67 research outputs found
The height dependence of temperature - velocity correlation in the solar photosphere
We derive correlation coefficients between temperature and line-of-sight
velocity as a function of optical depth throughout the solar photosphere for
the non-magnetic photosphere and a small area of enhanced magnetic activity.
The maximum anticorrelation of about -0.6 between temperature and line-of-sight
velocity in the non-magnetic photosphere occurs at log tau5 = -0.4. The
magnetic field is another decorrelating factor along with 5-min oscillations
and seeing.Comment: In press,"Modern Solar Facilities - Advanced Solar Science",
(Gottingen), Universitatsverlag Gottingen, 139-142, 200
Spectral Characteristics of the He I D3 Line in a Quiescent Prominence Observed by THEMIS
We analyze the observations of a quiescent prominence acquired by the
Telescope Heliographique pour l'Etude du Magnetisme et des Instabilites
Solaires (THEMIS) in the He I 5876 A (He I D3) multiplet aiming to measure the
spectral characteristics of the He I D3 profiles and to find for them an
adequate fitting model. The component characteristics of the He I D3 Stokes I
profiles are measured by the fitting system approximating them with a double
Gaussian. This model yields an He I D3 component peak intensity ratio of
, which differs from the value of 8 expected in the optically thin
limit. Most of the measured Doppler velocities lie in the interval km/s,
with a standard deviation of km/s around the peak value of 0.4 km/s.
The wide distribution of the full-width at half maximum has two maxima at 0.25
A and 0.30 A for the He I D3 blue component and two maxima at 0.22 A and 0.31 A
for the red component. The width ratio of the components is . We
show that the double-Gaussian model systematically underestimates the blue wing
intensities. To solve this problem, we invoke a two-temperature multi-Gaussian
model, consisting of two double-Gaussians, which provides a better
representation of He I D3 that is free of the wing intensity deficit. This
model suggests temperatures of 11.5 kK and 91 kK, respectively, for the cool
and the hot component of the target prominence. The cool and hot components of
a typical He I D3 profile have component peak intensity ratios of 6.6 and 8,
implying a prominence geometrical width of 17 Mm and an optical thickness of
0.3 for the cool component, while the optical thickness of the hot component is
negligible. These prominence parameters seem to be realistic, suggesting the
physical adequacy of the multi-Gaussian model with important implications for
interpreting He I D3 spectropolarimetry by current inversion codes.Comment: 25 pages,1 movie, 10 figures, 2 tables, 2 equations. The final
publication is available at Springer via
http://dx.doi.org/10.1007/s11207-017-1118-z The supplementary movie is
available for viewing and download at
https://www.dropbox.com/s/7tskvnc593tlbyv/Prominence_HeID3_GONG_AIA.mpg?dl=
Magnetic loop emergence within a granule
We investigate the temporal evolution of magnetic flux emerging within a
granule in the quiet-Sun internetwork at disk center. We combined IR
spectropolarimetry performed in two Fe I lines at 1565 nm with
speckle-reconstructed G-band imaging. We determined the magnetic field
parameters by a LTE inversion of the full Stokes vector using the SIR code, and
followed their evolution in time. To interpret the observations, we created a
geometrical model of a rising loop in 3D. The relevant parameters of the loop
were matched to the observations where possible. We then synthesized spectra
from the 3D model for a comparison to the observations. We found signatures of
magnetic flux emergence within a growing granule. In the early phases, a
horizontal magnetic field with a distinct linear polarization signal dominated
the emerging flux. Later on, two patches of opposite circular polarization
signal appeared symmetrically on either side of the linear polarization patch,
indicating a small loop-like structure. The mean magnetic flux density of this
loop was roughly 450 G, with a total magnetic flux of around 3x10^17 Mx. During
the ~12 min episode of loop occurrence, the spatial extent of the loop
increased from about 1 to 2 arcsec. The middle part of the appearing feature
was blueshifted during its occurrence, supporting the scenario of an emerging
loop. The temporal evolution of the observed spectra is reproduced to first
order by the spectra derived from the geometrical model. The observed event can
be explained as a case of flux emergence in the shape of a small-scale loop.Comment: 10 pages, 13 figures; accepted for Astronomy and Astrophysics; ps and
eps figures in full resolution are available at
http://www.astro.sk/~koza/figures/aa2009_loop
High-resolution spectroscopy of a chromospheric subflare: Ca II K line measurement
Anin vestigationof the quiet and active (subflare) solar atmosphere is made using high spatial and spectral resolution observations of the Ca II K line performed at the VTT, Observatorio del Teide, Tenerife. Spectral characteristics IK1, IK2, IK3, integrated intensity Iint, separations of K1 minima SepK1, separations of K2 maxima SepK2 and their ratios are compared for both quiet and active regions. Preliminary results are discussed
Dynamics of the solar photosphere and chromosphere derived from high resolution Fe I and Ca II spectra
The analysis of high-resolution spectra of the Fe I (522.5 nm, 557.6 nm) and Ca II K (393.3 nm) lines in the solar photosphere and chromosphere is presented. A dynamic coupling of the photosphere and chromosphere was
determined from the ratios of both the photospheric and chromospheric line characteristics. All results are discussed for quiet and plage regions. It is found that
inthe plage regionthe meanv alues of K1, K2, K3 intensities inCa II K are increased 2, 5 and 6 times, respectively, as compared to the quiet region. The mean values of Fe I line core intensities increased in plage only 1.32 and 1.64 times for the magnetic non-sensitive and magnetic sensitive line, respectively. The ranges of Fe I core intensity values are larger for the magnetic sensitive line than for the magnetic non-sensitive line
Temporal Variations in Fibril Orientation
We measure variations in orientation of fourteen dynamic fibrils as a
function of time in a small isolated plage and nearby network using a 10-min
time sequence of H-alpha filtergrams obtained by the Dutch Open Telescope. We
found motions with average angular velocities of the order of 1 deg/min
suggesting systematic turning from one limit position to another, particularly
apparent in the case of fibrils with lifetimes of a few minutes. Shorter
fibrils tend to turn faster than longer ones, which we interpret as due to
vortex flows in the underlying granulation that twist magnetic fields.Comment: In press,"Physics of Chromospheric Plasmas" (Coimbra), ASP 368, 115
(2007
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