2020ApJ...895...40G


Query : 2020ApJ...895...40G

2020ApJ...895...40G - Astrophys. J., 895, 40-40 (2020/May-3)

Evaluation of automated Fermi GBM localizations of Gamma-ray bursts.

GOLDSTEIN A., FLETCHER C., VERES P., BRIGGS M.S., CLEVELAND W.H., GIBBY M.H., HUI C.M., BISSALDI E., BURNS E., HAMBURG R., VON KIENLIN A., KOCEVSKI D., MAILYAN B., MALACARIA C., PACIESAS W.S., ROBERTS O.J. and WILSON-HODGE C.A.

Abstract (from CDS):

The capability of the Fermi Gamma-ray Burst Monitor (GBM) to localize gamma-ray bursts (GRBs) is evaluated for two different automated algorithms: the GBM Team's RoboBA algorithm and the independently developed BALROG algorithm. Through a systematic study utilizing over 500 GRBs with known locations from instruments like Swift and the Fermi Large Area Telescope, we directly compare the effectiveness of, and accurately estimate the systematic uncertainty for, both algorithms. We show that simple adjustments to the GBM Team's RoboBA, in operation since early 2016, yield significant improvement in the systematic uncertainty, removing the long tail identified in the systematic, and improve the overall accuracy. The systematic uncertainty for the updated RoboBA localizations is 1.°8 for 52% of GRBs and 4.°1 for the remaining 48%. Both from public reporting by BALROG and our systematic study, we find the systematic uncertainty of 1°-2° quoted in circulars for bright GRBs is an underestimate of the true magnitude of the systematic, which we find to be 2.°7 for 74% of GRBs and 33° for the remaining 26%. We show that, once the systematic uncertainty is considered, the RoboBA 90% localization confidence regions can be more than an order of magnitude smaller in area than those produced by BALROG.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Gamma-ray bursts - Astronomy data analysis

Simbad objects: 26

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Number of rows : 26
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 190531B gB 01 37 11.09 -41 57 30.3           ~ 18 0
2 GRB 190331A gB 01 54 17.40 +27 38 06.8           ~ 9 0
3 SN 2019oyw SN* 02 58 10.510 -08 57 27.20           ~ 218 0
4 GRB 190324A gB 03 18 27.77 -47 12 54.1           ~ 35 0
5 GRB 190606A gB 05 06.2 -00 41           ~ 12 0
6 GRB 190512A gB 05 29 36.50 -07 34 56.1           ~ 9 0
7 GRB 190515A gB 06 35 23.73 +52 19 00.4           ~ 14 0
8 GRB 190519A gB 07 39 04.24 -38 48 19.6           ~ 18 0
9 GRB 190320A gB 07 51 23.66 -45 53 16.1           ~ 12 0
10 GRB 190530A gB 08 02 07.73 +35 28 47.7           ~ 64 0
11 GRB 190511A gB 08 25 46.61 -20 15 34.1           ~ 20 0
12 GRB 190727B gB 08 25 59.90 -13 16 18.9           ~ 18 0
13 Fermi bn161228553 gB 08 37 +43.7           ~ 7 0
14 GRB 170522A gB 09 17 21.6 +25 40 12           ~ 19 0
15 GRB 190422A gB 12 08 08.46 -60 13 27.6           ~ 16 0
16 GRB 190613A gB 12 10 07.13 +67 14 07.0           ~ 26 0
17 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
18 GRB 190824A gB 14 21 13.19 -41 53 37.6           ~ 14 0
19 GRB 190719C gB 16 00 49.50 +13 00 00.6           ~ 43 0
20 GRB 190821A gB 16 40 13.17 -34 00 25.1           ~ 14 0
21 GRB 190828B gB 16 47 19.49 +27 16 51.2           ~ 18 0
22 GRB 190427A gB 18 40 52.00 +40 18 15.6           ~ 25 0
23 GRB 190613B gB 20 21 43.67 -04 38 50.4           ~ 31 0
24 GRB 190731A gB 22 38 52.76 -76 34 37.9           ~ 18 0
25 GRB 190415A gB ~ ~           ~ 6 0
26 GRB 190805B gB ~ ~           ~ 10 0

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