432 research outputs found
Quiet Sun Magnetic Field Measurements Based on Lines with Hyperfine Structure
The Zeeman pattern of MnI lines is sensitive to hyperfine structure (HFS)
and, they respond to hG magnetic field strengths differently from the lines
used in solar magnetometry. This peculiarity has been employed to measure
magnetic field strengths in quiet Sun regions. However, the methods applied so
far assume the magnetic field to be constant in the resolution element. The
assumption is clearly insufficient to describe the complex quiet Sun magnetic
fields, biasing the results of the measurements. We present the first syntheses
of MnI lines in realistic quiet Sun model atmospheres. The syntheses show how
the MnI lines weaken with increasing field strength. In particular, kG magnetic
concentrations produce NnI 5538 circular polarization signals (Stokes V) which
can be up to two orders of magnitude smaller than the weak magnetic field
approximation prediction. Consequently, (1) the polarization emerging from an
atmosphere having weak and strong fields is biased towards the weak fields, and
(2) HFS features characteristic of weak fields show up even when the magnetic
flux and energy are dominated by kG fields. For the HFS feature of MnI 5538 to
disappear the filling factor of kG fields has to be larger than the filling
factor of sub-kG fields. Stokes V depends on magnetic field inclination
according to the simple consine law. Atmospheres with unresolved velocities
produce asymmetric line profiles, which cannot be reproduced by simple
one-component model atmospheres. The uncertainty of the HFS constants do not
limit the use of MnI lines for magnetometry.Comment: Accepted for publication in ApJ. 10 pages, 14 figure
Theoretical formulation of Doppler redistribution in scattering polarization within the framework of the velocity-space density matrix formalism
Within the framework of the density matrix theory for the generation and
transfer of polarized radiation, velocity density matrix correlations represent
an important physical aspect that, however, is often neglected in practical
applications by adopting the simplifying approximation of complete
redistribution on velocity. In this paper, we present an application of the
Non-LTE problem for polarized radiation taking such correlations into account
through the velocity-space density matrix formalism. We consider a two-level
atom with infinitely sharp upper and lower levels, and we derive the
corresponding statistical equilibrium equations neglecting the contribution of
velocity-changing collisions. Coupling such equations with the radiative
transfer equations for polarized radiation, we derive a set of coupled
equations for the velocity-dependent source function. This set of equations is
then particularized to the case of a plane-parallel atmosphere. The equations
presented in this paper provide a complete and solid description of the physics
of pure Doppler redistribution, a phenomenon generally described within the
framework of the redistribution matrix formalism. The redistribution matrix
corresponding to this problem (generally referred to as R_I) is derived
starting from the statistical equilibrium equations for the velocity-space
density matrix and from the radiative transfer equations for polarized
radiation, thus showing the equivalence of the two approaches.Comment: Accepted for publication in Astronomy & Astrophysic
Isotropic inelastic and superelastic collisional rates in a multiterm atom
The spectral line polarization of the radiation emerging from a magnetized
astrophysical plasma depends on the state of the atoms within the medium, whose
determination requires considering the interactions between the atoms and the
magnetic field, between the atoms and photons (radiative transitions), and
between the atoms and other material particles (collisional transitions). In
applications within the framework of the multiterm model atom (which accounts
for quantum interference between magnetic sublevels pertaining either to the
same J-level or to different J-levels within the same term) collisional
processes are generally neglected when solving the master equation for the
atomic density matrix. This is partly due to the lack of experimental data
and/or of approximate theoretical expressions for calculating the collisional
transfer and relaxation rates (in particular the rates for interference between
sublevels pertaining to different J-levels, and the depolarizing rates due to
elastic collisions). In this paper we formally define and investigate the
transfer and relaxation rates due to isotropic inelastic and superelastic
collisions that enter the statistical equilibrium equations of a multiterm
atom. Under the hypothesis that the atom-collider interaction can be described
by a dipolar operator, we provide expressions that relate the collisional rates
for interference between different J-levels to the usual collisional rates for
J-level populations. Finally, we apply the general equations to the case of a
two-term atom with unpolarized lower term, illustrating the impact of inelastic
and superelastic collisions on scattering polarization through radiative
transfer calculations in a slab of stellar atmospheric plasma anisotropically
illuminated by the photospheric radiation field.Comment: Accepted for publication in Astronomy & Astrophysic
Accreting pre-main sequence models and abundance anomalies in globular clusters
We investigated the possibility of producing helium enhanced stars in
globular clusters by accreting polluted matter during the pre-main sequence
phase. We followed the evolution of two different classes of pre-main sequence
accreting models, one which neglects and the other that takes into account the
protostellar evolution.
We analysed the dependence of the final central helium abundance, of the
tracks position in the HR diagram and of the surface lithium abundance
evolution on the age at which the accretion of polluted material begins and on
the main physical parameters that govern the protostellar evolution. The later
is the beginning of the late accretion and the lower are both the central
helium and the surface lithium abundances at the end of the accretion phase and
in ZAMS (Zero Age Main Sequence). In order to produce a relevant increase of
the central helium content the accretion of polluted matter should start at
ages lower than 1 Myr. The inclusion of the protostellar evolution has a strong
impact on the ZAMS models too. The adoption of a very low seed mass (i.e. 0.001
M) results in models with the lowest central helium and surface
lithium abundances. The higher is the accretion rate and the lower is the final
helium content in the core and the residual surface lithium. In the worst case
-- i.e. seed mass 0.001 M and accretion rate M
yr -- the central helium is not increased at all and the surface lithium
is fully depleted in the first few million years.Comment: Accepted for pubblication in MNRAS. 19 pages, 15 figures, 2 table
Lithium-7 surface abundance in pre-MS stars. Testing theory against clusters and binary systems
The disagreement between theoretical predictions and observations for surface
lithium abundance in stars is a long-standing problem, which indicates that the
adopted physical treatment is still lacking in some points. However, thanks to
the recent improvements in both models and observations, it is interesting to
analyse the situation to evaluate present uncertainties. We present a
consistent and quantitative analysis of the theoretical uncertainties affecting
surface lithium abundance in the current generation of models. By means of an
up-to-date and well tested evolutionary code, FRANEC, theoretical errors on
surface 7Li abundance predictions, during the pre-main sequence (pre-MS) and
main sequence (MS) phases, are discussed in detail. Then, the predicted surface
7Li abundance was tested against observational data for five open clusters,
namely Ic 2602, \alpha Per, Blanco1, Pleiades, and Ngc 2516, and for four
detached double-lined eclipsing binary systems. Stellar models for the
aforementioned clusters were computed by adopting suitable chemical
composition, age, and mixing length parameter for MS stars determined from the
analysis of the colour-magnitude diagram of each cluster. We restricted our
analysis to young clusters, to avoid additional uncertainty sources such as
diffusion and/or radiative levitation efficiency. We confirm the disagreement,
within present uncertainties, between theoretical predictions and 7Li
observations for standard models. However, we notice that a satisfactory
agreement with observations for 7Li abundance in both young open clusters and
binary systems can be achieved if a lower convection efficiency is adopted
during the pre-MS phase with respect to the MS one.Comment: 10 pages, 5 figures. Accepted for publication in A&
Theoretical uncertainties on the radius of low- and very-low mass stars
We performed an analysis of the main theoretical uncertainties that affect
the radius of low- and very-low mass-stars predicted by current stellar models.
We focused on stars in the mass range 0.1-1Msun, on both the zero-age
main-sequence (ZAMS) and on 1, 2 and 5 Gyr isochrones. First, we quantified the
impact on the radius of the uncertainty of several quantities, namely the
equation of state, radiative opacity, atmospheric models, convection efficiency
and initial chemical composition. Then, we computed the cumulative radius error
stripe obtained by adding the radius variation due to all the analysed
quantities. As a general trend, the radius uncertainty increases with the
stellar mass. For ZAMS structures the cumulative error stripe of very-low mass
stars is about and percent, while at larger masses it increases
up to and percent. The radius uncertainty gets larger and age
dependent if isochrones are considered, reaching for Msun about
percent at an age of 5 Gyr. We also investigated the radius
uncertainty at a fixed luminosity. In this case, the cumulative error stripe is
the same for both ZAMS and isochrone models and it ranges from about
percent to and () percent. We also showed that the sole
uncertainty on the chemical composition plays an important role in determining
the radius error stripe, producing a radius variation that ranges between about
and percent on ZAMS models with fixed mass and about
and percent at a fixed luminosity.Comment: 18 pages, 20 figures, 1 table; accepted for publication in MNRA
Effect of planet ingestion on low-mass stars evolution: the case of 2MASS J08095427--4721419 star in the Gamma Velorum cluster
We analysed the effects of planet ingestion on the characteristics of a
pre-MS star similar to the Gamma Velorum cluster member 2MASS
J08095427--4721419 (#52). We discussed the effects of changing the age at
which the accretion episode occurs, the mass of the ingested planet and its
chemical composition. We showed that the mass of the ingested planet required
to explain the current [Fe/H]^#52 increases by decreasing the age and/or
by decreasing the Iron content of the accreted matter.
We compared the predictions of a simplified accretion method -- where only
the variation of the surface chemical composition is considered -- with that of
a full accretion model that properly accounts for the modification of the
stellar structure. We showed that the two approaches result in different
convective envelope extension which can vary up to 10 percent. We discussed the
impact of the planet ingestion on a stellar model in the colour-magnitude
diagram, showing that a maximum shift of about 0.06 dex in the colour and 0.07
dex in magnitude are expected and that such variations persist even much later
the accretion episode. We also analysed the systematic bias in the stellar mass
and age inferred by using a grid of standard non accreting models to recover
the characteristics of an accreting star. We found that standard non accreting
models can safely be adopted for mass estimate, as the bias is <= 6 percent,
while much more caution should be used for age estimate where the differences
can reach about 60 percent.Comment: Accepted for publication in MNRAS. 13 pages, 3 tables, 9 figure
Astrophysical implications of the proton-proton cross section updates
The p(p,e^+ \nu_e)^2H reaction rate is an essential ingredient for
theoretical computations of stellar models. In the past several values of the
corresponding S-factor have been made available by different authors. Prompted
by a recent evaluation of S(E), we analysed the effect of the adoption of
different proton-proton reaction rates on stellar models, focusing, in
particular, on the age of mid and old stellar clusters (1-12 Gyr) and on
standard solar model predictions. By comparing different widely adopted p(p,e^+
\nu_e)^2H reaction rates, we found a maximum difference in the temperature
regimes typical of main sequence hydrogen-burning stars (5x10^6 - 3x10^7 K) of
about 3%. Such a variation translates into a change of cluster age
determination lower than 1%. A slightly larger effect is observed in the
predicted solar neutrino fluxes with a maximum difference, in the worst case,
of about 8%. Finally we also notice that the uncertainty evaluation of the
present proton-proton rate is at the level of few \permil, thus the p(p,e^+
\nu_e)^2H reaction rate does not constitute anymore a significant uncertainty
source in stellar models.Comment: accepte
Diagnostic of prominence magnetic fields through spectropolarimetric observations
In recent times there has been a strong revival of interest in spectropolarimetric observations of solar prominences. This is due to the fact that new instruments, with unprecedented spectral resolution and polarimetric accuracy, are now available to solar physicists. These instruments open for the first time the possibility of unveiling the fine structure of magnetic fields and its correlation with velocity fields and density inhomogeneities in these fascinating objects. The interpretation of spectropolarimetric observations of solar prominences still stands, however, as one of the most challenging problems of what is nowadays known as atomic astrophysics, or, in other words, modern atomic physics applied to the diagnostic of astronomical objects. In this brief review, a hystorical account of the measurements of magnetic fields in prominences is given, and the present status of the theory, which stands at the basis of the interpretation of the observations, is dicussed. Some perspectives for future investigations are also presented
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