Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/6914
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dc.contributor.authorMegha, A-
dc.contributor.authorSampoorna, M-
dc.contributor.authorNagendra, K. N-
dc.contributor.authorSankarasubramanian, K-
dc.date.accessioned2020-11-11T07:44:16Z-
dc.date.available2020-11-11T07:44:16Z-
dc.date.issued2018-02-
dc.identifier.citationProceedings of the International Astronomical Union, Vol. 340, pp. 61-62en_US
dc.identifier.issn1743-9213-
dc.identifier.urihttp://prints.iiap.res.in/handle/2248/6914-
dc.descriptionRestricted Access © International Astronomical Union https://doi.org/10.1017/S1743921318001023en_US
dc.description.abstractThe polarization measurement of coronal forbidden emission lines is the most promising method of determining the direction of magnetic fields in the corona. A classical theory for the forbidden lines was presented in Megha et al. (2017) for the case of arbitrary strength magnetic fields. Here we apply that theoretical formalism to study the effect of density distributions, magnetic field configurations, and velocity fields on the Stokes profiles formed in corona. For illustrations we use the atomic parameters of the [Fe xiii] 10747 ˚A coronal forbidden line.en_US
dc.language.isoenen_US
dc.publisherCambridge University Pressen_US
dc.subjectSun: coronaen_US
dc.subjectSun: magnetic fieldsen_US
dc.subjectLine: profiles - polarizationen_US
dc.titleCoronal magnetic field measurements using forbidden emission linesen_US
dc.typeArticleen_US
Appears in Collections:IIAP Publications

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