论文标题
Astrosat观察X射线倾角和黑洞候选人Maxi J1803-298中的状态过渡
AstroSat Observation of X-ray Dips and State Transition in the Black Hole Candidate MAXI J1803-298
论文作者
论文摘要
我们使用Astrosat观察结果于5月11日至2日,2021年5月11日至121日介绍了黑洞候选Maxi J1803-298的宽带X射线时间和光谱分析获得的结果。在光线曲线中检测到四个周期性吸收下降,周期性为$ 7.02 \ pm 0.18 $。 Astrosat在从硬式中间状态过渡到软中间状态的过渡时观察了源。我们的时序分析揭示了功率密度光谱(PDS)中尖锐的C型准周期性振荡(QPO)的存在,其不断发展的QPO频率从$ 5.31 \ pm 0.02 $ 0.02 $ Hz到$ 7.61 \ $ 0.61 \ pm 0.09 $ hz。我们研究了QPO的能量依赖性,并且在30 KEV以上的PDS中找不到此功能。合并的$ 0.7-80 $ KEV SXT和LAXPC光谱均配备了由热多色黑体发射和组成的排放组件组成的型号。我们通过在观察的浸入和非浸入阶段提取光谱来执行时间分辨光谱。在浸入和非浸入阶段中检测到中性吸收剂,尽管浸入阶段也存在电离吸收剂的特征。在我们的观察过程中发现光谱和时间参数会发展。我们将系统的质量函数估计为$ f(m)= 2.1-7.2〜m _ {\ odot} $,而黑洞候选者的质量则在$ M _ {\ rm BH} \ sim 3.5-12.5〜m _ {\ odot} $中。
We present the results obtained from broadband X-ray timing and spectral analysis of black hole candidate MAXI J1803-298 using an AstroSat observation on May 11-12, 2021. Four periodic absorption dips with a periodicity of $7.02 \pm 0.18$ hour are detected in the light curve. AstroSat observe the source when it was undergoing a transition from hard-intermediate state to soft-intermediate state. Our timing analysis reveals the presence of a sharp type-C quasi periodic oscillation (QPO) in the power density spectra (PDS) with an evolving QPO frequency ranging from $5.31 \pm 0.02$ Hz to $7.61\pm 0.09$ Hz. We investigate the energy dependence of the QPO and do not find this feature in the PDS above 30 keV. The combined $0.7-80$ keV SXT and LAXPC spectra are fitted with a model consisting of thermal multi-colour blackbody emission and Comptonized emission components. We perform time-resolved spectroscopy by extracting spectra during the dip and non-dip phases of the observation. A neutral absorber is detected during the dip and non-dip phases though a signature of an ionized absorber is also present in the dip phases. The spectral and temporal parameters are found to evolve during our observation. We estimate the mass function of the system as $f(M) = 2.1-7.2~M_{\odot}$ and the mass of the black hole candidate in the range of $M_{\rm BH} \sim 3.5-12.5~M_{\odot}$.