2020A&A...644A.124K


Query : 2020A&A...644A.124K

2020A&A...644A.124K - Astronomy and Astrophysics, volume 644A124-124 (2020/12-1)

The POLAR gamma-ray burst polarization catalog.

KOLE M., DE ANGELIS N., BERLATO F., BURGESS J.M., GAUVIN N., GREINER J., HAJDAS W., LI H.C., LI Z.H., POLLO A., PRODUIT N., RYBKA D., SONG L.M., SUN J.C., SZABELSKI J., TYMIENIECKA T., WANG Y.H., WU B.B., WU X., XIONG S.L., ZHANG S.N. and ZHANG Y.J.

Abstract (from CDS):


Context. Despite over 50 years of research, many open questions remain about the origin and nature of gamma-ray bursts (GRBs). Linear polarization measurements of the prompt emission of these extreme phenomena have long been thought to be key to answering a range of these questions. The POLAR detector was designed to produce the first set of detailed and reliable linear polarization measurements in the 50 - 500 keV energy range. During late 2016 and early 2017, POLAR detected a total of 55 GRBs. The analysis results of 5 of these GRBs have been reported, and were found to be consistent with a low or unpolarized flux. However, previous reports by other collaborations found high levels of linear polarization, including some as high as 90%.
Aims. We study the linear polarization for the 14 GRBs observed by POLAR for which statistically robust inferences are possible. Additionally, time-resolved polarization studies are performed on GRBs with sufficient apparent flux.
Methods. A publicly available polarization analysis tool, developed within the Multi-Mission Maximum Likelihood framework (3ML), was used to produce statistically robust results. The method allows spectral and polarimetric data from POLAR to be combined with spectral data from the Fermi Gamma-ray Burst Monitor (Fermi-GBM) and the Neil Gehrels Swift Observatory to jointly model the spectral and polarimetric parameters.
Results. The time-integrated analysis finds all results to be compatible with low or zero polarization with the caveat that, when time-resolved analysis is possible within individual pulses, we observe moderate linear polarization with a rapidly changing polarization angle. Therefore, time-integrated polarization results, while pointing to lower polarization, are potentially an artifact of summing over the changing polarization signal and thus washing out the true moderate polarization. We therefore caution against overinterpretation of any time-integrated results inferred herein and encourage the community to wait for more detailed polarization measurements from forthcoming missions such as POLAR-2 and LEAP.

Abstract Copyright: © ESO 2020

Journal keyword(s): polarization - methods: data analysis - instrumentation: polarimeters - catalogs - gamma-ray burst: general

Simbad objects: 45

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Number of rows : 45
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 bn170121067 gB 00 12 -75.6           ~ 7 0
2 Fermi bn170114917 gB 00 48 -12.6           ~ 36 0
3 Fermi bn161212652 gB 01 40 +68.2           ~ 5 0
4 Fermi bn170305256 gB 02 35 +12.1           ~ 15 0
5 GRB 170219A gB 03 39 +50.1           ~ 14 0
6 Fermi bn170101116 gB 04 42 -01.6           ~ 10 0
7 Fermi bn161229878 gB 05 24 +06.3           ~ 10 0
8 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
9 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
10 GRB 170317A gB 06 12 20 +50 30.0           ~ 30 0
11 Fermi bn161228032 gB 07 43 +25.8           ~ 3 0
12 Fermi bn170109137 gB 07 49 -10.9           ~ 5 0
13 Fermi bn170325331 gB 08 29 55.92 +20 31 33.6           ~ 17 0
14 Fermi bn161228553 gB 08 37 +43.7           ~ 7 0
15 GRB 170105A gB 08 39 00 +27 54.2           ~ 14 0
16 Fermi bn170306588 gB 10 18 +51.6           ~ 10 0
17 GRB 160821A gB 11 25 01 +42 20.7           ~ 71 0
18 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
19 Fermi bn170206453 gB 14 11 09.60 +14 28 48.0           ~ 28 0
20 Fermi bn161217128 gB 14 26 +52.0           ~ 4 0
21 Fermi bn170210116 gB 15 04 -65.1           ~ 16 0
22 Fermi bn170315582 gB 15 22 +60.3           ~ 3 0
23 GRB 161218A gB 16 21 00 -04 06.8           ~ 20 0
24 Fermi bn170120471 gB 17 31 +12.6           ~ 3 0
25 GRB 170101A gB 17 48 21 +11 38.5           ~ 23 0
26 Fermi bn170130302 gB 18 04 -29.1           ~ 4 0
27 Fermi bn161210524 gB 18 52 +63.0           ~ 6 0
28 GRB 100826A gB 18 56 -23.2           ~ 79 0
29 Fermi bn170208553 gB 18 58 -00.1           ~ 5 0
30 Fermi bn161207224 gB 19 39 -09.9           ~ 4 0
31 Fermi bn170207906 gB 21 03 +55.7           ~ 15 0
32 Fermi bn161129300 gB 21 04 54.66 +32 08 05.5           ~ 65 0
33 Fermi bn161205561 gB 21 16 +47.7           ~ 3 0
34 Fermi bn161230511 gB 21 36 -09.0           ~ 3 0
35 GRB 170127C gB 22 37 -63.9           ~ 39 0
36 Fermi bn170131969 gB 22 45 47 +64 00.4           ~ 11 0
37 Fermi bn170228773 gB 23 44 +15.7           ~ 5 0
38 Fermi bn161228405 gB 23 54 -24.6           ~ 3 0
39 Fermi bn161218356 gB 23 54 -16.9           ~ 21 0
40 GRB 170309A gB ~ ~           ~ 2 0
41 GRB 161217C gB ~ ~           ~ 6 0
42 GRB 170206C gB ~ ~           ~ 2 0
43 GRB 161203A gB ~ ~           ~ 10 0
44 GRB 161207A gB ~ ~           ~ 3 0
45 GRB 170320A gB ~ ~           ~ 8 0

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