Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 35
... polarization , like that of a test charge ; hence , if particles are distributed at points X , ( t ) : ( III.3.11 ) q ( x , t ) Σe , d ( x - X , ( t ) ) , q ( 1 » , k ) = Σe.fdt exp [ — ik · X , ( t ) — iot ] , edt ( ∞ , k ) = 4л = 47 ...
... polarization , like that of a test charge ; hence , if particles are distributed at points X , ( t ) : ( III.3.11 ) q ( x , t ) Σe , d ( x - X , ( t ) ) , q ( 1 » , k ) = Σe.fdt exp [ — ik · X , ( t ) — iot ] , edt ( ∞ , k ) = 4л = 47 ...
Page 52
... polarization and the last factor ( 1 + cos2 ) for an unpolarized incident beam . If the only polarization of the electron density is that produced by random fluctuations An is given by ( V.1.5 ) , i.e. ( V.2.5 ) An ( w , k ) = ( 1 + G ...
... polarization and the last factor ( 1 + cos2 ) for an unpolarized incident beam . If the only polarization of the electron density is that produced by random fluctuations An is given by ( V.1.5 ) , i.e. ( V.2.5 ) An ( w , k ) = ( 1 + G ...
Page 211
... polarization vector normal to k ,, or is the plasma frequency and o , satisfies the dispersion relation ( A - 6.9 ) or = w2 + c2 k2 . The summation is over all vectors k permitted by the geometry of the model and all pairs of values of ...
... polarization vector normal to k ,, or is the plasma frequency and o , satisfies the dispersion relation ( A - 6.9 ) or = w2 + c2 k2 . The summation is over all vectors k permitted by the geometry of the model and all pairs of values of ...
Contents
W B THOMPSON Kinetic theory of plasma | 97 |
Topics in microinstabilities | 137 |
carrier mass | 159 |
Copyright | |
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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