Implications from Late-time X-Ray Detections of Optically Selected Tidal Disruption Events: State Changes, Unification, and Detection Rates

被引:54
|
作者
Jonker, P. G. [1 ,2 ]
Stone, N. C. [3 ,4 ,5 ,6 ]
Generozov, A. [5 ,6 ,7 ,8 ]
van Velzen, S. [9 ,10 ]
Metzger, B. [5 ,6 ]
机构
[1] SRON Netherlands Inst Space Res, SRON, Sorbonnelaan 2, NL-3584 CA Utrecht, Netherlands
[2] Radboud Univ Nijmegen, IMAPP, Dept Astrophys, POB 9010, NL-6500 GL Nijmegen, Netherlands
[3] Univ Maryland, Dept Astron, Stadium Dr, College Pk, MD 20742 USA
[4] Hebrew Univ Jerusalem, Racah Inst Phys, IL-91904 Jerusalem, Israel
[5] Columbia Univ, Dept Phys, Dept Astron, 538 W 120th St, New York, NY 10027 USA
[6] Columbia Univ, Columbia Astrophys Lab, 538 W 120th St, New York, NY 10027 USA
[7] Univ Colorado, JILA, 440 UCB, Boulder, CO 80309 USA
[8] NIST, 440 UCB, Boulder, CO 80309 USA
[9] NYU, Ctr Cosmol & Particle Phys, New York, NY 10003 USA
[10] Univ Maryland, Joint Space Sci Inst, College Pk, MD 20742 USA
基金
欧洲研究理事会; 美国国家航空航天局;
关键词
BLACK-HOLE MASSES; LIGHT CURVES; CHANDRA OBSERVATIONS; ACCRETION DISCS; FOLLOW-UP; OUTBURST; FLARES; CANDIDATE; STARS; EMISSION;
D O I
10.3847/1538-4357/ab659c
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present Chandra X-ray observations of four optically selected tidal disruption events (TDEs) obtained 4-9 yr after discovery. Three sources were detected with luminosities between 9 x 10(40) and 3 x 10(42) erg s(-1). The spectrum of PTF09axc is consistent with a power law of index 2.5 +/- 0.1, whereas the spectrum of PTF09ge is very soft. The power-law spectrum of PTF09axc and prior literature findings provide evidence that TDEs transition from an early-time soft state to a late-time hard state many years after disruption. We propose that the time to peak luminosity for optical and X-ray emission may differ substantially in TDEs, with X-rays being produced or becoming observable later. This delay helps explain the differences in observed properties such as L-opt/L-X of optically and X-ray-selected TDEs. We update TDE rate predictions for the eROSITA instrument: it ranges from 3 to 990 yr(-1), depending sensitively on the distribution of black hole spins and the time delay between disruption and peak X-ray brightness. We further predict an asymmetry in the number of retrograde and prograde disks in samples of optically and X-ray-selected TDEs. The details of the observational biases can contribute to observed differences between optically and X-ray-selected TDEs (with optically selected TDEs being fainter in X-rays for retrograde TDE disks).
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收藏
页数:17
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