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Polarization of absorption lines as a diagnostics of circumstellar, interstellar and intergalactic magnetic fields: Fine structure atoms

机译:吸收线的极化,用于诊断星际,星际和星际磁场:精细结构的原子

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摘要

The relative population of the fine structure sublevels of an atom's ground state is affected by radiative transitions induced by an anisotropic radiation flux. This causes the alignment of atomic angular momentum. In terms of observational consequences for the interstellar and intergalactic medium, this results in the polarization of the absorption lines. In the paper we consider the conditions necessary for this effect and provide calculations of polarization from a few astrophysically important atoms and ions with multiple upper and lower levels for an arbitrary orientation of magnetic fields to the a) source of optical pumping, b) direction of observation, c) absorbed source. We also consider an astrophysically important ``degenerate'' case when the source of optical pumping coincides with the source of the absorbed radiation. We present analytical expressions that relate the degree of linear polarization and the intensity of absorption to the 3D orientation of the magnetic field with respect to the pumping source, the source of the absorbed radiation, and the direction of observations. We discuss how all these parameters can be determined via simultaneous observations of several absorption lines and suggest graphical means that are helpful in practical data interpretation. We prove that studies of absorption line polarization provide a unique tool to study 3D magnetic field topology in various astrophysical conditions.
机译:原子基态精细结构子级的相对种群受各向异性辐射通量引起的辐射跃迁的影响。这导致原子角动量的对准。就星际和银河系中间介质的观测结果而言,这导致了吸收线的极化。在本文中,我们考虑了实现此效应的必要条件,并提供了从几个天体重要的原子和离子进行极化的计算,这些原子和离子具有任意上下方向的磁场,且磁场方向为a)光泵浦源,b)泵浦方向观察,c)吸收源。当光泵浦的源与吸收的辐射的源重合时,我们还考虑了天文学上重要的``退化''情况。我们提供了将线性极化程度和吸收强度与磁场相对于泵浦源,吸收辐射源以及观测方向的3D方向相关的分析表达式。我们讨论了如何通过同时观察几个吸收线来确定所有这些参数,并提出了有助于实际数据解释的图形方法。我们证明,吸收线极化的研究提供了独特的工具来研究各种天体条件下的3D磁场拓扑。

著录项

  • 作者

    Lazarian, H Y A;

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  • 年度 2006
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  • 原文格式 PDF
  • 正文语种 eng
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