| dc.contributor.author | Smitha, H. N | |
| dc.contributor.author | Nagendra, K. N | |
| dc.contributor.author | Stenflo, J. O | |
| dc.contributor.author | Bianda, M | |
| dc.contributor.author | Sampoorna, M | |
| dc.contributor.author | Ramelli, R | |
| dc.contributor.author | Anusha, L. S | |
| dc.date.accessioned | 2012-05-01T13:04:26Z | |
| dc.date.available | 2012-05-01T13:04:26Z | |
| dc.date.issued | 2012-05 | |
| dc.identifier.citation | Astronomy & Astrophysics, Vol. 541, A24 | en |
| dc.identifier.uri | http://hdl.handle.net/2248/5766 | |
| dc.description.abstract | The scattering polarization in the solar spectrum is traditionally modeled with each spectral line treated separately, but this is generally inadequate for multiplets where J-state interference plays a significant role. Through simultaneous observations of all the 3 lines of a Cr I triplet, combined with realistic radiative transfer modeling of the data, we show that it is necessary to include J-state interference consistently when modeling lines with partially interacting fine structure components. Polarized line formation theory that includes J-state interference effects together with partial frequency redistribution for a two-term atom is used to model the observations. Collisional frequency redistribution is also accounted for. We show that the resonance polarization in the Cr I triplet is strongly affected by the partial frequency redistribution effects in the line core and near wing peaks. The Cr I triplet is quite sensitive to the temperature structure of the photospheric layers. Our complete frequency redistribution calculations in semi-empirical models of the solar atmosphere cannot reproduce the observed near wing polarization or the cross-over of the Stokes Q/I line polarization about the continuum polarization level that is due to the J-state interference. When however partial frequency redistribution is included, a good fit to these features can be achieved. Further, to obtain a good fit to the far wings, a small temperature enhancement of the FALF model in the photospheric layers is necessary. | en |
| dc.language.iso | en | en |
| dc.publisher | EDP Sciences | en |
| dc.relation.uri | http://dx.doi.org/10.1051/0004-6361/201118466 | en |
| dc.rights | © ESO | en |
| dc.subject | Line: profiles | en |
| dc.subject | Line:polarization | en |
| dc.subject | Line:scattering | en |
| dc.subject | Methods: numerical | en |
| dc.subject | Methods: radiative transfer | en |
| dc.subject | Sun: atmosphere | en |
| dc.title | J-state interference signatures in the second solar spectrum. Modeling the Cr I triplet at 5204-5208 | en |
| dc.type | Article | en |