2013ApJ...767..161Z


Query : 2013ApJ...767..161Z

2013ApJ...767..161Z - Astrophys. J., 767, 161 (2013/April-3)

Illuminating the darkest gamma-ray bursts with radio observations.

ZAUDERER B.A., BERGER E., MARGUTTI R., LEVAN A.J., OLIVARES E.F., PERLEY D.A., FONG W., HORESH A., UPDIKE A.C., GREINER J., TANVIR N.R., LASKAR T., CHORNOCK R., SODERBERG A.M., MENTEN K.M., NAKAR E., CARPENTER J., CHANDRA P., CASTRO-TIRADO A.J., BREMER M., GOROSABEL J., GUZIY S., PEREZ-RAMIREZ D. and WINTERS J.M.

Abstract (from CDS):

We present X-ray, optical, near-infrared (IR), and radio observations of gamma-ray bursts (GRBs) 110709B and 111215A, as well as optical and near-IR observations of their host galaxies. The combination of X-ray detections and deep optical/near-IR limits establish both bursts as "dark." Sub-arcsecond positions enabled by radio detections lead to robust host galaxy associations, with optical detections that indicate z ≲ 4 (110709B) and z ~ 1.8-2.9 (111215A). We therefore conclude that both bursts are dark due to substantial rest-frame extinction. Using the radio and X-ray data for each burst we find that GRB 110709B requires AhostV ≳ 5.3 mag and GRB 111215A requires AhostV ≳ 8.5 mag (assuming z = 2). These are among the largest extinction values inferred for dark bursts to date. The two bursts also exhibit large neutral hydrogen column densities of N_H, int_ ≳ 1022/cm2 (z = 2) as inferred from their X-ray spectra, in agreement with the trend for dark GRBs. Moreover, the inferred values are in agreement with the Galactic AV-NHrelation, unlike the bulk of the GRB population. Finally, we find that for both bursts the afterglow emission is best explained by a collimated outflow with a total beaming-corrected energy of Eγ+ EK~ (7-9)x1051 erg (z = 2) expanding into a wind medium with a high density, {dot}M ~ (6-20) x 10–5 M☉/yr (n ~ 100-350/cm3 at ~1017 cm). While the energy release is typical of long GRBs, the inferred density may be indicative of larger mass-loss rates for GRB progenitors in dusty (and hence metal rich) environments. This study establishes the critical role of radio observations in demonstrating the origin and properties of dark GRBs. Observations with the JVLA and ALMA will provide a sample with sub-arcsecond positions and robust host associations that will help to shed light on obscured star formation and the role of metallicity in GRB progenitors.

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Journal keyword(s): dust, extinction - gamma-ray burst: general

Simbad objects: 37

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Number of rows : 37
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 GRB 041219 gB 00 24 27.7 +62 50 34           ~ 231 1
2 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
3 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
4 GRB 000210 gB 01 59 15 -40 40.0           ~ 175 0
5 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
6 NGC 1275 Bla 03 19 48.1599902040 +41 30 42.108850836   13.10 12.48 11.09   ~ 4243 3
7 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
8 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
9 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
10 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
11 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
12 GRB 111016A gB 10 15 20.16 +27 27 44.5           ~ 33 0
13 QSO B1045-188 Bla 10 48 06.62062314 -19 09 35.7272070   18.59 18.20 17.10   ~ 203 1
14 GRB 110709B gB 10 58 37.2 -23 27 18           ~ 92 0
15 PKS 1110-217 rG 11 12 49.84885865 -21 58 29.3504367   24.41       ~ 35 1
16 GRB 030115 gB 11 18 32.6 +15 02 59           ~ 90 1
17 GRB 060123 gB 11 58 47.83 +45 30 50.9           ~ 46 0
18 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 257 0
19 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
20 GRB 090417B gB 13 58 44.8 +47 00 55           ~ 119 1
21 IC 1127 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 3090 4
22 GRB 070521 gB 16 10 38.600 +30 15 22.70           ~ 164 0
23 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
24 GRB 060929 gB 17 32 28.920 +29 50 06.20           ~ 60 0
25 GRB 970828 gB 18 08 31.6 +59 18 51           ~ 353 1
26 EM* MWC 349 ** 20 32 45.499080 +40 39 36.74124   15.88 13.15 12.13   Bep 837 0
27 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
28 QSO B2232+282 BLL 22 36 22.47084387 +28 28 57.4132050   19.1 19.0 17.60   ~ 306 2
29 Fermi bn091024380 gB 22 37 +56.9           ~ 151 0
30 ICRF J225312.4+323604 QSO 22 53 12.49980744 +32 36 04.3267691           ~ 26 1
31 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 3004 2
32 GRB 020819 gB 23 00 12 -43 00.7           ~ 135 1
33 6C 230840+340844 Bla 23 11 05.32880063 +34 25 10.9049514     19.5 19.2   ~ 138 1
34 GRB 111215A gB 23 18 13.33 +32 29 38.5           ~ 68 0
35 ICRF J234029.0+264156 BLL 23 40 29.02947125 +26 41 56.8046329   20.0 20 19.24   ~ 60 1
36 GRB 061222 gB 23 53.0 +46 32           ~ 18 0
37 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 194 1

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