2022MNRAS.516.1584S


Query : 2022MNRAS.516.1584S

2022MNRAS.516.1584S - Mon. Not. R. Astron. Soc., 516, 1584-1600 (2022/October-3)

Polarimetry and photometry of gamma-ray bursts afterglows with RINGO3.

SHRESTHA M., STEELE I.A., KOBAYASHI S., SMITH R.J., GUIDORZI C., JORDANA-MITJANS N., JERMAK H., ARNOLD D., MUNDELL C.G. and GOMBOC A.

Abstract (from CDS):

We present photometric and polarimetric measurements of gamma-ray burst (GRB) optical afterglows observed by the RINGO3 imaging polarimeter over its ∼7 yr lifetime mounted on the Liverpool Telescope. During this time, RINGO3 responded to 67 GRB alerts. Of these, 28 had optical afterglows and a further ten were sufficiently bright for photometric and polarimetric analysis (R ⪅ 17). We present high quality multicolour light curves of ten sources: GRB 130606A, GRB 130610A, GRB 130612A, GRB 140430A, GRB 141220A, GRB 151215A, GRB 180325A, GRB 180618A, GRB 190114C, and GRB 191016A and polarimetry for seven of these (excluding GRB 130606A, GRB 130610A, and GRB 130612A, which were observed before the polarimetry mode was fully commissioned). Eight of these ten GRBs are classical long GRBs, one sits at the short-long duration interface with a T90 ∼ 4 s and one is a classical short, hard burst with extended emission. We detect polarization for GRB 190114C and GRB 191016A. While detailed analyses of several of these GRBs have been published previously, here we present a uniform re-reduction and analysis of the whole sample and investigation of the population in a broad context relative to the current literature. We use survival analysis to fully include the polarization upper limits in comparison with other GRB properties, such as temporal decay rate, isotropic energy, and redshift. We find no clear correlation between polarization properties and wider sample properties and conclude that larger samples of early time polarimetry of GRB afterglows are required to fully understand GRB magnetic fields.

Abstract Copyright: © The Author(s) 2022. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): magnetic fields - techniques: photometric - techniques: polarimetric - gamma-ray bursts

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 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
2 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
3 GRB 191016A gB 02 01 04.67 +24 30 35.3           ~ 31 0
4 GRB 180704A gB 02 10 38.50 +69 57 50.4           ~ 13 0
5 GRB 171020A gB 02 36 59.62 +15 12 14.6           ~ 28 0
6 SWIFT J0243.6+6124 HXB 02 43 40.4252869512 +61 26 03.757456824   13.71 12.84 12.57   O9.5Ve 208 0
7 GRB 141026A gB 02 56 20.29 +26 55 42.4           ~ 60 0
8 GRB 191011A gB 02 58 54.70 -27 50 43.4           ~ 38 0
9 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
10 GRB 151118A gB 03 48 41.16 +65 54 06.0           ~ 22 0
11 Fermi bn130216927 gB 04 31 36.0 +14 39 53           ~ 36 0
12 GRB 151215A gB 06 14 20.20 +35 30 58.3           ~ 47 0
13 GRB 140430A gB 06 51 44.58 +23 01 25.5           ~ 81 0
14 Fermi bn170208940 gB 08 30 -10.4           ~ 28 0
15 Fermi bn161022114 gB 08 36 00.34 +54 20 53.9           ~ 20 0
16 GRB 130408A gB 08 57 37.30 -32 21 38.9           ~ 98 0
17 Fermi bn141225959 gB 09 15 06.77 +33 47 30.9           ~ 64 0
18 GRB 150317A gB 09 15 56.32 +55 27 56.6           ~ 20 0
19 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
20 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 85 0
21 GRB 160705B gB 11 12 26.25 +46 41 59.6           ~ 17 0
22 Fermi bn180618030 G 11 19 45.8010 +73 50 15.030           ~ 38 0
23 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
24 GRB 150302A gB 11 42 07.44 +36 48 39.6           ~ 24 0
25 Fermi bn160316573 gB 11 52 +60.8           ~ 3 0
26 GRB 160313A gB 12 15 11.19 +57 17 01.0           ~ 22 0
27 Fermi bn141220252 gB 13 00 15.70 +32 08 47.2           ~ 81 0
28 GRB 180512A gB 13 27 45.12 +21 24 12.4           ~ 18 0
29 GRB 160119A gB 14 07 41.27 +20 27 39.3           ~ 26 0
30 Fermi bn130610133 gB 14 57 40.91 +28 12 25.8           ~ 89 0
31 Fermi bn160714097 gB 15 38 +63.8           ~ 22 0
32 Fermi bn170728961 G 15 51 55.5290 +70 07 22.038           ~ 54 0
33 GRB 120327A gB 16 27 27.49 -29 24 53.8           ~ 116 0
34 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
35 GRB 140516A gB 16 51 57.40 +39 57 46.3           ~ 38 0
36 Fermi bn130612141 gB 17 19 10.63 +16 43 11.8           ~ 89 0
37 GRB 180720C gB 17 42 32.63 -26 37 45.1           ~ 15 0
38 Fermi bn150831930 gB 18 04 09.35 -27 15 29.5           ~ 17 0
39 GRB 130504A gB 18 09 49.49 -16 18 48.6           ~ 26 0
40 GRB 120311A gB 18 12 22.160 +14 17 46.30           ~ 33 0
41 GRB 180904A gB 18 16 59.94 +46 37 46.9           ~ 20 0
42 Fermi bn150309958 gB 18 28 24.81 +86 25 43.6           ~ 30 0
43 GRB 171115A gB 18 33 33.16 +09 07 29.5           ~ 11 0
44 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
45 GRB 190427A gB 18 40 52.00 +40 18 15.6           ~ 25 0
46 GRB 110726A gB 19 06 52.21 +56 04 16.4           ~ 55 0
47 GRB 150428B gB 19 30 33.46 +04 07 31.8           ~ 23 0
48 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 113 0
49 GRB 100805A gB 19 59 30.51 +52 37 40.1           ~ 55 0
50 Fermi bn140709051 gB 20 18 38.96 +51 13 29.9           ~ 43 0
51 GRB 131030A gB 23 00 16.14 -05 22 05.2           ~ 126 0
52 GRB 161214A gB ~ ~           ~ 8 0
53 GRB 160401A gB ~ ~           ~ 10 0

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