4.7 Article

Monte Carlo simulations of relativistic radiation-mediated shocks: II. photon-starved regime

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 492, Issue 2, Pages 1902-1913

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stz3591

Keywords

plasmas; radiation mechanisms: non-thermal; radiative transfer; scattering shock; waves

Funding

  1. JSPS KAKENHI Grants [JP16K21630, JP16KK0109, JP19K03878, JP19H00693]
  2. RIKEN Interdisciplinary Theoretical & Mathematical Science Program (iTHEMS)
  3. RIKEN pioneering project Evolution of Matter in the Universe (r-EMU)
  4. Israel Science Foundation [1114/17]
  5. RIKEN pioneering project Extreme precisions to Explore fundamental physics with Exotic particles (E3-Project)

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Radiation-mediated shocks (RMS) play a key role in shaping the early emission observed in many transients. In most cases, e.g. shock breakout in supernovae, llGRBs, and neutron star mergers, the upstream plasma is devoid of radiation, and the photons that ultimately reach the observer are generated predominantly inside and downstream of the shock. Predicting the observed spectrum requires detailed calculations of the shock structure and thermodynamic state that account properly for the shock microphysics. We present results of self-consistent Monte Carlo simulations of photon-starved RMS, which yield the shock structure and emission for a broad range of shock velocities, from subrelativistic (beta(sh) = 0.1) to highly relativistic (Gamma(sh) = 20). Our simulations confirm that in relativistic RMS the immediate downstream temperature is regulated by exponential pair creation, ranging from 50 keV at beta(sh) = 0.5200 keV at Gamma(sh) = 20. At lower velocities, the temperature becomes sensitive to the shock velocity, with kT similar to 0.5 keV at beta(sh) = 0.1. We also confirm that in relativistic shocks the opacity is completely dominated by newly created pairs, which has important implications for the breakout physics. We find the transition to pair dominance to occur at beta(sh) = 0.5 roughly. In all cases examined, the spectrum below the upsilon F upsilon peak has been found to be substantially softer than the Planck distribution. This has important implications for the optical emission in fast and relativistic breakouts, and their detection. The applications to GRB 060218 and GRB 170817A are discussed.

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