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Polarization from magnetized accretion discs: II. The effects of absorption opacity on Faraday rotation

机译:磁化吸积盘的极化:II。的影响   法拉第旋转吸收不透明度

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摘要

Equipartition magnetic fields can dramatically affect the polarization ofradiation emerging from accretion disk atmospheres in active galactic nuclei.We extend our previous work on this subject by exploring the interactionbetween Faraday rotation and absorption opacity in local, plane-parallelatmospheres with parameters appropriate for accretion discs. Faraday rotationin pure scattering atmospheres acts to depolarize the radiation field byrotating the polarization planes of photons after last scattering. Absorptionopacity in an unmagnetized atmosphere can increase or decrease the polarizationcompared to the pure scattering case, depending on the thermal source functiongradient. Combining both Faraday rotation and absorption opacity, we find thefollowing results. If absorption opacity is much larger than scattering opacitythroughout the atmosphere, then Faraday rotation generally has only a smalleffect on the emerging polarization because of the small electron columndensity along a photon mean free path. However, if the absorption opacity isnot too large and it acts alone to increase the polarization, then the effectsof Faraday rotation can be enhanced over those in a pure scattering atmosphere.Finally, while Faraday rotation often depolarizes the radiation field, it canin some cases increase the polarization when the thermal source function doesnot rise too steeply with optical depth. We confirm the correctness of theSilant'ev (1979) analytic calculation of the high magnetic field limit of thepure scattering atmosphere, which we incorrectly disputed in our previouspaper.
机译:均分磁场可以极大地影响活跃银河原子核中吸积盘大气中产生的辐射的极化。我们通过研究法拉第旋转与局部平面平行大气中法拉第旋转与吸收不透明性之间的相互作用(具有适合吸积盘的参数)来扩展我们先前的工作。在纯散射环境中的法拉第旋转通过在最后一次散射之后旋转光子的极化平面来使辐射场去极化。与纯散射情况相比,在非磁化气氛中的吸收不透明性可以增加或减少极化,具体取决于热源功能的梯度。结合法拉第旋转和吸收不透明度,我们发现以下结果。如果吸收不透明度比整个大气中的散射不透明度大得多,则法拉第旋转通常对新兴的极化仅产生很小的影响,因为沿着光子平均自由程的电子列密度小。但是,如果吸收不透明度不是太大并且单独起作用以增加偏振,则法拉第旋转的效果会比纯散射大气中的效果增强。最后,虽然法拉第旋转经常使辐射场消极化,但在某些情况下它会增加当热源功能不会随光学深度而急剧上升时,偏振态会变大。我们证实了纯散射大气的高磁场极限的Silant'ev(1979)解析计算的正确性,这在我们之前的论文中是错误地提出的。

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