Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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... resonances appear . The potential due to a test charge q * ( k , w ) is then given by Φ - k2 2πί 4лq * ( k , ∞ ) ( ki v Ω 2xicôfdv , dv ̧v ̧ Σ 31⁄2 ( ' 1o102 ) 8 : ( 0 + n £ Q + k , v , ) [ k , af + av nQ af VL dv 3. Field of a test ...
... resonances appear . The potential due to a test charge q * ( k , w ) is then given by Φ - k2 2πί 4лq * ( k , ∞ ) ( ki v Ω 2xicôfdv , dv ̧v ̧ Σ 31⁄2 ( ' 1o102 ) 8 : ( 0 + n £ Q + k , v , ) [ k , af + av nQ af VL dv 3. Field of a test ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
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adiabatic invariant amplitude approximation Boltzmann equation boundary conditions boundary layer calculated cathode coefficient collision components consider constant contraction corresponds courbe critère current density d³k d³v Debye length derived differential equations discharge dispersion relation distribution function eigenvalue electric field electrons and ions electrostatic energy principle equations of motion equilibrium exp[i(k finite fluid theory frequency given Hence instability integral interaction ionized k₁ KRUSKAL l'axe magnétique limit Liouville function lowest order magnetic field Maxwell's equations mode nonlinear obtain Ohm's law P₁ parameter particle périodique perturbation Phys plasma oscillations Plasma Physics Poisson's equation potential problem quantities R₁ region Rendiconti S.I.F. satisfied saturation current solution solving stabilité stability temperature thermal tion v₁ values variables vector velocity x₁ zero zero-order Απ