2013ApJ...777..132D


Query : 2013ApJ...777..132D

2013ApJ...777..132D - Astrophys. J., 777, 132 (2013/November-2)

A search for pulsations in short gamma-ray bursts to constrain their progenitors.

DICHIARA S., GUIDORZI C., FRONTERA F. and AMATI L.

Abstract (from CDS):

We searched for periodic and quasi-periodic signals in the prompt emission of a sample of 44 bright short gamma-ray bursts (GRBs) detected with Fermi/GBM, Swift/BAT, and CGRO/BATSE. The aim was to look for the observational signature of quasi-periodic jet precession, which is expected from black hole (BH)-neutron star (NS) mergers, but not from double NS systems. Thus, this kind of search holds the key to identifying the progenitor systems of short GRBs and, in the interim before gravitational wave detectors become on-lines, represents the only direct way to constrain the progenitors. We tailored our search to the nature of the expected signal by properly stretching the observed light curves by an increasing factor with time, after calibrating the technique with synthetic curves. None of our GRBs showed evidence for periodic or quasi-periodic signals. In particular, for the seven unambiguously short GRBs with the best signal-to-noise ratios, we obtained significant upper limits to the amplitude of the possible oscillations. This result suggests that BH-NS systems do not dominate the population of short GRB progenitors, as described by the kinematic model of Stone et al.

Abstract Copyright: ∼

Journal keyword(s): accretion, accretion disks - gamma-ray burst: general - methods: data analysis - techniques: photometric

VizieR on-line data: <Available at CDS (J/ApJ/777/132): table1.dat>

Simbad objects: 44

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Number of rows : 44
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 bn120624309 gB 00 19 +07.2           ~ 22 0
2 Fermi bn120817168 gB 00 33 -26.4           ~ 25 0
3 GRB 990720 gB 00 46 -33.0           ~ 9 0
4 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
5 Fermi bn090308734 gB 01 27.6 -54 18           ~ 21 0
6 GRB 991002 gB 01 40.6 +03 45           ~ 16 1
7 GRB 080426 gB 01 45 59.79 +69 28 06.0           ~ 50 0
8 Fermi bn120811014 gB 02 55 -31.7           ~ 15 0
9 GRB 081209 gB 03 01 +63.5           ~ 28 0
10 GRB 120305A gB 03 10 08.73 +28 29 30.9           ~ 56 0
11 Fermi bn081107321 gB 03 24.0 +17 06           ~ 21 0
12 3B 940219 gB 04 14.0 +00 07           ~ 13 0
13 3B 940918 gB 04 22.1 +03 13           ~ 16 0
14 GRB 060313 G 04 26 28.4020 -10 50 39.901 20.55 21.03 19.66     ~ 156 0
15 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
16 Fermi bn120830297 gB 05 54 36.0 -28 59 04           ~ 22 0
17 GRB 980218B gB 06 02 55.2 -10 06 36           ~ 3 0
18 4B 960319 gB 06 19.4 -47 43           ~ 11 0
19 2B 930110 gB 06 39.4 +01 43           ~ 14 0
20 3B 930506C gB 06 47.3 -16 40           ~ 12 0
21 GRB 110526A gB 06 50 -16.4           ~ 11 0
22 GRB 090228 gB 07 07.2 -24 18           ~ 45 0
23 Fermi bn081223419 gB 07 30.0 +33 12           ~ 18 0
24 GRB 091109B gB 07 30 59.90 -54 05 30.6           ~ 57 0
25 GRB 110529A gB 07 53.3 +67 55           ~ 27 0
26 Fermi bn081216531 gB 08 37 +07.6           ~ 35 0
27 GRB 110705A gB 10 24 +40.1           ~ 22 0
28 2B 921123B gB 10 54.8 -33 35           ~ 14 0
29 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
30 GRB 111222A gB 11 56 52.92 +69 04 14.8           ~ 33 0
31 3B 940329 gB 12 00.0 +08 55           ~ 18 0
32 GRB 120804A G 15 35 47.5100 -28 46 56.110           ~ 99 0
33 3B 931101 gB 15 53.3 +00 47           ~ 15 0
34 Fermi bn090108020 gB 17 23 +46.0           ~ 23 0
35 GRB 990126B gB 17 56 00.0 +36 00 00           ~ 2 0
36 1B 910718 gB 18 24.3 -18 35           ~ 22 0
37 GRB 990208B gB 19 44 24.0 -39 24 00           ~ 2 0
38 Fermi bn090514726 gB 20 17 -24.4           ~ 12 0
39 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
40 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
41 Fermi bn120323507 gB 22 42 +29.7           ~ 60 0
42 GRB 100811A gB 23 04 +15.9           ~ 16 0
43 GRB 100213A gB 23 17 34.04 +43 22 44.1           ~ 31 0
44 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0

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