2013
DOI: 10.1007/s11214-013-9984-7
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Collisionless Shocks in Partly Ionized Plasma with Cosmic Rays: Microphysics of Non-thermal Components

Abstract: In this review we discuss some observational aspects and theoretical models of astrophysical collisionless shocks in partly ionized plasma with the presence of nonthermal components. A specific feature of fast strong collisionless shocks is their ability to accelerate energetic particles that can modify the shock upstream flow and form the shock precursors. We discuss the effects of energetic particle acceleration and associated magnetic field amplification and decay in the extended shock precursors on the lin… Show more

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Cited by 33 publications
(27 citation statements)
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References 139 publications
(221 reference statements)
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“…As a result, the shock does not have to decelerate to a velocity as low as when DSA is inefficient to achieve a downstream temperature at which the gas can cool down effectively through radiation. A similar result has also been obtained by Bykov et al (2013). This also means that when the shock became radiative, the shock was still strong enough to support NLDSA so that at that time P CR has already dominated the post-shock pressure to support the gas from collapsing drastically.…”
Section: Case Of Nldsa With Thermal Injectionsupporting
confidence: 81%
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“…As a result, the shock does not have to decelerate to a velocity as low as when DSA is inefficient to achieve a downstream temperature at which the gas can cool down effectively through radiation. A similar result has also been obtained by Bykov et al (2013). This also means that when the shock became radiative, the shock was still strong enough to support NLDSA so that at that time P CR has already dominated the post-shock pressure to support the gas from collapsing drastically.…”
Section: Case Of Nldsa With Thermal Injectionsupporting
confidence: 81%
“…This can lead to a more highly ionized gas compared to the equilibrium values at v 120 sk < km s −1 . Also, f ion can change if nonlinear feedback of DSA to the shock structure is considered (Bykov et al 2013), and the formulae in Hollenbach & McKee (1989) must be modified; shock modification by the CR pressure results in an increase of the total compression ratio and decrease of the subshock compression ratio, which leads to a reduction of the post-shock temperature relative to the standard value for unmodified shocks. This hastens the transition of the shock to the radiative phase, and the ion fraction can start to increase due to photoionization at a higher shock velocity.…”
Section: Diffusion Coefficient and Momentum Breakmentioning
confidence: 99%
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“…In the case of shocks propagating through partially ionized plasmas charge-exchange particle collisions provide a return flux of highly super-thermal neutrals heating the upstream plasma reducing the fluid Mach number and the compression ratio in Balmer-type shocks of velocities below 3,000 km s −1 (see, e.g., Blasi et al 2012). The efficient CR acceleration may also modify the structure and the ultraviolet-optical-infrared emission spectra of MHD radiative shocks (see, e.g., Bykov et al 2013c).…”
Section: Particle Acceleration By Collisionless Shocksmentioning
confidence: 99%
“…The structure of the radiative shock depends on the line opacity which, for radiative SNR shocks, typically allows the escape of some optical and fine-structure infrared (IR) lines of abundant ions providing observational diagnostics of the shocks (see e.g., Raymond 1979;Hollenbach and McKee 1989;Gnat and Sternberg 2009;Bykov et al 2013a). …”
Section: Radiative Shocksmentioning
confidence: 99%