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Fig. 7

image

Center-to-limb variation of intensity for the Sun. Solid lines (shifted on μ according to the limb position) and dotted line (not-shifted) correspond to the formal solution of differential radiative transfer equations for polarized light using the modified Feautrier method for spherical geometry with the HSRA solar model atmosphere. Dashed line shows the interpolation of observations by Neckel & Labs (1994)

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