RAPID COSMIC-RAY ACCELERATION AT PERPENDICULAR SHOCKS IN SUPERNOVA REMNANTS

@article{Takamoto2015RAPIDCA,
  title={RAPID COSMIC-RAY ACCELERATION AT PERPENDICULAR SHOCKS IN SUPERNOVA REMNANTS},
  author={Makoto Takamoto and John G. Kirk},
  journal={The Astrophysical Journal},
  year={2015},
  volume={809}
}
Perpendicular shocks are shown to be rapid particle accelerators that perform optimally when the ratio us of the shock speed to the particle speed roughly equals the ratio 1/η of the scattering rate to the gyro frequency. We use analytical methods and Monte-Carlo simulations to solve the kinetic equation that governs the anisotropy generated at these shocks, and find, for ηus ≈ 1, that the spectral index softens by unity and the acceleration time increases by a factor of two compared to the… 

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References

SHOWING 1-10 OF 45 REFERENCES

COSMIC RAY ACCELERATION AT PERPENDICULAR SHOCKS IN SUPERNOVA REMNANTS

Supernova remnants (SNRs) are believed to accelerate particles up to high energies through the mechanism of diffusive shock acceleration (DSA). Except for direct plasma simulations, all modeling

DIFFUSIVE ACCELERATION OF PARTICLES AT OBLIQUE, RELATIVISTIC, MAGNETOHYDRODYNAMIC SHOCKS

Diffusive shock acceleration (DSA) at relativistic shocks is expected to be an important acceleration mechanism in a variety of astrophysical objects including extragalactic jets in active galactic

Cosmic rays X. The cosmic ray knee and beyond: diffusive acceleration at oblique shocks

Our purpose is to evaluate the rate of the maximum energy and the acceleration rate that cosmic rays acquire in the non-relativistic diffusive shock acceleration as it could apply during their

THE MAXIMUM ENERGY OF ACCELERATED PARTICLES IN RELATIVISTIC COLLISIONLESS SHOCKS

The afterglow emission from gamma-ray bursts (GRBs) is usually interpreted as synchrotron radiation from electrons accelerated at the GRB external shock that propagates with relativistic velocities

The injection and acceleration of particles in oblique shocks - A unified Monte Carlo description

Standard Fermi particle acceleration may, for certain shock parameters, be enhanced in oblique shocks, in which the upstream magnetic field makes a significant angle Θ Bn1 to the shock normal,

SIMULATIONS OF ION ACCELERATION AT NON-RELATIVISTIC SHOCKS. I. ACCELERATION EFFICIENCY

We use two-dimensional and three-dimensional hybrid (kinetic ions–fluid electrons) simulations to investigate particle acceleration and magnetic field amplification at non-relativistic astrophysical

Particle acceleration by ultrarelativistic shocks: theory and simulations

We consider the acceleration of charged particles near ultra-relativistic shocks, with Lorentz factor Gamma_s >> 1. We present simulations of the acceleration process and compare these with results

Cosmic ray acceleration at relativistic shock waves in the presence of oblique magnetic fields with finite-amplitude perturbations

The process of first-order Fermi acceleration at relativistic shock waves is investigated by means of Monte Carlo particle simulations. The simulations are based on numerical integration of the

Observational constraints on energetic particle diffusion in young supernovae remnants: amplified magnetic field and maximum energy

Constraints on the diffusion and acceleration parameters in five young supernova remnants (SNRs) are derived from the observed thickness of their X-ray rims, as limited by the synchrotron losses of