2012MNRAS.425.2668C


Query : 2012MNRAS.425.2668C

2012MNRAS.425.2668C - Mon. Not. R. Astron. Soc., 425, 2668-2673 (2012/October-1)

The Swift short gamma-ray burst rate density: implications for binary neutron star merger rates.

COWARD D.M., HOWELL E.J., PIRAN T., STRATTA G., BRANCHESI M., BROMBERG O., GENDRE B., BURMAN R.R. and GUETTA D.

Abstract (from CDS):

Short gamma-ray bursts (SGRBs) observed by Swift potentially reveal the first insight into cataclysmic compact object mergers. To ultimately acquire a fundamental understanding of these events requires pan-spectral observations and knowledge of their spatial distribution to differentiate between proposed progenitor populations. Up to 2012 April, there are only some 30 per cent of SGRBs with reasonably firm redshifts, and this sample is highly biased by the limited sensitivity of Swift to detect SGRBs. We account for the dominant biases to calculate a realistic SGRB rate density out to z ≈ 0.5 using the Swift sample of peak fluxes, redshifts and those SGRBs with a beaming angle constraint from X-ray/optical observations. We find an SGRB lower rate density of 8-3+5 Gpc -3 yr -1 (assuming isotropic emission) and a beaming corrected upper limit of 1100-470+700 Gpc -3 yr -1. Assuming a significant fraction of binary neutron star mergers produce SGRBs, we calculate lower and upper detection rate limits of (1-180)/yr by an Advanced LIGO (aLIGO) and Virgo coincidence search. Our detection rate is similar to the lower and realistic rates inferred from extrapolations using Galactic pulsar observations and population synthesis.

Abstract Copyright: © 2012 The Authors Monthly Notices of the Royal Astronomical Society 2012 RAS

Journal keyword(s): gravitational waves - techniques: miscellaneous - gamma-ray burst: individual - stars: neutron

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 - 2026
#notes
1 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
2 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
3 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
4 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
5 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
6 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
7 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
8 GRB 061217 gB 10 41 39.320 -21 07 22.11           ~ 128 0
9 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
10 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
11 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
12 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 66 0
13 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
14 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
15 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
16 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
17 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1
18 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0

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