Author name code: stellmacher
ADS astronomy entries on 2022-09-14
author:"Stellmacher, Goetz"
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Title: Velocity Difference of Ions and Neutrals in Solar Prominences
Authors: Wiehr, E.; Stellmacher, G.; Balthasar, H.; Bianda, M.
Bibcode: 2021ApJ...920...47W
Altcode: 2021arXiv210813103W
Marked velocity excesses of ions relative to neutrals are obtained
from two time series of the neighboring emission lines He I 5015
Å and Fe II 5018 Å in a quiescent prominence. Their Doppler
shifts show time variations of quasi-periodic character where the
ions are faster than the neutrals, 1.0 ≤ Vmacro(Fe
II)/Vmacro(He I) ≤ 1.35 in series A and ≤1.25 in
series B. This "ratio excess" confirms our earlier findings of a 1.22
ion velocity excess, but the present study shows a restriction in
space and time of typically 5 Mm and 5 minutes. The ratio excess is
superposed by a time- and velocity-independent "difference excess"
of -0.3 ≤ Vmacro(Fe II)-Vmacro(He I) ≤
+0.7 km s-1 in series A (also indicated in series B). The
high repetition rate of 3.9 s enables the detection of high-frequency
oscillations with several damped 22 s periods in series A. These show
a ratio excess with a maximum of 1.7. We confirm the absence of a
significant phase delay of He neutrals with respect to the Fe ions.
Title: Evidence for the Two-fluid Scenario in Solar Prominences
Authors: Wiehr, E.; Stellmacher, G.; Bianda, M.
Bibcode: 2019ApJ...873..125W
Altcode: 2019arXiv190401536W
This paper presents observational evidence of the different dynamical
behavior of neutral and ionized species in solar prominences. The
analysis of a time-series of Sr II 4078 Å and Na D spectra in a
quiescent prominence yields systematically larger Doppler shifts
(line-of-sight velocities) for the ions V LOS(Sr II) = 1.22
× V LOS(Na D). Both lines show a 30 minute oscillation of
good coherence. Sixteen hours later the same prominence underwent marked
morphological changes (with a rising dome), and the Sr II velocity
excess dropped to V LOS(Sr II) = 1.11 ×V LOS(Na
D). The same excess is found for the line pair Fe II 5018 Å and He I
5015 Å. The widths of the ionic lines, mainly non-thermally broadened,
are not related to the macro-velocities. The emission ratio of Na D
and Sr II, a measure of the electron density, yields n e
= 4 × 1010 cm-3, shows no relation with the V
LOS variation or with height above the limb, and seems to be
reduced 16 hr later during the active phase. We apply a new wavelength
reference from aureola spectra, which is independent of photospheric
velocity fields.
Title: The Na I and Sr II Resonance Lines in Solar Prominences
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 2017SoPh..292...83S
Altcode: 2017arXiv170502475S
We estimate the electron density, ne, and its spatial
variation in quiescent prominences from the observed emission ratio
of the resonance lines Na I 5890 Å (D2) and Sr II 4078
Å. For a bright prominence (τα≈25 ) we obtain
a mean ne≈2 ×1010cm−3;
for a faint one (τα≈4 ) ne≈4
×1010cm−3 on two consecutive days with
moderate internal fluctuation and no systematic variation with height
above the solar limb. The thermal and non-thermal contributions to
the line broadening, Tkin and Vnth, required
to deduce ne from the emission ratio Na I/Sr II cannot be
unambiguously determined from observed widths of lines from atoms of
different mass. The reduced widths, Δ λD/λ0,
of Sr II 4078 Å show an excess over those from Na D2 and
Hδ 4101 Å, assuming the same Tkin and Vnth. We
attribute this excess broadening to higher non-thermal broadening
induced by interaction of ions with the prominence magnetic field. This
is suggested by the finding of higher macro-shifts of Sr II 4078 Å
as compared to those from Na D2.
Title: The Electron Density in a Quiescent Prominence
Authors: Wiehr, E.; Stellmacher, G.; Bianda, M.
Bibcode: 2016CEAB...40...79W
Altcode:
We estimate the electron density, n_e, from the emission ratio of the
Na I D_2 and Sr II 4078 Å resonance lines. For a quiescent prominence,
we find a range 1.7≤ n_e≤3.4\cdot 10^{10}cm^{-3} with significant
differences between neighboring structures but not with height above
the solar limb. After seven hours of moderate evolutionary changes,
the prominence shows the same n_e range.
Title: Non-thermal line-broadening in solar prominences
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 2015A&A...581A.141S
Altcode: 2016arXiv160507923S
Aims: We show that the line broadening in quiescent solar
prominences is mainly due to non-thermal velocities.
Methods:
We have simultaneously observed a wide range of optically thin lines
in quiescent prominences, selected for bright and narrow Mg b emission
without line satellites from macro-shifts.
Results: We find a
ratio of reduced widths, ΔλD/λ0, of Hγ and Hδ
of 1.05 ± 0.03, which can hardly be attributed to saturation, since
both are optically thin for the prominences observed: τγ
≤ 0.3, τδ ≤ 0.15. We confirm the ratio of reduced
widths of He 4772 (triplet) and He 5015 (singlet) of 1.1 ± 0.05 at
higher significance and detect a width ratio of Mg b2
and Mg 4571 (both from the triplet system) of 1.3 ± 0.1.
Conclusions: The discrepant widths of lines from different atoms,
and even from the same atom, cannot be represented by a unique pair
[Tkin; Vnth]. Values of Tkin deduced
from observed line radiances using models indicate low temperatures
down to Tkin ≈ 5000 K. Non-thermal velocities, related to
different physical states of the respective emitting prominence region,
seem to be the most important line broadening mechanism.
Title: The Temperature of Quiescent Prominences
Authors: Wiehr, E.; Stellmacher, G.
Bibcode: 2015CEAB...39...35W
Altcode:
We simultaneously observed in solar prominences faint metallic
emission lines together with Hγand two He I lines from the singlet
and triplet systems, respectively. We find that the reduced widths
ΔλD/λ0 are not linearly related to the
square-root of the inverse atomic mass, as is expected from the Doppler
formula. Instead, each emission line is individually broadened. The
gradients in the VD2(1/μ) diagrams correspond
to unrealistically high Tkin≥104 K, which
contradict values deduced from line radiance observations yielding
temperatures down to at most 5000 K. A scenario of down-falling gas
clumps by Low et al. (2012) offers a plausible explanation for these
discrepancies.
Title: The Hot Skin of Prominence Structures
Authors: Wiehr, E.; Stellmacher, G.; Ramelli, R.; Bianda, M.
Bibcode: 2013CEAB...37..487W
Altcode:
We observe various emission lines in solar prominences and compare
the widths of He II 4686 Å, He I 4472 Å (triplet) and He I 5015 Å
(singlet) with those of the optically thin Hγ and Mg b_2 lines. The
latter two yield a thermal line broadening of 9000<T_{kin}<11
000 K, which fits the width of He I 5015 Å (singlet). However, He I
4471 Å (triplet) shows an excess of 1.1 indicating an excitation of
the triplet in 1.2 times hotter prominence regions. He II 4686 Å is
1.65 times broader and thus emitted in 2.73 times hotter regions of the
prominence-corona transition layer, PCTR. The linear radiance relations
He tripl/He II=50 and Hγ/He tripl=11.8 suggest a PCTR between each
fine-structure thread and the surrounding hot coronal gas.
Title: Helium Emissions Observed in Ground-Based Spectra of Solar
Prominences
Authors: Ramelli, R.; Stellmacher, G.; Wiehr, E.; Bianda, M.
Bibcode: 2012SoPh..281..697R
Altcode: 2012SoPh..tmp..221R; 2012arXiv1208.2153R
The only prominent line of singly ionized helium in the visible
spectral range, He II 4686 Å, is observed together with the He I 5015
Å singlet and the He I 4471 Å triplet line in solar prominences. The
Na D2 emission is used as a tracer for He II emissions which
are sufficiently bright to exceed the noise level near 10−6
of the disk-center intensity. The prominences thus selected are
characterized by small non-thermal line broadening and almost absent
velocity shifts, yielding narrow line profiles without wiggles. The
reduced widths [ΔλD/λ] of He II 4686 Å are 1.5 times
broader than those of the He I 4471 Å triplet and 1.65 times broader
than those of the He I 5015 Å singlet. This indicates that the He
lines originate in a prominence-corona transition region with outwards
increasing temperature.
Title: Balmer and Lyman Emission Lines in Solar Prominences
Authors: Wiehr, E.; Stellmacher, G.
Bibcode: 2009CEAB...33...99W
Altcode:
Space observations of Lyman lines are compared with ground-based
observations of Balmer lines for quiescent solar prominences of
comparable brightness defined by their Hβ emission. The integrated
spectral line radiances of the Lyman and the Balmer emissions show
differences which diminish with increasing upper level u and converge
toward highest level numbers. Lyman lines emitted from u=5 originate
from 250 times less emitters than the corresponding Balmer lines from
the same upper level. For u=8 this difference still amounts to a factor
of 65, supporting the idea of a distinct origin of the emissions of
both hydrogen series.
Title: On the origin of the Balmer and Lyman emission lines in
solar prominences
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 2008A&A...489..773S
Altcode: 2012arXiv1209.6264S
Aims: We show how the observed hydrogen Balmer and Lyman emission lines
constrain the modeling of quiescent solar prominences.
Methods:
We compare space observations of Lyman lines with ground-based
observations of Balmer lines for quiescent solar prominences of
comparable brightness defined by their Hβ emission.
Results:
The effective number densities of hydrogen atoms emitting from the
same upper level u deduced from the corresponding emerging Lyman
and Balmer line emissions show large differences that diminish
with increasing level number and converge at the highest level
numbers. Hydrogen atoms excited in u=5 contribute 250 times less,
and those in u=8 still contribute 65 times less to the Lyman than to
the corresponding Balmer emission, supporting the idea of distinct
spatial origin of the emissions of both series. This is also indicated
by the line widths. The high optical thickness of all Lyman members
allows the brightness temperature Tb to be estimated from
the spectral radiance at line center, where Tb is found to
be largely independent of the upper level number, in contrast to the
(known) behavior of the Balmer lines.
Title: Imaging of the He D3/Hβ Emission Ratio in Quiescent
Solar Prominences
Authors: Hirzberger, J.; Wiehr, E.; Stellmacher, G.
Bibcode: 2007ASPC..368..321H
Altcode:
Quiescent solar prominences have been observed simultaneously in
profile-integrated He D3 and Hβ emission with the SST on
La Palma. The two-dimensional ratio maps of the He D3 and
Hβ intensities are used to study temporal variations of intrinsic
prominence parameters. Sub-areas with substantial variation of
the intensity distribution indicate the evolution of prominence
structures. When the emission ratio remains unchanged, the evolving
threads are of largely equal physical state. Other regions which show
a temporal varying emission ratio indicate substancial evolution of
the intrinsic physical conditions. We propose that distance variation
between the threads affects different penetration of the EUV irradiation
required for populating of the He triplet system.
Title: Two-dimensional imaging of the He D_3/Hbeta emission ratio
in quiescent solar prominences .
Authors: Stellmacher, G.; Wiehr, E.; Hirzberger, J.
Bibcode: 2007MmSAI..78..108S
Altcode:
Simultaneous prominences spectroscopy with THEMIS in the emission
lines H-alpha, H-beta, HeD3, NaD2, Mgb2 and He(singlet)5015 lead to
an extended study of two-dimensional images simultaneously in H-beta
and HeD3. The spatial variation of the integrated line intensities and
their ratio shows mainly two characteristics: (a) A constant emission
ratio (even) in regions with substantial intensity variations; this
can be explained by a varying number of superposing threads with equal
physical states. (b) A varying emission ratio (often) tightly related
to intensity changes; this indicates a superposition of threads with
different physical states (most likely the gas-pressure). We also
observe temporal changes of the emission ratio which seem to be too
fast for a variation of the gas-pressure; here, we suppose a change of
the packing density of threads along the line-of-sight which affects
the penetration of ionizing UV radiation required for the He triplet
excitation.
Title: Two-Dimensional Mapping of the He D3/Hβ Emission
Ratio in Solar Prominences
Authors: Wiehr, Eberhard; Stellmacher, Goetz; Hirzberger, Johann
Bibcode: 2007SoPh..240...25W
Altcode:
Solar prominences have been simultaneously observed in the integrated
light of the He D3 and the Hβ emissions on two successive
days, using the SST on La Palma with its tip-tilt mirror locked on a
nearby white-light limb facular grain. The spatial and the temporal
variation of the integrated line intensities and their ratio shows
mainly two characteristics: (A) Constant emission ratio (even)
in regions with substantial intensity variations and (B) varying
emission ratio (often) tightly related to intensity structures of the
prominence. (A) May be explained by a different number of superposing
threads along the line of sight having very similar physical state. (B)
Indicates threads with different intrinsic physical states; these
may depend on the gas pressure or the inner structure of each thread,
i.e., the "packing density," affecting the penetration of ionizing EUV
radiation, which affects the He I level populations and thus the rate
of the triplet excitation.
Title: Two-dimensional imaging of the HeD3/H[Beta] emission ratio
in quiescent solar prominences
Authors: Wiehr, E.; Stellmacher, G.; Hirzberger, J.
Bibcode: 2007msfa.conf..261W
Altcode:
We extend our earlier studies of two-dimensional prominence imaging
by simultaneous observations of the HeD3 and H[Beta] emissions at
the 1m SST on La Palma. The observed small spatial variations of the
HeD3/H[Beta] ratio indicate rather homogeneous physical conditions
within prominences. Sub-regions do exist which show a largely uniform
ratio in spite of substantial spatial intensity variations. Here, the
fine-structures will exhibit almost uniform physical conditions. In
other regions with variations of the ratio parallel to the emissions,
the structures will have different intrinsic physical state.
Title: Solar prominences with Na and Mg emissions and centrally
reversed Balmer lines
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 2005A&A...431.1069S
Altcode: 2012arXiv1210.5643S
We observed bright solar limb prominences with significant emission
of NaD2 and Mgb2 simultaneously with the Hα, Hβ, HeD3, He^+4685,
and the He^singl 5015 Å lines, using the THEMIS telescope on
Tenerife. We find that most prominences with significant NaD2 and
Mgb2 emissions show pronounced centrally reversed Hα profiles, and
occasionally even of Hβ; the strongest emissions reach integrated
intensities Eβ>16×{}104 [ erg/(cm2 s str)]
. The centrally reversed profiles are well reproduced by semi-infinite
models. The source function reaches Sα≤{}36 × {}104
[ erg/(cm2 s str Å)] corresponding to an excitation
temperature T_exα≈3950 K; here, the optically thickness of
Hα amounts τ^0α≈{}10. The line widths of the NaD2, Mgb2,
and HeD3 profiles yield kinetic temperatures 7000≤{}T_kin<8000
K and non-thermal broadening v_tu=5 km s-1.
Title: Spectroscopy of Solar Prominences Simultaneously From Space
and Ground
Authors: Stellmacher, G.; Wiehr, E.; Dammasch, I. E.
Bibcode: 2003SoPh..217..133S
Altcode: 2013arXiv1303.1126S
We present a comprehensive set of spectral data from two quiescent
solar prominences observed in parallel from space and ground: with
the VTT, simultaneous two-dimensional imaging of Hβ4862 Å and Caii
8542 Å yields a constant ratio, indicating small spatial pressure
variations over the prominence. With the Gregory, simultaneous spectra
of Caii 8542 Å and Hei 10830 Å were taken, their widths yielding
8000 K <Tkin<9000 K and 3<vnth<8
km s−1. The integrated line intensities show a distinct
relation E(Hei) versus E(Caii) for each prominence (`branching'). The
intensity ratio of the helium triplet components is used for a
simple estimate of the optical thickness, which is τ<1.0 for the
fainter prominence but reaches up to τ=2.0 for the brighter one. The
τ0 values allow us to deduce the source function from
the central line intensities and thus a mean excitation temperature
Texmean=3750 K, which determines the relative
populations of the helium 3S and 3P levels. With
SUMER, we sequentially observed six spectral windows containing
higher Lyman lines, `cool' emission lines from neutrals and singly
charged atoms, as well as `hot' emission lines from ions like Oiv,
Sv, Nv, Ov, and Svi. The spatial variation of the EUV lines along the
SUMER slit shows a pronounced maximum at the main prominence body and
`side-regions' where the `hot' lines are significantly enhanced with
respect to the `cool' lines from neutral and singly-ionized atoms. These
selected locations were averaged over 7'' and the resulting mean EUV
lines were fitted by Gaussians yielding realistic widths and integrated
line intensities. The intensities of `hot' lines blue-wards of the
Lyman series limit appear reduced in the main prominence body but
enhanced in the `side-regions'. This absorption is also visible in TRACE
images of Feix/x171 Å as fine dark structure which covers only parts
of the main (`cool') prominence body. The Lyman lines show a smooth
decrease of both line widths and integrated emission, with increasing
upper level k=5 to k=19; the widths are smaller for the prominence
that yields lower Tkin from the ground-based spectra. The
level populations along the line of sight follow for 5 lekle a smooth
Boltzmann distribution with Tex>6×104 K, the
levels k>8 appearing more and more overpopulated. The larger widths
of the Lyman lines require high non-thermal broadening close to that of
`hot' EUV lines. In contrast, the Heii emission is more related to the
`cool' lines.
Title: Spectroscopy of solar prominences from space and ground
Authors: Dammasch, I. E.; Stellmacher, G.; Wiehr, E.
Bibcode: 2003AN....324..338D
Altcode:
Two quiescent solar prominences were observed in July 2000 from
SUMER aboard SOHO and from the two German solar telescopes at
Tenerife. Two-dimensional images taken at the VTT simultaneously in the
spectral lines Hβ at 4862 Å and Ca II at 8542 Å show no significant
spatial variation of their pressure-sensitive emission ratio. Slit
spectra of the Ca II 8542 Å and He i 10830 Å lines obtained at the
Gregory-Coudé telescope yield 8000 K < T_kin < 9000 K and 3 km/s
< V_n-th < 8 km/s. Among the various spectral ranges observed with
SUMER, we first investigate the Lyman emission lines, which were fitted
by Gaussians yielding reliable spectral radiances and line widths for
the series members 5<k<18. A determination of the level population
gives for the lower series members a Boltzmann temperature of 60 000 K,
the higher members being over-populated. This temperature indicates an
origin of the Lyman lines from hot surroundings of the cool prominence
body seen in the ground-based data; this also holds for the `hotter'
SUMER lines.
Title: Spatial offsets between lines and continuum in limb faculae
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 2001SoPh..202..259S
Altcode:
High-spatial-resolution spectra of limb faculae show spatial
displacements of line cores relative to the adjacent continuum at cos
θ<0.35, confirming results from earlier photographic analyses. The
observed displacements are geometric measures which probe the upper
atmospheric layers of fluxtubes forming facular grains. We selected
spectra with highest contrast and smallest width of the facular
continuum streaks, in order to avoid clustered structures. The spatial
displacements of Stokes-Q and -V maxima were also measured: we find
Q-signals spatially located near the continuum, as is expected from
their origin in line wings; V-signals - which should give evidence
for the existence of horizontal fields - are not found, except for
one case of a 'hidden' pore.
Title: Two-dimensional photometric analysis of emission lines in
quiescent prominences
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 2000SoPh..196..357S
Altcode:
Emission lines from quiescent prominences were observed simultaneously
through narrow-band interference filters, thus integrating the total
line intensities without the use of a spectrograph. Simultaneous
exposures (50 ms) on three electronically connected CCD cameras at
the 70 cm VTT on Tenerife assured almost identical influence of the
Earth's atmosphere and a spatial resolution of ≤ 1 arc sec. The
resulting spatially high-resolution two-dimensional images in Hβ,
Hα, and Ca+8542, calibrated in units of the disk-center
intensities, allow a two-dimensional mapping of emission ratios yielding
relevant physical parameters. The emission relation between Hα and
Hβ, which depends on the total optical thickness, confirms earlier
photometric results from spectra, however, with a large sample of data
points from six prominences. It demonstrates the saturation effects
towards brighter prominences or prominence locations. The relation
between Ca+8542 and Hβ, which depends on the gas pressure,
is found to vary between different prominences but is nearly constant
within one prominence. Its mean spatial variation of ≤ 30% within
one prominence may be interpreted in terms of a magnetic field with
variations of ≤5%. The brightness distribution in most prominences
is not smooth but indicates preferred values, which are interpreted
as superpositions of several fine structures.
Title: Two-dimensional Mapping of Emission Ratios in Quiescent
Prominences
Authors: Wiehr, E.; Stellmacher, G.
Bibcode: 1999ESASP.448..435W
Altcode: 1999ESPM....9..435W; 1999mfsp.conf..435W
No abstract at ADS
Title: Continuum photometry of solar white-light faculae
Authors: Sütterlin, P.; Wiehr, E.; Stellmacher, G.
Bibcode: 1999SoPh..189...57S
Altcode:
We have determined absolute continuum intensities and brightness
temperatures of individual facular grains at a spatial resolution
limited by the φ=50 cm aperture of the SVST on La Palma. A facular
region at θ≈57° was observed simultaneously in three narrow
continuum windows at 450.5, 658.7, and 863.5 nm. We corrected for
image degradation by the Earth's atmosphere using the speckle masking
method. The brightness temperatures do not exactly follow the Planck
law. The differences of Tblue−Tred=220
K and Tir−Tred=−42 K reflect the
wavelength dependence of the continuum formation depth. The (red)
temperatures of 250 facular grains show excesses between 250
and 450 K above their undisturbed neighborhood. The wavelength
dependence of the relative intensity ratios Cλ=
[Ifac/Iphot] λshow a large scatter
around mean values of Cblue/Cred=1.075 and
Cir/Cred=0.98. We determined the center-to-limb
variation of the 863.5 nm continuum contrast for 0.17>cosθ>0.39
by measuring 270 grains in reconstructed facular images. The
upper envelope of the data points increases linearly to 1.5 at
cos θ=0.17. Application of the mean color dependence yields green
contrasts up to C550=1.7, which is far higher than previously
observed values. The behaviour for cos θ>0.17 is estimated from
(unreconstructed) frame-selected best images taken over a time interval
of 7 hours. Six distinct facular regions clearly discernible during
the whole time interval indicate a slight contrast decrease towards
the extreme limb. The observed quantities are useful for an adjustment
of model calculations and for a discrimination of competing models.
Title: The hot prominence periphery in EUV lines
Authors: de Boer, C. R.; Stellmacher, G.; Wiehr, E.
Bibcode: 1998A&A...334..280D
Altcode:
Two sets of He I and metallic lines were observed with the EUV
spectrograph SUMER in a quiescent prominence. H, He, and Ca II
lines were observed simultaneously with both German telescopes on
Tenerife. The visible lines from elements with different atomic
weights yield thermal and non-thermal broadening parameters of 7500
<= Tkin <= 8000 K and 2.5 <xi <5.0 km/s for the
cool prominence body. The EUV lines, however, show line widths which
correspond to much higher temperatures and non-thermal velocities. If
the calculated formation temperature for every individual ion is
assumed, the observed line widths require non-thermal velocities of 14 -
25 km/s. The narrowest reduced widths of the EUV He I 584 and He I 537
lines are 3.1 and 2.9 times broader than those of the visible He D_3
and He 3888 lines. If this is due to optical depth effects in the EUV
lines, one obtains tau_0 (584) ~ 8*10(3) and tau_0 (537) ~ 2*10(3)
, respectively. The emission ratios of the Ca II-to-Balmer lines
vary little inside the prominence, indicating a largely constant gas
pressure. The ratios of the visual He-to-Balmer lines as well as those
of the EUV He-to-metallic lines show a significant branching between
peripheral and central prominence regions. The total emissions in the
main prominence body amount to 13, 0.3, and 4 [Watt/ (m(2*) ster)]
for the 584, 537, and D_3 lines, respectively. The observed emission
ratio E(He 584)/E(He 537)= 45 agrees with model calculations whereas
their total emissions are about 37 times higher than calculated. The
observed ratio E(He D_3)/ E(He 584)~0.3 is about 15 times smaller
than model predictions. The observations indicate that the emissions
of different ions originate from individual (isothermal) threads with
different temperatures between 10(4) and 10(5) K.
Title: Prominence Emissions with SUMER and Optical Telescopes
Authors: Wiehr, E.; Stellmacher, G.; de Boer, C. R.; Sütterlin, P.
Bibcode: 1998ASPC..155..331W
Altcode: 1998sasp.conf..331W
No abstract at ADS
Title: About polar ejection events and surges
Authors: Loucif, M. L.; Koutchmy, S.; Stellmacher, G.; Georgakilas,
A.; Bocchialini, K.; Delaboudinière, J. -P.
Bibcode: 1998ESASP.421..299L
Altcode: 1998sjcp.conf..299L
No abstract at ADS
Title: Wave Activity and Prominence Eruption
Authors: Baudin, F.; Bocchialini, K.; Delannee, C.; Koutchmy, S.;
Stellmacher, G.; Shibata, K.; Veselovsky, I. S.; Panasenko, O. A.;
Zhukov, A. N.
Bibcode: 1998ASPC..150..314B
Altcode: 1998IAUCo.167..314B; 1998npsp.conf..314B
No abstract at ADS
Title: Prominence Emission Lines Observed with SUMER and Two
Ground-Based Telescopes
Authors: de Boer, C. R.; Stellmacher, G.; Wiehr, E.
Bibcode: 1998ASPC..150..196D
Altcode: 1998npsp.conf..196D; 1998IAUCo.167..196D
No abstract at ADS
Title: Three colour photometry of solar limb faculae.
Authors: de Boer, C. R.; Stellmacher, G.; Wiehr, E.
Bibcode: 1997A&A...324.1179D
Altcode:
The contrasts of limb faculae at various heliocentric angles are
observed in three continuum windows largely free of absorption
lines. Observations with interference filters show a contrast decrease
with wavelength which is not found when using an `UBF' to select the
shortest continuum window. Limb faculae in speckle-reconstructed images
yield contrasts being typically 1.2 times higher than those deduced from
the `best images' of the corresponding bursts. The fit of the wavelength
dependence (`colour index') to a black-body law is significantly better
for the contrasts deduced from the reconstructed images than for the
contrasts from the best images. The uncorrected contrasts yield a mean
facular temperature excess of 200-300K; those from the reconstructed
images yield about 470 K. The center-to-limb variation is found to be
much smaller than the fluctuations between individual faculae.
Title: The helium singlet-to-triplet line ratio in solar prominences.
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1997A&A...319..669S
Altcode:
The emissions of the He singlet line at 6678Å and the He triplet line
at 4471Å are simultaneously observed in three solar prominences. For
two of them, the line pairs He-D_3_/Hbeta_ and
Ca^+^8662/Hbeta_ were also observed. Comparisons with model
calculations show that the emission line ratios require low densities
(n_H_=~3.10^10^cm^-3^), low gas pressures (P_g_=~0.02dyn/cm^2^),
and large physical slab widths. The relative He-to-H number density
cannot be much lower than y=0.1.
Title: Emission Lines in a Quiescent Prominence Observed with the
SUMER, VTT, a nd Gregory Telescopes
Authors: Wiehr, E.; de Boer, C. R.; Stellmacher, G.; Sutterlin, P.
Bibcode: 1997ASPC..118..294W
Altcode: 1997fasp.conf..294W
A number of emission lines have been observed in a quiescent prominence
with the two German telescopes on Tenerife and with SUMER. The Gregory
telescope monitored simultaneously the lines H_8 3889, He 3888, Ca(+\:)
8498, the VTT simultaneously the lines H_β, He-D_3, Ca(+\:) 8542, and
H_α slit jaw pictures on 1024 x 1024 CCDs. At the same time, SUMER
monitored successively three combinations of EUV lines containing He
584, He 537 in the second, and Ar, N(+) , C, C(++) , O, O(+) , O(++)
, S(++) , S(+++) lines in the first order. Two dimensional images in
the various EUV lines establish the anti-relation between temperature
and Balmer brightness.
Title: Branching of the helium-to-Balmer emission ratio in solar
prominence structures.
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1995A&A...299..921S
Altcode:
The Halpha_, Hbeta_, and He D_3_ emission
lines are simultaneously observed with high spatial resolution at
the VTT on Tenerife. It is found that the emission ratios He D_3_/
Hbeta_ and He D_3_/Halpha_ show typical mean
values for each individual prominence. This branching is related
to the mean kinetic temperature and to the structuring of each
prominence. Whereas the Balmer excitation is almost uniformly
distributed throughout prominences, the He excitation is enhanced
in structured prominences of low Balmer brightness or outer parts
of unstructured bright prominences, where exciting and ionizing EUV
radiation can freely penetrate. In these regions the He ionization
may exceed that of hydrogen. The atmospheric prominence parameters
are not yet sufficiently known to allow a reliable determination of
the solar Helium abundance.
Title: The Hα and Hβ emissions in solar prominence structures.
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1994A&A...290..655S
Altcode:
High precision photometry of the Halpha_ and
Hbeta_ emissions is performed from spectra of four
spatially high resolved quiescent prominences. The data are
compared with recent observations and calculations. It is
found that for faint emissions the observed Balmer decrement
D=E_tot_(Halpha_)/E_tot_(Hbeta_) significantly
exceeds the limiting value D=10.0 calculated for slab models. In
contrast to former observations, the spatially and spectrally high
resolved emission profiles do not require a hot and a cool component
for an optimal fit. The deduced source functions do not yield a common
value for different prominences, but show an individual mean for each
prominence with a tendency for an increase with the optical thickness
of Halpha_. Optically thick Halpha_ emissions with
central absorptions are spatially related with narrow Hbeta_
emissions and hence with small kinetic temperatures. The narrow
Hbeta_ emissions exist over a large range of optical
thickness and show equal macroscopic shifts for individual emission
features favouring a picture of closely tied bundles of threads.
Title: Dependence of the He/H_8_ emission ratio on brightness,
temperature, and structuring of prominences
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1994A&A...286..302S
Altcode: 2012arXiv1211.3636S
The line pair He 3888 and H_8_ 3889 has been observed simultaneously
with the Ca^+^8498 line in a number of quiescent prominences. The
He/H_8_ emission ratio R is found to cover defined parts of a general
anti-correlation with the total H_8_ emission, depending on the
kinetic temperature, T_kin_, of the individual prominence: High H_8_
brightness is related to small R and Tkin values and preferably occurs
in prominences with less significant fine-structure.
Title: Chromospheric Faculae as Filaments Feet?
Authors: Koutchmy, S.; Stellmacher, G.
Bibcode: 1994emsp.conf...91K
Altcode:
No abstract at ADS
Title: Influence of non-thermal broadening on the He 3889/H8 emission
ratio in prominence fine-structures
Authors: Stellmacher, G.; Wiehr, E.; Grupe, D.
Bibcode: 1992A&A...265..781S
Altcode:
The neighboring emission lines H8 and He near 3889 A were observed in a
quiescent prominence at high spatial resolution. The systematic increase
of the He/H8 emission ratio R towards the edges of the prominence is
found to be largely cospatial with a corresponding behavior of the
nonthermal line-broadening parameter Xi while the thermal broadening
does not increase. The good relation between R and Xi also exists in
the fine-structures. This is explained by broadening of the absorption
coefficient increasing the efficiency of the exciting UV radiation
preferably for the (heavier) helium. Interpretation of the nonthermal
broadening parameter in terms of a velocity dispersion may favor the
influence of waves.
Title: Structural changes in the solar corona during the July
1991 eclipse
Authors: Zirker, J. B.; Koutchmy, S.; Nitschelm, C.; Stellmacher, G.;
Zimmermann, J. P.; Martinez, P.; Kim, I.; Dzyubenko, N.; Kurochka,
L.; Makarov, V.
Bibcode: 1992A&A...258L...1Z
Altcode:
Preliminary results of the analysis of radially filtered pictures
obtained at several hours interval during the July 11, 1991 total
solar eclipse are given. Instrumental parameters and method are
outlined. Structural changes are discussed.
Title: Modelling the moustache phenomenon in network regions
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1991A&A...251..675S
Altcode:
The intensity enhancement in the inner line wings (moustache) of
Mgb1 5183 and Fe 5434.5 A observed in Ca(+) K bright points outside
active regions is found to result from a superposition of a hot
component (representing the magnetic structure) surrounded by a cool
(intergranular) region. The I + V and I - V profiles of the magnetically
sensitive line Fe 6302.5, observed strictly simultaneously with Mgb1,
are equally well modeled by the same procedure (which in an earlier
paper had successfully been used to explain the gap effect of Zeeman
insensitive lines in plages). The Mgb1 moustaches are cospatial with
the simultaneously observed Fe 6302.5 gaps. Their equal spatial extent
indicates equal width of the temperature and the magnetic structures
of the Ca(+) K region.
Title: Geometric line elevation in solar limb faculae
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1991A&A...248..227S
Altcode:
Spectra of markedly visible white light faculae near the solar limb are
used to determine the geometric displacement, Delta-h, of line cores
with respect to their adjacent continuum. The observed Delta-h are
plotted as a function of the excitation potential and, respectively,
equivalent width of the different lines. Comparison with calculated
Delta-h from a photospheric LTE model shows that the observed facula
values significantly exceed the photospheric ones.
Title: Stokes-V in an active prominence
Authors: Wiehr, E.; Stellmacher, G.
Bibcode: 1991A&A...247..379W
Altcode:
Stokes-V spectra of the Ca(+)8542 emission were taken with a CCD in
an active prominence showing extremely high line-of-sight velocities
up to 25 km/s. The spatial resolution allows detecting prominence
fine-structures as small as 1.1 arcsec. Exact field strengths were
determined from the measured steepness of the individual emission line
flanks. Values between 75 and 180 Gs are obtained. No indication is
found for a dependence of the field strength on the spatial resolution
or on the line-of-sight velocity, nor on the emission brightness.
Title: The magnetic-field polarity of quiescent prominences
Authors: Kim, I. S.; Klepikov, V. Y.; Koutchmy, S.; Stepanov, A. I.;
Stellmacher, G.
Bibcode: 1990PAZh...16..545K
Altcode:
A statistical analysis of magnetographic data on quiescent solar
prominences is presented. The existence of two different magnetic
field systems in quiescent prominences is suggested. The first system
is oriented opposite to the underlying photospheric field; the angle
between the long axis of the filament and the field direction is
equal to 15 deg and B-parallel equals 15-18 G. The polarities of the
second system and of the underlying photospheric field are the same,
B-parallel = 5-7 G.
Title: Magnetic Field Polarity of Quiescent Prominences
Authors: Kim, I. S.; Klepikov, V. Y.; Koutchmy, S.; Stepanov, A. I.;
Stellmacher, G.
Bibcode: 1990SvAL...16..234K
Altcode:
No abstract at ADS
Title: Doppler Velocity Oscillations in Quiescent Prominences
Authors: Wiehr, E.; Balthasar, H.; Stellmacher, G.
Bibcode: 1990LNP...363..255W
Altcode: 1990IAUCo.117..255W; 1990doqp.coll..255W
No abstract at ADS
Title: Velocity and magnetic field fluctuations in penumbral
fine-structures
Authors: Wiehr, E.; Stellmacher, G.
Bibcode: 1989A&A...225..528W
Altcode:
Spatially very highly resolved spectra of sunspot penumbrae show that
the Evershed effect is not spatially related to the continuum intensity
fluctuations. The line asymmetry and the core shift (both a signature
of the Evershed effect) show fluctuations at a larger horizontal scale
than the continuum and a trend for an anticorrelation, in the sense
that locations with smaller asymmetry trend to show larger shifts. The
Zeeman broadening also shows variations at a larger spatial scale
than the continuum. There is no indication for field enhancements
in dark continuum streaks, some spots even show a certain trend for
enhanced field strengths in bright streaks. The absence of a general
relation to continuum streaks might be explained by the finding that
the continuum structures in the spectrum are almost invisible at
the formation height of the Fe 5576-A line, where a coarser spatial
structure of a few arcsec width occurs.
Title: Magnetic fields of solar prominences: strength and latitude
distribution.
Authors: Kim, I. S.; Klepikov, V. Yu.; Koutchmy, S.; Stepanov, A. I.;
Stellmacher, G.
Bibcode: 1989BSolD..11...98K
Altcode:
According to the data obtained by a Nikolsky-type magnetograph
during 1979 - 1986 there are two maxima in histograms
"occurrence-B∥": O - 21 G and 27 - 36 G. The probability of
the minimum between these maxima is equal to 82%. The first maximum may
be divided into three distributions with peaks at 8, 15 and 20 G. The
second maximum refers to active latitude prominences. The major part
of the data (80%) belongs to the pre-minimum and minimum epochs. For
this period the average latitude of prominence formation is less than
20°. The authors believe that the peak at 15 G characterizes the
critical field strength of prominence formation.
Title: Doppler Velocity Oscillations in Quiescent Prominences
Authors: Wiehr, E.; Balthasar, H.; Stellmacher, G.
Bibcode: 1989HvaOB..13..131W
Altcode:
No abstract at ADS
Title: Oscillations in presence of local magnetic fields.
Authors: Wiehr, E.; Balthasar, H.; Stellmacher, G.
Bibcode: 1988ESASP.286..269W
Altcode: 1988ssls.rept..269W
Oscillatory Doppler shifts in sunspots and in small fluxtubes are
observed using either the intensity profile of lines with negligible
magnetic splitting or the circular Zeeman profile (Stokes-V inversion
point) of lines with strong Zeeman splitting. Sunspot umbrae
show local 5 min oscillations of reduced amplitude as compared to
the neighbouring photosphere. Occasionally the authors find 5 min
oscillations of opposite phase at both outer penumbral borders. This
could be interpreted as tilting and bobbing of the spot as a whole
on the oscillating solar surface. In contrast to these larger scale
sunspot fluxtubes the gas in the small fluxtubes of a few hundred km
diameter seems to fully participate in the photospheric oscillations
without any interaction with the magnetic field. Prominence magnetic
fields show sometimes a reaction to the photospheric 5 min and to the
chromospheric 3 min oscillations, in addition several other periods
are found. Indication is found for eigenmodes of Alfvén waves.
Title: Periodic and quasiperiodic Doppler velocity variations in
solar prominences along one spatial direction
Authors: Balthasar, H.; Wiehr, E.; Stellmacher, G.
Bibcode: 1988A&A...204..286B
Altcode:
Temporal variations of the Doppler displacement of the Hα-emission
line were measured in four quiescent prominences in autumn 1986 at
the recently installed Gregory telescope on Tenerife. As detector,
a 100×100 pixel diode array was used. The length of the time series
was up to seven hours. The slit was oriented parallel to the solar
limb in the first case and perpendicular in the others. In November
1987 another prominence was observed with a 256×256 pixel camera
simultaneously in Ca+H and Hɛ over five hours. In this case,
the slit was oriented parallel to the solar limb. The result for the
two lines are in good agreement. The authors earlier result of periods
near one hour is confirmed. Short periods near five and three minutes
are found in some parts of the prominences. They might be interpreted
as a reaction of the prominence on the photospheric and chromospheric
oscillations. For the time series of more than five hours indications
of eigenmodes of the prominences are found.
Title: Spectroscopic analysis of prominence emissions
Authors: Bendlin, C.; Wiehr, E.; Stellmacher, G.
Bibcode: 1988A&A...197..274B
Altcode:
Prominence spectra of fairly high spatial resolution of 3arcsec
to 4arcsec are analysed. The total optical thickness of the
Ca+K emission is determined from the self-absorption
factor, using the true upper level population obtained from the
Ca+8542 emission. Turbulence values determined from the
widths of optically thin lines show fair agreement with microturbulence
values obtained from the emission relation of the optically thick
Ca+H and K lines. Variations of the emission ratio
E8542/Eβ in prominences may be related
to different gas pressures.
Title: On variation of prominence heights with the solar cycle.
Authors: Kim, I. S.; Klepikov, V. Yu.; Koutchmy, S.; Stepanov, A. I.;
Stellmacher, G.
Bibcode: 1988BSolD...5...77K
Altcode:
The behaviour of prominence heights with the solar cycle is
studied. Prominence pictures taken by the Nikolsky magnetograph in
1979 - 1986 are used. A dependence of the average height with time
is analysed. The minimum height took place in the fall of 1984, 2
years before the solar activity minimum. Histograms of "prominence
occurrence versus height" were constructed for different phases of
the solar cycle. It is pointed out that the behaviour of the average
prominence height depends on the variation of the distribution of
prominence heights with the solar cycle. The minimum height is due to
a relative increase of the number of prominences which is less than
25 arcsec. The occurrence of these prominences has a peak before the
minimum of solar activity. Such prominences are predominantly located
at the latitudes 0 - 20°.
Title: Spectrophotometric analysis of small sunspots
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1988A&A...191..149S
Altcode:
High resolution spectra of two small sunspots were obtained with the
Gregory Vacuum Telescope at Izaña (Tenerife) on 1986 Oct. 8 and 9. The
two lines Fe+ 6149 and Li7 6707 (doublet) were
chosen for their very different behaviour in umbra atmospheres. Detailed
shape analysis shows that cold spot models (Teff ≅ 4000K)
cannot explain the present observations; a higher Teff ≅
4600K has to be assumed. The influence of parasitic light produced by
penumbral blurring and the contribution of dots is discussed.
Title: On the distribution of prominence heights.
Authors: Kim, I. S.; Klepikov, V. Yu.; Koutchmy, S.; Stepanov, A. I.;
Stellmacher, G.
Bibcode: 1988BSolD1988...75K
Altcode:
The distribution of prominence heights is studied. Prominence
pictures obtained in 1979 - 1986 by the Nikolsky magnetograph are
used. Discreteness in the distribution of heights is found. There are
two peaks: the first narrow peak at 20 - 25 arc sec and the second
one at 35 - 45 arc sec. One finds that the prominences with heights
less than 25 arc sec locate mainly at the latitude interval 0 <
φ ≤ 20°. During the preminimum and minimum of solar activity the
average latitude of the filaments (prominences) formation is 18 -
21°. The most likely height interval for prominence formation is at
20 - 25 arc sec (which is the critical height).
Title: Velocity variations of prominences.
Authors: Balthasar, H.; Wiehr, E.; Stellmacher, G.
Bibcode: 1988AGAb....1R..12B
Altcode:
No abstract at ADS
Title: Oscillatory motions of the Hα-emission line in
quiescent prominences.
Authors: Balthasar, H.; Wiehr, E.; Stellmacher, G.
Bibcode: 1988dssp.conf...63B
Altcode:
Temporal variations of the Doppler displacement of the
Hα-emission were measured in 4 prominences (September 28
through October 5, 1986) at the recently installed Gregory telescope at
Tenerife, using a 100×100 pixel diode array. Long periods near one hour
confirm former results. The amplitude of these long periods vary with
height and also in the direction parallel to the limb. Short periods
near 5 minutes and near 3 minutes are found which might be interpreted
as perturbations by the photospheric and chromospheric oscillations.
Title: Spectroscopic analysis of prominence emissions.
Authors: Wiehr, E.; Bendlin, C.; Stellmacher, G.
Bibcode: 1988dssp.conf...67W
Altcode:
Spatially well resolved prominence spectra of Ca+ and H lines
are used to determine (1) optical thickness of Ca+K from
the self-absorption factor, taking the true upper level population from
Ca+8542; (2) turbulence values from the emission relations
of the thick Ca+H and K lines yielding results similar to
those from the widths of optically thin lines; (3) gas pressure from
the emission ratio Ca+8542/Hβ.
Title: Some Statistical Properties of the Magnetic Field in
Prominences
Authors: Kim, I.; Koutchmy, S.; Stellmacher, G.; Stepanow, A. I.
Bibcode: 1987rfsm.conf..289K
Altcode:
Magnetic field observations based on the Zeeman effect, measuring the
longitudinal component B∥ of the field with an entrance
hole of 6.4 arcsec diameter, were obtained for a great number of
prominences during 1979 to 1985.
Title: Spectroscopic Analysis of Prominence Emissions
Authors: Wiehr, E.; Bendlin, C.; Stellmacher, G.
Bibcode: 1987dssp.work...67W
Altcode: 1987ASSL..150...67W
No abstract at ADS
Title: Properties of a Concentrated Magnetic Field Region
Authors: Koutchmy, S.; Stellmacher, G.
Bibcode: 1987rfsm.conf..103K
Altcode:
Further results concerning the fine structure of concentrated magnetic
field regions or network elements, observed near disk center well
outside of active regions, are presented.
Title: High Resolution Spectroscopy of Sunspot Penumbrae
Authors: Wiehr, E.; Knölker, M.; Grosser, H.; Stellmacher, G.
Bibcode: 1987rfsm.conf..162W
Altcode:
The spatial variation of velocity- and magnetic field within penumbral
finestructures is investigated from two very highly resolved spectra.
Title: The 1981 total solar eclipse. III - Photometric study of the
prominence remnant in the reversing south polar field
Authors: Stellmacher, G.; Koutchmy, S.; Lebecq, C.
Bibcode: 1986A&A...162..307S
Altcode:
High resolution white light colour pictures obtained during the
1981 total solar eclipse were used for a photometric analysis of
the S-pole region. A small helmet-like streamer was visible over
the S-polar limb overlying a faint polar prominence from the polar
crown belt of filament channels that reached 87° latitude at the
eclipse date. Typical electron densities deduced are ne
≅ 2×109cm-3 for the activated top of the
prominence and ne ≅ 6×108cm-3
for the associated coronal structures. Upward velocities up to 160 km
s-1 are obtained for the eruptive prominence parts. The
authors found that dynamic processes are controlled by magnetic
forces for fields B ≥ 3.5 Gauss, and that the coronal structures
are apparently connected with the faintest and most dynamic parts of
the prominence.
Title: Evidence for quasi-periodic Doppler motions in solar
prominences
Authors: Balthasar, H.; Knoelker, M.; Wiehr, E.; Stellmacher, G.
Bibcode: 1986A&A...163..343B
Altcode:
Observations of Doppler displacements in solar prominences have been
performed using the Hα emission line. Evidence is found for the
existence of quasi-periodic line-of-sight velocities in the range of
2.5 - 4.7 mHz. Former findings of long time variations near one hour
are confirmed. Possible influences by misguiding and by image motion
can be excluded. Scattered light from the solar aureola cannot produce
the observed amplitudes.
Title: The sharp decrease of Evershed effect and magnetic field at
the outer sunspot border
Authors: Wiehr, E.; Knoelker, M.; Grosser, H.; Stellmacher, G.
Bibcode: 1986A&A...155..402W
Altcode:
Spatially high-resolved spectra of a small split line (g = 0.5) in
four sunspots at different heliographic angles show that the combined
effect of line core velocities and line asymmetries (defined as Evershed
effect) is strongly limited to the sunspot area defined by the continuum
intensity step. Occasionally observed 'adjoining velocity maxima'
just outside the sunspot edges are not related to line asymmetries,
thus indicating a different origin than that of the classical Evershed
effect. A similar concentration of the very spot area is found for
the magnetic line broadening of two large split lines. Both results
indicate that magnetic field and velocity field are sharply restricted
to the visible sunspot, the often observed smooth discontinuity of
both quantities are thus considered to be due to seeing.
Title: Measurement of Magnetic Fields in Solar Prominences
Authors: Nikolskii, G. M.; Kim, I. S.; Koutchmy, S.; Stepanov, A. I.;
Stellmacher, G.
Bibcode: 1985SvA....29..669N
Altcode:
No abstract at ADS
Title: The 1981 total solar eclipse corona. II. Global absolute
photometric analysis.
Authors: Lebecq, C.; Koutchmy, S.; Stellmacher, G.
Bibcode: 1985A&A...152..157L
Altcode:
Detailed results of the absolute photometry of the solar corona
during the July 31, 1981 total eclipse are presented together with
a morphological analysis. The basic calibration method uses the
detailed photometry of images of stars present on the same coronal
picture. Both sky intensity and coronal aureola variations over the
field are carefully evaluated. The recent axi-symmetric non-spherical
model of the F-corona is introduced and the relevant K-corona intensity
variations are derived. The determinations of the Ludendorf index of
flattening and the integrated total brightness of the K-corona alone
are made and discussed in relation to the phase of the sunspot cycle
of activity.
Title: Evershed Effect and Magnetic Field in Penumbral Finestructures
Authors: Wiehr, E.; Stellmacher, G.
Bibcode: 1985LNP...233..198W
Altcode: 1985hrsp.proc..198W
A highly resolved penumbra spectrum obtained from the Locarno telescope
on July 4, 1982 is studied. It is observed that line core shifts are
predominant in dark spectrum streaks and line asymmetries in bright
spectrum streaks. The relationship between line widths and continuum
brightness is investigated. A continuous dependence of these line
parameters on the continuum brightness is detected; decreasing continuum
brightness results in increasing line widths. Explanations for this
increase are discussed. The effect of line widths/brightness variations
on magnetic field fluctuations in penumbral fine structures is examined.
Title: Influence of Umbral Dots on Sunspot Models
Authors: Wiehr, E.; Stellmacher, G.
Bibcode: 1985LNP...233..254W
Altcode: 1985hrsp.proc..254W
A photoelectric investigation was conducted of umbrae of different
brightness in three clean continuum windows at 4365 + or - 1/8, 6305 +
or - 1/4, and 8089 + or - 1/2. These were conducted simultaneously
in the 13th, 9th and 7th order of the f = 10 m echelle grating
spectrograph. It was found that the presence of umbral dots could
not account for observed differences in umbral brightness. In effect,
it is proposed that the dots represent a less important additive for
umbrae of different temperatures.
Title: The gas pressure in solar prominences
Authors: Hellwig, J.; Wiehr, E.; Stellmacher, G.
Bibcode: 1984A&A...140..449H
Altcode:
Attention is given to the results of new measurements of the emission
relation of Ca(+)8542 and H-beta, which indicate that the emission
ratio E(Ca/+/8542)/E(H-beta), at about 0.16, is significantly lower
than the value of about 0.3 obtained by Landsman et al. (1977). The
presently undertaken comparison of these results with those of the
Heasley and Milkey (1978) model indicates that a much higher value
of the gas pressure, approximately 0.1 dyn/sq cm, must be assumed in
order to match the observed lower ratio.
Title: The influence of penumbral fine structures on line profiles
Authors: Wiehr, E.; Koch, A.; Knoelker, M.; Kueveler, G.; Stellmacher,
G.
Bibcode: 1984A&A...140..352W
Altcode:
An experimental investigation of the effect of penumbral fine structure
on the line profiles of Ti 5222.7 A and Fe(+) 5264.8 is presented. The
highly resolved penumbral spectrum was observed with the evacuated
Locarno telescope of the Goettingen observatory. It is shown that the
highly excited Fe(+) line has a strong correlation in its line symmetry
to bright spectrum streaks. Line core shift was correlated with dark
spectrum streaks. The Doppler shift of the Be(+) line increased by 1.2
km/s, and that of the Ti line by 0.7 km/s for a continuum brightness
decrease of 20 percent. On the basis of the observational data, it
is concluded that the two-component model of sunspot penumbrae is
unlikely. It is suggested that Evershed asymmetry originates mainly
from a mixture of fine structure.
Title: Comparative magnetographic observations in different prominence
lines
Authors: Nikolsky, G. M.; Kim, I. S.; Koutchmy, S.; Stellmacher, G.
Bibcode: 1984A&A...140..112N
Altcode: 1984A&A...140..112K
Analysis of the longitudinal field strength in prominences obtained
by measurements of Zeeman polarization in HeD3, Hα, and Hβ is
presented. The measurements were performed with the spectrally scanning
magnetograph installed at the 53 cm coronograph of the Kislovodsk high
altitude station. The observations allow to correlate the values of
the equivalent widths and those of the half widths with magnetographic
data. No systematic dependence of field strengths on line widths is
found. High field strengths persist for large Doppler shifts and low
emissions. In the histogram showing the distribution of observed field
strengths two peaks near B∥ ≅ 8 Gauss and B∥
≅ 20 Gauss appear. The second peak corresponds to prominences
mainly related to active regions for latitudes <±35°. A similar
distribution is obtained from a set of data deduced from observation
of the Hanle effect and corresponding to the same epoch.
Title: Oscillations of the Hα Emission in Solar Prominences
Authors: Wiehr, E.; Stellmacher, G.; Balthasar, H.
Bibcode: 1984SoPh...94..285W
Altcode:
The time dependence of Doppler shift and line-center intensity
is simultaneously observed for the Hα emission of three solar
prominences, each one during about two hours. Doppler oscillations
with periods near one hour and amplitudes between 1 and 2 km
s−1 are conspicuously visible in the recordings of all
three prominences. Fourier analysis yields periods of 50, 60, and
64 min, as well as slight indications of short periods near 3 and 5
min. No oscillations are found in the line-center brightness.
Title: The electron density of faint prominences observed during
the solar eclipse of July 31, 1981
Authors: Koutchmy, S.; Lebecq, C.; Stellmacher, G.
Bibcode: 1983A&A...119..261K
Altcode:
Prominences visible on the narrow band filtergrams of the
eclipsed Sun, July 3t, 1981, are analysed. The ratio of the Hβ
line intensity to the continuum intensity at λ=6073 Å is used to
derive the electron density ne as a function of electron
temperature Te. The prominences present on that day were
of low brightness: Eβ,max ≃ 0.2 104 [erg
cm-2 s-1 sterad-1]. An electron density
ne = 5.7 109 [cm-3] at Te
= 10,000° is obtained, being typical for prominence edges.
Title: Magnetic field in solar prominences measured with a new
spectrally scanning magnetograph
Authors: Kim, I. S.; Nikolsky, G. M.; Koutchmy, S.; Stellmacher, G.
Bibcode: 1982A&A...114..347K
Altcode:
Observations of the longitudinal field strength in quiescent prominences
obtained with the new redesigned spectrally scanning magnetograph
installed in the Coude focus of the 53 cm coronograph of the Kislovodsk
station are presented. With the instrument one can obtain magnetographic
data as well as central intensities, equivalent widths, line widths,
and shifts of the analyzed prominence lines. A first discussion,
correlating magnetographic and spectroscopic data, is given
Title: Magnetfeld, Intensität und Strömung in
Penumbra-Feinstrukturen
Authors: Stellmacher, G.; Wiehr, E.; Knölker, M.
Bibcode: 1982MitAG..55...68S
Altcode:
No abstract at ADS
Title: Line profiles and magnetic field in penumbral fine structures
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1981A&A...103..211S
Altcode:
Spectra at high spatial resolution are taken in a sunspot penumbra at
disc center. The magnetic low sensitive lines Fe (+) 5264.8 (g equals
0.1) and Ti 5222.7 (g equals 0) as well as the large split line Fe
6302.3 are analyzed by comparison with model calculations. No systematic
fluctuations of the magnetic field strength and inclination are found
in the bright and dark spectral streaks, b and d. It is shown that this
result is still compatible with actual field fluctuations of less than
or equal to 1,000 G between the individual penumbral bright and dark
regions, BR and DR. The observed fluctuations of the central intensity
of the two oppositely temperature sensitive Fe(+) and Ti lines are
essentially smaller than expected from the continuum fluctuations. The
DR model requires a larger macro turbulence parameter than the BR model
in agreement with a spatially low resolved Evershed flow in the DR.
Title: Joint Soviet - French Investigations of the Solar Corona -
Part Three - Structure and Some Dynamic Features of the Solar Corona
of 1973JUN30
Authors: Vsekhsvyatskii, S. K.; Dzyubenko, N. I.; Ivanchuk, V. I.;
Popov, O. S.; Rubo, G. A.; Koutchmy, S.; Koutchmy, O.; Stellmacher, G.
Bibcode: 1981SvA....25..463V
Altcode:
No abstract at ADS
Title: On the branching in the emission relations of Ca+
in prominences
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1981SoPh...71..299S
Altcode: 2012arXiv1211.3641S
Spatially well resolved prominence spectra of the three lines
Ca+ K, Hβ, and Ca+ 8542 are analysed. It is
confirmed that the branching in the emission relations of Ca+
versus Hβ correlates with the magnitude of non-thermal (turbulent)
broadening.
Title: Joint Soviet / French Investigations of the Solar Corona -
Part Two - Photometry of the Solar Corona of 1973JUN30
Authors: Vsekhsvyatskii, S. K.; Dzyubenko, N. I.; Ivanchuk, V. I.;
Popov, O. S.; Rubo, G. A.; Koutchmy, S.; Koutchmy, O.; Stellmacher, G.
Bibcode: 1981SvA....25..211V
Altcode:
No abstract at ADS
Title: Umbral Models with Enhanced Continuum Opacity
Authors: Stellmacher, G.; Wiehr, E.
Bibcode: 1981A&A....95..229S
Altcode:
Umbral models based on the assumption of an additional continuum opacity
(Zwaan, 1974; Kollatschny et al., 1979: M4) are compared with model M3
by Stellmacher and Wiehr (1975) which is based on the standard continuum
opacity.