2011MNRAS.416.2193N


Query : 2011MNRAS.416.2193N

2011MNRAS.416.2193N - Mon. Not. R. Astron. Soc., 416, 2193-2201 (2011/September-3)

Constraints on cold magnetized shocks in gamma-ray bursts.

NARAYAN R., KUMAR P. and TCHEKHOVSKOY A.

Abstract (from CDS):

We consider a model in which the ultrarelativistic jet in a gamma-ray burst (GRB) is cold and magnetically accelerated. We assume that the energy flux in the outflowing material is partially thermalized via internal shocks or a reverse shock, and we estimate the maximum amount of radiation that could be produced in such magnetized shocks. We compare this estimate with the available observational data on prompt γ-ray emission in GRBs. We find that, even with highly optimistic assumptions, the magnetized jet model is radiatively too inefficient to be consistent with observations. One way out is to assume that much of the magnetic energy in the post-shock, or even pre-shock, jet material is converted to particle thermal energy by some unspecified process, and then radiated. This can increase the radiative efficiency sufficiently to fit observations. Alternatively, jet acceleration may be driven by thermal pressure rather than magnetic fields. In this case, which corresponds to the traditional fireball model, sufficient prompt GRB emission could be produced either from shocks at a large radius or from the jet photosphere closer to the centre. Possible detection of two giant extrasolar planets orbiting the eclipsing polar UZ Fornacis

Abstract Copyright: 2011 The Authors Monthly Notices of the Royal Astronomical Society2011 RAS

Journal keyword(s): acceleration of particles - MHD - radiation mechanisms: non-thermal - relativistic processes - shock waves - gamma-ray burst: general

CDS comments: In chap. 3.2 : GRB 980159 is a misprint for GRB 980519.

Simbad objects: 13

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Number of rows : 13
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 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
2 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 430 0
3 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
4 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
5 GRB 000418 gB 12 25 21 +20 05.0           ~ 219 0
6 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 499 1
7 GRB 010222 G 14 52 12.5 +43 01 06           ~ 364 1
8 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
9 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 361 0
10 GRB 991208 gB 16 33 53.51 +46 27 21.5           ~ 269 1
11 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
12 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
13 GRB 980519 gB 23 22 21.5 +77 15 43           ~ 203 0

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