2008
DOI: 10.1086/590054
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Production of Magnetic Turbulence by Cosmic Rays Drifting Upstream of Supernova Remnant Shocks

Abstract: We present results of two-and three-dimensional Particle-In-Cell simulations of magnetic-turbulence production by isotropic cosmic-ray ions drifting upstream of supernova remnant shocks. The studies aim at testing recent predictions of a strong amplification of short-wavelength magnetic field and at studying the subsequent evolution of the magnetic turbulence and its backreaction on cosmic ray trajectories. We observe that an oblique filamentary mode grows more rapidly than the non-resonant parallel modes foun… Show more

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Cited by 153 publications
(200 citation statements)
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“…It is thus probable that the growth of the former modes simply results in mere heating of the plasma from the standpoint of the latter. Bell's modes have motivated many studies over the past years, and a number of theoretical 229,234 and numerical works 230,235,236 have now enriched the initial MHD theory.…”
Section: -30mentioning
confidence: 99%
“…It is thus probable that the growth of the former modes simply results in mere heating of the plasma from the standpoint of the latter. Bell's modes have motivated many studies over the past years, and a number of theoretical 229,234 and numerical works 230,235,236 have now enriched the initial MHD theory.…”
Section: -30mentioning
confidence: 99%
“…This instability also requires super-Alfvenic cosmic ray streaming, but is driven by the thermal electron current that is assumed to flow in the background to cancel the cosmic ray current. 44,45,[73][74][75][76][77][78][79] The instability occurs when the cosmic ray energy density U cr , background magnetic energy density U B , and cosmic ray streaming velocity v D satisfy the inequality U cr =U B > c=v D . When this criterion is satisfied, the wavelength of the fastest growing mode is below the gyroradius of GeV cosmic rays.…”
Section: B Acceleration At Shocksmentioning
confidence: 99%
“…We then included a mono-energetic beam that was homogeneous throughout the numerical box. To keep the total current zero in these models in their initial states, we introduced an initial return current by shifting the background plasma electrons in the velocity space according to the relation v d = −v b n b /n e , where v b is the velocity of the electron beam, and n b and n e are the beam and background plasma densities; for an example of this type of initialization, see Niemiec et al (2008). In principle, it is possible to start from a zero initial return current.…”
Section: Simulation Modelmentioning
confidence: 99%