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Fig. 6


Dimensionless emissivity for the linear polarization e1, J1 = 1 − R1, as a function of photon energy E for condensed Fe surface at different magnetic field strengths and geometric settings. Top panel: magnetic field B = 1013 G is normal to the surface, and angles of radiation incidence are θk = 0, π/6, π/4, and π/3. Bottom panel: B = 1013.5 G, magnetic field lines and the photon beam are both inclined at θB = θk = π/4, and the azimuthal angle takes values ϕ = 0, π/4, and π/2. Solid lines show the numerical results, and dashed lines demonstrate the fit.

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