Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/7430
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dc.contributor.authorSampoorna, M-
dc.contributor.authorNagendra, K. N-
dc.contributor.authorSowmya, K-
dc.contributor.authorStenflo, J. O-
dc.contributor.authorAnusha, L. S-
dc.date.accessioned2020-11-26T15:47:15Z-
dc.date.available2020-11-26T15:47:15Z-
dc.date.issued2019-10-01-
dc.identifier.citationThe Astrophysical Journal, Vol. 833, No. 2, 188en_US
dc.identifier.issn0004-637X-
dc.identifier.urihttp://prints.iiap.res.in/handle/2248/7430-
dc.descriptionRestricted Access © The American Astronomical Society https://doi.org/10.3847/1538-4357/ab3805en_US
dc.description.abstractQuantum interference effects, together with partial frequency redistribution (PFR) in line scattering, produce subtle signatures in the so-called Second Solar Spectrum (the linearly polarized spectrum of the Sun). These signatures are modified in the presence of arbitrary strength magnetic fields via the Hanle, Zeeman, and Paschen–Back effects. In the present paper we solve the problem of polarized line formation in a magnetized atmosphere taking into account scattering in a two-level atom with hyperfine structure splitting together with PFR. To this end we incorporate the collisionless PFR matrix derived in Sowmya et al. in the polarized transfer equation. We apply the scattering expansion method to solve this transfer equation. We study the combined effects of PFR and the Paschen–Back effect on polarized line profiles formed in an isothermal one-dimensional planar atmosphere. For this purpose, we consider the cases of D2 lines of Li i and Na i.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.subjectline: formationen_US
dc.subjectpolarizationen_US
dc.subjectradiative transferen_US
dc.subjectscatteringen_US
dc.subjectSun: magnetic fieldsen_US
dc.titlePolarized Line Formation in Arbitrary Strength Magnetic Fields: The Case of a Two-level Atom with Hyperfine Structure Splittingen_US
dc.typeArticleen_US
Appears in Collections:IIAP Publications



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