2014ApJ...780..118F


Query : 2014ApJ...780..118F

2014ApJ...780..118F - Astrophys. J., 780, 118 (2014/January-2)

Short GRB 130603B: discovery of a jet break in the optical and radio afterglows, and a mysterious late-time X-ray excess.

FONG W., BERGER E., METZGER B.D., MARGUTTI R., CHORNOCK R., MIGLIORI G., FOLEY R.J., ZAUDERER B.A., LUNNAN R., LASKAR T., DESCH S.J., MEECH K.J., SONNETT S., DICKEY C., HEDLUND A. and HARDING P.

Abstract (from CDS):

We present radio, optical/NIR, and X-ray observations of the afterglow of the short-duration Swift and Konus-Wind GRB 130603B, and uncover a break in the radio and optical bands at ~0.5 day after the burst, best explained as a jet break with an inferred jet opening angle of ~4°-8°. GRB 130603B is only the third short GRB with a radio afterglow detection to date, and represents the first time that a jet break has been evident in the radio band. We model the temporal evolution of the spectral energy distribution to determine the burst explosion properties and find an isotropic-equivalent kinetic energy of ~(0.6-1.7)x1051 erg and a circumburst density of ~5x10–3-30/cm3. From the inferred opening angle of GRB 130603B, we calculate beaming-corrected energies of Eγ~ (0.5-2)x1049 erg and EK~ (0.1-1.6)x1049 erg. Along with previous measurements and lower limits we find a median opening angle of ~10°. Using the all-sky observed rate of 10 G/pc3/yr, this implies a true short GRB rate of ~20/yr within 200 Mpc, the Advanced LIGO/VIRGO sensitivity range for neutron star binary mergers. Finally, we uncover evidence for significant excess emission in the X-ray afterglow of GRB 130603B at ≳ 1 day and conclude that the additional energy component could be due to fall-back accretion or spin-down energy from a magnetar formed following the merger.

Abstract Copyright:

Journal keyword(s): gamma-ray burst: individual: 130603B

Simbad objects: 17

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Number of rows : 17
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 120 0
2 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 940 1
3 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 129 0
4 Fermi bn081226044 gB 08 02 00.36 -69 01 46.0           ~ 55 0
5 4C 12.39 Bla 11 18 57.30143432 +12 34 41.7179609   19.39 19.25 19.10   ~ 258 1
6 ICRF J112027.8+142054 Sy2 11 20 27.80814059 +14 20 54.9730732   20 20.935 20.100   ~ 167 1
7 GRB 130603B gB 11 28 48.16 +17 04 18.2           ~ 346 0
8 GRB 090426 gB 12 36 19.49 +32 59 05.5           ~ 205 0
9 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4341 2
10 GRB 120804A gB 15 35 47.55 -28 46 56.9           ~ 85 0
11 GRB 090305 gB 16 07 02.0 -31 34 00           ~ 47 0
12 GRB 050724 gB 16 24 44.400 -27 32 27.90     19.70     ~ 439 1
13 GRB 080503 gB 19 06 28.74 +68 47 35.8           ~ 155 0
14 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 59 0
15 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1821 2
16 GRB 051221 gB 21 54 48.626 +16 53 27.16 19.49         ~ 351 1
17 GRB 050709 gB 23 01 26.960 -38 58 39.50           ~ 297 1

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