Astronomy and Astrophysics – Astronomy
Scientific paper
Jul 1995
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=1995apj...448l..29m&link_type=abstract
Astrophysical Journal Letters v.448, p.L29
Astronomy and Astrophysics
Astronomy
23
Gamma Rays: Bursts, Magnetic Fields, Radiative Transfer, Stars: Neutron
Scientific paper
All three soft gamma-ray repeaters (SGRs) are associated with supernova remnants; consequently, models of SGRs involving young neutron stars have attracted close attention. From the distances to the supernova remnants and the observed burst fluxes, the luminosity of a typical burst from an SGR is ~1041-1042 ergs s-1; the 1979 March 5 event from SGR 0526-66 had an inferred peak luminosity of ~5 x 1044 ergs s-1. These luminosities are orders of magnitude larger than the Eddington luminosity LE ~ 2 x 1038 ergs s-1 for a neutron star. Many models of SGRs assume that the atmosphere is hydrostatic. To reconcile this requirement with the large luminosities of SGRs, it has been suggested that the neutron stars that produce SGRs have extremely high magnetic fields. Then for a photon with frequency omega much less than the electron cyclotron frequency omega c, the scattering cross section (and thus the radial radiation force) in the perpendicular polarization mode is decreased by a factor ~(omega / omega c)2 compared to the magnetic field B = 0 case. It has been assumed that if essentially all of the radiation emerges in the perpendicular mode, then the maximum hydrostatic luminosity rises to Lcrit ~(omega c / omega )2LE. Thus, to allow a hydrostatic atmosphere for a burst luminosity ~1042 ergs s-1 and a typical photon energy & omega ~50keV , it has been thought that a magnetic field B ~ 5 x 1014 G would suffice. We show that this is not correct. Although most of the luminosity emerges in the perpendicular mode, the fraction ~( omega / omega c) that scatters into the parallel mode dominates the radiation force. Hence the maximum luminosity is only Lcrit ~5(omega c / omega)LE. Thus, for a typical SGR burst, the magnetic field must be at least B ~ 1016 G to ensure a hydrostatic atmosphere, and for the March 5 event B > 5 x 1018 G is required. These field strengths are unreasonably high. We therefore suggest that SGRs do not have hydrostatic atmospheres and that models which invoke magnetic confinement are more promising.
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