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The Spin of the Black Hole GRS 1716-249 Determined from the Hard Intermediate State

Lian TaoKey Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People’s Republic of ChinaJohn A. TomsickSpace Sciences Laboratory, 7 Gauss Way, University of California, Berkeley, CA 94720-7450, USAJinlu QuKey Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People’s Republic of ChinaShu ZhangKey Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People’s Republic of ChinaShuangnan ZhangKey Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People’s Republic of ChinaQingcui BuKey Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People’s Republic of China
2019en
ABI

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Abstract We present three simultaneous/quasi-simultaneous NuSTAR and Swift data sets of the black hole (BH) GRS 1716-249 in its hard intermediate state. The accretion disk in this state may have reached the innermost stable circular orbit, and the NuSTAR spectra show a broad relativistic iron line and a strong Compton hump. To measure the BH spin, we construct a joint model consisting of a relativistic disk model kerrbb and a reflection model relxill , to fit the continuum and the reflection components, respectively. By applying this model to each data set independently, a consistent result is obtained on the BH spin and the disk inclination. The BH spin is a * ≳ 0.92, and the inclination angle ( i ) is around 40°–50°, based on the measurements of all data sets. In the third data set, a high BH mass ( M BH ) is strongly disfavored by the spectral fits. By unfreezing the BH mass, we find a * > 0.92, , and M BH < 8.0 M ⊙ , at a 90% confidence level. Considering the lower limit derived from a previous optical constraint, M BH is in a range of 4.9–8.0 M ⊙ .

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