2013MNRAS.436L..54A


Query : 2013MNRAS.436L..54A

2013MNRAS.436L..54A - Mon. Not. R. Astron. Soc., 436, L54-L58 (2013/November-3)

Comptonization of photons near the photosphere of relativistic outflows.

AKSENOV A.G., RUFFINI R. and VERESHCHAGIN G.V.

Abstract (from CDS):

We consider the formation of photon spectrum at the photosphere of ultrarelativistically expanding outflow. We use the Fokker-Planck approximation to the Boltzmann equation, and obtain the generalized Kompaneets equation which takes into account anisotropic distribution of photons developed near the photosphere. This equation is solved numerically for relativistic steady wind and the observed spectrum is found in agreement with previous studies. We also study the photospheric emission for different temperature dependences on radius in such outflows. In particular, we found that for Tr-2 the Band low-energy photon index of the observed spectrum is α ≃ -1, as typically observed in Gamma-Ray Bursts.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

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

Simbad objects: 12

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Number of rows : 12
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 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 940 1
2 GRB 071227A gB 03 52 31.09 -55 59 03.3           ~ 175 0
3 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 638 1
4 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 421 0
5 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 548 0
6 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 357 0
7 GRB 050509B gB 12 36 18.000 +29 01 24.00           ~ 309 1
8 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 390 0
9 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 320 0
10 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 215 0
11 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 612 1
12 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 295 0

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