论文标题
观察X射线光谱上黑洞事件地平线的烙印
Observing imprints of black hole event horizon on X-ray spectra
论文作者
论文摘要
中子星(NS)和黑洞(BH)之间的基本差异是后者没有物理表面。因此,在其事件范围内推动了积聚在BH上的任何剩余的动能。在NS的情况下,相反,积分材料在NS表面下降,其动能最终被辐射消失。 NS表面产生的大量软光子将影响硬态X射线二进制谱的组成组分的性质。因此,构成光谱的参数 - 电子温度$ kt _ {\ rm e} $和compton $ y $ - 参数可以作为将BHS与NSS区分开的重要工具。在本文中,我们使用档案rxte/pca和rxte/hexte观察结果系统地,系统地分析了在坚硬状态下从BH和NS X射线二进制文件中最大的光谱样本。我们发现,BHS和NSS在$ y-kt _ {\ rm e} $平面中占据明显不同的区域,而NSS的特征在于$ y $ - 参数和电子温度的系统上较低的值。由于$ y-kt _ {\ rm e} $ plane上BHS和NSS之间的边界形状,他们的一维$ y $和$ kt _ {\ rm e} $ distributions有一些重叠。 Compton放大因子$ a $提供了一个更清洁的一个参数诊断,即X射线二进制文件中紧凑型对象的性质,而BHS和NSS之间的边界则位于$ A \ a \ 3.5-4 $。到目前为止,这是对稳定的恒星质量BHS X射线光谱上事件范围的最显着检测。
A fundamental difference between a neutron star (NS) and a black hole (BH) is the absence of a physical surface in the latter. For this reason, any remaining kinetic energy of the matter accreting onto a BH is advected inside its event horizon. In the case of an NS, on the contrary, accreting material is decelerated on the NS surface, and its kinetic energy is eventually radiated away. Copious soft photons produced by the NS surface will affect the properties of the Comptonised component dominating spectra of X-ray binaries in the hard state. Thus, parameters of the Comptonised spectra -- the electron temperature $kT_{\rm e}$ and the Compton $y$-parameter, could serve as an important tool for distinguishing BHs from NSs. In this paper, we systematically analyse heretofore the largest sample of spectra from the BH and NS X-ray binaries in the hard state for this purpose, using archival RXTE/PCA and RXTE/HEXTE observations. We find that the BHs and NSs occupy distinctly different regions in the $y-kT_{\rm e}$ plane with NSs being characterised by systematically lower values of $y$-parameter and electron temperature. Due to the shape of the boundary between BHs and NSs on the $y-kT_{\rm e}$ plane, their one-dimensional $y$ and $kT_{\rm e}$ distributions have some overlap. A cleaner one parameter diagnostic of the nature of the compact object in X-ray binaries is provided by the Compton amplification factor $A$, with the boundary between BHs and NSs lying at $A\approx 3.5-4$. This is by far the most significant detection of the imprint of the event horizon on the X-ray spectra for stable stellar-mass BHs.