
  event. Because the solar and heliospheric background conditions for
  the May 12 1997 eruption were relatively simple, this event became
  a key event in many collaborative campaigns such as SHINE-GEM-CEDAR,
  MURI, and CISM. The biggest problem is that the 1997 event was not well
  observed and many essential data sets are not available. Therefore,
  various simulations, methods, inferences and theoretical ideas which
  arose from this campaign study could not be satisfactory tested against
  observations. It is thus, essential to continue these focused event
  oriented studies. The recent May 13 flare was well covered by Big Bear
  Solar Observatory (Halpha images and vector magnetograms) as well as
  SOHO, TRACE, RHESSI and ACE satellites. In this presentation we will
  discuss the structure of the May 13, 2005 eruption and analyze the
  flare light curves produced by Halpha and X- ray sources. We will also
  present vector magnetic field data and flow maps. We will analyze the
  evolution of the AR magnetic field (flux emergence and cancellation;
  magnetic gradients; magnetic flux change) and compare them to the flare
  activity and interplanetary data on the associated magnetic cloud that
  was observed at 1AU. Finally we will discuss our findings in terms of
  the existing CME models and provide observational restrains to modelers.

---------------------------------------------------------
Title: Magnetic Reconnection Flux and Coronal Mass Ejection Velocity
Authors: Qiu, Jiong; Yurchyshyn, Vasyl B.
2005ApJ...634L.121Q    Altcode:
  We explore the relationship between the total reconnection flux
  ψ<SUB>rec</SUB> estimated from flare observations and the velocity
  V<SUB>CME</SUB> of coronal mass ejections (CMEs) observed with the
  Large Angle and Spectrometric Coronagraph (LASCO) Experiment. Our
  study includes 13 events with varying magnetic configurations in
  source regions. It is shown that V<SUB>CME</SUB> is proportional to
  ψ<SUB>rec</SUB>, with a linear cross-correlation of 89% and confidence
  level greater than 99.5%. This result confirms the importance of
  magnetic flux transferred by magnetic reconnection in the early stage
  of fast CMEs. On the other hand, the CME velocity and kinematic energy
  are probably independent of magnetic configurations of source regions.

---------------------------------------------------------
Title: Evolution of Barb Angle and Filament Eruption
Authors: Su, J. T.; Liu, Y.; Zhang, H. Q.; Kurokawa, H.; Yurchyshyn,
   V.; Shibata, K.; Bao, X. M.; Wang, G. P.; Li, C.
2005ApJ...630L.101S    Altcode:
  Hα observations of a quiescent U-shaped filament were obtained at Big
  Bear Solar Observatory and at Hida Observatory with the Flare Monitoring
  Telescope. The filament was located in the southern hemisphere on
  1998 November 4. We study the evolution of the angle of a barb with
  respect to the axis of the filament and find the evolution can be
  divided into two phases: a rise from the acute phase to the obtuse
  phase and a fall. Thus, this indicates that the chirality of this barb
  changes with time. Moreover, in the process of evolution, we find that
  interconnection of the part of the filament bearing the barb with the
  whole filament became either weakened or strengthened. We impute the
  final eruption of the filament to the chirality evolution of the barb.

---------------------------------------------------------
Title: Structure of magnetic fields in NOAA active regions 0486 and
    0501 and in the associated interplanetary ejecta
Authors: Yurchyshyn, Vasyl; Hu, Qiang; Abramenko, Valentyna
2005SpWea...3.8C02Y    Altcode:
  Spectacular burst of solar activity in October-November 2003, when large
  solar spots and intense solar flares dominated the solar surface for
  many consecutive days, caused intense geomagnetic storms. In this paper
  we analyze solar and interplanetary magnetic fields associated with the
  storms in October-November 2003. We used space- and ground-based data in
  order to compare the orientations of the magnetic fields on the solar
  surface and at 1 AU as well as to estimate parameters of geomagnetic
  storms during this violent period of geomagnetic activity. Our study
  further supports earlier reports on the correlation between the
  coronal mass ejection speed and the strength of the magnetic field in
  an interplanetary ejecta. A good correspondence was also found between
  directions of the helical magnetic fields in interplanetary ejecta and
  in the source active regions. These findings are quite significant in
  terms of their potential to predict the severity of geomagnetic activity
  1-2 days in advance, immediately after an Earth directed solar eruption.

---------------------------------------------------------
Title: Magnetic structures of active regions and their link to
    coronal mass ejections
Authors: Yurchyshyn, V.
2005AGUSMSH51C..03Y    Altcode:
  olar coronal mass ejections (CMEs) are a principal link that connects
  the chain of events in the solar atmosphere, interplanetary space and
  the earth's magnetic environment. The central objective of our study is
  to advance our understanding of physical processes in CMEs and related
  phenomena, including their ultimate origin, precursors and near sun
  evolution as well as their link to the interplanetary phenomena. Earlier
  studies unanimously suggest that there is a straightforward relationship
  between the magnetic fields of erupted filaments and magnetic clouds at
  1AU. However, the situation is more complicated and less understood
  in the case of eruptions from solar active regions. We combined
  photospheric magnetograms, chromospheric and coronal images as well
  as solar wind data of high spatial and temporal resolution in order
  to i) determine the basic characteristics of the initial pre-eruption
  magnetic configuration in an active region and ii) find a link between
  these characteristics and the magnetic fields in interplanetary CMEs
  (ICMEs) at 1AU. Our results show a good correspondence between the
  directions of the helical magnetic fields in interplanetary ejecta
  and in the source active regions. We will also demonstrate how the
  combination of the solar surface and solar wind data may be used to
  discriminate between different CME models and to predict the sign of
  the interplanetary magnetic field at 1AU.

---------------------------------------------------------
Title: Towards Real-Time Automated Prediction of Geo-Magnetic Storms
    Based on Observations of Source Regions of Halo CMEs
Authors: Song, H.; Yurchyshyn, V.; Wang, H.
2005AGUSMSP23A..01S    Altcode:
  Halo Coronal Mass Ejections (CMEs), originating near disk center,
  are possible sources of large geomagnetic storms. Our goal is to
  predict geomagnetic activities automatically and in real time based
  on the observations of source regions of CMEs. We have achieved the
  following two steps: (1) We studied the magnetic structure of a number
  of famous active regions that produced large flares (X5 or larger), and
  found a close correlation between magnetic gradient and magnetic shear;
  and magnetic gradient could be even a better proxy to predict where a
  major flare might occur. Therefore, we can avoid complication of using
  vector magnetograms to derive magnetic shear. (2) We investigated the
  relationship between geoeffectiveness and the orientation of magnetic
  field in source active regions. Based on the flaring neutral lines
  detected by step (1), we extrapolated the magnetic structure in active
  region with three-dimensional (3D) numerical models. We started with
  the potential field model. We attempt to find relationship between the
  the orientation of magnetic field in the source region and the hourly
  averaged ACE measurements of the Bz component of the interplanetary
  magnetic fields, that is believed to be the indicator of geomagnetic
  storms.

---------------------------------------------------------
Title: On the Relationship Among Magnetic Twist, Reconnection Rate
    and Acceleation in Solar Eruptions
Authors: Jing, J.; Yurchyshyn, V.; Qiu, J.; Xu, Y.; Wang, H.
2005AGUSMSP44A..03J    Altcode:
  We investigate the statistical correlation between the magnetic
  twist and properties of solar eruptions such as acceleration of
  eruptive filaments and magnetic reconnection rate of corresponding
  two-ribbon flares. We anticipate to provide observational evidence
  for, or against, the speculation that increasing magnetic twist
  is more likely giving rise to the violent solar eruptions. The
  magnetic twist is characterized by the linear force-free (LFFF)
  magnetic field constant α. We adopt a method for the reconstruction
  of the LFFF magnetic field in a bounded domain that was described in
  Abramenko and Yurchishin (1996). The best-fit value of α is selected
  so that the extrapolated field gives the closest match to the coronal
  observations. The magnetic reconnection rate of two-ribbon flares, in
  terms of electric field inside the reconnecting current sheet(RCS) and
  flux change rate involved in magnetic reconnection in the low corona,
  is derived by measuring the expansion of flare ribbons across the the
  magnetic field. Based our limited events studied so far, there appears
  to be a tendency that the magnetic field with higher α shows higher
  filament acceleration and magnetic reconnection rate.

---------------------------------------------------------
Title: Photospheric sources of very fast coronal mass ejections
Authors: Yurchyshyn, V.; Yashiro, S.; Gopalswamy, N.
2005AGUSMSH51C..04Y    Altcode:
  We identified photospheric sources for 39 very fast (v &gt; 1100
  km/s) front-side coronal mass ejections that erupted between 1999 and
  2001. For our study we used data on CMEs and their sources provided
  by the CME Catalog, SOHO spacecraft (LASCO, EIT, MDI), Big Bear Solar
  Observatory (Halpha, magnetograms), Mount Wilson Observatory (sunspot
  drawings) and Joint USAF/NOAA active region summary. Our results are
  as follows. We distinguished three different groups of active regions
  which are responsible for very fast CMEs: 1) Complex delta spots (21
  events). This group of active regions is characterized by the presence
  of at least two large opposite polarity sunspots located close to
  each other. 2) Simple delta spots (8 events). A typical configuration
  of this type consists of one large twisted tadpole-shaped sunspot,
  surrounded by many small satellite-sunspots. 3) Extended magnetic
  regions, which consist of two adjacent decaying active regions or a
  new active region emerging inside a decaying active region.

---------------------------------------------------------
Title: Statistical Distributions of Speeds of Coronal Mass Ejections
Authors: Yurchyshyn, V.; Yashiro, S.; Abramenko, V.; Wang, H.;
   Gopalswamy, N.
2005ApJ...619..599Y    Altcode:
  We studied the distribution of plane-of-sky speeds determined for
  4315 coronal mass ejections (CMEs) detected by the Large Angle and
  Spectrometric Coronagraph Experiment on board the Solar and Heliospheric
  Observatory (SOHO LASCO). We found that the speed distributions
  for accelerating and decelerating events are nearly identical and
  to a good approximation they can be fitted with a single lognormal
  distribution. This finding implies that, statistically, there is no
  physical distinction between the accelerating and the decelerating
  events. The lognormal distribution of the CME speeds suggests that
  the same driving mechanism of a nonlinear nature is acting in both
  slow and fast dynamical types of CMEs.

---------------------------------------------------------
Title: Magnetic Flux Ropes from the Sun to 1 AU*
Authors: Krall, J.; Yurchyshyn, V. B.; St. Cyr, O. C.; Chen, J.
2004AGUFMSH22A..07K    Altcode:
  Any practical model of the dynamics of a coronal mass ejection (CME)
  and its interplanetary counterpart (ICME) must conform to available
  observational constraints from sun and to the earth; the upcoming
  STEREO mission will add significantly to those constraints. We present
  model/data comparisons for specific CME/ICME events near the sun
  (using coronagraph image data) and in the heliosphere (using in situ
  measurements) to show that the flux rope model of Chen and Krall[1-2]
  provides an accurate physics-based characterization of flux-rope
  CMEs over this range. We further show that quantitative results,
  such as the field energy required for eruption, depend on specific
  aspects of the flux rope geometry, such as the ratio (length/width)
  of the elliptical shape traced out by the flux-rope axis. It is this
  geometry that will be determined, for the first time, by STEREO. [1]
  Chen, J. 1996, JGR, 101, 27499 [2] Krall, J. et al., 2000, ApJ, 539,
  964 *Work supported by ONR, NASA and NSF

---------------------------------------------------------
Title: On the Relation between Filament Eruptions, Flares, and
    Coronal Mass Ejections
Authors: Jing, Ju; Yurchyshyn, Vasyl B.; Yang, Guo; Xu, Yan; Wang,
   Haimin
2004ApJ...614.1054J    Altcode:
  We present a statistical study of 106 filament eruptions, which were
  automatically detected by a pattern recognition program implemented
  at Big Bear Solar Observatory using Hα full-disk data from 1999
  to 2003. We compare these events with Geostationary Operational
  Environmental Satellite soft X-ray time profiles, solar-geophysical
  data (SGD) solar event reports, Michelson Doppler Imager magnetograms,
  and Large Angle and Spectrometric Coronagraph (LASCO) data to determine
  the relationship between filament eruptions and other phenomena of solar
  activity. (1) Excluding eight events with no corresponding LASCO data,
  55% or 56% of 98 events were associated with coronal mass ejections
  (CMEs). (2) Active region filament eruptions have a considerably
  higher flare association rate of 95% compared to quiescent filament
  eruptions with 27%, but a comparable CME association rate, namely, 43%
  for active region filament eruptions and 54% for quiescent filament
  eruptions. (3) 54% or 68% of 80 disk events were associated with new
  flux emergence. In addition, we derived the sign of magnetic helicity
  and the orientation of the magnetic field associated with seven halo
  CMEs and demonstrated that the geoeffectiveness of a halo CME can be
  predicted by these two parameters.

---------------------------------------------------------
Title: On the Temporal Relationship between Hα Filament Eruptions
    and Soft X-Ray Emissions
Authors: Schuck, P. W.; Chen, J.; Schwartz, I. B.; Yurchyshyn, V.
2004ApJ...610L.133S    Altcode:
  A technique for investigating the temporal relationship between
  Hα filament eruptions and soft X-ray flux is presented. The method
  is fast, simple, based on statistical measures, and requires no a
  priori knowledge regarding the location of the filaments on the solar
  disk. The method is used to study the filament eruption associated
  with a coronal mass ejection and the M-class flare that originated
  from NOAA Active Region 9163 on 2000 September 12. The technique
  provides a quantitative determination of the temporal relationship
  between changes in the Hα filament and soft X-ray flux. We conclude
  that the filament eruption begins 2 hr prior to the first detectable
  enhancement in soft X-ray flux.

---------------------------------------------------------
Title: Topological changes of the photospheric magnetic field inside
active regions: A prelude to flares?
Authors: Sorriso-Valvo, Luca; Carbone, Vincenzo; Veltri, Pierluigi;
   Abramenko, Valentina I.; Noullez, Alain; Politano, Hélène; Pouquet,
   Annick; Yurchyshyn, Vasyl
2004P&SS...52..937S    Altcode:
  The detection of magnetic field variations as a signature of flaring
  activity is one of the main goals in solar physics. Past efforts gave
  apparently no unambiguous observations of systematic changes. In the
  present study, we discuss recent results from observations that scaling
  laws of turbulent current helicity inside a given flaring active region
  change in response to large flares in that active region. Such changes
  can be related to the evolution of current structures by a simple
  geometrical argument, which has been tested using high Reynolds number
  direct numerical simulations of the MHD equations. Interpretation
  of the observed data within this picture indicates that the change
  in scaling behavior of the current helicity seems to be associated
  with a topological reorganization of the footpoint of the magnetic
  field loops, namely with the dissipation of small scales structures
  in turbulent media.

---------------------------------------------------------
Title: Coronal ejecta in October - November of 2003 and predictions
    of the associated geomagnetic events
Authors: Yurchyshyn, V.
2004AAS...204.0217Y    Altcode: 2004BAAS...36..670Y
  Recently we found that the B<SUB>z</SUB> component in the interplanetary
  magnetic field is correlated with the projected speed of coronal mass
  ejections (CME). The relationship is better pronounced for very fast
  ejecta with speeds higher than 1200 km/s, while slower events display
  larger scatter. In turn, the B<SUB>z</SUB> in IMF is correlated with
  the intensity of the Dst index of geomagnetic activity. Based on this
  result we are elaborating a procedure to routinely predict the magnitude
  of the B<SUB>z</SUB> and the intensity of geomagnetic storms 1-2 days
  in advance by measuring speeds of halo CMEs as they propagate across
  the LASCO C3 field of view. Here we present our predictions made for
  9 halo CMEs ejected during the period of violent solar activity in
  October-November 2003. The comparison between the predicted values of
  the B<SUB>z</SUB> and the Dst index and the observed data shows that we
  were abble to satisfactory predict all three major geomagnetic events
  when the Dst index decreased below -300 nT.

---------------------------------------------------------
Title: Characterizing Solar Surface Turbulence
Authors: Schuck, P.; Chen, J.; Schwartz, I.; Yurchyshyn, V.
2004AAS...204.3711S    Altcode: 2004BAAS...36..710S
  The identification and characterization of solar surface turbulence
  is particularly important for understanding the dynamics associated
  with eruptive phenomena. In this paper, we present a wavelet
  analysis for characterizing surface turbulence associated with solar
  eruptions. By definition, solar eruptions represent impulsive events
  rather than a statistical steady state and the analysis of impulsive
  events requires both time and frequency localization for proper
  robust characterization. Thus, the wavelet (time-frequency) basis
  represents integral ingredient for the analysis. <P />In this paper,
  H-α turbulence on the solar disk is characterized by estimating the
  local-frequency-wavenumber distribution (local dispersion relation)
  of the fluctuations. The local frequency wavenumber distribution is
  computed by generalizing established two-point multi-scale wavelet
  interferometric techniques [1-3] for the multipoint data represented
  by solar images. The local-wavenumber-distribution produces robust
  estimates for the phase velocities of fluctuations in the sequence
  of solar images. <P />[1] J. L. Pinçon, P. M. Kintner, P. W. Schuck
  and C. E. Seyler, Observation and analysis of lower hybrid solitary
  structures as rotating eigenmodes, \textit{J. Geophys. Res.},
  \textbf{102}, 17283\--17296, 1997. <P />[2] P. W. Schuck, C. E. Seyler,
  J. L. Pinçon, John Bonnell, and P. M. Kintner, Theory, simulation and
  observation of discrete eigenmodes associated with lower hybrid solitary
  structures, \textit{J. Geophys. Res.}, \textbf{103}, 6935\--6953,
  1998. <P />[3] J. W. Bonnell, P. W. Schuck, J.\--L. Pinçon,
  C. E. Seyler, and P. M. Kintner, Observation of bound states and
  counter\--rotating lower hybrid eigenmodes in the auroral ionosphere,
  \textit{Phys. Rev. Lett.}, \textbf{80}, 5734\--5737, 1998. <P />Work
  Supported by ONR

---------------------------------------------------------
Title: Traces of the Dynamic Current Sheet during a Solar Flare
Authors: Ji, Haisheng; Wang, Haimin; Goode, Philip R.; Jiang, Yunchun;
   Yurchyshyn, V.
2004ApJ...607L..55J    Altcode:
  High-cadence and high-resolution time sequences of far Hα
  off-band images provide a unique tool to study the evolution of
  the fine structure of flare kernels. The fine structure contains
  important information on flare topology and the triggering
  mechanism. In this Letter, we concentrate on the rapid changes
  of the relative positions of two conjugate flare footpoints. In
  order to carry out this study with the highest physical precision,
  we use r<SUB>c</SUB>=Σr<SUB>j</SUB>I<SUB>j</SUB>/ΣI<SUB>j</SUB>
  (I<SUB>j</SUB> is the Hα brightness at r<SUB>j</SUB>) to compute the
  centroid of an Hα bright kernel region caused by solar flares. Using
  this, we probe the fine temporal structures connected to the distance
  between the centroids of two conjugate kernels of an M2.3 flare. The
  flare, which occurred on 2002 September 9 in NOAA Active Region 0105,
  was observed at Big Bear Solar Observatory at the far off-band center
  wavelength of H α-1.3 Å, with a cadence of ~40 ms. The flare was also
  observed by RHESSI. The time profile of the separation distance shows
  an excellent anticorrelation to that of the hard X-ray (HXR) emissions
  in 25-50 keV, which exhibit a number of separate spikes (the linear
  Pearson correlation coefficient is found to be ~-0.83). The separation
  between the two centroids decreases at the rising periods of four HXR
  spikes, then it increases after the peak time of the flare to show
  the expected separation motion. The most obvious decreasing, which
  occurred during the first HXR peak, was confirmed by corresponding
  images. This implies that during the impulsive phases, the energy
  transported from the corona is deposited increasingly inwardly between
  the two kernels. This new and perhaps surprising tendency for the
  energy deposition can be explained as being caused by current sheet
  pinch motions, which, at the same time, enhance the magnetic energy
  reconnection rate to produce the observed HXR spikes.

---------------------------------------------------------
Title: Magnetic Field, Hα, and RHESSI Observations of the 2002 July
    23 Gamma-Ray Flare
Authors: Yurchyshyn, Vasyl; Wang, Haimin; Abramenko, Valentyna;
   Spirock, Thomas J.; Krucker, Säm
2004ApJ...605..546Y    Altcode:
  In this paper we examine two aspects of the 2002 July 23 gamma-ray flare
  by using multiwavelength observations. First, the data suggest that the
  interaction of the erupted field with an overlying large-scale coronal
  field can explain the offset between the gamma-ray and the hard X-ray
  sources observed in this event. Second, we pay attention to rapid and
  permanent changes in the photospheric magnetic field associated with
  the flare. MDI and BBSO magnetograms show that the following magnetic
  flux had rapidly decreased by 1×10<SUP>20</SUP> Mx immediately after
  the flare, while the leading polarity was gradually increasing for
  several hours after the flare. Our study also suggests that the changes
  were most probably associated with the emergence of new flux and the
  reorientation of the magnetic field lines. We interpret the magnetograph
  and spectral data for this event in terms of the tether-cutting model.

---------------------------------------------------------
Title: Evidence of Rapid Flux Emergence Associated with the M8.7
    Flare on 2002 July 26
Authors: Wang, Haimin; Qiu, Jiong; Jing, Ju; Spirock, Thomas J.;
   Yurchyshyn, Vasyl; Abramenko, Valentina; Ji, Haisheng; Goode,
   Phillip R.
2004ApJ...605..931W    Altcode:
  In this paper, we present a detailed study of the M8.7 flare
  that occurred on 2002 July 26 using data from the Big Bear Solar
  Observatory (BBSO), Ramaty High Energy Solar Spectroscopic Imager
  (RHESSI), the Transition Region and Coronal Explorer (TRACE), and the
  Solar and Heliospheric Observatory (SOHO). This flare has interesting
  properties similar to a number of flares that we studied previously,
  such as a rapid increase of magnetic flux in one polarity and an
  increase in transverse fields and magnetic shear associated with the
  flare. However, this event had the most comprehensive observations; in
  particular, the high-resolution high-cadence BBSO vector magnetograph
  observations. At the time of the flare, across the flare neutral
  line, there was a sudden emergence of magnetic flux at the rate
  of 10<SUP>20</SUP> Mx hr<SUP>-1</SUP> in both the longitudinal and
  transverse components. The emerging flux mostly occurred at the sites
  of the flare. It was very inclined and led to impulsively enhanced
  shear in the magnetic fields. We discuss these observations in the
  context of magnetic reconnection triggered by rapid flux emergence. It
  is also possible that the new flux signifies flare-related change in
  the field line inclination.

---------------------------------------------------------
Title: Correlation between speeds of coronal mass ejections and the
    intensity of geomagnetic storms
Authors: Yurchyshyn, Vasyl; Wang, Haimin; Abramenko, Valentyna
2004SpWea...2.2001Y    Altcode:
  We studied the relationship between the projected speed of coronal
  mass ejections (CMEs), determined from a sequence of Solar and
  Heliospheric Observatory/Large Angle and Spectrometric Coronagraph
  Experiment (SOHO/LASCO) images, and the hourly averaged magnitude of
  the B<SUB>z</SUB> component of the magnetic field in an interplanetary
  ejecta, as measured by the Advanced Composition Explorer (ACE)
  magnetometer in the Geocentric Solar Magnetospheric Coordinate System
  (GSM). For CMEs that originate at the central part of the solar
  disk we found that the intensity of B<SUB>z</SUB> is correlated with
  the projected speed of the CME, V<SUB>p</SUB>. The relationship is
  more pronounced for very fast ejecta (V<SUB>p</SUB> &gt; 1200 km/s),
  while slower events display larger scatter. We also present data which
  support earlier conclusions about the correlation of B<SUB>z</SUB>
  and the Dst index of geomagnetic activity. A possible application of
  the results to space weather forecasting is discussed.

---------------------------------------------------------
Title: The earthshine spectrum
Authors: Montañés Rodriguez, P.; Pallé, E.; Goode, P. R.; Hickey,
   J.; Qiu, J.; Yurchyshyn, V.; Chu, M. C.; Kolbe, E.; Brown, C. T.;
   Koonin, S. E.
2004AdSpR..34..293M    Altcode:
  Since 1998 the Earthshine Project has been a collaborative effort
  between Big Bear Solar Observatory/New Jersey Institute of Technology
  and California Institute of Technology. Cyclic spectroscopic
  observations of the dark and bright sides of the moon (or earthshine
  and moonshine, respectively) have been carried out in the visible
  region at Palomar Observatory. From these data, the ratio of the
  earthshine to moonshine characterizes the globally averaged Earth's
  spectrum. Information concerning the search for extra-solar, terrestrial
  planets can be also obtained from these observations.

---------------------------------------------------------
Title: The Earthshine Project: update on photometric and spectroscopic
    measurements
Authors: Pallé, E.; Montañés Rodriguez, P.; Goode, P. R.; Qiu,
   J.; Yurchyshyn, V.; Hickey, J.; Chu, M. -C.; Kolbe, E.; Brown, C. T.;
   Koonin, S. E.
2004AdSpR..34..288P    Altcode:
  The Earthshine Project is a collaborative effort between Big Bear
  Solar Observatory (New Jersey Institute of Technology) and the
  California Institute of Technology. Our primary goal is the precise
  determination of a global and absolutely calibrated albedo of the Earth
  and the characterization of its synoptic, seasonal and inter-annual
  variability. Photometric observations of the Earth's reflectance have
  been regularly carried out during the past 4 years. The up-to-date
  synoptic, seasonal and long-term variation in the Earth's albedo
  are reported in this paper, together with a comparison to model
  albedos using modern cloud satellite data and Earth Radiation Budget
  Experiment scene models. The Earth's albedo has a major role in
  determining the Earth's climate. The possibility of a response of
  this parameter to solar activity is also discussed. Simultaneously,
  spectrometric observations of the earthshine have been carried out
  at Palomar Observatory. The main goals and first results of those
  observations are also presented.

---------------------------------------------------------
Title: On the time coincidence between \boldmath{H<SUB>α
    </SUB>}-filament eruptions and soft X-ray emissions
Authors: Schuck, P. W.; Chen, J.; Schwartz, I.; Yurchyshyn, V.
2003AGUFMSH22B..05S    Altcode:
  The interrelationships among coronal mass ejections, solar flares,
  and filament eruptions have been a long standing issue in solar
  physics. In particular, timing and spatial relationships among such
  eruptive phenomena play a key role in understanding any possible
  causality among them. Presently, observational ambiguities often
  result from insufficient temporal and spatial resolution. However,
  we expect that observational capabilities will continue to improve,
  and in the near future, produce large volumes of solar data with
  high time-cadence and spatial resolution. We present a technique for
  quantitatively characterizing dynamics in H<SUB>α </SUB>-data. We
  report on the result of applying this technique to a sequence of 1-min
  H<SUB>α </SUB>-images from the Kanzelhöhe Solar Observatory. We
  chose H<SUB>α </SUB>-data for our initial application because many
  solar eruptive phenomena have observable signatures in chromospheric
  dynamics and long periods of H<SUB>α </SUB>-observations are readily
  available. The data set contains quiescent filaments and a filament
  eruption accompanied by a two-ribbon flare. The analysis reveals
  the spatially and temporally correlated phenomena on the H<SUB>α
  </SUB>-solar disk. The H<SUB>α </SUB>-dynamics are compared with
  variations in the integrated soft X-ray flux detected by the GOES 8
  satellite. <P />Work supported by ONR, NSF ATM 0205157, and ATM 9903515.

---------------------------------------------------------
Title: Photospheric Sources of Very Fast (&gt;1100 km/s) CMEs Between
    1999 and 2001
Authors: Yurchyshyn, V.
2003AGUFMSH22B..06Y    Altcode:
  We identified photospheric sources for 39 very fast (faster then
  1100 km/s) front-side coronal mass ejections, which occurred between
  1999 and 2001. For our study we used data on CMEs and their sources
  provided by the CME Catalog, SOHO spacecraft (LASCO, EIT, MDI), Big
  Bear Solar Observatory (Hα, magnetograms), Mount Wilson Observatory
  (sunspot drawings) and Joint USAF/NOAA active region summary. We
  distinguished three different groups of active regions which are
  responsible for very fast CMEs: 1) Complex delta spots (delta spots
  with a Mt. Wilson classification of beta gamma). This group of active
  regions (21 events) can be represented by active regions 9393 and 9415
  and is characterized by the presence of at least two large opposite
  polarity sunspots located close to each other. 2) Simple delta spots
  (8 events). A typical configuration of this type can be represented
  by active regions 8375 and 9236 and consists of one large twisted
  tadpole-shaped sunspot, surrounded by many small satellite-sunspots. 3)
  Extended magnetic regions, which consist of two adjacent decaying active
  regions or a new active region emerging inside a decaying active region
  (active regions 9046 and 9085). In this presentation we will discuss in
  detail the evolution and the type of the magnetic structures which are
  responsible for very fast CMEs originating from delta-configurations.

---------------------------------------------------------
Title: Signature of an Avalanche in Solar Flares as Measured by
    Photospheric Magnetic Fields
Authors: Abramenko, V. I.; Yurchyshyn, V. B.; Wang, H.; Spirock,
   T. J.; Goode, P. R.
2003ApJ...597.1135A    Altcode:
  We analyzed time variations of turbulent parameters of the photospheric
  magnetic field of four active regions obtained during the course of
  major solar flares using longitudinal magnetograms from the Big Bear
  Solar Observatory and from SOHO/MDI full-disk measurements. Analysis of
  the data indicated that, before each flare, the degree of intermittency
  of the magnetic field had been increasing for 6-33 minutes and reached
  a maximum value approximately 3-14 minutes before the peak of the
  hard X-ray emission for each event. This result seems to suggest the
  existence in an active region of a turbulent phase prior to a solar
  flare. We also found that the maximum of the correlation length of
  the magnetic energy dissipation field tends to follow (or to occur
  nearly simultaneously) with the peak of the hard X-ray emission. The
  data suggest that the peak in the correlation length might be a trace
  of an avalanche of coronal reconnection events. We discuss the results
  in the framework of the concept of self-organized criticality.

---------------------------------------------------------
Title: Themis, BBSO, MDI and trace observations of a filament eruption
Authors: Contarino, L.; Romano, P.; Yurchyshyn, V. B.; Zuccarello, F.
2003SoPh..216..173C    Altcode:
  We describe a filament destabilization which occurred on 5 May 2001 in
  NOAA AR 9445, before a flare event. The analysis is based on Hα data
  acquired by THEMIS operating in IPM mode, Hα data and magnetograms
  obtained at the Big Bear Solar Observatory, MDI magnetograms and 171 Å
  images taken by TRACE. Observations at 171 Å show that ∼ 2.5 hours
  before the flare peak, the western part of the EUV filament channel
  seems to split into two parts. The bifurcation of the filament in the
  Hα line is observed to take place ∼ 1.5 hours before the flare peak,
  while one thread of the filament erupts ∼10 min before the peak of
  the flare. Our analysis of longitudinal magnetograms shows the presence
  of a knot of positive flux inside a region of negative polarity, which
  coincides with the site of filament bifurcation. We interpret this
  event as occurring in two steps: the first step, characterized by the
  appearance of a new magnetic feature and the successive reconnection
  in the lower atmosphere between its field lines and the field lines
  of the old arcade sustaining the filament, leads to a new filament
  channel and to the observed filament bifurcation; the second step,
  characterized by the eruption of part of the filament lying on the
  old PIL, leads to a second reconnection, occurring higher in the corona.

---------------------------------------------------------
Title: Cancellations and structures in the solar photosphere:
    signature of flares
Authors: Sorriso-Valvo, L.; Abramenko, V.; Carbone, V.; Noullez, A.;
   Politano, H.; Pouquet, A.; Veltri, P.; Yurchyshyn, V.
2003AIPC..679..695S    Altcode:
  The topological properties of the typical current structures in
  a turbulent magnetohydrodynamic flow can be measured using the
  cancellations analysis. In two-dimensional numerical simulations, this
  reveals current filaments being the most typical current structures. The
  observations of the topology of photospheric current structures within
  active regions shows that modifications occur correspondingly with
  strong flares.

---------------------------------------------------------
Title: Sunshine, Earthshine and Climate Change: II. Solar Origins
    of Variations in the Earth's Albedo
Authors: Goode, P. R.; Pallé, E.; Yurchyshyn, V.; Qiu, J.; Hickey,
   J.; Rodriguez, P. Montañés; Chu, M. -C.; Kolbe, E.; Brown, C. T.;
   Koonin, S. E.
2003JKAS...36S..83G    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Signature of Avalanche in Solar Flares as Measured by
    Photospheric Magnetic Fields
Authors: Abramenko, V. I.; Yurchyshyn, V. B.; Wang, H.; Spirock,
   T. J.; Goode, P. R.
2003SPD....34.1507A    Altcode: 2003BAAS...35..831A
  Turbulent/fractal parameters of the longitudinal magnetic field,
  B<SUB>z</SUB>, for four powerful solar flares were analyzed utilizing
  the correlation length, l, of the magnetic energy dissipation
  field and the scaling exponent, b, which characterizes the measure
  of intermittency of the B<SUB>z</SUB> structure. We select a set of
  four two-ribbon flares, which were followed by coronal mass ejections,
  for the study of magnetic structure. During the course of each flare,
  we found a peak in b which was followed by a peak in l in all of the
  cases studied in this paper. These two peaks were separated by the time
  interval t<SUB>l</SUB> during which a rapid growth of the soft X-ray
  and Hα flux occurred. The peak in b was preceded by a time period
  t<SUB>b</SUB> during which b increased gradually. For all of the flares
  t<SUB>b</SUB> was longer than the time interval t<SUB>l</SUB>. The
  maximum of l occurred nearly simultaneously, within an accuracy of
  about 2-5 minutes, with the maximum of the hard X-ray emission. For
  the four flares considered in this paper, we concluded that the more
  impulsive and/or more powerful a flare is, the shorter the b growth
  time, t<SUB>b</SUB>, and the l growth time, t<SUB>l</SUB>, are. In
  the framework of the theory of non-linear dissipative processes,
  these results may be interpreted as follows. Before a solar flare
  occurs there is a significant increase in the number of magnetic field
  discontinuities (b increasing), which is followed by an avalanche
  (increase of the correlation length) of magnetic energy dissipation
  events. The avalanche event occupies the entire active region from the
  corona to the photosphere. Our study indicates that the more abrupt
  is the avalanche, the stronger and/or more impulsive a flare is. The
  time profiles of an avalanche is either Gaussian, which satisfies
  the logistic avalanche model, or exponential with an abrupt drop,
  which satisfies the exponential avalanche model. The driving time,
  t<SUB>b</SUB>, was longer than the avalanching time, t<SUB>l</SUB>,
  for all of the events. This qualitatively agrees with the requirements
  of the self-organized criticality theory. <P />This work was supported
  by NSF-ATM 0076602, 0205157, 9903515 and NASA NAG5-12782 grants.

---------------------------------------------------------
Title: Rapid Changes in the Longitudinal Magnetic Field Associated
    with the July 23, 2002 γ -ray Flare
Authors: Yurchyshyn, V. B.; Wang, H.; Abramenko, V. I.; Spirock,
   T. J.; Krucker, S.
2003SPD....34.1508Y    Altcode: 2003BAAS...35Q.832Y
  In this paper we analyze and discuss rapid changes of the magnetic field
  associated with the July 23, 2002 γ -ray flare. MDI magnetic flux
  profiles and BBSO vector magnetograms showed that immediately after
  the flare the leading polarity had increased by 2*E<SUP>20</SUP>Mx,
  while the following polarity decreased only by 1*E<SUP>20</SUP>Mx. The
  observed changes were permanent and not caused by variations in seeing
  or changes in the line profile, which we used to measure the magnetic
  field. In this active region we distinguish two separate locations,
  which show the most dramatic changes in the magnetic field. The
  first location showed an increase in the magnetic field strength
  and a new penumbra area and it was associated with emergence of new
  magnetic flux. At the second location the position of the neutral
  line had changed and it coincided with the footpoints of a rapidly
  growing post-flare loop system. Linear force-free field simulations
  showed that the re-orientation of the magnetic field during the flare
  was capable of producing the observed changes in the total magnetic
  flux. We also discuss a possible magnetic configuration responsible
  for the flare. This work was supported in part by NSF ATM-0086999 and
  ATM-0205157 and under NASA NAG5-10910 NAG5-12782 grants.

---------------------------------------------------------
Title: Chromospheric Dynamics: An Examination of Spatio-temporal
    Phenomena in \boldmathH<SUB>α </SUB> -Data
Authors: Schuck, P. W.; Chen, J.; Schwartz, I. .; Yurchyshyn, V.
2003SPD....34.1612S    Altcode: 2003BAAS...35..834S
  The interrelationships among coronal mass ejections, solar flares,
  and filament eruptions have been a long standing issue in solar
  physics. In particular, timing and spatial relationships among such
  eruptive phenomena play a key role in understanding any possible
  causality among them. Presently, observational ambiguities often
  result from insufficient temporal and spatial resolution. However,
  we expect that observational capabilities will continue to improve,
  and in the near future, produce large volumes of solar data with high
  time-cadence and spatial resolution. We have developed a method of
  identifying and extracting coherent structures from multi-dimensional
  sequences of data. The technique is general and may be applied to
  sequences of solar images in any frequency (e.g., white light, X-rays,
  UV), magnetograms, and other astrophysical and laboratory data. The
  spatio-temporal dynamics revealed using this method can provide a
  new, improved quantitative understanding of coherent and eruptive
  phenomena. We report on the result of applying this technique to a
  sequence of 1-min H<SUB>α </SUB>-images from the Kanzelhöhe Solar
  Observatory. We chose H<SUB>α </SUB>-data for our initial application
  because many solar eruptive phenomena have observable signatures in
  chromospheric dynamics and long periods of H<SUB>α </SUB>-observations
  are readily available. The data set contains quiescent filaments
  and a filament eruption accompanied by a two-ribbon flare. The
  analysis reveals the spatially and temporally correlated phenomena and
  self-similar structures on the solar disk in extraordinary detail. <P
  />Work supported by ONR, NSF ATM 0205157, and ATM 9903515.

---------------------------------------------------------
Title: How directions and helicity of erupted solar magnetic fields
    define geoeffectiveness of coronal mass ejections
Authors: Yurchyshyn, Vasyl; Wang, Haimin; Abramenko, Valentyna
2003AdSpR..32.1965Y    Altcode:
  In this study we report on the relationship between the projected speed
  of CMEs, measured at 20R from SOHO/LASCO images, and the hourly averaged
  magnitude of the southwardly directed magnetic field, B <SUB>z</SUB>,
  at the leading edge of interplanetary ejecta, as measured by the ACE
  magnetometer. We found that those CMEs that originate at the central
  part of the solar disk ( r &lt; 0.6 R<SUB>⊙</SUB>) are the most
  geoeffective and the intensity of B <SUB>z</SUB> is an exponential
  function of the CME's speeds. We propose an approach to estimate the
  strength of the southward IMF at least one day in advance, immediately
  after a CME started. The predicted value of the B <SUB>z</SUB>
  component can be then used to estimate the intensity of a geomagnetic
  storm caused by the eruption. The prediction method is based on the
  correlation between the speeds of CMEs and magnitudes of the southward
  IMF as well as the fact that the orientation and chirality of the
  erupted solar filaments correspond to the orientation and chirality
  of interplanetary ejecta.

---------------------------------------------------------
Title: Cancellations analysis of photospheric magnetic structures
    and flares
Authors: Sorriso-Valvo, L.; Abramenko, V.; Carbone, V.; Noullez, A.;
   Politano, H.; Pouquet, A.; Veltri, P.; Yurchyshyn, V.
2003MmSAI..74..631S    Altcode:
  The topological properties of the typical current structures in
  a turbulent magnetohydrodynamic flow can be measured using the
  cancellations analysis. In two-dimensional numerical simulations, this
  reveals current filaments being the most typical current structures. The
  observations of the topology of photospheric current structures within
  active regions shows that modifications occur correspondingly with
  strong flares.

---------------------------------------------------------
Title: A process of low-lying magnetic reconnection observed by
    THEMIS, BBSO and TRACE
Authors: Contarino, L.; Romano, P.; Zuccarello, F.; Yurchyshyn, V. B.
2003MmSAI..74..647C    Altcode:
  We describe the results obtained from the study of a filament eruption
  associated to a two-ribbon flare, occurred in NOAA AR 9445 on May 5,
  2001. We interpret the event in a two-step reconnection scenario. The
  first reconnection takes place in the lower atmosphere and is due to a
  slow, but continuous, magnetic flux cancellation near the filament. The
  second reconnection, which is explosive and takes place in the corona,
  is caused by the eruption of the filament which triggers a two-ribbon
  flare. The analysis is based on Hα data acquired by THEMIS operating
  in IPM mode, Hα data and magnetograms obtained at the Big Bear Solar
  Observatory, and 171 Å images taken by TRACE.

---------------------------------------------------------
Title: Optical and EUV observation of a filament destabilization
    and pre-eruption reconnection
Authors: Contarino, L.; Romano, P.; Zuccarello, F.; Yurchyshyn, V. B.
2002ESASP.506..573C    Altcode: 2002ESPM...10..573C; 2002svco.conf..573C
  Filament eruption occurring prior to solar flares or CME may be
  related to changes in the magnetic field structure in and around
  the filament. In particular, when the magnetic field topology is
  characterized by great complexity, or new magnetic flux emerges in
  the surrouding of the main arcade supporting the filament, a so-called
  pre-eruption reconnection is likely to take place. In this framework,
  using both ground-based (THEMIS and BBSO) and satellite (TRACE)
  images and BBSO magnetograms, we have followed a filament eruption
  occurred in AR 9445 on May 5, 2001, before a two-ribbon flare. Our
  analysis has shown that the event was characterized by the following
  steps: a) presence of a knot of positive polarity inside the region of
  negative polarity where the arcade loops were anchored; b) appearance
  of a bright knot in Hα images at the same location where the positive
  polarity knot was observed; c) spread of the filament into two threads
  and bifurcation near the Hα bright knot; d) eruption of part of the
  filament and two-ribbon flare; e) EUV post-flare loops anchored in a
  region near the Hα bright knot. The interpretation of these phenomena
  in terms of a pre-eruption, low-lying magnetic reconnection, followed
  by a post-eruption, high-lying reconnection, is discussed.

---------------------------------------------------------
Title: Rapid Changes of Magnetic Fields Associated with Six X-Class
    Flares
Authors: Wang, Haimin; Spirock, Thomas J.; Qiu, Jiong; Ji, Haisheng;
   Yurchyshyn, Vasyl; Moon, Yong-Jae; Denker, Carsten; Goode, Philip R.
2002ApJ...576..497W    Altcode:
  In this paper, we present the results of the study of six X-class
  flares. We found significant changes in the photospheric magnetic
  fields associated with all of the events. For the five events in 2001,
  when coronagraph data were available, all were associated with halo
  coronal mass ejections. Based on the analyses of the line-of-sight
  magnetograms, all six events had an increase in the magnetic flux
  of the leading polarity of order of a few times 10<SUP>20</SUP> Mx
  while each event had some degree of decrease in the magnetic flux
  of the following polarity. The flux changes are considered impulsive
  because the “changeover” time, which we defined as the time to change
  from preflare to postflare state, ranged from 10 to 100 minutes. The
  observed changes are permanent. Therefore, the changes are not due
  to changes in the line profile caused by flare emissions. For the
  three most recent events, when vector magnetograms were available,
  two showed an impulsive increase of the transverse field strength
  and magnetic shear after the flares, as well as new sunspot area in
  the form of penumbral structure. One of the events in this study was
  from the previous solar cycle. This event showed a similar increase
  in all components of the magnetic field, magnetic shear, and sunspot
  area. We present three possible explanations to explain the observed
  changes: (1) the emergence of very inclined flux loops, (2) a change
  in the magnetic field direction, and (3) the expansion of the sunspot,
  which moved some flux out of Zeeman saturation. However, we have no
  explanation for the polarity preference; i.e., the flux of leading
  polarity tends to increase while the flux of following polarity tends
  to decrease slightly.

---------------------------------------------------------
Title: Evidence of a Flux-Rope Model for Corona Mass Ejections Based
    on Observations of the Limb Prominence Eruption on 2002 January 4
Authors: Yurchyshyn, Vasyl B.
2002ApJ...576..493Y    Altcode:
  We report on a prominence eruption as seen in Kanzelhöhe Solar
  Observatory Hα images, Solar and Heliospheric Observatory (SOHO) EUV
  Imaging Telescope (EIT) 195 Å images, and coronal SOHO Large Angle
  Spectrometric Coronograph C2 images. Our data favor the flux-rope
  model for coronal mass ejections (CMEs), which suggests that a flux
  rope is formed long before the eruption. Our conclusion is based on a
  three-part structure of the pre-erupted configuration of the magnetic
  field and on the fact that the first Hα, SOHO EIT 195 Å brightenings
  occurred some 15 minutes after the filament began to ascend. The data
  also clearly demonstrate two rarely observed components of the standard
  flare model: (1) magnetic loops that overlay the pre-erupted filament
  and (2) magnetic field lines stretched vertically by the ascending
  filament. These field lines are compressed horizontally and move
  toward each other where they reconnect to form an apparently growing
  post-flare loop system.

---------------------------------------------------------
Title: Scaling Behavior of Structure Functions of the Longitudinal
    Magnetic Field in Active Regions on the Sun
Authors: Abramenko, V. I.; Yurchyshyn, V. B.; Wang, H.; Spirock,
   T. J.; Goode, P. R.
2002ApJ...577..487A    Altcode:
  In the framework of a refined Kolmogorov hypothesis, the scaling
  behavior of the B<SUB>z</SUB>-component of the photospheric
  magnetic field is analyzed and compared with flaring activity in
  solar active regions. We use Solar and Heliospheric Observatory
  Michelson Doppler Imager, Huairou (China), and Big Bear measurements
  of the B<SUB>z</SUB>-component in the photosphere for nine active
  regions. We show that there is no universal behavior in the scaling
  of the B<SUB>z</SUB>-structure functions for different active
  regions. Our previous study has shown that scaling for a given active
  region is caused by intermittency in the field, ɛ<SUP>(B)</SUP>(x),
  describing the magnetic energy dissipation. When intermittency is
  weak, the B<SUB>z</SUB> field behaves as a passive scalar in the
  turbulent flow, and the energy dissipation is largely determined by
  the dissipation of kinetic energy in the active regions with low flare
  productivity. However, when the field ɛ<SUP>(B)</SUP>(x) is highly
  intermittent, the structure functions behave as transverse structure
  functions of a fully developed turbulent vector field, and the scaling
  of the energy dissipation is mostly determined by the dissipation of the
  magnetic energy (active regions with strong flaring productivity). Based
  on this recent result, we find that the dissipation spectrum of the
  B<SUB>z</SUB>-component is strongly related to the level of flare
  productivity in a solar active region. When the flare productivity is
  high, the corresponding spectrum is less steep. We also find that during
  the evolution of NOAA Active Region 9393, the B<SUB>z</SUB> dissipation
  spectrum becomes less steep as the active region's flare activity
  increases. Our results suggest that the reorganization of the magnetic
  field at small scales is also relevant to flaring: the relative fraction
  of small-scale fluctuations of magnetic energy dissipation increases
  as an active region becomes prone to producing strong flares. Since
  these small-scale changes seem to begin long before the start of a
  solar flare, we suggest that the relation between scaling exponents,
  calculated by using only measurements of the B<SUB>z</SUB>-component,
  and flare productivity of an active region can be used to monitor and
  forecast flare activity.

---------------------------------------------------------
Title: Flare Activity and Magnetic Helicity Injection by Photospheric
    Horizontal Motions
Authors: Moon, Y. -J.; Chae, Jongchul; Choe, G. S.; Wang, Haimin;
   Park, Y. D.; Yun, H. S.; Yurchyshyn, Vasyl; Goode, Philip R.
2002ApJ...574.1066M    Altcode:
  We present observational evidence that the occurrence of homologous
  flares in an active region is physically related to the injection of
  magnetic helicity by horizontal photospheric motions. We have analyzed
  a set of 1 minute cadence magnetograms of NOAA AR 8100 taken over a
  period of 6.5 hr by the Michelson Doppler Imager on board the Solar
  and Heliospheric Observatory. During this observing time span, seven
  homologous flares took place in the active region. We have computed
  the magnetic helicity injection rate into the solar atmosphere by
  photospheric shearing motions and found that a significant amount of
  magnetic helicity was injected during the observing period. In a strong
  M4.1 flare, the magnetic helicity injection rate impulsively increased
  and peaked at the same time as the X-ray flux. The flare X-ray flux
  integrated over the X-ray emission time strongly correlates with the
  magnetic helicity injected during the flaring interval. The integrated
  X-ray flux is found to be a logarithmically increasing function of
  the injected magnetic helicity. Our results suggest that injection of
  helicity and abrupt increase of helicity magnitude play a significant
  role in flare triggering.

---------------------------------------------------------
Title: Solar activity monitoring and forecasting capabilities at
    Big Bear Solar Observatory
Authors: Gallagher, P. T.; Denker, C.; Yurchyshyn, V.; Spirock, T.;
   Qiu, J.; Wang, H.; Goode, P. R.
2002AnGeo..20.1105G    Altcode:
  The availability of full-disk, high-resolution Ha

---------------------------------------------------------
Title: Topological changes of the photospheric magnetic field inside
active regions: a prelude to flares
Authors: Sorriso-Valvo, L.; Carbone, V.; Abramenko, V.; Yurchyshyn,
   V.; Noullez, A.; Politano, H.; Pouquet, A.; Veltri, P.
2002astro.ph..7244S    Altcode:
  The observations of magnetic field variations as a signature of flaring
  activity is one of the main goal in solar physics. Some efforts in
  the past give apparently no unambiguous observations of changes. We
  observed that the scaling laws of the current helicity inside a given
  flaring active region change clearly and abruptly in correspondence with
  the eruption of big flares at the top of that active region. Comparison
  with numerical simulations of MHD equations, indicates that the change
  of scaling behavior in the current helicity, seems to be associated to a
  topological reorganization of the footpoint of the magnetic field loop,
  namely to dissipation of small scales structures in turbulence. It is
  evident that the possibility of forecasting in real time high energy
  flares, even if partially, has a wide practical interest to prevent
  the effects of big flares on Earth and its environment.

---------------------------------------------------------
Title: Rapid Changes in the Longitudinal Magnetic Field Related to
    the 2001 April 2 X20 Flare
Authors: Spirock, Thomas J.; Yurchyshyn, Vasyl B.; Wang, Haimin
2002ApJ...572.1072S    Altcode:
  Big Bear Solar Observatory observed the X20 flare that occurred at
  approximately 21:50 UT on 2001 April 2 with its standard complement of
  instruments. In this paper, we discuss the evolution of high-resolution
  and high-cadence longitudinal magnetograph observations in the region
  of the flare. The data reveal that there was a significant increase
  in the magnetic field on the limbward side of the neutral line of the
  active region at the location of the flare, while the magnetic field
  on the side of the neutral line closer to the disk center remained
  constant. We discuss possible rearrangements in the active region's
  magnetic field that could lead to the observed changes.

---------------------------------------------------------
Title: Limb Prominence Eruption on 11 August 2000 as Seen From Ground-
    and Space-Based Observations
Authors: Shakhovskaya, A. N.; Abramenko, V. I.; Yurchyshyn, V. B.
2002SoPh..207..369S    Altcode:
  We report on a prominence eruption as seen in Hα with the Crimean
  Lyot coronagraph, the global Hα network, and coronal images from
  the LASCO C2 instrument on board SOHO. We observed an Hα eruption
  at the northwest solar limb between 07:38:50 UT and 07:58:29 UT on
  11 August 2000. The eruption originated in a quiet-Sun region and
  was not associated with an Hα filament. No flare was associated with
  the eruption, which may indicate that, in this case, a flux rope was
  formed prior to the eruption of the magnetic field. The Hα images
  and an Hα Dopplergram show a helical structure present in the erupted
  magnetic field. We suggest that the driving mechanism of the eruption
  may be magnetic flux emergence or magnetic flux injection. The limb
  Hα observations provide missing data on CME speed and acceleration
  in the lower corona. Our data show that the prominence accelerated
  impulsively at 5.5 km s<SUP>−2</SUP> and reached a speed slightly
  greater than 800 km s<SUP>−1</SUP> in a narrow region (h&lt;0.14
  R<SUB>⊙</SUB>) above the solar surface. The observations presented
  here also imply that, based only on a CME's speed and acceleration,
  it cannot be determined whether a CME is the result of a flare or an
  eruptive prominence.

---------------------------------------------------------
Title: Scaling Behavior of Structure Functions of the Longitudinal
    Magnetic Field in Active Regions on the Sun
Authors: Abramenko, V. I.; Yurchyshyn, V. B.; Wang, H.; Spirock,
   T. J.; Goode, P. R.
2002AAS...200.0309A    Altcode: 2002BAAS...34..643A
  In the framework of a refined Kolmogorov's hypotheses, the scaling
  behavior of the B<SUB>Z</SUB>--component of the photospheric magnetic
  field is analyzed and compared with flaring activity in solar active
  regions. We used SOHO/MDI, Huairou (China) and Big Bear measurements
  of the B<SUB>z</SUB>-component in the photosphere for nine active
  regions. We show that there is no universal behavior in the scaling
  of the B<SUB>z</SUB>-structure functions for different active
  regions. Scaling for a given active region is caused by intermittency
  in the field, ǎrepsilon<SUP>(B)</SUP>(ěc x), of magnetic energy
  dissipation. When intermittency is weak, the B<SUB>z</SUB>-field
  behaves as a passive scalar in the turbulent flow and the energy
  dissipation is largely determined by the dissipation of kinetic energy
  in active regions with low flare productivity. However, when the field
  ǎrepsilon<SUP>(B)</SUP>(ěc x) is highly intermittent, the structure
  functions behave as transverse structure functions of a fully developed
  turbulent vector field and the scaling of the energy dissipation is
  mostly determined by the dissipation of the magnetic energy (active
  regions with strong flaring productivity). We found that the spectrum
  of dissipation of the B<SUB>z</SUB> component is strongly related
  to the level of flare productivity of a solar active region. When
  the flare productivity is high, the corresponding spectrum is less
  steep. We also found that during the evolution of an NOAA AR 9393 the
  B<SUB>z</SUB> dissipation spectrum becomes less steep as the active
  region's flare activity increases. We suggest that the relation between
  scaling exponents and flare productivity of an active region enables
  us to monitor and forecast flare activity using only measurements of
  the B<SUB>z</SUB> component of the photospheric magnetic field. This
  work was supported in part by the Ukrainian Ministry of Science and
  Education, NSF-ATM (0076602 and 0086999) and NASA (9682 and 9738)
  grants. SOHO is a project of international cooperation between ESA
  and NASA.

---------------------------------------------------------
Title: Orientation of Magnetic Fields in Erupted Solar Filaments
    and Geoeffectiveness of Coronal Mass Ejections
Authors: Yurchyshyn, V. B.
2002AAS...200.3606Y    Altcode: 2002BAAS...34..693Y
  Coronal mass ejections (CMEs) are often associated with erupted magnetic
  fields or disappeared chromospheric filaments. The majority of CMEs
  headed directly toward the earth (halo CMEs) are observed at 1AU as
  magnetic clouds (MC). The 3D structure of a MC can be represented by a
  force-free flux rope. When CMEs reach the earth, they may or may not
  cause magnetic storms. The geoeffectiveness of CMEs depends on the
  orientation of the magnetic field in them. In our previous study we
  showed that the direction of the axial field in a MC and its helicity
  are consistent with the direction of the axial field and helicity of
  the erupted filaments. We also suggested that geoeffectiveness of
  a CME can be forecasted by using daily Big Bear Solar Observatory
  full disk Hα and SOHO EIT 195Å images and SOHO/MDI magnetograms,
  as well. Here we continue to study the orientation of magnetic
  fields in CMEs and its correlation with the occurrence of geomagnetic
  storms. The study includes 11 earth directed CMEs for which photospheric
  sources were reliably defined. Our results further demonstrate that
  the geoeffectiveness of a CME can be predicted by considering the
  orientation of the CME's magnetic fields. This work was supported in
  part by ATM-0076602, ATM-9903515 and NASA (NAG5-9682) grants. SOHO is
  a project of international cooperation between ESA and NASA.

---------------------------------------------------------
Title: Flare Activity and Magnetic Helicity Injection By Photospheric
    Horizontal Motions
Authors: Moon, Y. -J.; Chae, J.; Choe, G.; Wang, H.; Park, Y. D.;
   Yun, H. S.; Yurchyshyn, V.; Goode, P. R.
2002AAS...200.2002M    Altcode: 2002BAAS...34..673M
  We present observational evidence that the occurrence of homologous
  flares in an active region is physically related to the injection
  of magnetic helicity by horizontal photospheric motions. We have
  analyzed a set of 1 minute cadence magnetograms of NOAA AR 8100 taken
  over a period of 6.5 hours by Michelson Doppler Imager (MDI) on board
  Solar and Heliospheric Observatory (SOHO). During this observing time
  span, seven homologous flares took place in the active region. We have
  computed the magnetic helicity injection rate into the solar atmosphere
  by photospheric shearing motions, and found that a significant amount
  of magnetic helicity was injected during the observing period. In a
  strong M4.1 flare, the magnetic helicity injection rate impulsively
  increased and peaked at the same time as the X-ray flux did. The flare
  X-ray flux integrated over the X-ray emission time strongly correlates
  with the magnetic helicity injected during the flaring interval. The
  integrated X-ray flux is found to be a logarithmically increasing
  function of the injected magnetic helicity. Our results suggest that
  injection of helicity and abrupt increase of helicity magnitude play
  a significant role in flare triggering. This work has been supported
  by NASA grants NAG5-10894 and NAG5-7837, by MURI grant of AFOSR, by
  the US-Korea Cooperative Science Program (NSF INT-98-16267), by NRL
  M10104000059-01J000002500 of the Korean government, and by the BK 21
  project of the Korean government.

---------------------------------------------------------
Title: Core and Large-Scale Structure of the 2000 November 24 X-Class
    Flare and Coronal Mass Ejection
Authors: Wang, Haimin; Gallagher, Peter; Yurchyshyn, Vasyl; Yang,
   Guo; Goode, Philip R.
2002ApJ...569.1026W    Altcode:
  In this paper, we present three important aspects of the X1.8 flare
  and the associated coronal mass ejection (CME) that occurred on 2000
  November 24: (1) The source of the flare is clearly associated with
  a magnetic channel structure, as was noted in a study by Zirin &amp;
  Wang , which is due to a combination of flux emergence inside the
  leading edge of the penumbra of the major leading sunspot and proper
  motion of the sunspot group. The channel structure provides evidence for
  twisted flux ropes that can erupt, forming the core of a CME, and may
  be a common property of several superactive regions that have produced
  multiple X-class flares in the past. (2) There are actually three flare
  ribbons visible. The first can be seen moving away from the flare site,
  while the second and third make up a stationary ribbon near the leader
  spot. The moving ribbons could be due to a shock associated with the
  erupting flux rope or due to the interaction of erupting rope and the
  surrounding magnetic fields. In either case, the ribbon motion does
  not fit the classical Kopp-Pneuman model, in which the separation
  of ribbons is due to magnetic reconnection at successively higher
  and higher coronal altitudes. (3) From the coronal dimming observed
  with the EUV Imaging Telescope (EIT), the CME involved a much larger
  region than the initial X-class flare. By comparing high-resolution
  full-disk Hα and EIT observations, we found that a remote dimming
  area is cospatial with the enhanced Hα emission. This result is
  consistent with the recent model of Yokoyama &amp; Shibata that some
  dimming areas near footpoints may be due to chromospheric evaporation.

---------------------------------------------------------
Title: Space Weather: The Scientific Forecast
Authors: Wang, H.; Gallagher, P. T.; Yurchyshyn, V.
2002stma.conf..375W    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: How directions and helicity of the magnetic field in erupted
    solar filaments define geoeffectiveness of coronal mass ejections?
Authors: Yurchyshyn, V.
2002cosp...34E1426Y    Altcode: 2002cosp.meetE1426Y
  Coronal mass ejections (CMEs) are often associated with erupted magnetic
  fields or disappeared chromospheric filaments. The majority of CMEs
  headed directly toward the earth (halo CMEs) are observed at 1AU as
  magnetic clouds (MC). The 3D structure of a MC can be represented by a
  force-free flux rope. When CMEs reach the earth, they may or may not
  cause magnetic storms. The geoeffectiveness of CMEs depends on the
  orientation of the magnetic field in them. In our previous study we
  showed that the direction of the axial field in a MC and its helicity
  are consistent with the direction of the axial field and helicity of
  the erupted filaments. We also suggested that geoeffectiveness of
  a CME can be forecasted by using daily Big Bear Solar Observatory
  full disk H and SOHO EIT 195Å images and SOHO/MDI magnetograms,
  as well. Here we continue to study the orientation of magnetic
  fields in CMEs and its correlation with the occurrence of geomagnetic
  storms. The study includes earth directed CMEs for which photospheric
  sources were reliably defined. Our results further demonstrate that
  the geoeffectiveness of a CME can be predicted by considering the
  orientation of the CME's magnetic fields. This work was supported in
  part by ATM-0076602, ATM-9903515 and NASA (NAG5-9682) grants. SOHO is
  a project of international cooperation between ESA and NASA.

---------------------------------------------------------
Title: Analysis of Cancellations of Photospheric Current Helicity
    and Flares Forecasting
Authors: Sorriso-Valvo, L.; Abramenko, V.; Carbone, V.; Noullez, A.;
   Politano, H.; Pouquet, A.; Veltri, P.; Yurchyshyn, V.
2002EGSGA..27.3215S    Altcode:
  The observations of magnetic field variations as a signature of flaring
  activity is one of the main goal in solar physics. Some efforts in
  the past give apparently no unambigu- ous observations of changes. We
  observed that the scaling laws of the current helicity inside a given
  flaring active region change clearly and abruptly before the eruption
  of big flares at the top of that active region. Comparison with
  numerical simulations of MHD equations, indicates that the change of
  scaling behavior in the current helicity, seems to be associated to a
  topological reorganization of the footpoint of the magnetic field loop,
  namely to dissipation of small scales structures in turbulence. It is
  evident that the possibility of forecasting in real time high energy
  flares, even if partially, has a wide practical interest to prevent
  the effects of big flares on Earth and its environment.

---------------------------------------------------------
Title: Orientation of the Magnetic Fields in Interplanetary Flux
    Ropes and Solar Filaments
Authors: Yurchyshyn, Vasyl B.; Wang, Haimin; Goode, Philip R.; Deng,
   Yuanyong
2001ApJ...563..381Y    Altcode:
  Coronal mass ejections (CMEs) are often associated with erupting
  magnetic structures or disappearing filaments. The majority of CMEs
  headed directly toward the Earth are observed at 1 AU as magnetic
  clouds-the region in the solar wind where the magnetic field strength
  is higher than average and there is a smooth rotation of the magnetic
  field vectors. The three-dimensional structure of magnetic clouds can
  be represented by a force-free flux rope. When CMEs reach the Earth,
  they may or may not cause magnetic storms, alter Earth's magnetic field,
  or produce the phenomena known as auroras. The geoeffectiveness of a
  solar CME depends on the orientation of the magnetic field in it. Two
  M-class solar flares erupted on 2000 February 17. The second flare
  occurred near a small active region, NOAA Active Region 8872. This
  eruption was accompanied by a halo CME. However, the February 17 CME did
  not trigger any magnetic activity when it arrived at the Earth. Another
  powerful flare, on 2000 July 14, was also associated with a halo CME,
  which caused the strongest geomagnetic activity of solar cycle 23. Using
  ACE measurements of the interplanetary magnetic fields, we study the
  orientation of the magnetic flux ropes in both sets of magnetic clouds
  and compare them with the orientation of the solar magnetic fields
  and disappearing filaments. We find that the direction of the axial
  field and helicity of the flux ropes are consistent with those of
  the erupted filaments. Thus, the geoeffectiveness of a CME is defined
  by the orientation and structure of the erupted filament and by its
  magnetic helicity as well. We also suggest that the geoeffectiveness
  of a CME can be forecasted using daily full-disk Hα and Yohkoh images
  and MDI magnetograms as well.

---------------------------------------------------------
Title: Photospheric Plasma Flows Around a Solar Spot
Authors: Yurchyshyn, Vasyl B.; Wang, Haimin
2001SoPh..203..233Y    Altcode:
  We study photospheric plasma flows in an active region NOAA 8375, by
  using uninterrupted high-resolution SOHO/MDI observations (137 intensity
  images, 44 hours of observations). The active region consists of a
  stable large spot and many small spots and pores. Analyzing horizontal
  flow maps, obtained with local correlation tracking technique, we
  found a system of stable persistent plasma flows existing in the
  active region. The flows start on either side of the sunspot and
  extend over 100” to the east. Our measurements show that the speed
  of small sunspots and pores, averaged over 44 hours, was about 100 m
  s<SUP>−1</SUP>, which corresponds to root-mean-square longitudinal
  drifts of sunspots of 0.67°-0.76° day<SUP>−1</SUP>. We conclude
  that these large-scale flows are due to faster proper motion of the
  large sunspot relative to the ambient photospheric plasma. We suggest
  that the flows may be a good carrier to transport magnetic flux from
  eroding sunspots into the outer part of an active region.

---------------------------------------------------------
Title: Inter-Active Region Connection of Sympathetic Flaring on 2000
    February 17
Authors: Wang, Haimin; Chae, Jongchul; Yurchyshyn, Vasyl; Yang, Guo;
   Steinegger, Michael; Goode, Philip
2001ApJ...559.1171W    Altcode:
  We have analyzed high-resolution Hα full disk data from Big
  Bear Solar Observatory (BBSO); magnetograph and EUV data from the
  Michelson Doppler Imager, Large Angle and Spectrometric Coronagraph,
  and Extreme Ultraviolet Imaging Telescope on board SOHO; and Yohkoh
  soft X-ray data of 2000 February 17. Two sympathetic M-class solar
  flares erupted in succession in NOAA Active Region 8869 and 8872,
  respectively. The eruption from AR 8872 was followed by an extremely
  symmetric halo coronal mass ejection (CME). We demonstrate the loop
  activation, which appears to be the consequence of the first flare in
  AR 8869 and the cause of the second flare in AR 8872. The activation
  started in the form of a surge just after a filament eruption and its
  associated flare in AR 8869. The surge quickly turned into a set of
  disturbances that propagated at a speed of about 80 km s<SUP>-1</SUP>
  toward the other active region AR 8872. The second flare followed in
  less than an hour after the arrival of the disturbances at AR 8872. The
  moving disturbances appeared in absorption in both Hα and EUV 195
  Å images. The disturbances may represent mass transfer, which had
  a significant velocity component perpendicular to the field lines
  and, hence, caused the transport of field lines. In this case, the
  disturbances may be considered to be a special kind of surge, which we
  may call a “sweeping closed-loop surge.” We also demonstrated large
  area dimmings associated with the CME in three active regions. The
  dimming started from AR 8869 and AR 8872 and was extended to AR 8870,
  which was on the opposite side of the solar equator. We believe that
  both the activation of inter-active region loops and the large-scale
  dimming are the signatures of large-scale restructuring associated
  with the CME.

---------------------------------------------------------
Title: Parameters of the Turbulent Magnetic Field in the Solar
Photosphere: Power Spectrum of the Line-of-Sight Field
Authors: Abramenko, V. I.; Yurchyshyn, V. B.; Wang, H.; Goode, P. R.
2001ARep...45..824A    Altcode:
  Ground-based (Big Bear Solar Observatory) and extra-atmospheric
  (SOHO/MDI) measurements of the photospheric line-of-sight magnetic field
  of one active and two quiet regions are used to calculate power spectra
  of the field, taking into account the characteristic function for the
  diffraction limit of the telescope resolution. At high frequencies, the
  physically meaningful linear interval in the spectrum extends to a wave
  number of k=4.6 Mm-1 (spatial scale l=1.4 Mm) for the quiet regions and
  k=3.35 Mm-1 (l=1.9 Mm) for the active region. A high-frequency spectral
  break at k≥3 Mm-1 is associated with the characteristic telescope
  function; the position of the break and the spectral slope beyond the
  break do not reflect the turbulent state of the field. As the field
  recording improves, the break shifts toward higher frequencies. The
  spectral indices in the physically meaningful linear interval are
  substantially different for the active and quiet regions: in the active
  region (NOAA 8375), the spectrum behaves as E(k)≈k -1.7 (very close
  to the Kolmogorov index, -5/3) in the interval 0.78≤k≤3.35 Mm-1,
  while in the quiet regions E(k)≈k -1.3 for 0.77≤k≤4.57 Mm-1. This
  difference can be explained by the additional effect of a small-scale
  turbulent dynamo in the unperturbed photosphere. In this case, this
  mechanism can generate at least 6% of the magnetic energy of the
  photospheric line-of-sight field in quiet regions.

---------------------------------------------------------
Title: Magnetic Flux Cancellation Observed in the Sunspot Moat
Authors: Yurchyshyn, Vasyl B.; Wang, Haimin
2001SoPh..202..309Y    Altcode:
  In this paper we study the evolution of magnetic fields of a 1F/2.4C
  solar flare and following magnetic flux cancellation. The data are Big
  Bear Solar Observatory and SOHO/MDI observations of active region NOAA
  8375. The active region produced a multitude of subflares, many of them
  being clustered along the moat boundary in the area with mixed polarity
  magnetic fields. The study indicates a possible connection between the
  flare and the flux cancellation. The cancellation rate, defined from
  the data, was found to be 3×10<SUP>19</SUP> Mx h<SUP>−1</SUP>. We
  observed strong upward directed plasma flows at the cancellation
  site. Suggesting that the cancellation is a result of reconnection
  process, we also found a reconnection rate of 0.5 km s<SUP>−1</SUP>,
  which is a significant fraction of Alfvén speed. The reconnection
  rate indicates a regime of fast photospheric reconnection happening
  during the cancellation.

---------------------------------------------------------
Title: Magnetic Power Spectra Derived from Ground and Space
    Measurements of the Solar Magnetic Fields
Authors: Abramenko, V.; Yurchyshyn, V.; Wang, H.; Goode, P. R.
2001SoPh..201..225A    Altcode:
  We study magnetic power spectra of active and quiet regions by using
  Big Bear Solar Observatory and SOHO/MDI measurements of longitudinal
  magnetic fields. The MDI power spectra were corrected with Gaussian
  Modulation Transfer Function. We obtained reliable magnetic power
  spectra in the high wave numbers range, up to k=4.6 Mm<SUP>−1</SUP>,
  which corresponds to a spatial scale l=1.4 Mm. We find that the
  occurrence of the spectral discontinuity at high wave numbers,
  k≥3 Mm<SUP>−1</SUP>, largely depends on the spatial resolution
  of the data and it appears at progressively higher wave numbers as
  the resolution of the data improves. The spectral discontinuity in
  the raw spectra is located at wave numbers about 3 times smaller
  than wave numbers, corresponding to the resolution of the data, and
  about 1.5-2.0 times smaller in the case of the noise- and-resolution
  corrected spectra. The magnetic power spectra for active and quiet
  regions are different: active-region power spectra are described as
  ∼k<SUP>−1.7</SUP>, while in a quiet region the spectrum behaves
  as ∼k<SUP>−1.3</SUP>. We suggest that the difference can be
  due to small-scale dynamo action in the quiet-Sun photosphere. Our
  estimations show that the dynamo can generate more than 6% of the
  observed magnetic power.

---------------------------------------------------------
Title: Earthshine observations of the Earth's reflectance
Authors: Goode, P. R.; Qiu, J.; Yurchyshyn, V.; Hickey, J.; Chu,
   M. -C.; Kolbe, E.; Brown, C. T.; Koonin, S. E.
2001GeoRL..28.1671G    Altcode:
  Regular photometric observations of the moon's “ashen light”
  (earthshine) from the Big Bear Solar Observatory (BBSO) since December
  1998 have quantified the earth's optical reflectance. We find large
  (∼5%) daily variations in the reflectance due to large-scale weather
  changes on the other side of the globe. Separately, we find comparable
  hourly variations during the course of many nights as the earth’s
  rotation changes that portion of the earth in view. Our data imply
  an average terrestrial albedo of 0.297±0.005, which agrees with
  that from simulations based upon both changing snow and ice cover and
  satellite-derived cloud cover (0.296±0.002). However, we find seasonal
  variations roughly twice those of the simulation, with the earth being
  brightest in the spring. Our results suggest that long-term earthshine
  observations are a useful monitor of the earth's albedo. Comparison
  with more limited earthshine observations during 1994-1995 show a
  marginally higher albedo then.

---------------------------------------------------------
Title: Magnetic Power Spectra Derived From Photospheric Magnetic
    Fields
Authors: Abramenko, V. I.; Yurchyshyn, V.; Wang, H.; Goode, P. R.
2001AGUSM..SP41C04A    Altcode:
  We study magnetic power spectra of active and quiet regions by using
  Big Bear Solar Observatory and SOHO/MDI measurements of longitudinal
  magnetic fields. The MDI power spectra were corrected with Gaussian
  Modulation Transfer Function. We obtained reliable magnetic power
  spectra in the high wave numbers range, up to k=4.6 Mm<SUP>-1</SUP>,
  which corresponds to a spatial scale l=1.4 Mm. We find that the
  occurrence of the spectral discontinuity at high wavenumbers, k &gt;=
  3 Mm<SUP>-1</SUP>, largely depends on the spatial resolution of the data
  and it appears at progressively higher wave numbers as the resolution
  of the data improves. The spectral discontinuity in the raw spectra
  is located at wave numbers about 3 times smaller than wavenumbers,
  corresponding to the resolution of the data, and about 1.5 -- 2.0 times
  smaller in the case of the noise-and-resolution corrected spectra. The
  magnetic power spectra for active and quiet regions are different:
  active region power spectra are described as ~ k<SUP>-1.7</SUP>,
  while in a quiet region the spectrum behaves as ~ k<SUP>-1.3</SUP>. We
  suggest, that the difference can be due to small-scale dynamo action
  in the quiet sun photosphere. Our estimations show that the dynamo
  can generate more than 6% of the observed magnetic power.

---------------------------------------------------------
Title: Inter-Active Region Connection of Sympathetic Flaring on 2000
    February 17
Authors: Wang, H.; Chae, J.; Yurchyshyn, V.; Yang, G.; Steinegger,
   M.; Goode, P. R.
2001AGUSM..SP42A03W    Altcode:
  We have analyzed high resolution Hα full disk data from Big Bear
  Solar Observatory (BBSO), magnetograph and EUV data from MDI, LASCO
  and EIT on board SOHO, and Yohkoh soft X-ray data of February 17,
  2000. Two sympathetic M-class solar flares erupted in succession
  in NOAA 8869 and 8872, respectively. The eruption from AR 8872 was
  followed by an extremely symmetric halo CME. We demonstrate a new
  kind of loop activation, which appears to be the consequence of
  the first flare in AR 8869 and the cause of the second flare in
  AR 8872. The activation started in the form of a surge just after
  a filament eruption and its associated flare in AR 8869. The surge
  quickly turned into a set of disturbances that propagated at a speed of
  about 80 km/s toward the other active region AR 8872. The second flare
  followed in less than an hour after the arrival of the disturbances
  at AR 8872. The moving disturbances appeared in absorption in both
  Hα and EUV 195A images. The disturbances may represent mass transfer
  which had a significant velocity component perpendicular to the field
  lines and, hence, caused the transport of field lines. In this case,
  the disturbances may be considered to be a special kind of surge,
  which we may call a "sweeping closed-loop surge". Alternatively, the
  disturbances may represent fronts of compressive magnetohydrodynamic
  waves that were driven by the surge. We also demonstrated large area
  dimmings associated with the CME in three active regions. The dimming
  started from ARs 8869 and 8872, and was extended to AR 8870 which was
  on the opposite side of the solar equator. We believe that both the
  activation of inter-active region loops and the large scale dimming are
  the signatures of large scale re-structuring associated with the CME.

---------------------------------------------------------
Title: Orinetation of the Magnetic Fields in Interplanetary Flux
    Ropes and Solar Filaments
Authors: Yurchyshyn, V.; Wang, H.; Goode, P. R.; Deng, Y.
2001AGUSM..SH61A02Y    Altcode:
  Coronal mass ejections are often associated with erupting magnetic
  structures or disappearing filaments. Majority of CMEs headed directly
  toward the earth are observed at 1AU as magnetic clouds --- region in
  the solar wind where the magnetic field strength is higher than average
  and smooth rotation of the magnetic field vectors. The 3D structure
  of magnetic clouds can be represented by force-free flux rope. When a
  CME reaches the earth, it may or may not cause magnetic storms, alter
  Earth's magnetic field or produce the phenomena known as auroras. The
  geoeffectiveness of a solar CME depends on the orientation of the
  magnetic field in it. Two M-class solar flares erupted on February
  17, 2000. The second flare occurred near a small active region NOAA
  8872. The eruption was accompanied by a halo CME. However the February
  17 CME did not trigger any magnetic activity at the time it arrived at
  the earth. Another powerful flare on July 14, 2000 was also associated
  with a halo CME, which caused strongest geomagnetic activity in the
  solar cycle 23. Using ACE measurements of the interplanetary magnetic
  fields we study the orientation of the magnetic flux ropes in both
  magnetic clouds and compare it to the orientaion of solar magnetic
  fields and disappearing filaments. We find that the direction of
  the axial filed in the flux ropes and their helicity are consistent
  with the direction of the axial field and helicity of the erupted
  filaments. Thus, the geoeffectiveness of a CME is defined by the
  orientation and structure of the erupted filament and by its magnetic
  helicity as well. We also suggest that geoeffectiveness of a CME can
  be forecasted using daily full disk Hα and Yohkoh images and MDI
  magnetograms as well.

---------------------------------------------------------
Title: On the Correlation Between the Orientation of Moving Magnetic
    Features and the Large-Scale Twist of Sunspots
Authors: Yurchyshyn, V.; Wang, H.; Goode, P. R.
2001AGUSM..SP41C03Y    Altcode:
  We present new results on the nature of moving magnetic features
  (MMFs) deduced from Big Bear Solar Observatory observations of the
  longitudinal magnetic fields of two large solar spots. MMFs are small
  magnetic bipoles that move outward, across the moat of an eroding
  sunspot. We find that MMFs are not randomly oriented. To wit, in 21
  out of 28 (75%) MMF pairs, the magnetic element having the polarity
  of the sunspot was located farther from the sunspot. Furthermore,
  there is a correlation between the orientation of the bipole and that
  of the twist in a sunspot. For the two nearly round sunpots we studied,
  we found that the bipoles were rotated counterclockwise in the case of a
  clockwise twisted sunspot and clockwise for a spot with counterclockwise
  twist. We also found a correlation between the orientation of MMF
  bipole and the amount of twist in the spot. The MMF bipoles around
  the highly twisted sunspot are oriented nearly tangential to the edge
  of the sunspot; while in the slightly twisted sunspot the bipoles are
  oriented nearly radially, so that they point back to the spot.

---------------------------------------------------------
Title: On the Correlation between the Orientation of Moving Magnetic
    Features and the Large-Scale Twist of Sunspots
Authors: Yurchyshyn, Vasyl B.; Wang, Haimin; Goode, Philip R.
2001ApJ...550..470Y    Altcode:
  We present new results on the nature of moving magnetic features
  (MMFs) deduced from Big Bear Solar Observatory observations of the
  longitudinal magnetic fields of two large solar spots. MMFs are small
  magnetic bipoles that move outward across the moat of an eroding
  sunspot. We find that MMFs are not randomly oriented. To wit, in 21
  out of 28 (75%) MMF pairs, the magnetic element having the polarity
  of the sunspot was located farther from the sunspot. Furthermore,
  there is a correlation between the orientation of the bipole and that
  of the twist in a sunspot. For the two nearly round sunpots we studied,
  we found that the bipoles were rotated counterclockwise in the case of a
  clockwise twisted sunspot and clockwise for a spot with counterclockwise
  twist. We also found a correlation between the orientation of MMF
  bipole and the amount of twist in the spot. The MMF bipoles around
  the highly twisted sunspot are oriented nearly tangential to the edge
  of the sunspot, while in the slightly twisted sunspot the bipoles are
  oriented nearly radially so that they point back to the spot.

---------------------------------------------------------
Title: Magnetic Topology in 1998 November 5 Two-Ribbon Flare as
    Inferred from Ground-based Observations and Linear Force-free Field
    Modeling
Authors: Yurchyshyn, V. B.; Wang, H.; Qiu, J.; Goode, P. R.; Abramenko,
   V. I.
2000ApJ...540.1143Y    Altcode:
  We analyzed the three-dimensional structure of the linear force-free
  magnetic field. A longitudinal magnetogram of Active Region NOAA
  8375 has been used as the photospheric boundary condition. The 1998
  November 5 2B/M8.4 two-ribbon flare can be explained in the framework
  of quadrupolar reconnection theory: the interaction of two closed
  magnetic loops that have a small spatial angle. The energy derived from
  soft X-ray telescope (SXT)/Yohkoh data (3-6×10<SUP>30</SUP> ergs)
  is 1 order of magnitude higher than the lower limit of flare energy
  predicted by Melrose's model. The latter estimation was made using
  the linear force-free extrapolation. It was suggested that, taking
  into account the nonlinear character of the observed magnetic field,
  we can increase the lower limit of the magnetic energy stored in the
  studied magnetic configuration. The revealed magnetic configuration
  allows us to understand the observed location and evolution of the flare
  ribbons and the additional energy released during the gradual phase
  of the flare, as well. Besides, reconnection of closed magnetic loops
  can logically explain the connection between a two-ribbon flare and a
  giant X-ray postflare arch, which usually is observed after the flare
  onset. We emphasize that unlike the Kopp and Pneuman configuration,
  the model discussed here does not necessarily require destabilization
  and opening of the magnetic field.

---------------------------------------------------------
Title: Flare-Related Changes of an Active Region Magnetic Field
Authors: Yurchyshyn, V. B.; Abramenko, V. I.; Carbone, V.
2000ApJ...538..968Y    Altcode:
  It was shown recently that current helicity, calculated
  using the photospheric magnetic field vector measurements,
  possesses a well-pronounced scaling behavior. The sign
  singularity of two-dimensional structures of current helicity,
  h<SUB>c</SUB>=B<SUB>z</SUB>˙(∇XB)<SUB>z</SUB>, can be studied by
  introducing a signed measure and by calculating the power-law exponent,
  the cancellation exponent κ. The time variations of the cancellation
  exponent seem to be related to flare activity of an active region
  (AR). Periods of enhanced flaring are accompanied by a drop and
  subsequent rise of the cancellation exponent. Here we focus on the
  changes in the vortex structure of the photospheric magnetic field
  during the transition of an active region from low flaring to enhanced
  flaring state. We analyzed variations of the cancellation exponent,
  helicity imbalance, and total electric current in four flaring active
  regions and one quiet one. We show that the transition of an active
  region from a low flaring state to an enhanced one is always accompanied
  (in this study, the corresponding time interval is less than 2 hr)
  by the 30%-45% decrease of the cancellation exponent. In two active
  regions, a reliable 13%-22% decrease of the total electric current took
  place, and in three active regions the helicity imbalance changed. This,
  possibly, implies a reinforcement of the anticoriolis twist of the whole
  magnetic configuration. For comparison, the decrease of κ in the quiet
  active region does not exceed 10%. This can be interpreted as a real
  preflare reorganization of the vortex structure of the photospheric
  magnetic field: a combination of the exhausting of small-scale eddies
  along with the reinforcement of the total anticoriolis twist of the
  magnetic structure.

---------------------------------------------------------
Title: Energy Release in an Impulsive Flare
Authors: Qiu, J.; Wang, H.; Yurchyshyn, V. B.; Goode, P. R.;
   BBSO/NJIT Team
2000SPD....31.0258Q    Altcode: 2000BAAS...32..821Q
  We analyze the multi-spectral observations on an impulsive short-lived
  flare event, and demonstrate that the flare consisted of several
  flaring components with different evolution profiles, morphologies,
  energy spectra, and magnetic configurations. These observations suggest
  that the magnetic energy was released in this event in several ways. (1)
  Two hard X-ray components were observed by Yohkoh HXT. One component was
  brightened and reached its emission maximum more slowly than the other
  component by &gt; 15 seconds, and the spectrum of the slow component
  was much softer than the fast component. The coordinated high resolution
  ground-based observations from Big Bear Solar Observatory (BBSO) further
  demonstrate that these two hard X-ray components were each co-aligned
  with complicated Hα and magnetic field structures. Therefore, the two
  hard X-ray components should come from different magnetic reconnection
  processes at different locations. (2) Accompanying the flare, we find
  both hot and cool mass ejections. The cool mass ejection was related
  to the fast-varying non-thermal flare component, while the hot mass
  ejection was related to the flare component which exhibited a strong
  heating process. The hot mass ejection, or bright surge, also led
  to a long-lasting (for at least a few hours) bright EUV loop. Such
  observation offers a strong evidence that both pre-flare and post-flare
  heating of the chromospheric material occurred at the root of the
  bright surge. (3) We study the magnetic field configurations of the
  flare components, and propose that both the non-thermal and thermal
  components of the flare, together with the cool and hot surges, were
  produced by the magnetic reconnection of the large scale over-lying
  open field lines with the low-lying magnetic loops, while the gradual
  and thermal flare components and bright surge were located in the area
  of magnetic quadrupolar structures where moving magnetic features and
  flux cancellation were observed. The observations suggest that the
  proper motions in the region of the quadrupolar structure may enhance
  electric current along the separatrix and neutral point, and produce
  heating via current dissipation in the quadrupolar areas in the lower
  atmosphere both before and after the fast reconnection occurred.

---------------------------------------------------------
Title: Earthshine and the Earth's Reflectivity
Authors: Goode, P. R.; Hickey, J.; Qiu, J.; Yurchyshyn, V. B.; Koonin,
   S. E.; Brown, T.; Kolbe, E.; Chu, M.
2000SPD....3102121G    Altcode: 2000BAAS...32..833G
  The earth's climate is driven by the net sunlight reaching
  the earth, which depends on the solar irradiance and the earth's
  reflectivity. Changes in the the solar irradiance have been well-studied
  for twenty years, but the degree of variation in the earth's albedo
  is not so clear. We have been measuring the earthshine from Big Bear
  Solar Observatory (BBSO) since December 1998. Earthshine, or "ashen
  light", is sunlight reaching the eye of a nighttime observer after
  being successively reflected from the day side of the earth, and the
  dark face of the moon. The ratio of reflected light from the dark
  part of the moon to that from the bright part provides an absolutely
  calibrated, large scale measure of the earth's albedo. We have solved
  the long-standing problem of determining the scattering of sunlight
  from the moon as a function of lunar phase. Earthshine measurements
  of the earth's albedo are complementary to those from satellites. We
  find the earth's albedo varies by 20% with season, and by as much at
  5% from night to night. We put contemporaneous cloud cover data into
  a scene model and calculate a good agreement with our observations,
  but we also find some interesting differences. Using the scene model
  and monthly averaged cloud cover data from ISCCP, we find between 1986
  and 1990 (solar minimum to near solar maximum) that the change in the
  net irradiance into the climate system is several times larger from
  the varying albedo than from the varying solar irradiance. The two
  changes are in phase.

---------------------------------------------------------
Title: Magnetic Topology in November 5, 1998 Two-Ribbon Flare as
    Inferred from Ground-Based Observations and Linear Force-Free Field
    Modeling
Authors: Yurchyshyn, V. B.; Wang, H.; Qiu, J.; Goode, P. R.; Abramenko,
   V. I.
2000SPD....31.0153Y    Altcode: 2000BAAS...32..810Y
  We analyzed the 3D structure of the linear force-free magnetic field in
  an active region. A longitudinal magnetogram of AR NOAA 8375 has been
  used as the photospheric boundary condition. The Nov 5, 1998 2B/M8.4
  two-ribbon flare can be explained in the framework of quadrupolar
  reconnection theory: the interaction of two closed magnetic loops which
  have a small spatial angle. The energy derived from SXT/YOHKOH data (3
  - 6 x 10<SUP>30</SUP> ergs) is one order of magnitude higher than the
  lower limit of flare energy predicted by Melrose's model. The latter
  estimation was made using the linear force-free extrapolation. It is
  suggested that by taking into account the non-linear character of the
  observed magnetic field we can increase the lower limit of the magnetic
  energy stored in the studied magnetic configuration. The revealed
  magnetic configuration allows us to understand the observed location
  and evolution of the flare ribbons and the additional energy released
  during the gradual phase of the flare, as well. Also, the reconnection
  of closed magnetic loops can logically explain the connection between
  a two-ribbon flare and the giant X-ray post-flare arch which usually
  is observed after flare onset. We emphasize that unlike the Kopp and
  Pneuman configuration, the model discussed here doesn't necessarily
  need destabilization and opening of the magnetic field. This work was
  supported in part by NSF-ATM (97-14796) and NASA (NAG5-4919) grants.

---------------------------------------------------------
Title: Magnetic Topology in November 5, 1998 Two-Ribbon Flare as
    Inferred from Ground-Based Observations and Linear Force-Free Field
    Modeling
Authors: Yurchyshyn, V.; Wang, H.; Qiu, J.; Goode, P. R.; Abramenko,
   V. I.
2000ESASP.463..463Y    Altcode: 2000sctc.proc..463Y
  No abstract at ADS

---------------------------------------------------------
Title: Magnetic Power Spectra in the Solar Photosphere derived from
    Ground and Space based Observations
Authors: Abramenko, V.; Yurchyshyn, V. B.
2000ESASP.463..273A    Altcode: 2000sctc.proc..273A
  No abstract at ADS

---------------------------------------------------------
Title: On the Correlation between the Orientation of Moving Magnetic
    Features and the Large-Scale Twist of Sunpots
Authors: Yurchyshyn, V.; Wang, Haimin; Goode, Philip R.
2000ESASP.463..459Y    Altcode: 2000sctc.proc..459Y
  No abstract at ADS

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Title: Flare Associated Changes in the Helicity of the Solar
    Magnetic Field
Authors: Abramenko, V. I.; Yurchyshyn, V. B.; Carbone, V.
1999ESASP.448..679A    Altcode: 1999mfsp.conf..679A; 1999ESPM....9..679A
  No abstract at ADS

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Title: The Changes of the Current Helicity Scaling Prior to a Strong
    Solar Flare
Authors: Yurchyshyn, V. B.; Abramenko, V. I.; Carbone, V.
1999AAS...194.5404Y    Altcode: 1999BAAS...31..909Y
  Recently it has been shown (Abramenko et al., Sol. Phys. 178) the
  current helicity calculated by the photospheric magnetic field vector
  possesses a well pronounced scaling behavior. The sign-singularity of
  the 2D structures of current helicity can be studied by introducing the
  signed measure and by calculating some power-law exponent: cancellation
  exponent kappa . The time variations of the cancellation exponent
  seem to be related to flare activity of an active region: the periods
  of enhanced flaring are accompanied by a drop and subsequent rise of
  the cancellation exponent (Abramenko et al., A&amp;A. 334). Here we
  continue to study the flare-related changes of cancellation exponent
  paying special attention to the preflare situation. We have found
  that the significant decrease of kappa begins 1-3 hours prior to
  a strong flare. The reduce of the kappa means the changes in the
  transverse magnetic field structure. The preflare energy release
  produced by small-scale currents dissipation seems to supply observed
  preflare energetic phenomena such as preflare flocculi brightening and
  enhanced X-ray and microwave emission. So we are able to conclude that
  small-scale energy release in the transverse photospheric magnetic
  field take place prior to a strong flare. As soon as the evaluation
  of kappa needs only the calibrated vector magnetogram and some minutes
  for calculations the preflare drop of the cancellation exponent could
  be used for the short-time prediction of strong flares.

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Title: Evidence of preflare small-scale energy release on the basis
    of the magnetic field fractal analysis.
Authors: Abramenko, V. I.; Yurchyshyn, V. B.; Carbone, V.
1999joso.proc..188A    Altcode:
  The preflare changes in the complexity of the photospheric magnetic
  fields were studied. The two-dimensional structures of the current
  helicity of magnetic field were analyzed using the method of fractal
  analysis. It was shown that several hours prior to a strong flare the
  decreasing of the cancellation exponent of current helicity begins. This
  result assumes the preflare dissipation of small-scale photospheric
  electric currents and should be used for the short-time prediction of
  strong flares.

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Title: Magnetic fields and electric current in the filament of active
    region NOAA 7597, in connection with two-ribbon flare.
Authors: Yurchyshyn, V. B.
1999joso.proc..107Y    Altcode:
  By comparing the orientation of the photospheric transverse magnetic
  field with that of chromospheric fibrils the author shows that they
  significantly differ. It seems that the active region filament matches
  to the inversion polarity configuration.