2024A&A...685A.166R


Query : 2024A&A...685A.166R

2024A&A...685A.166R - Astronomy and Astrophysics, volume 685A166 (2024/5-1)

Insights into the physics of gamma-ray bursts from the high-energy extension of their prompt emission spectra.

RAVASIO M.E., GHIRLANDA G. and GHISELLINI G.

Abstract (from CDS):

The study of the high-energy part (MeV-GeV) of the spectrum of gamma-ray bursts (GRBs) can play a crucial role in investigating the physics of prompt emission, but it is often hampered by low statistics and the paucity of GeV observations. In this work, we analyze the prompt emission spectra of the 22 brightest GRBs which have been simultaneously observed by Fermi/GBM and Fermi/LAT, spanning six orders of magnitude in energy. The high-energy photon spectra can be modeled with a power-law N(E)∝E^-β^ possibly featuring an exponential cutoff. We find that, with the inclusion of the LAT data, the spectral index β is softer than what is typically inferred from the analysis of Fermi/GBM data alone. Under the assumption that the emission is synchrotron, we derived a median value of the index p ∼ 2.79 of the power-law energy distribution of accelerated particles (N(γ)∝γ^-p^). In nine out of 22 GRB spectra, we find a significant presence of an exponential cutoff at high energy, ranging between 14 and 298 MeV. By interpreting the observed cutoff as a sign of pair-production opacity, we estimate the jet bulk Lorentz factor Γ, finding values in the range 130-330. These values are consistent with those inferred from the afterglow light curve onset time. Finally, by combining the information from the high-energy prompt emission spectrum with the afterglow light curve, we exploited a promising method to derive the distance R from the central engine where the prompt emission occurs. The distances (R > 10^13 - 15^ cm) inferred for the only two GRBs in our sample that are suitable for the application of this method, which have only lower limits on their cutoff energies, suggest large emitting regions, although they are still compatible with the standard model. Larger samples of GRBs with measured cutoff energies and afterglow deceleration time will allow for more informative values to be derived. These results highlight the importance of including high-energy data, when available, in the study of prompt spectra and their role in addressing the current challenges of the GRB standard model.

Abstract Copyright: © The Authors 2024

Journal keyword(s): acceleration of particles - radiation mechanisms: non-thermal - relativistic processes - gamma-ray burst: general

Simbad objects: 30

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Number of rows : 30
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 180720A gB 00 02 06.70 -02 55 01.2           ~ 11 0
2 GRB 180720B gB 00 02 06.99 -02 55 07.8           ~ 215 0
3 GRB 220101A gB 00 05 24.89 +31 46 07.7           ~ 85 0
4 Fermi bn180113116 gB 01 08 +63.3           ~ 16 0
5 GRB 150202A gB 02 36 54.54 -33 08 53.2           ~ 17 0
6 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
7 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
8 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
9 GRB 151006A gB 09 49 42.18 +70 30 10.5           ~ 42 0
10 GRB 131108A gB 10 26 00.480 +09 39 44.05           ~ 96 0
11 Fermi bn160905471 gB 10 48 59.06 -50 48 03.9           ~ 34 0
12 GRB 160821A gB 11 25 01 +42 20.7           ~ 71 0
13 GRB 160625A gB 11 47 39.82 -65 08 41.1           ~ 25 0
14 Fermi bn110131780 gB 12 15 +72.9           ~ 8 0
15 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
16 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
17 Fermi bn150902733 gB 14 19 54.18 -69 21 09.9           ~ 30 0
18 GRB 160910A gB 14 45 46.04 +39 04 01.3           ~ 45 0
19 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
20 GRB 170214A gB 17 05 21.94 -01 53 14.9           ~ 54 0
21 GRB 130504A gB 18 09 49.49 -16 18 48.6           ~ 26 0
22 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
23 GRB 100826A gB 18 56 -23.2           ~ 79 0
24 Fermi bn100116897 gB 20 20 +14.4           ~ 42 0
25 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
26 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
27 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
28 GRB 110721A gB 22 10 -38.6           ~ 155 0
29 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 177 0
30 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0

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