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Particle Acceleration at Shocks: An Introduction

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arxiv 2307.00284 v2 pith:VJDZLGJ2 submitted 2023-07-01 astro-ph.HE physics.plasm-phphysics.space-ph

classification astro-ph.HEphysics.plasm-phphysics.space-ph
keywords accelerationshocksdiscussednon-thermalparticleshockspecialtheory
verification ladder T0 review T1 audit T2 compute T3 formal
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These notes present the fundamentals of Fermi acceleration at shocks, with a special attention to the role that supernova remnants have in producing Galactic cosmic rays. Then, the recent discoveries in the theory of diffusive shock acceleration (DSA) that stem from first-principle kinetic plasma simulations are discussed. When ion acceleration is efficient, the back-reaction of non-thermal particles and self-generated magnetic fields becomes prominent and leads to both enhanced shock compression and particle spectra significantly softer than those predicted by the standard test-particle DSA theory. These results are discussed in the context of the non-thermal phenomenology of astrophysical shocks, with a special focus on the remnant of SN1006.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. OpenAlex reports about 4 citations worldwide. Full citation record

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    Cosmic-ray protons in a simulated solar-neighborhood ISM steepen from an injected p^-4.3 spectrum to p^-4.6, matching observations, with a two-zone model predicting slope gamma = (4/3)gamma_inj - 1.

  2. Modeling Cosmic Ray Electron Spectra and Synchrotron Emission in the Multiphase ISM

    astro-ph.HE 2025-06 conditional novelty 6.0 of 10

    A post-processed MHD simulation of a solar-neighborhood galactic disk reproduces the observed steepening of the cosmic-ray electron spectrum from 1-100 GeV and shows that radio spectral indices can recover the electro...

  3. Speed-dependent Threshold for Electron Injection into Diffusive Shock Acceleration

    astro-ph.HE 2025-06 conditional novelty 6.0 of 10

    Electrons enter diffusive shock acceleration once their speed exceeds the shock speed, producing nonthermal tails that start at low momenta.

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