574 research outputs found
The scattering polarization of the Ly-alpha lines of H I and He II taking into account PRD and J-state interference effects
Recent theoretical investigations have pointed out that the cores of the
Ly-alpha lines of H I and He II should show measurable scattering polarization
signals when observing the solar disk, and that the magnetic sensitivity,
through the Hanle effect, of such linear polarization signals is suitable for
exploring the magnetism of the solar transition region. Such investigations
were carried out in the limit of complete frequency redistribution (CRD) and
neglecting quantum interference between the two upper J-levels of each line.
Here we relax both approximations and show that the joint action of partial
frequency redistribution (PRD) and J-state interference produces much more
complex fractional linear polarization (Q/I) profiles, with large amplitudes in
their wings. Such wing polarization signals turn out to be very sensitive to
the temperature structure of the atmospheric model, so that they can be
exploited for constraining the thermal properties of the solar chromosphere.
Finally, we show that the approximation of CRD without J-state interference is
however suitable for estimating the amplitude of the linear polarization
signals in the core of the lines, where the Hanle effect operates.Comment: Accepted for publication in The Astrophysical Journal Letter
Scattering Polarization of Hydrogen Lines in Weakly Magnetized Stellar Atmospheres I. Formulation and Application to Isothermal Models
Although the spectral lines of hydrogen contain valuable information on the
physical properties of a variety of astrophysical plasmas, including the upper
solar chromosphere, relatively little is known about their scattering
polarization signals whose modification via the Hanle effect may be exploited
for magnetic field diagnostics. Here we report on a basic theoretical
investigation of the linear polarization produced by scattering processes and
the Hanle effect in Ly-a, Ly-b and H-a taking into account multilevel radiative
transfer effects in an isothermal stellar atmosphere model, the fine-structure
of the hydrogen levels, as well as the impact of collisions with electrons and
protons. The main aim of this first paper is to elucidate the physical
mechanisms that control the linear polarization in the three lines, as well as
its sensitivity to the perturbers density and to the strength and structure of
micro-structured and deterministic magnetic fields. To this end, we apply an
efficient radiative transfer code we have developed for performing numerical
simulations of the Hanle effect in multilevel systems with overlapping line
transitions. For low density plasmas such as that of the upper solar
chromosphere collisional depolarization is caused mainly by collisional
transitions between the fine-structure levels of n=3, so that it is virtually
insignificant for Ly-a but important for Ly-b and H-a. We show the impact of
the Hanle effect on the three lines taking into account the radiative transfer
coupling between the different hydrogen line transitions. For example, we
demonstrate that the linear polarization profile of the H-a line is sensitive
to the presence of magnetic field gradients in the line core formation region
and that in solar-like chromospheres selective absorption of polarization
components does not play any significant role on the emergent scattering
polarization.Comment: 24 pages, 16 figures, 2 tables, accepted for publication in Ap
On the magnetic field of off-limb spicules
Determining the magnetic field related to solar spicules is vital for
developing adequate models of these plasma jets, which are thought to play a
key role in the thermal, dynamic and magnetic structure of the Chromosphere.
Here we report on the magnetic properties of off-limb spicules in a very quiet
region of the solar atmosphere, as inferred from new spectropolarimetric
observations in the He I 10830 A triplet obtained with the Tenerife Infrared
Polarimeter. We have used a novel inversion code for Stokes profiles caused by
the joint action of atomic level polarization and the Hanle and Zeeman effects
(HAZEL) to interpret the observations. Magnetic fields as strong as ~40G were
detected in a very localized area of the slit, which could represent a possible
lower value of the field strength of organized network spicules.Comment: Accepted for publication in ApJ, 24 pages, 5 Figure
Scattering Polarization and Hanle Effect in Stellar Atmospheres with Horizontal Inhomogeneities
Scattering of light from an anisotropic source produces linear polarization
in spectral lines and the continuum. In the outer layers of a stellar
atmosphere the anisotropy of the radiation field is typically dominated by the
radiation escaping away, but local horizontal fluctuations of the physical
conditions may also contribute, distorting the illumination and hence, the
polarization pattern. Additionally, a magnetic field may perturb and modify the
line scattering polarization signals through the Hanle effect. Here, we study
such symmetry-breaking effects. We develop a method to solve the transfer of
polarized radiation in a scattering atmosphere with weak horizontal
fluctuations of the opacity and source functions. It comprises linearization
(small opacity fluctuations are assumed), reduction to a quasi-planeparallel
problem through harmonic analysis, and numerical solution by generalized
standard techniques. We apply this method to study scattering polarization in
atmospheres with horizontal fluctuations in the Planck function and opacity. We
derive several very general results and constraints from considerations on the
symmetries and dimensionality of the problem, and we give explicit solutions of
a few illustrative problems of especial interest. For example, we show (a) how
the amplitudes of the fractional linear polarization signals change when
considering increasingly smaller horizontal atmospheric inhomogeneities, (b)
that in the presence of such inhomogeneities even a vertical magnetic field may
modify the scattering line polarization, and (c) that forward scattering
polarization may be produced without the need of an inclined magnetic field.
These results are important to understand the physics of the problem and as
benchmarks for multidimensional radiative transfer codes.Comment: 27 pages, 13 figures, to appear in Ap
Are collisions with neutral hydrogen important for modelling the Second Solar Spectrum of Ti I and Ca II ?
The physical interpretation of scattering line polarization offers a novel
diagnostic window for exploring the thermal and magnetic structure of the quiet
regions of the solar atmosphere. Here we evaluate the impact of isotropic
collisions with neutral hydrogen atoms on the scattering polarization signals
of the 13 lines of multiplet 42 of Ti I and on those of the K line and of the
IR triplet of Ca II, with emphasis on the collisional transfer rates between
nearby J-levels. To this end, we calculate the linear polarization produced by
scattering processes considering realistic multilevel models and solving the
statistical equilibrium equations for the multipolar components of the atomic
density matrix. We confirm that the lower levels of the 13 lines of multiplet
42 of Ti I are completely depolarized by elastic collisions. We find that
upper-level collisional depolarization turns out to have an unnoticeable impact
on the emergent linear polarization amplitudes, except for the {\lambda 4536
line for which it is possible to notice a rather small depolarization caused by
the collisional transfer rates. Concerning the Ca II lines, we show that the
collisional rates play no role on the polarization of the upper level of the K
line, while they have a rather small depolarizing effect on the atomic
polarization of the metastable lower levels of the Ca II IR triplet.Comment: Accepted for publication in Astronomy and Astrophysic
Determining the Magnetization of the Quiet Sun Photosphere from the Hanle Effect and Surface Dynamo Simulations
The bulk of the quiet solar photosphere is thought to be significantly
magnetized, due to the ubiquitous presence of a tangled magnetic field at
subresolution scales with an average strength ~ 100 G. This conclusion was
reached through detailed three-dimensional (3D) radiative transfer modeling of
the Hanle effect in the Sr I 4607 line, using the microturbulent field
approximation and assuming that the shape of the probability density function
of the magnetic field strength is exponential. Here we relax both
approximations by modeling the observed scattering polarization in terms of the
Hanle effect produced by the magnetic field of a 3D photospheric model
resulting from a (state-of-the-art) magneto-convection simulation with surface
dynamo action. We show that the scattering polarization amplitudes observed in
the Sr I 4607 line can be explained only after enhancing the magnetic strength
of the photospheric model by a sizable scaling factor, F=10, which implies
= 130 G in the upper photosphere. We argue also that in order to explain both
the Hanle depolarization of the Sr I 4607 line and the Zeeman signals observed
in Fe I lines we need to introduce a height-dependent scaling factor, such that
the ensuing = 160 G in the low photosphere and = 130 G in the upper
photosphere.Comment: To appear in ApJ Letter
On the physical origin of the second solar spectrum of the Sc II line at 4247 A
The peculiar three-peak structure of the linear polarization profile shown in
the second solar spectrum by the Ba II line at 4554 A has been interpreted as
the result of the different contributions coming from the barium isotopes with
and without hyperfine structure (HFS). In the same spectrum, a triple peak
polarization signal is also observed in the Sc II line at 4247 A. Scandium has
a single stable isotope (^{45}Sc), which shows HFS due to a nuclear spin I=7/2.
We investigate the possibility of interpreting the linear polarization profile
shown in the second solar spectrum by this Sc II line in terms of HFS. A
two-level model atom with HFS is assumed. Adopting an optically thin slab
model, the role of atomic polarization and of HFS is investigated, avoiding the
complications caused by radiative transfer effects. The slab is assumed to be
illuminated from below by the photospheric continuum, and the polarization of
the radiation scattered at 90 degrees is investigated. The three-peak structure
of the scattering polarization profile observed in this Sc II line cannot be
fully explained in terms of HFS. Given the similarities between the Sc II line
at 4247 A and the Ba II line at 4554 A, it is not clear why, within the same
modeling assumptions, only the three-peak Q/I profile of the barium line can be
fully interpreted in terms of HFS. The failure to interpret this Sc II
polarization signal raises important questions, whose resolution might lead to
significant improvements in our understanding of the second solar spectrum. In
particular, if the three-peak structure of the Sc II signal is actually
produced by a physical mechanism neglected within the approach considered here,
it will be extremely interesting not only to identify this mechanism, but also
to understand why it seems to be less important in the case of the barium line.Comment: 8 pages, 8 figures, and 1 table. Accepted for publication in
Astronomy and Astrophysic
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