2019MNRAS.484.1912R


Query : 2019MNRAS.484.1912R

2019MNRAS.484.1912R - Mon. Not. R. Astron. Soc., 484, 1912-1925 (2019/April-1)

On the α-intensity correlation in gamma-ray bursts: subphotospheric heating with varying entropy.

RYDE F., YU H.-F., DERELI-BEGUE H., LUNDMAN C., PE'ER A. and LI L.

Abstract (from CDS):

The emission mechanism during the prompt phase in gamma-ray bursts (GRBs) can be investigated through correlations between spectral properties. Here, we revisit the correlation relating the instantaneous flux, F, and the photon index below the spectral break, α, in individual emission pulses, by studying the 38 most prominent pulses in the Fermi/Gamma-ray Burst Monitor GRB catalogue. First, we search for signatures of the bias in the determination of α due to the limited spectral coverage (window effect) expected in the synchrotron case. The absence of such a characteristic signature argues against the simplest synchrotron models. We instead find that the observed correlation between F and α can, in general, be described by the relation F(t) ∝e^k α(t)^, for which the median k = 3. We suggest that this correlation is a manifestation of subphotospheric heating in a flow with a varying entropy. Around the peak of the light curve, a large entropy causes the photosphere to approach the saturation radius, leading to an intense emission with a narrow spectrum. As the entropy decreases the photosphere secedes from the saturation radius, and weaker emission with a broader spectrum is expected. This simple scenario naturally leads to a correlated variation of the intensity and spectral shape, covering the observed range.

Abstract Copyright: © 2019 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): gamma-ray burst: general - gamma-ray burst: individual - radiation mechanism: thermal - methods: data analysis

Simbad objects: 35

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Number of rows : 35
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 150306A gB 00 02 -58.5           ~ 9 0
2 Fermi bn100507577 gB 00 11.6 -79 01           ~ 31 0
3 GRB 111017A gB 00 32 -07.0           ~ 16 0
4 GRB 081125 gB 02 51 -18.9           ~ 30 0
5 Fermi bn090530760 gB 04 53 +13.8           ~ 22 0
6 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
7 Fermi bn100122616 gB 05 16.8 -02 43           ~ 26 0
8 Fermi bn101126198 gB 05 39 -22.6           ~ 18 0
9 GRB 090820 gB 05 51 +27.1           ~ 44 0
10 GRB 151021B gB 06 57 -11.0           ~ 9 0
11 Fermi bn130815660 gB 07 30 -02.1           ~ 11 0
12 Fermi bn130305486 gB 07 46 59.45 +52 02 00.2           ~ 35 0
13 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
14 Fermi bn090804940 gB 08 42 -11.3           ~ 21 0
15 GRB 160530B gB 08 54 +43.5           ~ 14 0
16 Fermi bn090626189 gB 11 20 -33.5           ~ 54 0
17 GRB 081224A gB 13 26.8 +75 06           ~ 32 0
18 Fermi bn110920338 gB 13 59 -27.6           ~ 28 0
19 GRB 110920 gB 13 59 16.8 -27 33 36           ~ 11 0
20 GRB 120919A gB 14 19.1 -45 34           ~ 18 0
21 GRB 160910A gB 14 45 46.04 +39 04 01.3           ~ 45 0
22 GRB 090620 gB 15 49.4 +61 09           ~ 29 0
23 Fermi bn130612456 gB 16 32 +31.0           ~ 6 0
24 Fermi bn081009140 gB 16 42 +18.4           ~ 40 0
25 GRB 140508A gB 17 01 51.95 +46 46 49.5           ~ 76 0
26 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
27 GRB 100528A gB 20 44 29 +27 48.6           ~ 37 0
28 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 109 0
29 Fermi bn130614997 gB 21 37 -33.9           ~ 10 0
30 GRB 110721A gB 22 10 -38.6           ~ 155 0
31 Fermi bn110817191 gB 22 24 -45.8           ~ 17 0
32 GRB 090719 gB 22 45 -67.9           ~ 41 0
33 Fermi bn100707032 gB 23 24 -06.6           ~ 44 0
34 GRB 100612B gB 23 28 -01.8           ~ 23 0
35 Fermi bn160215773 gB 23 47 09.6 +01 43 48           ~ 10 0

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