## Proceedings of the International School of Physics "Enrico Fermi.", Volume 25N. Zanichelli, 1953 - Nuclear physics |

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Page 166

"pi an exps zul y F + 0 (F)*eos Note that when F" A 0 at u0, there is a

the integrand on the right side of eq. (22). Difficulties arising from the

corresponding logarithmic

only A' ...

"pi an exps zul y F + 0 (F)*eos Note that when F" A 0 at u0, there is a

**singularity**inthe integrand on the right side of eq. (22). Difficulties arising from the

corresponding logarithmic

**singularity**in p' are avoided here, since we consideronly A' ...

Page 197

The scattering kernel derived in the present article is in some 1espects preferable

to that derived in the earlier article, in that it does not display a

directions of a pair of wave vectors coalesce. Nevertheless, it seems that the ...

The scattering kernel derived in the present article is in some 1espects preferable

to that derived in the earlier article, in that it does not display a

**singularity**as thedirections of a pair of wave vectors coalesce. Nevertheless, it seems that the ...

Page 205

One may also verify that there is no

IV Canonical transformation for reduction of perturbation Hamiltonian. Consider a

dynamical system described by dynamical variables p, , q, , and a Hamiltonian ...

One may also verify that there is no

**singularity**at k, -i-k, -k, -i-k, - 0. A P P E N DIXIV Canonical transformation for reduction of perturbation Hamiltonian. Consider a

dynamical system described by dynamical variables p, , q, , and a Hamiltonian ...

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### Contents

LEZIONI | 1 |

carrier mass | 159 |

hydrodynamique au voisinage dun axe magnétique | 214 |

Copyright | |

2 other sections not shown

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### Common terms and phrases

adiabatic invariant amplitude approximation assumed Boltzmann equation boundary conditions boundary layer calculated cathode charge coefficient collision components consider const constant contraction corresponds courbe critère current density Debye length derived differential equations discharge dispersion relation distribution function dºr eigenvalue electric field electromagnetic waves electrostatic energy principle equations of motion equilibrium exp i(k exp ioctl exp ior experimental finite fluid theory frequency given Hence instability integral interaction ioctl ionized KRUSKAL l'axe magnétique lignes limit lowest order magnetic field Maxwell's equations negative ions nonlinear obtain parameter particle perturbation Phys plasma oscillations Plasma Physics Poisson's equation potential problem quantities radial region satisfied saturation current ſº solution solving stabilité stability surface temperature thermal tion values vanish variables vector velocity voisinage waves in plasmas zero zero-order