2019A&A...629A..69B


Query : 2019A&A...629A..69B

2019A&A...629A..69B - Astronomy and Astrophysics, volume 629A69-69 (2019/9-1)

Is spectral width a reliable measure of GRB emission physics?

BURGESS J.M.

Abstract (from CDS):

The spectral width and sharpness of unfolded, observed gamma-ray burst (GRB) spectra have been presented as a new tool to infer physical properties about GRB emission via spectral fitting of empirical models. Following the tradition of the "line-of-death", the spectral width has been used to rule out synchrotron emission in a majority of GRBs. This claim is investigated via reexamination of previously reported width measures. Then, a sample of peak-flux GRB spectra are fit with an idealized, physical synchrotron model. It is found that many spectra can be adequately fit by this model even when the width measures would reject it. Thus, the results advocate for fitting a physical model to be the sole tool for testing that model. Finally, a smoothly-broken power law is fit to these spectra allowing for the spectral curvature to vary during the fitting process in order to understand why the previous width measures poorly predict the spectra. It is found that the failing of previous width measures is due to a combination of inferring physical parameters from unfolded spectra as well as the presence of multiple widths in the data beyond what the Band function can model.

Abstract Copyright: © J. M. Burgess 2019

Journal keyword(s): gamma-ray burst: general - methods: data analysis - methods: statistical

CDS comments: Table 2 GRBs 130704, 130815 and 160215 not in Simbad.

Simbad objects: 41

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Number of rows : 41
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 bn150201574 gB 00 47 19.84 -37 37 07.8           ~ 30 0
2 GRB 160118A gB 01 10.9 +59 47           ~ 3 0
3 GRB 101014A gB 01 47.8 -51 04           ~ 31 0
4 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
5 GRB 160422A gB 02 48 22.69 -57 52 29.9           ~ 16 0
6 GRB 131028A gB 03 48 +72.2           ~ 14 0
7 Fermi bn140209313 gB 05 25 19.00 +32 29 56.1           ~ 47 0
8 GRB 090820 gB 05 51 +27.1           ~ 44 0
9 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
10 GRB 150213A gB 06 21 -04.8           ~ 15 0
11 Fermi bn080925775 gB 06 24.4 +18 12           ~ 28 0
12 Fermi bn120921877 gB 06 26 -64.8           ~ 7 0
13 GRB 100719A gB 07 29 17 -05 51.4           ~ 14 0
14 GRB 150627A gB 07 49 52.95 -51 29 22.5           ~ 24 0
15 GRB 160530A gB 07 55 53.8 -25 27 50           ~ 14 0
16 Fermi bn100131730 gB 08 01.6 +16 29           ~ 22 0
17 Fermi bn120217808 gB 08 10 +36.8           ~ 12 0
18 GRB 081215A gB 08 22 +54.0           ~ 57 0
19 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
20 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
21 GRB 080817 gB 10 05 09.600 -19 15 36.00           ~ 27 0
22 Fermi bn150824079 gB 11 10 -56.8           ~ 7 0
23 Fermi bn090626189 gB 11 20 -33.5           ~ 54 0
24 Fermi bn160101030 gB 14 38 36.16 -13 48 53.9           ~ 13 0
25 GRB 080906 gB 15 12 13 -80 32.4           ~ 63 0
26 GRB 110301A gB 15 17.4 +29 24           ~ 53 0
27 GRB 090620 gB 15 49.4 +61 09           ~ 29 0
28 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
29 GRB 091003A gB 16 46 04.680 +36 37 31.08           ~ 135 0
30 Fermi bn120102095 gB 18 24 53.89 +24 42 47.1           ~ 42 0
31 GRB 110625A gB 19 06 55.85 +06 45 19.2           ~ 69 0
32 GRB 120707A gB 19 24 -34.4           ~ 21 0
33 Fermi bn110921577 gB 19 36 23.46 +36 19 43.0           ~ 44 0
34 GRB 090809 gB 21 54 43.2 -00 05 02           ~ 90 0
35 Fermi bn090829672 gB 21 56.8 -34 12           ~ 30 0
36 Fermi bn150330828 gB 21 57 +50.0           ~ 22 0
37 GRB 131127A gB 22 10 55.22 +36 36 33.5           ~ 33 0
38 GRB 090131 gB 23 29.2 +21 12           ~ 37 0
39 GRB 100701A gB ~ ~           ~ 4 0
40 GRB 150105A gB ~ ~           ~ 2 0
41 GRB 160521A gB ~ ~           ~ 4 0

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