Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 112
... mechanics and quantum mechanics to our problem . + To prove this assertion we make use of our preceding calculations for the cathode , the inertia - limited zone and the contraction region . As a result we have already the electron ...
... mechanics and quantum mechanics to our problem . + To prove this assertion we make use of our preceding calculations for the cathode , the inertia - limited zone and the contraction region . As a result we have already the electron ...
Page 196
... quantum conditions governing the interaction of waves in quantum mechanics . Since energy and momentum of a wave are related to the action by [ 15 ] ( 6.4 ) and E = Jo , ( 6.5 ) P = Jk , we see that energy and momentum are separately ...
... quantum conditions governing the interaction of waves in quantum mechanics . Since energy and momentum of a wave are related to the action by [ 15 ] ( 6.4 ) and E = Jo , ( 6.5 ) P = Jk , we see that energy and momentum are separately ...
Page 255
An example of an adiabatic invariant in quantum mechanics would be the distribution over energy states of a system as the Hamiltonian is changed by external means , such as changing the volume of the boundaries of the system without ...
An example of an adiabatic invariant in quantum mechanics would be the distribution over energy states of a system as the Hamiltonian is changed by external means , such as changing the volume of the boundaries of the system without ...
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