Slim Disk Model for Ultraluminous X-Ray Sources

Author(s):  
Ken-ya Watarai ◽  
Shin Mineshige ◽  
Tsunefumi Mizuno
Keyword(s):  
1975 ◽  
Vol 199 ◽  
pp. L153 ◽  
Author(s):  
D. M. Eardley ◽  
A. P. Lightman ◽  
S. L. Shapiro

2020 ◽  
Vol 899 (1) ◽  
pp. 80 ◽  
Author(s):  
Askar B. Abdikamalov ◽  
Dimitry Ayzenberg ◽  
Cosimo Bambi ◽  
Thomas Dauser ◽  
Javier A. García ◽  
...  

2020 ◽  
Vol 72 (3) ◽  
Author(s):  
Shuntaro Ide ◽  
Kiyoshi Hayashida ◽  
Hirofumi Noda ◽  
Hiroyuki Kurubi ◽  
Tomokage Yoneyama ◽  
...  

Abstract We report the serendipitous discovery of a transient X-ray source, Suzaku J1305−4930, ∼3 kpc southwest of the nucleus of the Seyfert 2 galaxy NGC 4945. Among the seven Suzaku observations of NGC 4945 from 2005 to 2011, Suzaku J1305−4930 was detected four times in July and August in 2010. The X-ray spectra are better approximated with a multi-color disk model than a power-law model. At the first detection on 2010 July 4–5, its X-ray luminosity was $(8.9^{+0.2}_{-0.4}) \times 10^{38}\:$erg s−1 and the temperature at the inner-disk radius (kTin) was 1.12 ± 0.04 keV. At the last detection with Suzaku on 2010 August 4–5, the luminosity decreased to $(2.2^{+0.3}_{-0.8}) \times 10^{38}\:$erg s−1 and kTin was 0.62 ± 0.07 keV. The source was not detected on 2011 January 29, about six months after the first detection, with a luminosity upper limit of 2.4 × 1038 erg s−1. We also find an absorption feature which is similar to that reported in Cyg X-1. Assuming the standard disk, we suggest that Suzaku J1305−4930 consists of a black hole with a mass of ∼10 $M_\odot$. The relation between the disk luminosity and kTin is not reproduced with the standard model of a constant inner radius but is better approximated with a slim-disk model.


1996 ◽  
Vol 158 ◽  
pp. 139-140
Author(s):  
S.-W. Kim ◽  
J. C. Wheeler ◽  
S. Mineshige

We present time-dependent, irradiated, accretion disk models for the black hole X-ray novae in the first hundred days of the dwarf nova-like outbursts, including the rise, precursor, maximum and the secondary re-flare. This work is based on the disk instability model (Kim, Mineshige & Wheeler 1996, Kim, Wheeler & Mineshige 1996). The model is reasonably consistent with the observed optical light curves. The irradiators are the central hot region around the black hole, and the corona or chromosphere above the accretion disk. In addition, we include the time-dependent shadowing effect and consequent blocking of the outer portions of the disk from the central irradiator. We find the stagnation phenomenon whereby the disk stays in the intermediate temperature stage between the hot and cool state. This can explain the recently discovered optical precursor rise prior to the maximum light in Nova Sco 1994 (Bailyn et al. 1995: see Fig. 1). We suggest the secondary re-flare after the maximum is due to the coupled effects of the irradiation and stagnation. In the model, the stagnation phenomenon during the rise results from the partial ionization and molecular opacity. In addition, we find irradiation-induced stagnation during the decay phase, which is consistent with the observed secondary re-flare in X-ray novae (see Fig. 1). In the overall evolution of model outbursts in the first hundred days, the outer disk is blocked from the irradiation and, in turn, the companion star may not be strongly irradiated. This suggests that there is no appreciable increase of mass transfer rate during the decay prior to the secondary re-flare, unlike the behaviour in the mass transfer burst models.


2003 ◽  
Vol 596 (2) ◽  
pp. L199-L201 ◽  
Author(s):  
Xiang-Dong Li
Keyword(s):  

2000 ◽  
Vol 52 (3) ◽  
pp. 499-508 ◽  
Author(s):  
Shin Mineshige ◽  
Toshihiro Kawaguchi ◽  
Mitsuru Takeuchi ◽  
Kiyoshi Hayashida
Keyword(s):  

1997 ◽  
Vol 487 (1) ◽  
pp. 388-395 ◽  
Author(s):  
R. Misra ◽  
V. R. Chitnis ◽  
F. Melia ◽  
A. R. Rao
Keyword(s):  

1998 ◽  
Vol 188 ◽  
pp. 404-405
Author(s):  
M. Takeuchi

The new model for X-ray fluctuations of Cyg X-1, which is based on the fluid dynamics, is presented. The model is the optically thin and advection-dominated accretion disk model, which has a critical behavior.


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