Plane Polarization in Comptonization process : a Monte Carlo study

IF 4.5 3区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Publications of the Astronomical Society of Australia Pub Date : 2024-01-29 DOI:10.1017/pasa.2024.8
Nagendra Kumar
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Abstract

High energies emissions observed in X-ray binaries (XRBs), active galactic nuclei (AGNs) are linearly polarized. The prominent mechanism for X-ray is the Comptonization process. We revisit the theory for polarization in Compton scattering with unpolarized electrons, and note that the (k×k′)-coordinate (in which, (k×k) acts as a z-axis, here k and k are incident and scattered photon momentum respectively) is more convenient to describe it. Interestingly, for a fixed scattering plane the degree of polarization PD after single scattering for random oriented low-energy unpolarized incident photons is ~0.3. At the scattering angle θ = 0 orθ≡ [0,25◦], the modulation curve of k exhibits the same PD and PA (angle of polarization) of k, and even the distribution of projection of electric vector of k (ke) on perpendicular plane to the k indicates same (so, an essential criteria for detector designing). We compute the polarization state in Comptonization process using Monte Carlo methods with considering a simple spherical corona. We obtain the PD of emergent photons as a function of =-angle (or alternatively, the disk inclination angle i) on a meridian plane (i.e., the laws of darkening, formulated by Chandrasekhar, 1946) after single scattering with unpolarized incident photons. To explore the energy dependency we consider a general spectral parameter set corresponding to hard and soft states of XRBs, we find that for average scattering no. 〈Nsc〉 ~1.1 the PD is independent of energy and PA ~ 90◦ (ke is parallel to the disk plane), and for hNsci ~5 the PD value is maximum for i = 45◦. We also compare the results qualitatively with observation of IXPE for five sources.
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康普顿化过程中的平面极化:蒙特卡洛研究
在 X 射线双星(XRBs)、活动星系核(AGNs)中观测到的高能辐射是线性极化的。X射线的主要机制是康普顿化过程。我们重温了与非极化电子发生康普顿散射时的极化理论,并注意到(k×k′)坐标(其中,(k×k′)充当z轴,此处k和k′分别为入射和散射光子动量)更便于描述它。有趣的是,对于一个固定的散射平面,随机方向的低能无偏振入射光子单次散射后的偏振 PD 度约为 0.3。在散射角θ = 0 或θ≡ [0,25◦]时,k′的调制曲线显示出相同的 PD 和 PA(偏振角),甚至 k′的电矢量投影(k′e)在与 k 垂直面上的分布也显示出相同(因此,这是设计探测器的一个重要标准)。我们使用蒙特卡洛方法计算了康普顿化过程中的偏振态,并考虑了一个简单的球形日冕。我们得到了与非偏振入射光子发生单次散射后,在子午面上出现的光子的 PD 与 = 角(或圆盘倾角 i)的函数关系(即 Chandrasekhar,1946 年制定的暗化定律)。为了探索能量相关性,我们考虑了与 XRB 的硬态和软态相对应的一般光谱参数集。Nsc〉〜1.1时,PD与能量和PA〜90◦(k′e平行于盘面)无关,而当hNsci〜5时,PD值在i=45◦时最大。我们还将结果与对五个星源的 IXPE 观测结果进行了定性比较。
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来源期刊
Publications of the Astronomical Society of Australia
Publications of the Astronomical Society of Australia 地学天文-天文与天体物理
CiteScore
5.90
自引率
9.50%
发文量
41
审稿时长
>12 weeks
期刊介绍: Publications of the Astronomical Society of Australia (PASA) publishes new and significant research in astronomy and astrophysics. PASA covers a wide range of topics within astronomy, including multi-wavelength observations, theoretical modelling, computational astronomy and visualisation. PASA also maintains its heritage of publishing results on southern hemisphere astronomy and on astronomy with Australian facilities. PASA publishes research papers, review papers and special series on topical issues, making use of expert international reviewers and an experienced Editorial Board. As an electronic-only journal, PASA publishes paper by paper, ensuring a rapid publication rate. There are no page charges. PASA''s Editorial Board approve a certain number of papers per year to be published Open Access without a publication fee.
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