Scattering polarization in strong chromospheric lines. I. Explanation of the triplet peak structure

Details Scattering polarization in strong chromospheric lines. I. Explanation of the triplet peak structure Scattering polarization in strong chromospheric lines. I. Explanation of the triplet peak structure

May 2005

adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2005a%26a...434..713h&link_type=abstract

Astronomy and Astrophysics, Volume 434, Issue 2, May I 2005, pp.713-724

Astronomy and Astrophysics

Astrophysics

24

Line: Formation, Polarization, Radiative Transfer, Scattering, Sun: Atmosphere

Scientific paper

Although the triplet polarization structure of the Na I D2 and Ca I 4227 Å lines in the second solar spectrum has been known for more than two decades, a clear and consistent explanation has been lacking. Here we show that the qualitative profile shape may be explained in terms of the anisotropy of the radiation field and partial frequency redistribution (PRD) effects. The complicated frequency and depth dependence of the anisotropy can be understood in terms of simple arguments that involve the source function gradient and boundary effects. We show in particular that the triplet peak structure of the polarization profile of Na I D2 has basically the same origin as for the Ca I 4227 Å line. Hyperfine structure and lower-level atomic polarization only modify the core polarization without altering the overall qualitative features. For our calculations we adopt a numerical method that combines the advantages of both the classical formalism with integral source function and the density-matrix formalism. In a first step, a multi-level, PRD-capable MALI code, which solves the statistical equilibrium and the radiative transfer equation self-consistently, computes intensity, opacities and collision rates. Keeping these quantities fixed, we obtain the scattering polarization in a second step by solving the radiative transfer equation for the transitions of interest with the classical formalism, which assumes a two-level atomic model with unpolarized lower level. Quantum interferences and lower-level atomic polarization are included in terms of a wavelength dependent polarizability W_2, which is independently obtained with the density-matrix formalism.

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