2020ApJ...889..166J


Query : 2020ApJ...889..166J

2020ApJ...889..166J - Astrophys. J., 889, 166-166 (2020/February-1)

Implications from late-time X-ray detections of optically selected tidal disruption events: state changes, unification, and detection rates.

JONKER P.G., STONE N.C., GENEROZOV A., VAN VELZEN S. and METZGER B.

Abstract (from CDS):

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 1040 and 3 x 1042 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 Lopt/LX 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).

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Astrophysical black holes - Tidal disruption - Active galactic nuclei - High energy astrophysics - X-ray transient sources

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 Z 500-36 AG? 00 29 57.0542865144 +32 53 37.265932104           ~ 155 0
2 LEDA 87392 Sy1 00 39 15.8339634552 -51 17 01.481641692   15.77 15.28 15.66   ~ 134 0
3 XMMSL1 J074008.2-853927 X 07 40 08.2 -85 39 27           ~ 52 0
4 SN 2006jd SN* 08 02 07.43 +00 48 31.5   22.5 21.8 20.4 21.3 SNIIn 128 1
5 2MASS J11084011+3405523 G 11 08 40.1149579272 +34 05 52.337925924           ~ 142 0
6 SDSS J114726.69+494257.8 G 11 47 26.69774 +49 42 57.8329   17.43 17.10     ~ 26 0
7 2MASS J12013602+3003052 G 12 01 36.0281668104 +30 03 05.576406012           ~ 47 0
8 IC 3599 Sy1 12 37 41.1939398400 +26 42 27.484266888   15.7 16.5     ~ 191 0
9 RX J1242.6-1119 PaG 12 42 36.9 -11 19 35           ~ 49 1
10 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
11 LEDA 2725953 G 14 46 05.1793580544 +68 57 30.776717844           ~ 19 0
12 PTF 09axc SN* 14 53 13.06 +22 14 32.2           SNII 52 0
13 SDSS J145313.07+221432.2 G 14 53 13.0713207528 +22 14 32.181525924           ~ 5 0
14 PSN K0905-001 SN? 14 57 03.10 +49 36 40.8           ~ 85 0
15 SDSS J145703.17+493640.9 G 14 57 03.1849787088 +49 36 40.908142296           ~ 5 0
16 NGC 5905 H2G 15 15 23.3280793632 +55 31 01.926808032   13.6       ~ 287 1
17 MAXI J1535-571 XB* 15 35 19.73 -57 13 48.1           ~ 214 0
18 PS1-10jh ev 16 09 28.296 +53 40 23.52           ~ 153 0
19 2MASX J16245665+7554560 BLL 16 24 56.5716973728 +75 54 55.975695048     16.60     ~ 59 0
20 PTF 09djl SN* 16 33 55.94 +30 14 16.3           SNII 74 0
21 SDSS J163355.97+301416.6 G 16 33 55.9698742776 +30 14 16.633711680           ~ 4 0
22 iPTF 16axa ev 17 03 34.36 +30 35 36.8           ~ 54 0
23 2MASS J18472513-6317252 G 18 47 25.1287042560 -63 17 25.304943912     16.67   15.56 ~ 16 0
24 ASASSN -15oi SN* 20 39 09.096 -30 45 20.71           ~ 184 0
25 AT 2018fyk ev 22 50 16.10 -44 51 53.5           ~ 114 0

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