Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |
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Page 252
... adiabatic invariant to all orders inspired KRUSKAL to attempt the more difficult problem , which SEMINARI SULL'INVARIANZA ADIABATICA pag 1 54 97 137 159 180 214 234 KULSRUD Introduction for papers on adiabatic invariance KULSRUD.
... adiabatic invariant to all orders inspired KRUSKAL to attempt the more difficult problem , which SEMINARI SULL'INVARIANZA ADIABATICA pag 1 54 97 137 159 180 214 234 KULSRUD Introduction for papers on adiabatic invariance KULSRUD.
Page 254
Adiabatic Invariant of the Harmonic Oscillator ( " ) . R. M. KULSRUD Project Matterhorn , Princeton University - Princeton , N. J. 1 ... adiabatic invariant in quantum mechanics would Adiabatic invariant of the harmonic oscillator.
Adiabatic Invariant of the Harmonic Oscillator ( " ) . R. M. KULSRUD Project Matterhorn , Princeton University - Princeton , N. J. 1 ... adiabatic invariant in quantum mechanics would Adiabatic invariant of the harmonic oscillator.
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 ... ADIABATIC INVARIANT OF THE HARMONIC OSCILLATOR 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 ... ADIABATIC INVARIANT OF THE HARMONIC OSCILLATOR 255.
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