2018MNRAS.478.3525L


Query : 2018MNRAS.478.3525L

2018MNRAS.478.3525L - Mon. Not. R. Astron. Soc., 478, 3525-3529 (2018/August-2)

An MAD explanation for the correlation between bulk Lorentz factor and minimum variability time-scale.

LLOYD-RONNING N., LEI W.-H. and XIE W.

Abstract (from CDS):

We offer an explanation for the anticorrelation between the minimum variability time-scale (MTS) in the prompt emission light curve of gamma-ray bursts (GRBs) and the estimated bulk Lorentz factor of these GRBs, in the context of a magnetically arrested disc (MAD) model. In particular, we show that previously derived limits on the maximum available energy per baryon in a Blandford-Znajek jet leads to a relationship between the characteristic MAD time-scale in GRBs and the maximum bulk Lorentz factor: tMAD ∝ Γ–6, somewhat steeper than (although within the error bars of) the fitted relationship found in the GRB data. Similarly, the MAD model also naturally accounts for the observed anticorrelation between MTS and gamma-ray luminosity L in the GRB data, and we estimate the accretion rates of the GRB disc (given these luminosities) in the context of this model. Both these correlations (MTS-Γ and MTS-L) are also observed in the Active Galactic Nuclei (AGN) data, and we discuss the implications of our results in the context of both GRB and blazar systems.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): gamma-ray burst: general

Simbad objects: 28

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Number of rows : 28
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 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
2 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
3 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
4 Fermi bn100728439 gB 02 56 13.44 +00 16 51.6           ~ 142 0
5 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
6 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 170 0
7 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
8 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
9 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
10 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
11 GRB 071010B gB 10 02 09.20 +45 43 52.2           ~ 173 0
12 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 213 0
13 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
14 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
15 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
16 Fermi bn100414097 gB 12 48 30.0 +08 41 35           ~ 136 0
17 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
18 GRB 091003A gB 16 46 04.680 +36 37 31.08           ~ 135 0
19 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
20 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
21 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
22 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
23 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 158 0
24 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
25 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
26 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 165 0
27 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
28 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0

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