2019ApJ...881...75K


Query : 2019ApJ...881...75K

2019ApJ...881...75K - Astrophys. J., 881, 75-75 (2019/August-2)

Tidal disruptions of stars by black hole remnants in dense star clusters.

KREMER K., LU W., RODRIGUEZ C.L., LACHAT M. and RASIO F.A.

Abstract (from CDS):

In a dense stellar environment, such as the core of a globular cluster (GC), dynamical interactions with black holes (BHs) are expected to lead to a variety of astrophysical transients. Here we explore tidal disruption events (TDEs) of stars by stellar-mass BHs through collisions and close encounters. Using state-of-the-art cluster simulations, we show that these TDEs occur at significant rates throughout the evolution of typical GCs and we study how their relative rates relate to cluster parameters such as mass and size. By incorporating a realistic cosmological model of GC formation, we predict a BH-main-sequence-star TDE rate of approximately 3 Gpc–3 yr–1 in the local universe (z < 0.1) and a cosmological rate that peaks at roughly 25 Gpc–3 yr–1 for redshift 3. Furthermore, we show that the ejected mass associated with these TDEs could produce optical transients of luminosity ∼1041-1044 erg s–1 with timescales of about a day to a month. These should be readily detectable by optical transient surveys such as the Zwicky Transient Facility. Finally, we comment briefly on BH-giant encounters and discuss how these events may contribute to the formation of BH-white-dwarf binaries.

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

Journal keyword(s): globular clusters: general - methods: numerical - stars: black holes - stars: kinematics and dynamics

Simbad objects: 8

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Number of rows : 8
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 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
2 NGC 3201 GlC 10 17 36.82 -46 24 44.9           ~ 1001 0
3 M 49 Sy2 12 29 46.8 +08 00 01   13.21 12.17     ~ 2174 2
4 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
5 M 5 GlC 15 18 33.22 +02 04 51.7     5.95     ~ 2095 0
6 M 10 GlC 16 57 09.05 -04 06 01.1     4.98     ~ 857 0
7 M 92 GlC 17 17 07.39 +43 08 09.4     6.52     ~ 2240 0
8 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0

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