2014MNRAS.445.4105C


Query : 2014MNRAS.445.4105C

2014MNRAS.445.4105C - Mon. Not. R. Astron. Soc., 445, 4105-4109 (2014/December-3)

The change of GRB polarization angles in the magnetic-dominated jet model.

CHANG Z. and LIN H.-N.

Abstract (from CDS):

The polarimetric measurement on the prompt phase of GRB 100826A shows that the polarization angle changes ∼ 90° between two adjacent time intervals. We will show that this phenomenon can be naturally interpreted in the framework of the magnetic-dominated jet (MDJ) model. The MDJ model suggests that the bulk Lorentz factor of the outflow increases as Γ∝r1/3, until reaching a saturated value Γsat. Electrons move in the globally ordered magnetic field advected by the jet from the central engine and produce synchrotron photons. The polarized synchrotron photons travel alone the jet direction and then collide with the cold electrons at the front of the jet. After the Compton scattering process, these photons escape from the jet and are detected by the observer locating slightly off-axis. If photons are emitted before the bulk Lorentz factor saturates, the change of polarization angle is a natural result of the acceleration of the outflow.

Abstract Copyright: © 2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2014)

Journal keyword(s): polarization - radiation mechanisms: non-thermal - scattering - gamma-ray burst: individual: GRB 100826A

CDS comments: In chap. 3 : GRB 100812A is a misprint for GRB 100826A.

Simbad objects: 7

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Number of rows : 7
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 041219 gB 00 24 27.7 +62 50 34           ~ 231 1
2 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 499 1
3 GRB 110301A gB 15 17.4 +29 24           ~ 53 0
4 GRB 021206 gB 16 00 46.8 -09 42 36           ~ 112 0
5 GRB 100826A gB 18 56 -23.2           ~ 79 0
6 GRB 061122A gB 20 15 19.840 +15 31 02.50           ~ 48 0
7 GRB 110721A gB 22 10 -38.6           ~ 155 0

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