2022A&A...659A..34C


Query : 2022A&A...659A..34C

2022A&A...659A..34C - Astronomy and Astrophysics, volume 659A, 34-34 (2022/3-1)

A detailed spectroscopic study of tidal disruption events.

CHARALAMPOPOULOS P., LELOUDAS G., MALESANI D.B., WEVERS T., ARCAVI I., NICHOLL M., PURSIAINEN M., LAWRENCE A., ANDERSON J.P., BENETTI S., CANNIZZARO G., CHEN T.-W., GALBANY L., GROMADZKI M., GUTIERREZ C.P., INSERRA C., JONKER P.G., MULLER-BRAVO T.E., ONORI F., SHORT P., SOLLERMAN J. and YOUNG D.R.

Abstract (from CDS):

Spectroscopically, tidal disruption events (TDEs) are characterized by broad (∼104 km s–1) emission lines and show a large diversity as well as different line profiles. After carefully and consistently performing a series of data reduction tasks including host galaxy light subtraction, we present here the first detailed, spectroscopic population study of 16 optical and UV TDEs. We study a number of emission lines prominent among TDEs including Hydrogen, Helium, and Bowen lines and we quantify their evolution with time in terms of line luminosities, velocity widths, and velocity offsets. We report a time lag between the peaks of the optical light curves and the peak luminosity of Hα spanning between ∼7 and 45 days.If interpreted as light echoes, these lags correspond to distances of ∼2 - 12 x 1016 cm, which are one to two orders of magnitudes larger than the estimated blackbody radii (RBB) of the same TDEs and we discuss the possible origin of this surprisingly large discrepancy. We also report time lags for the peak luminosity of the HeI 5876 Å line, which are smaller than the ones of Hα for H TDEs and similar or larger for NIII Bowen TDEs. We report that NIII Bowen TDEs have lower Hα velocity widths compared to the rest of the TDEs in our sample and we also find that a strong X-ray to optical ratio might imply weakening of the line widths. Furthermore, we study the evolution of line luminosities and ratios with respect to their radii (RBB) and temperatures (TBB). We find a linear relationship between Hα luminosity and the RBB (Lline ∝ RBB) and potentially an inverse power-law relation with TBB (Lline ∝ TBB–β), leading to weaker Hα emission for TBB ≥ 25 000 K. The HeII/HeI ratio becomes large at the same temperatures, possibly pointing to an ionization effect. The HeII/Hα ratio becomes larger as the photospheric radius recedes, implying a stratified photosphere where Helium lies deeper than Hydrogen. We suggest that the large diversity of the spectroscopic features seen in TDEs along with their X-ray properties can potentially be attributed to viewing angle effects.

Abstract Copyright: © ESO 2022

Journal keyword(s): black hole physics - line: formation - techniques: spectroscopic - Galaxy: nucleus

Simbad objects: 18

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Number of rows : 18
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 AT 2016fnl ev 00 29 57.050 +32 53 37.27           ~ 92 0
2 AT 2019qiz ev 04 46 37.880 -10 13 34.92           ~ 50 0
3 AT 2018lna ev 07 03 18.649 +23 01 44.70           ~ 17 0
4 ATLAS 18nej ev 07 56 54.537 +34 15 43.61           ~ 59 0
5 ASASSN -19dj SN* 08 13 16.937 +22 38 53.80           ~ 66 0
6 PTF 15af SN* 08 48 28.13 +22 03 33.4           ~ 43 0
7 ASASSN -18zj SN* 10 06 50.875 +01 41 33.96           SNII 51 0
8 ASASSN -14ae SN* 11 08 40.11 +34 05 52.4           ~ 99 0
9 LEDA 43234 G 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 243 0
10 PSN K0905-001 SN? 14 57 03.10 +49 36 40.8           ~ 68 0
11 PS1-10jh ev 16 09 28.296 +53 40 23.52           ~ 128 0
12 AT 2018dyb ev 16 10 58.774 -60 55 23.16           ~ 41 0
13 PTF 09djl SN* 16 33 55.94 +30 14 16.3           SNII 59 0
14 iPTF 16axa ev 17 03 34.36 +30 35 36.8           ~ 39 0
15 ASASSN -15oi SN* 20 39 09.096 -30 45 20.71           ~ 117 0
16 AT 2017eqx ? 22 26 48.370 +17 08 52.40           ~ 16 0
17 AT 2018fyk ev 22 50 16.10 -44 51 53.5           ~ 54 0
18 LSQ 12dyw SN* 23 29 24.82 -07 23 20.4           SNIcpec 5 0

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2023.09.22-23:54:11

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