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Alfven-cyclotron fluctuations : linear Vlasov theory

Conference ·
Linear Vlasov dispersion theory for a homogeneous, isotropic, collisionless, electron-proton plasma is used to examine the damping of Alfven-cyclotron fluctuations. Fluctuations of sufficiently long wavelength are essentially undamped, but as k{sub {parallel}}, the wavevector component parallel to the background magnetic field B{sub o}, reaches a characteristic dissipation value k{sub d}, the protons become cyclotron resonant and damping begins abruptly. For proton cyclotron damping, k{sub d}c/{omega}{sub p} {approx} 1 for 10{sup -3} {approx}< {beta}{sub p} {approx}< 10{sup -1} where {beta}{sub p} {identical_to} 8{pi}n{sub p}k{sub B}T{sub p}/B{sub o}{sup 2} and {omega}{sub p}/c is the proton inertial length. At k{sub {parallel}} < k{sub d}, m{sub e}/m{sub p} < {beta}{sub e} and {beta}{sub p} {approx}< 0.10, the electron Landau resonance becomes the primary contributor to fluctuation dissipation, yielding a damping rate which scales as {omega}{sub r} {radical}{beta}{sub e}(k{perpendicular}c/{omega}{sub p}){sup 2} where {omega}{sub r} is the real frequency and k{perpendicular} is the wavevector component perpendicular to B{sub o}. Over 0.10 < {beta}{sub p} {approx}< 10 the proton Landau resonance dominates damping of these waves, although no simple analytic expression for this damping rate has been found. Analytic expressions for proton cyclotron and electron Landau damping are used in a simple model of magnetic turbulent transport to calculate the dissipation range magnetic power spectra which may result from these two types of wave-particle interactions.
Research Organization:
Los Alamos National Laboratory
Sponsoring Organization:
DOE
OSTI ID:
977494
Report Number(s):
LA-UR-04-1428
Country of Publication:
United States
Language:
English

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