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Gamma-Ray Burst Spectral Breaks and Source Beaming

Published online by Cambridge University Press:  12 April 2016

Matthew G. Baring*
Affiliation:
Laboratory for High Energy Astrophysics, Code 665, NASA Goddard Space Flight Center, Greenbelt, MD 20771

Abstract

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The principal discovery of the Compton Gamma-Ray Observatory (GRO) concerning gamma-ray bursts is that these sources are isotropic but with a comparative deficiency of fainter sources, suggesting that they are probably cosmological in origin. If they are at such large distances from Earth then they are extremely luminous and compact. A consequence of this is that two-photon pair production attenuation of the gamma-ray continuum cannot be avoided unless the source radiation is substantially beamed. Most sources do not display gamma-ray turnovers although a few GRB detected by GRO exhibit distinct spectral breaks in the MeV range. A derivation of the relationship defining of the degree of beaming in burst sources with spectral breaks due to γ-γ attenuation, as a function of source spectral index and break energy, is presented. It is found that sources at distances of ~1 Gpc must typically be beamed with bulk Lorentz factors of around 103 -104 , indicating powerful bulk acceleration in bursts, although these Lorentz factors are reduced markedly for steep source spectra. Since the source spectra are not strongly Comptonized, such beaming will blueshift the γ-γ attenuation breaks to energies much higher than 1 MeV; an absolute lower bound to the source bulk Lorentz factor is determined from this additional constraint. This blueshifting suggests that those sources with MeV breaks may not be cosmological, or that their breaks are produced by a mechanism that dominates γ-γ attenuation at these energies.

Subject headings: gamma-rays: bursts — radiation mechanisms: nonthermal

Type
Poster Papers
Copyright
Copyright © The American Astronomical Society 1994

References

Baring, M.G. 1993, ApJ, 90, 899 Google Scholar
Cavallo, G., & Rees, M.J. 1978, MNRAS, 183, 359 CrossRefGoogle Scholar
Eichler, D., Livio, M., Piran, T., & Schramm, D.N. 1989, Nature, 340, 126 CrossRefGoogle Scholar
Fenimore, E.E., Epstein, R.E., & Ho, C. 1992, in AIP Conf. Proc. 265, Gamma-Ray Bursts, ed. Paciesas, W.S. & Fishman, G.J. (New York: AIP), 158 Google Scholar
Gould, R.J., & Schreder, G.P. 1967, Phys. Rev., 155, 1404 CrossRefGoogle Scholar
Gradshteyn, I.S., & Ryzhik, I.M. 1980, Table of Integrals, Series and Products (New York: Academic)Google Scholar
Kouveliotou, C., et al. 1994, ApJL, submittedGoogle Scholar
Krolik, J.H., & Pier, E.A. 1991, ApJ, 373, 277 CrossRefGoogle Scholar
Kwok, P.W., et al. 1993, in Proc. Compton Observatory Symposium (St. Louis, MO) (New York: AIP), in pressGoogle Scholar
Lightman, A.P., & Zdziarski, A.A. 1987, ApJ, 319, 643 CrossRefGoogle Scholar
Mao, S., & Paczyński, B. 1992a, ApJ, 388, L45 CrossRefGoogle Scholar
Mao, S., & Paczyński, B. 1992b, ApJ, 389, L13 CrossRefGoogle Scholar
Meegan, C., et al. 1992, Nature, 355, 143 CrossRefGoogle Scholar
Mészáros, P., & Rees, M.J. 1992, MNRAS, 257, 29PCrossRefGoogle Scholar
Paczyński, B. 1986, ApJ, 308, L43 CrossRefGoogle Scholar
Rees, M.J., & Mészáros, P. 1992, MNRAS, 258, 41PCrossRefGoogle Scholar
Schaefer, B.E., et al. 1992, ApJ, 393, L51 CrossRefGoogle Scholar
Schmidt, W.K.H. 1978, Nature, 271, 525 CrossRefGoogle Scholar
Schneid, E.J. 1992, A&A, 255, L13 Google Scholar
Sommer, M., et al. 1994, ApJL, in pressGoogle Scholar
Stepney, S., & Guilbert, P.W. 1983, MNRAS, 204, 1269 CrossRefGoogle Scholar
Svensson, R. 1987, MNRAS, 227, 403 CrossRefGoogle Scholar
Weinberg, S. 1972, Gravitation and Cosmology (New York: Wiley)Google Scholar