2015MNRAS.449.2919L


Query : 2015MNRAS.449.2919L

2015MNRAS.449.2919L - Mon. Not. R. Astron. Soc., 449, 2919-2936 (2015/May-3)

A detailed study of the optical attenuation of gamma-ray bursts in the Swift era.

LITTLEJOHNS O.M., BUTLER N.R., CUCCHIARA A., WATSON A.M., FOX O.D., LEE W.H., KUTYREV A.S., RICHER M.G., KLEIN C.R., PROCHASKA J.X., BLOOM J.S., TROJA E., RAMIREZ-RUIZ E., DE DIEGO J.A., GEORGIEV L., GONZALEZ J., ROMAN-ZUNIGA C.G., GEHRELS N. and MOSELEY H.

Abstract (from CDS):

We present optical and near-infrared (NIR) photometry of 28 gamma-ray bursts (GRBs) detected by the Swift satellite and rapidly observed by the Reionization and Transients Infrared/Optical (RATIR) camera. We compare the optical flux at fiducial times of 5.5 and 11 h after the high-energy trigger to that in the X-ray regime to quantify optical darkness. 46±9 per cent (13/28) of all bursts in our sample and 55±10 per cent (13/26) of long GRBs are optically dark, which is statistically consistently with previous studies. Fitting RATIR optical and NIR spectral energy distributions of 19 GRBs, most (6/7) optically dark GRBs either occur at high redshift (z > 4.5) or have a high dust content in their host galaxies (AV > 0.3). Performing Kolmogorov-Smirnov tests, we compare the RATIR sample to those previously presented in the literature, finding our distributions of redshift, optical darkness, host dust extinction and X-ray-derived column density to be consistent. The one reported discrepancy is with host galaxy dust content in the BAT6 sample, which appears inconsistent with our sample and other previous literature. Comparing X-ray-derived host galaxy hydrogen column densities to host galaxy dust extinction, we find that GRBs tend to occur in host galaxies with a higher metal-to-dust ratio than our own Galaxy, more akin to the Large and Small Magellanic Clouds. Finally, to mitigate time evolution of optical darkness, we measure βOX, rest at a fixed rest-frame time, trest = 1.5 h and fixed rest-frame energies in the X-ray and optical regimes. Choosing to evaluate optical flux at λrest = 0.25µm, we remove high redshift as a source of optical darkness, demonstrating that optical darkness must result from either high redshift, dust content in the host galaxy along the GRB sight line, or a combination of the two.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

Journal keyword(s): gamma-ray bursts: general - galaxies: distances and redshifts - galaxies: ISM

Simbad objects: 39

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Number of rows : 39
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 bn140703026 gB 00 51 58.99 +45 06 05.4           ~ 70 0
2 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 11146 1
3 GRB 140129A gB 02 31 33.83 -01 35 43.3           ~ 25 0
4 GRB 140710A gB 02 44 16.26 +35 29 56.7           ~ 37 0
5 Fermi bn130925164 gB 02 44 42.38 -26 09 15.8           ~ 153 0
6 SN 2013ez SN* 02 53 56.70 +13 23 13.6           ~ 95 0
7 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17432 0
8 GRB 130327A gB 06 08 09.26 +55 42 53.1           ~ 26 0
9 GRB 140215A gB 06 56 35.83 +41 47 11.8           ~ 35 0
10 GRB 140419A gB 08 27 57.56 +46 14 25.3           ~ 78 0
11 GRB 140331A gB 08 59 27.46 +02 43 02.3           ~ 24 0
12 Fermi bn130502743 gB 09 14 16.53 -00 07 24.1           ~ 35 0
13 Fermi bn130514560 gB 09 50 26.03 -18 57 54.7           ~ 13 0
14 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 206 1
15 GRB 130418A gB 09 56 08.86 +13 40 01.8           ~ 63 0
16 Fermi bn130609129 gB 10 10 40.44 +24 07 56.6           ~ 27 0
17 GRB 130603B gB 11 28 48.16 +17 04 18.2           ~ 346 0
18 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 513 1
19 GRB 140318A gB 12 16 21.43 +20 12 32.5           ~ 35 0
20 GRB 140114A gB 12 34 05.10 +27 57 02.6           ~ 49 0
21 GRB 130122A gB 12 57 08.30 +59 00 53.5           ~ 26 0
22 Fermi bn130420313 gB 13 04 25.49 +59 25 26.8           ~ 93 0
23 GRB 140311A gB 13 57 13.29 +00 38 31.7           ~ 69 0
24 GRB 130907A gB 14 23 34.03 +45 36 27.1           ~ 100 0
25 Fermi bn130610133 gB 14 57 40.91 +28 12 25.8           ~ 69 0
26 GRB 140518A gB 15 09 00.60 +42 25 05.6           ~ 53 0
27 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 154 0
28 Fermi bn130612141 gB 17 19 10.63 +16 43 11.8           ~ 75 0
29 GRB 130504A gB 18 09 49.49 -16 18 48.6           ~ 23 0
30 Fermi bn130626452 gB 18 12 30.60 -09 31 29.9           ~ 25 0
31 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 90 0
32 GRB 130514A gB 19 45 07.33 -07 58 41.1           ~ 62 0
33 Fermi bn140709051 gB 20 18 38.96 +51 13 29.9           ~ 40 0
34 TYC 5783-1382-1 SB* 21 08 38.7890361600 -14 25 08.875132428   12.178 11.552     ~ 5 0
35 GRB 140622A gB 21 08 41.56 -14 25 09.5           ~ 48 0
36 GRB 140614B gB 21 30 31.50 +14 55 46.9           ~ 16 0
37 Fermi bn140118064 gB 22 04 -17.9           ~ 13 0
38 GRB 131030A gB 23 00 16.14 -05 22 05.2           ~ 106 0
39 GRB 130701A gB 23 48 55.05 +36 06 01.2           ~ 69 0

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