2013ApJ...766...41S


Query : 2013ApJ...766...41S

2013ApJ...766...41S - Astrophys. J., 766, 41 (2013/March-3)

Identifying the location in the host galaxy of the short GRB 111117A with the Chandra subarcsecond position.

SAKAMOTO T., TROJA E., AOKI K., GUIRIEC S., IM M., LELOUDAS G., MALESANI D., MELANDRI A., DE UGARTE POSTIGO A., URATA Y., XU D., D'AVANZO P., GOROSABEL J., JEON Y., SANCHEZ-RAMIREZ R., ANDERSEN M.I., BAI J., BARTHELMY S.D., BRIGGS M.S., FOLEY S., FRUCHTER A.S., FYNBO J.P.U., GEHRELS N., HUANG K., JANG M., KAWAI N., KORHONEN H., MAO J., NORRIS J.P., PREECE R.D., RACUSIN J.L., THONE C.C., VIDA K. and ZHAO X.

Abstract (from CDS):

We present our successful Chandra program designed to identify, with subarcsecond accuracy, the X-ray afterglow of the short GRB 111117A, which was discovered by Swift and Fermi. Thanks to our rapid target of opportunity request, Chandra clearly detected the X-ray afterglow, though no optical afterglow was found in deep optical observations. The host galaxy was clearly detected in the optical and near-infrared band, with the best photometric redshift of z = 1.31+0.46–0.23 (90% confidence), making it one of the highest known short gamma-ray burst (GRB) redshifts. Furthermore, we see an offset of 1.0±0.2 arcsec, which corresponds to 8.4±1.7 kpc, between the host and the afterglow position. We discuss the importance of using Chandra for obtaining subarcsecond X-ray localizations of short GRB afterglows to study GRB environments.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: individual: GRB 111117A

Simbad objects: 36

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Number of rows : 36
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 bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
2 GRB 080426 gB 01 45 59.79 +69 28 06.0           ~ 50 0
3 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
4 Fermi bn081024245 gB 01 51 33.80 +61 21 08.2           ~ 75 0
5 QSO B0235+1624 BLL 02 38 38.93010450 +16 36 59.2745528   16.46 15.50 15.92   ~ 1614 2
6 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
7 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
8 GRB 060313 G 04 26 28.4020 -10 50 39.901 20.55 21.03 19.66     ~ 156 0
9 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
10 GRB 091109B gB 07 30 59.90 -54 05 30.6           ~ 57 0
11 Fermi bn081226044 G 08 02 00.4500 -69 01 49.500           ~ 63 0
12 GRB 051227 gB 08 20 58.107 +31 55 32.01           ~ 127 0
13 NAME GRB 060121 HOST Galaxy G 09 09 52.0260 +45 39 45.538       26.6   ~ 127 0
14 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
15 GRB 061217 gB 10 41 39.320 -21 07 22.11           ~ 128 0
16 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
17 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
18 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
19 GRB 090607 gB 12 44 46.70 +44 06 28.4           ~ 40 0
20 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
21 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
22 GRB 050813 gB 16 07 57.190 +11 14 57.80           ~ 147 0
23 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
24 GRB 080919 gB 17 40 53.00 -42 22 29.5           ~ 49 0
25 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 153 1
26 GRB 080503 gB 19 06 28.74 +68 47 35.8           ~ 172 0
27 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 66 0
28 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
29 GRB 080702A gB 20 52 12.21 +72 18 46.7           ~ 47 0
30 Fermi bn090621922 gB 20 53 49.30 +69 02 02.9           ~ 65 0
31 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
32 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
33 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
34 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
35 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
36 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0

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