Please use this identifier to cite or link to this item:
http://hdl.handle.net/2248/5958
Full metadata record
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Smitha, H. N | - |
dc.contributor.author | Nagendra, K. N | - |
dc.contributor.author | Sampoorna, M | - |
dc.contributor.author | Stenflo, J. O | - |
dc.date.accessioned | 2012-12-28T10:01:57Z | - |
dc.date.available | 2012-12-28T10:01:57Z | - |
dc.date.issued | 2013-01 | - |
dc.identifier.citation | Journal of Quantitative Spectroscopy and Radiative Transfer, Vol. 115, pp. 46–59 | en |
dc.identifier.uri | http://hdl.handle.net/2248/5958 | - |
dc.description | Restricted Access | en |
dc.description.abstract | An expression for the partial frequency redistribution (PRD) matrix for line scattering in a two-term atom, which includes the J-state interference between its fine structure line components is derived. The influence of collisions (both elastic and inelastic) and an external magnetic field on the scattering process is taken into account. The lower term is assumed to be unpolarized and infinitely sharp. The linear Zeeman regime in which the Zeeman splitting is much smaller than the fine structure splitting is considered. The inelastic collision rates between the different levels are included in our treatment. We account for the depolarization caused by the collisions coupling the fine structure states of the upper term, but neglect the polarization transfer between the fine structure states. When the fine structure splitting goes to zero, we recover the redistribution matrix that represents the scattering on a two-level atom (which exhibits only m-state interference—namely the Hanle effect). The way in which the multipolar index of the scattering atom enters into the expression for the redistribution matrix through the collisional branching ratios is discussed. The properties of the redistribution matrix are explored for a single scattering process for a L=0→1→0 scattering transition with S=1/2 (a hypothetical doublet centered at 5000 Å and 5001 Å). Further, a method for solving the Hanle radiative transfer equation for a two-term atom in the presence of collisions, PRD, and J-state interference is developed. The Stokes profiles emerging from an isothermal constant property medium are computed. | en |
dc.language.iso | en | en |
dc.publisher | Elsevier B.V. | en |
dc.relation.uri | http://dx.doi.org/10.1016/j.jqsrt.2012.09.002 | en |
dc.relation.uri | http://arxiv.org/abs/1209.0243 | en |
dc.rights | © Elsevier B.V. | en |
dc.subject | Atomic processes | en |
dc.subject | Line profiles | en |
dc.subject | Magnetic fields | en |
dc.subject | Polarization | en |
dc.subject | Scattering | en |
dc.subject | Sun atmosphere | en |
dc.title | Polarized line formation with J-state interference in the presence of magnetic fields: A Heuristic treatment of collisional frequency redistribution | en |
dc.type | Article | en |
Appears in Collections: | IIAP Publications |
Files in This Item:
File | Description | Size | Format | |
---|---|---|---|---|
Polarized line formation with J-state interference in the presence of magnetic fields.pdf Restricted Access | Restricted Access | 539.76 kB | Adobe PDF | View/Open Request a copy |
Items in DSpace are protected by copyright, with all rights reserved, unless otherwise indicated.