2013ApJ...762L..18G


Query : 2013ApJ...762L..18G

2013ApJ...762L..18G - Astrophys. J., 762, L18 (2013/January-2)

Compact binary progenitors of short gamma-ray bursts.

GIACOMAZZO B., PERNA R., REZZOLLA L., TROJA E. and LAZZATI D.

Abstract (from CDS):

In recent years, detailed observations and accurate numerical simulations have provided support to the idea that mergers of compact binaries containing either two neutron stars (NSs) or an NS and a black hole (BH) may constitute the central engine of short gamma-ray bursts (SGRBs). The merger of such compact binaries is expected to lead to the production of a spinning BH surrounded by an accreting torus. Several mechanisms can extract energy from this system and power the SGRBs. Here we connect observations and numerical simulations of compact binary mergers, and use the current sample of SGRBs with measured energies to constrain the mass of their powering tori. By comparing the masses of the tori with the results of fully general-relativistic simulations, we are able to infer the properties of the binary progenitors that yield SGRBs. By assuming a constant efficiency in converting torus mass into jet energy, εjet= 10%, we find that most of the tori have masses smaller than 0.01 M☉, favoring "high-mass" binary NSs mergers, i.e., binaries with total masses ≳ 1.5 the maximum mass of an isolated NS. This has important consequences for the gravitational wave signals that may be detected in association with SGRBs, since "high-mass" systems do not form a long-lived hypermassive NS after the merger. While NS-BH systems cannot be excluded to be the engine of at least some of the SGRBs, the BH would need to have an initial spin of ∼0.9 or higher.

Abstract Copyright: ∼

Journal keyword(s): accretion, accretion disks - gamma-ray burst: general - gravitational waves - methods: numerical - stars: neutron

Simbad objects: 24

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Number of rows : 24
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 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
2 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
3 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
4 GRB 070729 gB 03 45 16.04 -39 19 19.9           ~ 81 0
5 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
6 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
7 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
8 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
9 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
10 GRB 061217 gB 10 41 39.320 -21 07 22.11           ~ 128 0
11 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
12 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
13 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
14 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
15 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
16 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 153 1
17 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
18 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
19 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
20 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
21 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
22 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
23 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0
24 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1

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