2001/04/06 by M. Ostrowski, Ostrowski, M.
Physics and Astronomy · #Astrophysics (astro-ph) #Astrophysics and Cosmic Phenomena #FOS: Physical sciences #Gamma-ray bursts and supernovae #Solar and Space Plasma Dynamics #astro-ph
paper · pdf · doi:10.48550/arxiv.astro-ph/0104120
submitted to Proc. Recontres de Moriond 'Very High Energy Phenomena in the Universe', Les Arcs, January 20-27, 2001
arxiv created 2001/04/06 · openalex publication_date 2001/04/06 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
We review the present status of the cosmic ray acceleration theory in mildly relativistic shock waves. Due to the involved substantial particle anisotropies analytical methods can tackle only simple situations involving weakly turbulent conditions near the shock. The numerical Monte Carlo methods are used to study the acceleration process in more general conditions. Contrary to non-relativistic shocks, the cosmic ray spectra at relativistic shock waves depend substantially on the magnetic field configurations and turbulence spectra. Depending on these conditions both very flat and very steep spectra can be created, with the characteristic acceleration time scales changing non-monotonously with the turbulence amplitude. Thus, the discussed theory is not able to uniquely explain the observed synchrotron spectra of relativistic shocks. We also mention an interesting possibility of particle acceleration at incompressible flow discontinuities (shear layers) at boundaries of relativistic jets.