2022ApJ...940..169D


Query : 2022ApJ...940..169D

2022ApJ...940..169D - Astrophys. J., 940, 169 (2022/December-1)

The Closure Relations in Optical Afterglow of Gamma-Ray Bursts.

DAINOTTI M.G., LEVINE D., FRAIJA N., WARREN D. and SOURAV S.

Abstract (from CDS):

Gamma-ray bursts (GRBs) are extremely high-energy events that can be observed at very high redshift. In addition to γ rays, they can emit in X-ray, optical, and sometimes radio wavelengths. Here, following the approach in Srinivasaragavan et al.; Dainotti et al.; and Dainotti et al., we consider 82 GRBs from Dainotti et al. that have been observed in optical wavelengths and fitted with a broken power law. We consider the relations between the spectral and temporal indices (closure relations; CRs) according to the synchrotron forward-shock model evolving in the constant-density interstellar medium (ISM; k = 0) and the stellar wind environment (k = 2) in both slow- and fast-cooling regimes, where the density profile is defined as n ∝ r–k. We find the $\nu \gt \max \{{\nu }_{{\rm{c}}},{\nu }_{{\rm{m}}}\}$ regime is most favored, where νc and νm are the cooling and characteristic frequencies, respectively. Finally, we test the 2D Dainotti correlation between the rest-frame end time of the plateau and the luminosity at that time on GRBs that fulfill the most-favored CRs. When we compare the intrinsic scatter σint of those 2D correlations to the scatter presented in Dainotti et al., we see the scatters of our correlations generally agree with the previous values within 1σ, both before and after correction for selection bias. This new information has helped us to pinpoint subsamples of GRBs with features that could drive the GRB emission mechanism, and eventually allow for GRBs to be used as standard candles.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts

Simbad objects: 89

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Number of rows : 89
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 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 220 0
2 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
3 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
4 GRB 060708 gB 00 31 13.850 -33 45 32.40 19.07 19.79 17.37     ~ 109 0
5 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
6 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
7 GRB 050824 gB 00 48 56.100 +22 36 32.00 19.66 21.03 20.46 23.70   ~ 184 0
8 GRB 041006 gB 00 54 50.17 +01 14 07.0           ~ 202 2
9 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
10 GRB 040924 gB 02 06 22.52 +16 08 48.8           ~ 169 1
11 GRB 170714A gB 02 17 17 +01 58.0           ~ 50 0
12 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
13 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
14 GRB 140801A gB 02 56 16.50 +30 56 16.8           ~ 55 0
15 GRB 191011A gB 02 58 54.70 -27 50 43.4           ~ 38 0
16 GRB 140907A gB 03 12 34.98 +46 36 17.2           ~ 81 0
17 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
18 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
19 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
20 Fermi bn120907017 gB 04 58 59.99 -09 18 53.7           ~ 89 0
21 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
22 GRB 160131A gB 05 12 40.31 -07 02 59.4           ~ 86 0
23 GRB 061126 gB 05 46 24.460 +64 12 38.49 18.62 18.79 19.20     ~ 182 1
24 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
25 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
26 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
27 GRB 140430A gB 06 51 44.58 +23 01 25.5           ~ 81 0
28 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
29 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 138 0
30 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
31 Fermi bn180205184 gB 08 27 16.72 +11 32 32.6           ~ 60 0
32 GRB 110503A gB 08 51 06.31 +52 12 27.7           ~ 115 0
33 GRB 050502B gB 09 30 10.024 +16 59 48.07           ~ 169 0
34 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
35 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
36 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 85 0
37 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 145 0
38 GRB 100513A gB 11 18 26.83 +03 37 40.8           ~ 74 0
39 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
40 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
41 GRB 080603B gB 11 46 07.46 +68 03 38.5           ~ 153 0
42 GRB 030328 gB 12 10 48.4 -09 20 51           ~ 148 0
43 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
44 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
45 GRB 070810A gB 12 39 51.18 +10 45 02.8           ~ 80 0
46 GRB 160227A gB 12 59 13.71 +78 40 45.1           ~ 69 0
47 GRB 060512 gB 13 03 05.810 +41 11 27.21 19.12 19.63 17.20     ~ 142 0
48 Fermi bn140423356 gB 13 09 06.20 +49 50 18.3           ~ 114 0
49 Fermi bn141221338 gB 13 13 09.02 +08 12 18.3           ~ 76 0
50 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 149 0
51 GRB 050502A gB 13 29 46.250 +42 40 27.50           ~ 65 0
52 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
53 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 164 0
54 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
55 SN 2013dx SN* 14 29 14.77 +15 46 26.6           ~ 178 0
56 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
57 Fermi bn160804065 gB 14 46 31.20 +09 59 56.1           ~ 79 0
58 GRB 010222 G 14 52 12.5 +43 01 06           ~ 364 1
59 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
60 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
61 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
62 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 177 0
63 GRB 120404A gB 15 40 02.29 +12 53 06.3           ~ 104 0
64 GRB 110715A gB 15 50 44.090 -46 14 06.53           ~ 120 0
65 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
66 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
67 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
68 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
69 GRB 201020A gB 17 24 54.73 +31 25 41.7           ~ 30 0
70 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
71 GRB 210210A gB 17 31 04.90 +14 39 45.1           ~ 30 0
72 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
73 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 103 0
74 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
75 GRB 080603A gB 18 37 37.95 +62 44 39.6           ~ 89 0
76 GRB 110726A gB 19 06 52.21 +56 04 16.4           ~ 55 0
77 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 163 0
78 GRB 071003A gB 20 07 25 +10 56.9           ~ 7 0
79 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
80 GRB 190919B gB 20 47 30.62 -44 41 43.3           ~ 14 0
81 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
82 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
83 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
84 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
85 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
86 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
87 Fermi bn091024380 gB 22 37 +56.9           ~ 151 0
88 Fermi bn090927422 gB 22 55 53.41 -70 58 49.3           ~ 112 0
89 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 223 0

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