2004
DOI: 10.1142/s0218271804004980
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On the Instantaneous Spectrum of Gamma-Ray Bursts

Abstract: A theoretical attempt to identify the physical process responsible for the afterglow emission of Gamma-Ray Bursts (GRBs) is presented, leading to the occurrence of thermal emission in the comoving frame of the shock wave giving rise to the bursts. The determination of the luminosities and spectra involves integration over an infinite number of Planckian spectra, weighted by appropriate relativistic transformations, each one corresponding to a different viewing angle in the past light cone of the observer. The … Show more

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Cited by 62 publications
(156 citation statements)
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“…This allows us to assume, to a first approximation, a modeling of thin spherical shells for the CBM distribution and consequently only consider their radial dependence (Ruffini et al 2002). The emission process is assumed to be thermal in the comoving frame of the shell (Ruffini et al 2004). The observed GRB non-thermal spectral shape is produced by the convolution of a very large number of thermal spectra with different temperatures and different Lorentz and Doppler factors.…”
Section: The Fireshell Modelmentioning
confidence: 99%
“…This allows us to assume, to a first approximation, a modeling of thin spherical shells for the CBM distribution and consequently only consider their radial dependence (Ruffini et al 2002). The emission process is assumed to be thermal in the comoving frame of the shell (Ruffini et al 2004). The observed GRB non-thermal spectral shape is produced by the convolution of a very large number of thermal spectra with different temperatures and different Lorentz and Doppler factors.…”
Section: The Fireshell Modelmentioning
confidence: 99%
“…Within the fireshell model (Ruffini et al 2002(Ruffini et al , 2004(Ruffini et al , 2005(Ruffini et al , 2009Bianco et al 2005a,b), all GRBs originate from an optically thick e ± plasma of total energy E e ± tot in the range 10 49 -10 54 erg and a temperature T in the range 1-4 MeV. After an early expansion, the e ± -photon plasma reaches thermal equilibrium with the engulfed baryonic matter M B described by the dimensionless parameter B = M B c 2 /E e ± tot , which must be B < 10 −2 to allow the fireshell to expand further.…”
Section: Brief Summary Of the Fireshell Modelmentioning
confidence: 99%
“…This second parameter takes into account the CBM filamentary structure (Ruffini et al 2004) and the possible occurrence of fragmentation in the shell (Dainotti et al 2007). The emission from the baryonic matter shell is spherically symmetric.…”
Section: Brief Summary Of the Fireshell Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…Ruffini et al 2001Ruffini et al , 2009, and references therein) has led to identifying a canonical GRB structure described by two parameters: the total energy E e ± tot of the initially optically thick electronpositron plasma and its baryon load B = M B c 2 /E e ± tot . To this information characterizing the source is added the information on the density and filamentary distribution of the circumburst medium (CBM) (Ruffini et al 2004b(Ruffini et al , 2005Patricelli et al 2010Patricelli et al , 2011.…”
Section: Introductionmentioning
confidence: 99%