NASA NTRS1993
Colliding comets in the Solar System may be an important source of gamma ray bursts. The spherical gamma ray comet cloud required by the results of the Venera Satellites (Mazets and Golenetskii, 1987) and the Burst and Transient Source Experiment (BATSE) detector on the Compton Satellite (Meegan et al., 1992a, b) is neither the Oort Cloud nor the Kuiper Belt. To satisfy observations of N(greater than P(sub max)) vs P(sub max) for the maximum gamma ray fluxes, P(sub max) greater than 10(exp -5) ergs/sq cm/ s (about 30 bursts/yr), the comet density, n, should increase as n approximately a(exp 1) from about 40 to 100 AU where a is the comet heliocentric distance. The turnover above 100 AU requires n approximately a(exp -1/2) to 200 AU to fit the Venera results and n approximately a(exp 1/4) to 400 AU to fit the BATSE data. Then the masses of comets in the 3 regions are from: 40-100 AU, about 9 earth masses, m(sub E); 100-200 AU about 25 m(sub E); and 100-400 AU, about 900 m(sub E). The flux of 10(exp -5) ergs/sq cm/s corresponds to a luminosity at 100 AU of 3 x 10(exp 26) ergs/s. Two colliding spherical comets at a distance of 100 AU, each with nucleus of radius R of 5 km, density of 0.5 g/cu cm and Keplerian velocity 3 km/s have a combined kinetic energy of 3 x 10(exp 28) erg, a factor of about 100 greater tha required by the burst maximum fluxes that last for one second.