论文标题

超紧凑型X射线二进制4U 1543-624的同时和Nustar观察

Simultaneous NICER and NuSTAR Observations of the Ultra-compact X-ray Binary 4U 1543-624

论文作者

Ludlam, R. M., Jaodand, A. D., García, J. A., Degenaar, N., Tomsick, J. A., Cackett, E. M., Fabian, A. C., Gandhi, P., Buisson, D. J. K., Shaw, A. W., Chakrabarty, D.

论文摘要

我们介绍了第一个联合nustar,并且对超紧凑型X射线二进制(UCXB)4U 1543 $ - $ 624在2020年4月获得。来源的发光度为$ l_ {0.5-50 \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ {2} {2} \ times10^{36} $ ergs s $ ngs s $^{ - 1} $,并显示了fe kum kum kum kum kum kump in os n os o n os n os o vi i vii and o vi i vii and o vi in comply, 光谱。我们使用了一个完整的反射模型,称为Xillverco,该模型是针对UCXBS中的非典型丰度量身定制的,以解释反射的发射。我们测试了O和Fe系组件的发射半径,并得出结论,它们源自积聚磁盘最内向区域的公共磁盘半径($ r _ {\ rm in} \ leq1.07 \ r _ {\ r _ {\ r _ {\ mathrm {isco {isco}} $)。假设紧凑的吸积是中子星(NS),并且内盘的位置是alfvén半径,我们对磁场强度的上限为$ b \ leq0.7(d/7 \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ mathrm {kpc})\ times10^{8} $ g在POLES上。鉴于缺乏检测到的脉动和$ r _ {\ rm in} $的位置,很可能是在ns表面和增生盘的内边缘之间形成边界层区域,范围为1.2 km。这意味着$ r _ {\ mathrm {ns}} \ leq 12.1 $ km的中子星的最大半径在假定规范NS质量为1.4 $ m _ {\ odot} $时。

We present the first joint NuSTAR and NICER observations of the ultra-compact X-ray binary (UCXB) 4U 1543$-$624 obtained in 2020 April. The source was at a luminosity of $L_{0.5-50\ \mathrm{keV}} = 4.9 (D/7\ \mathrm{kpc})^{2}\times10^{36}$ ergs s$^{-1}$ and showed evidence of reflected emission in the form of an O VIII line, Fe K line, and Compton hump within the spectrum. We used a full reflection model, known as xillverCO, that is tailored for the atypical abundances found in UCXBs, to account for the reflected emission. We tested the emission radii of the O and Fe line components and conclude that they originate from a common disk radius in the innermost region of the accretion disk ($R_{\rm in} \leq1.07\ R_{\mathrm{ISCO}}$). Assuming that the compact accretor is a neutron star (NS) and the position of the inner disk is the Alfvén radius, we placed an upper limit on the magnetic field strength to be $B\leq0.7(D/7\ \mathrm {kpc})\times10^{8}$ G at the poles. Given the lack of pulsations detected and position of $R_{\rm in}$, it was likely that a boundary layer region had formed between the NS surface and inner edge of the accretion disk with an extent of 1.2 km. This implies a maximum radius of the neutron star accretor of $R_{\mathrm{NS}}\leq 12.1$ km when assuming a canonical NS mass of 1.4 $M_{\odot}$.

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