2019A&A...628A..59O


Query : 2019A&A...628A..59O

2019A&A...628A..59O - Astronomy and Astrophysics, volume 628A, 59-59 (2019/8-1)

Prompt optical emission as a signature of synchrotron radiation in gamma-ray bursts.

OGANESYAN G., NAVA L., GHIRLANDA G., MELANDRI A. and CELOTTI A.

Abstract (from CDS):

Information on the spectral shape of prompt emission in gamma-ray bursts (GRB) is mostly available only at energies ≥10keV, where the main instruments for GRB detection are sensitive. The origin of this emission is still very uncertain because of the apparent inconsistency with synchrotron radiation, which is the most obvious candidate, and the resulting need for considering less straightforward scenarios. The inclusion of data down to soft X-rays (∼0.5keV), which are available only in a small fraction of GRBs, has firmly established the common presence of a spectral break in the low-energy part of prompt spectra, and even more importantly, the consistency of the overall spectral shape with synchrotron radiation in the moderately fast-cooling regime, the low-energy break being identified with the cooling frequency. In this work we further extend the range of investigation down to the optical band. In particular, we test the synchrotron interpretation by directly fitting a theoretically derived synchrotron spectrum and making use of optical to gamma-ray data. Secondly, we test an alternative model that considers the presence of a black-body component at ∼keV energies, in addition to a non-thermal component that is responsible for the emission at the spectral peak (100keV-1MeV). We find that synchrotron radiation provides a good description of the broadband data, while models composed of a thermal and a non-thermal component require the introduction of a low-energy break in the non-thermal component in order to be consistent with optical observations. Motivated by the good quality of the synchrotron fits, we explore the physical parameter space of the emitting region. In a basic prompt emission scenario we find quite contrived solutions for the magnetic field strength (5G<B'<40G) and for the location of the region where the radiation is produced (Rγ>1016cm). We discuss which assumptions of the basic model would need to be relaxed in order to achieve a more natural parameter space.

Abstract Copyright: © ESO 2019

Journal keyword(s): gamma-ray burst: general - radiation mechanisms: general - radiation mechanisms: non-thermal

Simbad objects: 23

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Number of rows : 23
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 199 0
2 GRB 070616 gB 02 08 36.430 +56 56 44.91           ~ 75 0
3 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 165 0
4 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 118 0
5 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 326 0
6 Fermi bn121217313 gB 10 14 50.32 -62 21 03.3           ~ 60 0
7 GRB 111123A gB 10 19 23.17 -20 38 41.9           ~ 68 0
8 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 185 0
9 GRB 130907A gB 14 23 34.03 +45 36 27.1           ~ 100 0
10 GRB 130606B gB 14 34 07.04 -22 06 08.2           ~ 38 0
11 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 218 0
12 GRB 060510B gB 15 56 29.200 +78 34 12.00           ~ 143 0
13 Fermi bn110102788 gB 16 23 31.41 +07 36 49.8           ~ 57 0
14 GRB 090715B gB 16 45 21.59 +44 50 20.1           ~ 124 0
15 GRB 111103B gB 17 42 46.37 +01 36 36.3           ~ 39 0
16 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 197 0
17 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 102 0
18 GRB 130514A gB 19 45 07.33 -07 58 41.1           ~ 62 0
19 Fermi bn121123421 gB 20 29 16.30 -11 51 35.6           ~ 52 0
20 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 171 0
21 Fermi bn140108721 gB 21 40 26.77 +58 44 41.4           ~ 52 0
22 GRB 151021A gB 22 30 34.43 -33 11 50.4           ~ 54 0
23 Fermi bn110119931 gB 23 14 21 +05 58.9           ~ 42 0

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