Gamma-ray novae as probes of relativistic particle acceleration at non-relativistic shocks
Brian D. Metzger, Thomas Finzell, Indrek Vurm, Romain Hascoet, Andrei, M. Beloborodov, Laura Chomiuk

TL;DR
This paper investigates gamma-ray emissions from classical novae, analyzing shock acceleration of particles and their role in producing gamma-rays and optical emissions, with implications for nova models.
Contribution
It provides the first constraints on the efficiency of relativistic particle acceleration in novae using gamma-ray and optical luminosity ratios.
Findings
Gamma-ray to optical luminosity ratio constrains particle acceleration efficiency.
Inverse Compton gamma-ray models are disfavored due to low electron acceleration efficiency.
Shocks may power a significant fraction of optical emission in novae.
Abstract
The Fermi LAT discovery that classical novae produce >100 MeV gamma-rays establishes that shocks and relativistic particle acceleration are key features of these events. These shocks are likely to be radiative due to the high densities of the nova ejecta at early times coincident with the gamma-ray emission. Thermal X-rays radiated behind the shock are absorbed by neutral gas and reprocessed into optical emission, similar to Type IIn (interacting) supernovae. Gamma-rays are produced by collisions between relativistic protons with the nova ejecta (hadronic scenario) or Inverse Compton/bremsstrahlung emission from relativistic electrons (leptonic scenario), where in both scenarios the efficiency for converting relativistic particle energy into LAT gamma-rays is at most a few tens of per cent. The ratio of gamma-ray and optical luminosities, L_gam/L_opt, thus sets a lower limit on the…
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