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arXiv 2307.08023astro-ph.HE
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康普顿化过程中的平面偏振:一项 Monte Carlo 研究

Plane Polarization in Comptonization process : a Monte Carlo study

Nagendra Kumar

AI总结:

本文利用 Monte Carlo 方法模拟简单球形日冕中的康普顿化偏振,给出单次与多次散射下偏振度随倾角和能量的变化,并与 IXPE 五个源的观测定性比较。

摘要:

在 X 射线双星(XRBs)和活动星系核(AGNs)中观测到的高能辐射是线偏振的。X 射线的主要产生机制是康普顿化过程。我们重新考察了与非偏振电子发生康普顿散射时偏振的理论,并指出 ($k \times k'$) 坐标系(其中 ($k \times k'$) 作为 $z$ 轴,这里 $k$ 和 $k'$ 分别是入射光子和散射光子的动量)更便于描述这一过程。有趣的是,对于固定的散射面,随机取向的低能非偏振入射光子在单次散射后的偏振度 PD 约为 0.33。在散射角 $θ=0$ 或 $θ\equiv[0,25^o]$ 时,$k'$ 的调制曲线表现出与 $k$ 相同的 PD 和 PA(偏振角),甚至 $k'$ 的电矢量($k'_e$)在垂直于 $k$ 的平面上的投影分布也表明相同(因此,这是探测器设计的一个关键标准)。我们使用 Monte Carlo 方法,并考虑一个简单的球形日冕,计算了康普顿化过程中的偏振状态。对于非偏振入射光子的单次散射,我们得到了出射光子的 PD 作为子午平面上 $θ$ 角(或者等价地,吸积盘倾角 $i$)的函数(即临边昏暗定律,由 \citealp{Chandrasekhar1946} 公式化)。为了探究能量依赖性,我们考虑了对应于 XRBs 硬态和软态的一组通用光谱参数;我们发现,对于平均散射次数 $\langle N_{sc}\rangle\sim1.1$,PD 与能量无关,且 PA 约为 $90^o$($k'_e$ 平行于吸积盘平面);而对于 $\langle N_{sc}\rangle\sim5$,PD 值在 $i=45^o$ 时达到最大。我们还将结果与 IXPE 对五个源的观测进行了定性比较。

英文摘要:

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 ($k \times k'$)-coordinate (in which, ($k \times k'$) 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 $\sim$0.33. At the scattering angle $θ$ = 0 or $θ\equiv$ [0,25$^o$], 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 $k'$ ($k'_e$) 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 $θ$-angle (or alternatively, the disk inclination angle $i$) on a meridian plane (i.e., the laws of darkening, formulated by \citealp{Chandrasekhar1946}) 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. $\langle N_{sc}\rangle$ $\sim$1.1 the PD is independent of energy and PA $\sim 90^o$ ($k'_e$ is parallel to the disk plane), and for $\langle N_{sc}\rangle$ $\sim$5 the PD value is maximum for $i=45^o$. We also compare the results qualitatively with observation of IXPE for five sources.

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