Jet Break Time – Flux Density Relationship and Constraints on Physical Parameters of Grb Afterglows
نویسندگان
چکیده
We derive a relation between the flux density Fν,j at the light curve break of a GRB afterglow and the break time tj. The break is due to the transition from the spherical-like to jet-like evolution of the afterglow when the Lorentz factor of the jet equals the inverse of the initial half opening angle, i.e. γ = 1/θ0. We show that this relation indeed behaves as Fν,j ∝ t −p j among GRBs for the slow cooling case, where p is the power-law index of electron distribution. A statistical analysis of the optical jet breaks of 9 GRBs gives p = 2.10± 0.21, which is consistent with the shock acceleration theory. The value of p derived in this way is different from the observed temporal index α2 (Fν ∝ t−α2 ) of the late-time light curve after tj, which suffers several uncertainties from the unclear hydrodynamics of the sideways expansion and exhibits a large dispersion. Our results not only confirm that the remnants of GRBs are standard candles, but also provide the first evidence that the physical parameters of relativistic shocks are universal, with the favored values ǫe ∼ 0.1 and ǫB ∼ 10−3. Subject headings: gamma rays: bursts—gamma rays: observations—ISM: jets and outflows—methods: statistical
منابع مشابه
Jet Break Time – Flux Density Relationship and Constraints on Physical Parameters of Gamma-ray Burst Afterglows
We derive a relation between the flux density Fν, j at the light-curve break of a gamma-ray burst (GRB) afterglow and the break time t j. The break is due to the transition from the spherical-like to jet-like evolution of the afterglow, when the Lorentz factor of the jet equals the inverse of the initial half-opening angle, i.e., γ = 1/θ0. We show that this relation indeed behaves as Fν, j ∝ t ...
متن کاملProperties of Relativistic Jets in Eight Gamma-ray Burst Afterglows
We extend our calculation of physical parameters of GRB afterglows through modelling of their broadband emission to three other cases: 980519, 000926, and 010222. Together with 990123, 990510, 991208, 991216, and 000301c, there are eight afterglows whose optical and radio emission allow determination of the burst collimation. The jet energies (after the GRB phase) obtained for this sample of ei...
متن کاملBroadband modeling of gamma - ray burst afterglows
— According to the fireball model gamma-ray burst (GRB) afterglows are the result of a shock pushed into the surrounding medium by an extremely relativistic outflow from the GRB. By modeling the broadband spectrum, ranging from X-ray to radio wavelengths, on time scales of hours to years after the GRB, we can determine several burst parameters, e.g. the burst energy, the circumburst medium dens...
متن کاملDecay phases of Swift X-ray afterglows and the forward-shock model.
The X-ray flux of the gamma-ray burst (GRB) afterglows monitored by the Swift satellite from January 2005 to July 2006 displays one to four phases of flux power-law decay. In chronological order, they are: the GRB tail, the 'hump', the standard decay and the post-jet-break decay. More than half of the GRB tails can be identified with the large-angle emission produced during the burst (but arriv...
متن کاملProperties of Relativistic Jets in Gamma-ray Burst Afterglows
We extend our calculation of physical parameters of GRB jets by modeling the broadband emission of the afterglows 970508, 980519, 991208, 000926, 000418, and 010222. Together with 990123, 990510, 991216, and 000301c, there are ten well-observed afterglows for which the initial opening angle of the GRB jet can be constrained. The jet energies (after the GRB phase) obtained for this set of afterg...
متن کامل