Download presentation
Presentation is loading. Please wait.
1
Andrei M. Beloborodov Columbia University
Blast waves from GRBs Andrei M. Beloborodov Columbia University Blast wave 2. GeV – TeV flashes
2
Meszaros, Rees (1993) Sari, Piran (1999)
4
Self-similar adiabatic blast wave: m = const
G 2 (Blandford, McKee 1976)
5
Thompson & Madau (2000), Beloborodov (2002)
7
Beloborodov (2002)
11
Beloborodov (2005)
12
GRB blast wave at the deceleration stage
13
GRB blast wave at the deceleration stage
16 R ~ c ~ ( /300) cm t G G b b n n
14
Optical flash in GRB The optical synchrotron flash is emitted by relativistic electrons (Lorentz factor ~ 100 in the fluid frame). The electrons are also exposed to the GRB photons which have ~ keV energy in the fluid frame. Compton cooling of the flash electrons by GRB photons and Production of GeV-TeV flash much stronger than its optical counterpart. (Akerlof et al. 1999)
15
Expected GeV-TeV flashes
Flash spectrum below GeV has the same slope as the low-energy part (0.1 MeV) of the main GRB. At higher energies –- fast-cooling spectrum ( E ). The flash is a few times longer than the prompt GRB. The flash has a smooth light curve. 1/2 (Beloborodov 2005)
16
GRB Gonzalez et al. 2003
17
Summary The huge G makes the explosion qualitatively different from other known explosions: -- MeV radiation front opens the gap (R ~ cm) -- blast wave is loaded with e+/- pairs (R ~ cm) -- survived neutrons leak out of the decelerated ejecta and change the shock mechanism (R ~ cm) Swift will observe the early stage of the explosion. A flat optical spectrum is expected from e+/- loaded blast wave. GeV-TeV flashes must be produced by GRBs, which can be easily observed by GLAST. 15 16 16 17
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.