2020NatAs...4..174B


Query : 2020NatAs...4..174B

2020NatAs...4..174B - Nature Astronomy, 4, 174-179 (2020/February-0)

Gamma-ray bursts as cool synchrotron sources.

BURGESS J.M., BEGUE D., GREINER J., GIANNIOS D., BACELJ A. and BERLATO F.

Abstract (from CDS):

Gamma-ray bursts (GRBs) are the most energetic electromagnetic sources in the Universe, releasing 1042-1047 J (refs. 1,2) in prompt gamma-ray radiation. Fifty years after their discovery, the physical origin of this emission is still unknown. Synchrotron emission has been an early contender3,4, but was criticized because spectral fits of empirical models suggest too hard a slope of the low-energy power law, violating the so-called synchrotron line-of-death5,6, and for its inefficient extraction of energy when the electrons are not fully cooled, reviving models of photospheric emission7-9. Fitting proper synchrotron spectra10 (rather than heuristic functions) and taking electron cooling into account was shown to work for several GRB spectra10-14. Here, we show that idealized synchrotron emission, when properly incorporating time-dependent cooling of the electrons, is capable of fitting ∼95% of all time-resolved spectra of single-peaked GRBs observed by Fermi's Gamma-ray Burst Monitor. Thus, the past exclusion of synchrotron radiation as an emission mechanism derived via the line-of-death was misleading. Our analysis probes the microphysical processes operating within these ultra-relativistic outflows and provides estimates of magnetic field strengths and Lorentz factors of the emitting region directly from spectral fits. The resulting parameter distributions are largely compatible with theoretical spectral15-17 and outflow predictions18. The emission energetics implied by the observed, uncooled electrons remain challenging for all theoretical models.

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Simbad objects: 22

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Number of rows : 22
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 bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 122 0
2 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
3 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
4 GRB 131011A gB 02 10 06.11 -04 24 42.5           ~ 45 0
5 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
6 Fermi bn100728439 gB 02 56 13.44 +00 16 51.6           ~ 142 0
7 Fermi bn090926914 gB 03 05 14.30 -38 59 50.9           ~ 149 1
8 Fermi bn081118876 gB 03 38.4 -43 18           ~ 15 0
9 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
10 Fermi bn100704149 gB 08 54 33.92 -24 12 09.7           ~ 103 0
11 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
12 Fermi bn120811649 gB 13 18 43.82 +62 18 02.8           ~ 113 0
13 GRB 130606B gB 14 34 07.04 -22 06 08.2           ~ 47 0
14 Fermi bn140808038 gB 14 44 53.27 +49 12 52.7           ~ 45 0
15 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
16 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
17 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
18 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
19 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
20 iPTF 14bfu SN* 21 52 30.00 +32 00 52.5           SNIc 80 0
21 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0
22 GRB 130518A gB 23 42 39.79 +47 27 55.2           ~ 86 0

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