2023A&A...675A..99P


Query : 2023A&A...675A..99P

2023A&A...675A..99P - Astronomy and Astrophysics, volume 675A99 (2023/7-1)

Hunting for gamma-ray emission from fast radio bursts.

PRINCIPE G., DI VENERE L., NEGRO M., DI LALLA N., OMODEI N., DI TRIA R., MAZZIOTTA M.N. and LONGO F.

Abstract (from CDS):

Context. Fast radio bursts (FRBs) are a recently discovered class of GHz-band, ms-duration, Jansky-level-flux astrophysical transients. Although hundreds of models have been proposed so far for FRB progenitors (the most popular ones involve magnetars), their physical origin and emission mechanism are still a mystery, making them one of the most compelling problems in astrophysics.
Aims. FRBs are caused by astrophysical processes that are not yet understood. Exploring their high-energy counterpart is crucial for constraining their origin and emission mechanism.
Methods. Thanks to more than 13 years of gamma-ray data collected by the Large Area Telescope on board the Fermi Gamma-ray Space Telescope, and to more than 1000 FRB events (from 561 non-repeating and 22 repeating sources), one of the largest samples created thus far, we performed the largest and deepest search for high-energy emission from FRB sources to date (between 100 MeV and 1 TeV). In addition to the analysis involving individual FRB events on different timescales (from a few seconds up to several years), we performed, for the first time, a stacking analysis on the full sample of FRB events as well as a search for triplet photons in coincidence with the radio event.
Results. We do not detect significant emission, reporting the most stringent constraints, on short timescales, for the FRB-like emission from SGR 1935+2154 with Eγ < 1041 erg, corresponding to a factor η < 107 with respect to the emitted radio energy. Similarly, for the stacked signal of steady emission from all repeaters, the obtained upper limit (UL) on the FRBs luminosity (Lγ < 1.6 × 1043 erg s–1) is more than two orders of magnitude lower than those derived from the individual sources. Finally, no individual or triplet photons have been significantly associated with FRB events. We derived the LAT ms-sensitivity to be ∼0.3 ph cm–2 s–1 and constrained the gamma-ray energy $ E_{\gamma, \delta_{\mathrm{T}} = 1\,\mathrm{ms}} \lesssim 10^{47} ({D}_{\mathrm{L}}/150\,\mathrm{Mpc})^2 $ erg, ruling out a gamma-ray-to-radio energy ratio greater than 109 on ms timescales.
Conclusions. The results reported here represent the most stringent UL reported so far on the high-energy emission from FRBs on short and long time scales, as well as on cumulative emission and individual photon searches. While the origin of FRBs is still unclear, our work provides important constraints for FRB modelling, which might shed light on their emission mechanism.

Abstract Copyright: © The Authors 2023

Journal keyword(s): gamma rays: general

VizieR on-line data: <Available at CDS (J/A+A/675/A99): tablec1.dat>

Status at CDS : All or part of tables of objects could be ingested in SIMBAD with priority 2.

Simbad objects: 42

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Number of rows : 42
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 Sculptor Dwarf Galaxy G 01 00 09.4 -33 42 32   9.79 8.6 8.81   ~ 1498 4
2 FRB 010724 rB 01 18 06.0 -72 12 19           ~ 94 1
3 FRB 20180916B rB 01 58 00.750 +65 43 00.30           ~ 457 0
4 FRB 20180924A rB 02 21 50.4000 +37 31 12.000           ~ 10 0
5 4FGL J0221.8+3730 Bz? 02 21 52.6 +37 30 40           ~ 8 0
6 FRB 20191221A rB 02 57 21.600 +79 43 12.00           ~ 34 0
7 NAME FRB 180814.J0422+73 rB 04 22 44.0 +73 39 52           ~ 112 0
8 NAME FRB 181128.J0456+63 rB 04 55 41.0 +63 15 27           ~ 18 0
9 FRB 010305 rB 04 57 19.5000 -52 36 24.668           ~ 7 0
10 FRB 20201124A rB 05 07 57.600 +26 11 24.00           ~ 307 0
11 FRB 010312 rB 05 26 54.90 -64 56 19.2           ~ 20 0
12 FRB 20181119D rB 05 31 58.6980 +33 08 52.588           ~ 933 0
13 FRB 170606 rB 05 34 00.00 +41 45 00.0           ~ 3 0
14 FRB 180324 rB 06 16.0 -34 47           ~ 15 0
15 FRB 180430 rB 06 51.0 -09 57           ~ 10 0
16 M 81 Sy2 09 55 33.1726556496 +69 03 55.062505368   7.89 6.94     ~ 4725 3
17 FRB 20200120E rB 09 57 56.7 +68 49 32           ~ 219 0
18 NAME FRB 181030.J1054+73 rB 10 33 24.0000 +73 47 24.000           ~ 79 0
19 FRB 20180906B rB 12 23 00.0000 +56 25 12.000           ~ 12 0
20 NAME FRB 180908.J1232+74 rB 12 32 48.0 +74 10 21           ~ 23 0
21 NAME FRB 181119.J12+65 rB 12 41 52.0 +65 07 02           ~ 26 0
22 FRB 190523 rB 13 48 15.6 +72 28 11           ~ 109 0
23 FRB 20190303A G 13 51 59.77 +48 06 57.6           ~ 58 0
24 FRB 20190220A rB 15 48 50.4000 +74 09 36.000           ~ 7 0
25 3FGL J1550.3+7409 Bla 15 49 25.3 +74 09 59           ~ 19 0
26 NAME FRB 180814.J1554+74 rB 15 53 02.4000 +74 01 12.000           ~ 12 0
27 FRB 20190520B rB 16 02 04.270 -11 17 17.32           ~ 211 0
28 FRB 20190520A rB 18 14 04.8000 +26 19 12.000           ~ 11 0
29 NAME FRB J1852-08 rB 18 52 05.0 -08 29 35           ~ 54 0
30 FRB 20190221B rB 19 07 04.8000 +27 51 36.000           ~ 7 0
31 NAME Sgr 1935+2154 * 19 34 55.68 +21 53 48.2           ~ 820 1
32 FRB 190611 rB 21 22 58.91 -79 23 51.3           ~ 82 0
33 FRB 180309 rB 21 24 43.80 -33 58 44.5           ~ 27 0
34 PSR J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
35 FRB 190102 rB 21 29 39.76 -79 28 32.5           ~ 83 0
36 FRB 180924 rB 21 44 25.255 -40 54 00.10           ~ 140 0
37 FRB 181112 rB 21 49 23.630 -52 58 15.39           ~ 131 0
38 FRB 20190711A rB 21 57 40.7 -80 21 29           ~ 114 0
39 QSO B2201+1711 BLL 22 03 26.89368237 +17 25 48.2477620     19.50 14.76   ~ 221 1
40 FRB 181017 rB 22 05 54.820 -08 50 34.22           ~ 15 0
41 FRB 171020 rB 22 15.0 -19 40           ~ 54 0
42 FRB 190608 rB 22 16 04.74 -07 53 53.6           ~ 102 0

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