2024A&A...689A.286P


Query : 2024A&A...689A.286P

2024A&A...689A.286P - Astronomy and Astrophysics, volume 689A286 (2024/9-1)

Constraints on fast radio burst emission in the aftermath of gamma-ray bursts.

PATRICELLI B., BERNARDINI M.G. and FERRO M.

Abstract (from CDS):

Context. Fast radio bursts (FRBs) are highly energetic radio transients with a duration of some milliseconds. Their physical origin is still unknown. Many models consider magnetars as possible FRB sources, which is supported by the observational association of FRBs with the galactic magnetar SGR 1935+2154. Magnetars are also thought to be the source of the power of a fraction of gamma-ray bursts (GRBs), which means that the two extreme phenomena might have a common progenitor.
Aims. We placed constrains on this hypothesis by searching for possible associations between GRBs and FRBs with currently available catalogues and by estimating whether an association can be ruled out based on the lack of a coincident detection.
Methods. We cross-matched all the Neil Gehrels Swift Observatory (Swift) GRBs detected so far with all the well-localised FRBs reported in the FRBSTATS catalogue, and we looked for FRB-GRB associations considering both spatial and temporal constraints. We also simulated a synthetic population of FRBs associated with Swift GRBs to estimate how likely a joint detection with current and future radio facilities is.
Results. We recovered two low-significance possible associations that were reported before from a match of the catalogues: GRB 110715A/FRB 20171209A and GRB 060502B/FRB 20190309A. However, our study shows that based on the absence of any unambiguous association so far between Swift GRBs and FRBs, we cannot exclude that the two populations are connected because of the characteristics of current GRB and FRB detectors.
Conclusions. Currently available observational data are not sufficient to clearly exclude or confirm whether GRBs and FRBs are physically associated. In the next decade, the probability of detecting joint GRB-FRB events will be higher with new generations of GRB and FRB detectors, if any: future observations will therefore be key to placing more stringent constraints on the hypothesis that FRBs and GRBs have common progenitors.

Abstract Copyright: © The Authors 2024

Journal keyword(s): gamma-ray burst: general - stars: magnetars

Simbad objects: 51

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Number of rows : 51
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 FRB 20190316A rB 00 20 55.2000 +20 30 36.000           ~ 6 0
2 GRB 060912A gB 00 21 08.11 +20 58 18.9           ~ 116 1
3 FRB 20180916B rB 01 58 00.750 +65 43 00.30           ~ 457 0
4 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 650 1
5 FRB 20201124A rB 05 07 57.600 +26 11 24.00           ~ 307 0
6 FRB 20181119D rB 05 31 58.6980 +33 08 52.588           ~ 933 0
7 GRB 110801A gB 05 57 44.87 +80 57 21.1           ~ 90 0
8 FRB 20190208B rB 06 04 00.0000 +80 52 48.000           ~ 7 0
9 GRB 090904A gB 06 43 32.35 +50 12 10.8           ~ 43 0
10 FRB 20190317B rB 06 44 02.4000 +49 43 48.000           ~ 5 0
11 FRB 20221128A rB 07 30.0 -42 30           ~ 6 0
12 FRB 20190224C rB 08 16 12.0000 +19 46 48.000           ~ 9 0
13 GRB 140211A gB 08 16 53.59 +20 14 35.5           ~ 17 0
14 FRB 20190409B rB 08 26 36.0000 +63 28 12.000           ~ 12 0
15 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
16 GRB 060515 gB 08 29 09.490 +73 34 02.82           ~ 37 0
17 FRB 20181213A rB 08 30 38.4000 +73 52 12.000           ~ 9 0
18 GRB 151006A gB 09 49 42.18 +70 30 10.5           ~ 42 0
19 FRB 20190612A rB 09 52 38.4000 +70 25 12.000           ~ 10 0
20 FRB 20200120E rB 09 57 56.7 +68 49 32           ~ 219 0
21 FRB 20180907E rB 11 11 31.2000 +47 05 24.000           ~ 10 0
22 GRB 160705B gB 11 12 26.25 +46 41 59.6           ~ 17 0
23 FRB 20190303C rB 11 32 57.6000 +26 19 12.000           ~ 6 0
24 GRB 030226 gB 11 33 04.9 +25 53 56           ~ 212 0
25 FRB 20181214C rB 11 43 43.2000 +60 01 12.000           ~ 10 0
26 GRB 060319 gB 11 45 33.050 +60 00 39.61 20.10         ~ 73 0
27 FRB 20190425B rB 14 00 28.8000 +88 36 00.000           ~ 12 0
28 FRB 20190609B rB 14 01 57.6000 +88 21 00.000           ~ 10 0
29 Fermi bn090813174 gB 15 00 15.60 +88 34 15.8           ~ 62 0
30 FRB 20181221A rB 15 22 19.2000 +25 51 36.000           ~ 17 0
31 GRB 100526A gB 15 23 04.60 +25 37 55.9           ~ 35 0
32 FRB 171209 rB 15 50 25.0 -46 10 20           ~ 27 0
33 GRB 110715A gB 15 50 44.090 -46 14 06.53           ~ 120 0
34 FRB 20181017B rB 15 51 02.4000 +78 30 00.000           ~ 13 0
35 GRB 060510B gB 15 56 29.200 +78 34 12.00           ~ 155 0
36 GRB 100316A gB 16 47 55.56 +71 49 40.0           ~ 34 0
37 FRB 20190409C rB 16 50 24.0000 +71 37 12.000           ~ 5 0
38 FRB 20181013A rB 17 31 19.2000 +38 24 36.000           ~ 6 0
39 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 153 1
40 FRB 20190309A rB 18 35 50.4000 +52 24 36.000           ~ 8 0
41 FRB 20190429A rB 18 44 21.6000 +59 25 12.000           ~ 4 0
42 Fermi bn140713780 gB 18 44 25.13 +59 38 00.8           ~ 40 0
43 NAME Sgr 1935+2154 * 19 34 55.68 +21 53 48.2           ~ 820 1
44 GRB 120213A gB 20 04 02.83 +65 24 40.6           ~ 37 0
45 FRB 20180918A rB 20 05 04.8000 +64 57 36.000           ~ 7 0
46 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
47 FRB 20190519H rB 22 51 57.6000 +87 22 12.000           ~ 10 0
48 FRB 20190609A rB 23 01 12.0000 +87 56 24.000           ~ 16 0
49 GRB 110223A gB 23 03 22.68 +87 33 28.5           ~ 29 0
50 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 194 1
51 FRB 20190608A rB 23 56 55.2000 +19 10 12.000           ~ 10 0

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