1973
DOI: 10.1007/bf00152298
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Theoretical study of the Fraunhofer lines polarization: The case of Ca i 4227

Abstract: The measurements by Brfickner (1963) of the Ca 1 4227 polarization at the Sun's limb provides us with a test for the theory of line polarization. Computations are developed taking into account: (a) the transfer polarization, due to the anisotropy of radiation field; (b) the depolarizing collisions acting in the wings. The magnetic field is not taken into account and the theory is not valid in the Doppler core. In the wings a very good fit is obtained, using appropriate source-functions fitting the observed pr… Show more

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Cited by 25 publications
(21 citation statements)
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“…Moreover, these three spectral lines have the same polarisation factor E 1 = 0.5 as deduced from Dumont et al (1973). In Stenflo & Stenholm (1976), an optically thin transition region, at the limb, will produce a p = 0.17 for the Si iv line.…”
Section: Possible Importance Of Linear Polarisationmentioning
confidence: 62%
“…Moreover, these three spectral lines have the same polarisation factor E 1 = 0.5 as deduced from Dumont et al (1973). In Stenflo & Stenholm (1976), an optically thin transition region, at the limb, will produce a p = 0.17 for the Si iv line.…”
Section: Possible Importance Of Linear Polarisationmentioning
confidence: 62%
“…Dumont et al (1977) were the first to consider line polarization with angle-dependent PRD, using the Hummer (1962)'s type I redistribution function. McKenna (1985) used Hummer's types I, II, andIII, andFaurobert (1987, 1988) the type II 1 .…”
Section: Introductionmentioning
confidence: 99%
“…They differ rather strongly from previous methods used for angle-dependent PRD. In Dumont et al (1977), Faurobert (1987Faurobert ( , 1988, Nagendra et al (2002), Sampoorna et al (2008a), the radiation field is described by the two Stokes parameters I and Q and the transfer equations for I and Q are solved by Feautrier-type methods, sometimes associated with a perturbation method, or fully perturbative methods, which is based on the linear polarization created by resonance scattering being a few percent only. In McKenna (1985), the radiation field is also described by I and Q, but the radiative transfer equations are solved by a moment equation method.…”
Section: Introductionmentioning
confidence: 99%
“…Note that the polarization in the lines has been calculated previously [13][14][15] for a similar problem by direct solution of the transfer equation (1). In the case of 0 = β we can compare our calculations with that part of the results ( ) shows that our results agree with those of the earlier work [13][14][15].…”
Section: Calculating the Matrix ( ) Z : Resultsmentioning
confidence: 99%