2015ApJ...806...15Z


Query : 2015ApJ...806...15Z

2015ApJ...806...15Z - Astrophys. J., 806, 15 (2015/June-2)

An analysis of Chandra deep follow-up gamma-ray bursts: implications for off-axis jets.

ZHANG B.-B., VAN EERTEN H., BURROWS D.N., RYAN G.S., EVANS P.A., RACUSIN J.L., TROJA E. and MacFADYEN A.

Abstract (from CDS):

We present a sample of 27 gamma-ray bursts (GRBs) with detailed Swift light curves supplemented by late-time Chandra observations. To answer the missing jet-break problem in general, we develop a numerical-simulation-based model that can be directly fit to the data using Monte Carlo methods. Our numerical model takes into account all the factors that can shape a jet break: (i) lateral expansion, (ii) edge effects, and (iii) off-axis effects. Our results provide improved fits to the light curves and constraints on physical parameters. More importantly, our results suggest that off-axis effects are important and must be included in interpretations of GRB jet breaks.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - methods: numerical

Simbad objects: 53

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Number of rows : 53
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 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
2 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
3 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
4 GRB 091117A gB 02 03 46.90 -16 56 38.0           ~ 39 0
5 Fermi bn090113778 gB 02 08 16.00 +33 26 08.4           ~ 92 0
6 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
7 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
8 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
9 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 136 0
10 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
11 GRB 090407 gB 04 35 54.98 -12 40 45.5           ~ 87 0
12 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
13 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
14 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
15 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
16 GRB 110422A gB 07 28 11.21 +75 06 24.0           ~ 113 0
17 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
18 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
19 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
20 GRB 110503A gB 08 51 06.31 +52 12 27.7           ~ 115 0
21 GRB 080307 gB 09 06 30.73 +35 08 19.8           ~ 53 0
22 GRB 061021 gB 09 40 36.120 -21 57 05.40 18.21 19.20 16.82     ~ 160 0
23 GRB 060108 gB 09 48 01.980 +31 55 08.59           ~ 107 0
24 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
25 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
26 GRB 110312A gB 10 29 55.47 -05 15 45.2           ~ 33 0
27 GRB 110709B gB 10 58 37.2 -23 27 18           ~ 92 0
28 Fermi bn120624933 gB 11 23 31.98 +08 55 42.1           ~ 100 0
29 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
30 Fermi bn100615083 gB 11 48 49.25 -19 28 52.2           ~ 133 0
31 GRB 050412 gB 12 04 25.060 -01 12 03.60           ~ 85 0
32 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
33 Fermi bn130420313 gB 13 04 25.49 +59 25 26.8           ~ 112 0
34 GRB 110402A gB 13 09 36.54 +61 15 10.3           ~ 67 0
35 GRB 080319A gB 13 45 19.97 +44 04 49.1           ~ 79 0
36 GRB 080207 gB 13 50 03.02 +07 30 08.0           ~ 114 0
37 GRB 090417B gB 13 58 44.8 +47 00 55           ~ 119 1
38 GRB 120320A gB 14 10 04.300 +08 41 47.26           ~ 34 0
39 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
40 GRB 100628A gB 15 03 53.59 -31 39 50.4           ~ 50 0
41 GRB 120804A G 15 35 47.5100 -28 46 56.110           ~ 99 0
42 GRB 090404 gB 15 56 55.80 +35 31 03.4           ~ 79 0
43 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
44 Fermi bn100413732 gB 17 44 53.22 +15 50 02.4           ~ 62 0
45 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
46 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 66 0
47 GRB 110915A gB 20 43 17.87 -00 43 23.2           ~ 44 0
48 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
49 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1
50 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
51 GRB 111215A gB 23 18 13.33 +32 29 38.5           ~ 68 0
52 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0
53 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 194 1

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