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Annihilation radiation from thermal electron-positron plasma on the ground Landau level: The case of low magnetic fields
Authors:A D Kaminker  G G Pavlov  P G Mamradze
Institution:(1) A. F. Ioffe Institute of Physics and Technology, Academy of Sciences of the USSR, Leningrad, USSR;(2) Abastumani Astrophysical Observatory, Academy of Sciences of the Georgian SSR, Tbilisi, USSR
Abstract:The intensity and polarization of two-photon annihilation in a magnetic fuieldBLtB cr =4.4×1013 G are studied in detail for a, one-dimensional thermal distribution of annihilating electrons and positrons on the ground Landau level. With the increase of temperatureT the total annihilation rate and energy losses decrease, being higher than for the isotropic thermal distributions at the sameT. The shapes of intensity spectra at sin rhov=0 (rhov is the angle betweenB and wave-vector) are close to those in the isotropic case. The widths and blue-shifts of the spectra decrease with increasing sin rhov and increase with increasingT. Logarthmic singularities arise in the spectra atE»mc 2/sin rhov. Power-like parts are formed in the wings of the spectra forkTGtmc 2 and not too small sin rhov. The direction-integrated spectra reach their (finite) maxima, atE=mc 2 for anyT. The radiation concentrates near the plane, perpendicular to the magnetic field forE close tomc 2 and is beamed along the magnetic field forE far frommc 2. Energy-integrated angular distributions are stretched alongB, the stronger the higherT. The rediation is linearly polarized in the plane formed by the magnetic field and weve-vector. Typical values of the polarization inside the cores of the annihilation spectra are sim(kT/mc 2) sin rhov and ln (kT/mc 2)]–1 forkTLtmc 2 andkT sin rhovGtmc 2, respectively. Annihilation radiation dominates over Bremsstrahlung in thee mnplus plasma atkTlap7mc 2. The results are useful for interpretation of the annihilation radiation in the gamma-ray bursts. They permit to estimate temperature, gravitational potential, and emission measure of radiating regions and the beaming of the radiation.
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