2021ApJ...908....4V


Query : 2021ApJ...908....4V

2021ApJ...908....4V - Astrophys. J., 908, 4-4 (2021/February-2)

Seventeen tidal disruption events from the first half of ZTF survey observations: entering a new era of population studies.

VAN VELZEN S., GEZARI S., HAMMERSTEIN E., ROTH N., FREDERICK S., WARD C., HUNG T., CENKO S.B., STEIN R., PERLEY D.A., TAGGART K., FOLEY R.J., SOLLERMAN J., BLAGORODNOVA N., ANDREONI I., BELLM E.C., BRINNEL V., DE K., DEKANY R., FEENEY M., FREMLING C., GIOMI M., GOLKHOU V.Z., GRAHAM M.J., HO A.Y.Q., KASLIWAL M.M., KILPATRICK C.D., KULKARNI S.R., KUPFER T., LAHER R.R., MAHABAL A., MASCI F.J., MILLER A.A., NORDIN J., RIDDLE R., RUSHOLME B., VAN SANTEN J., SHARMA Y., SHUPE D.L. and SOUMAGNAC M.T.

Abstract (from CDS):

While tidal disruption events (TDEs) have long been heralded as laboratories for the study of quiescent black holes, the small number of known TDEs and uncertainties in their emission mechanism have hindered progress toward this promise. Here we present 17 new TDEs that have been detected recently by the Zwicky Transient Facility along with Swift UV and X-ray follow-up observations. Our homogeneous analysis of the optical/UV light curves, including 22 previously known TDEs from the literature, reveals a clean separation of light-curve properties with spectroscopic class. The TDEs with Bowen fluorescence features in their optical spectra have smaller blackbody radii, lower optical luminosities, and higher disruption rates compared to the rest of the sample. The small subset of TDEs that show only helium emission lines in their spectra have the longest rise times, the highest luminosities, and the lowest rates. A high detection rate of Bowen lines in TDEs with small photometric radii could be explained by the high density that is required for this fluorescence mechanism. The stellar debris can provide a source for this dense material. Diffusion of photons through this debris may explain why the rise and fade timescale of the TDEs in our sample are not correlated. We also report, for the first time, the detection of soft X-ray flares from a TDE on ∼day timescales. Based on the fact that the X-ray flares peak at a luminosity similar to the optical/UV blackbody luminosity, we attribute them to brief glimpses through a reprocessing layer that otherwise obscures the inner accretion flow.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Astrophysical black holes - Tidal disruption - Galaxy nuclei

Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.

Simbad objects: 35

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Number of rows : 35
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 OGLE16aaa ev 01 07 20.88 -64 16 20.7           ~ 72 0
3 SDSS J010733.63+232834.2 G 01 07 33.6367520523 +23 28 34.282762347           ~ 37 0
4 2MASS J01580475-0052221 Sy1 01 58 04.7506373016 -00 52 21.927742716   18.84 18.34     SNII 114 1
5 AT 2018lni ev 04 09 37.652 +73 53 41.66           ~ 15 0
6 AT 2019qiz ev 04 46 37.880 -10 13 34.92           ~ 143 0
7 AT 2019ahk ev 07 00 11.410 -66 02 25.16           ~ 57 0
8 AT 2018lna ev 07 03 18.649 +23 01 44.70           ~ 29 0
9 SDSS J075654.53+341543.6 G 07 56 54.5382395520 +34 15 43.641537336           ~ 96 0
10 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
11 AT 2018bsi ev 08 15 26.621 +45 35 31.95           ~ 20 0
12 PTF 15af SN* 08 48 28.13 +22 03 33.4           ~ 69 0
13 PS1-11af ev 09 57 26.815 +03 14 01.00           ~ 71 0
14 2MASS J10065085+0141342 G 10 06 50.8773292152 +01 41 34.006164648   18.082   17.032   SNII 127 0
15 2MASS J11084011+3405523 G 11 08 40.1149579272 +34 05 52.337925924           ~ 142 0
16 SDSS J112849.64+154022.3 G 11 28 49.6469654133 +15 40 22.339118003           ~ 18 0
17 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
18 AT 2019cho ev 12 55 09.210 +49 31 09.93           ~ 16 0
19 SDSS J140941.88+552928.0 AGN 14 09 41.8833027816 +55 29 28.058874792           ~ 55 0
20 PTF 09axc SN* 14 53 13.06 +22 14 32.2           SNII 52 0
21 PSN K0905-001 SN? 14 57 03.10 +49 36 40.8           ~ 85 0
22 AT 2019bhf ev 15 09 15.975 +16 14 22.52           ~ 18 0
23 PS1-10jh ev 16 09 28.296 +53 40 23.52           ~ 153 0
24 2MASX J16105891-6055250 AG? 16 10 58.8863559654 -60 55 24.411688282           ~ 78 0
25 AT 2019mha ev 16 16 27.799 +56 25 56.29           ~ 19 0
26 PTF 09djl SN* 16 33 55.94 +30 14 16.3           SNII 74 0
27 iPTF 16axa ev 17 03 34.36 +30 35 36.8           ~ 54 0
28 AT 2018iih ev 17 28 03.930 +30 41 31.42           ~ 26 0
29 AT 2019meg ev 18 45 16.180 +44 26 19.21           ~ 22 0
30 ASASSN -15oi SN* 20 39 09.096 -30 45 20.71           ~ 184 0
31 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
32 ASASSN -15lh ev 22 02 15.4 -61 39 34           ~ 187 1
33 AT 2017eqx ev 22 26 48.370 +17 08 52.40           ~ 30 0
34 AT 2018fyk ev 22 50 16.10 -44 51 53.5           ~ 114 0
35 AT 2019lwu ev 23 11 12.305 -01 00 10.71           ~ 17 0

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