## Proceedings of the International School of Physics "Enrico Fermi.", Volume 23N. Zanichelli, 1963 - Nuclear physics |

### From inside the book

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Page 143

It is easy to see qualitatively when interference betweed D.I. and C.N. should

occur (shape elastic

both are on the same time scale). It has a length vT, where D.I. ' 71 oT Consider a

...

It is easy to see qualitatively when interference betweed D.I. and C.N. should

occur (shape elastic

**scattering**behaves of course just as D.I. in this respect, sinceboth are on the same time scale). It has a length vT, where D.I. ' 71 oT Consider a

...

Page 175

Moreover, in a many-particle system, two nucleons which

by all other nucleons present. ... We see that even without the hard core vai, the

operator for free nucleon

nuclear ...

Moreover, in a many-particle system, two nucleons which

**scatter**are influencedby all other nucleons present. ... We see that even without the hard core vai, the

operator for free nucleon

**scattering**, might well differ from the**scattering**innuclear ...

Page 185

Within what are generally called the ^-1-corrections to elastic

possible to consider the couplings of the possible independent excitations. The

most simple of these are the interaction between the optical state nucleon and ...

Within what are generally called the ^-1-corrections to elastic

**scattering**it ispossible to consider the couplings of the possible independent excitations. The

most simple of these are the interaction between the optical state nucleon and ...

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### Contents

Lectures | 1 |

G E Brown Collective motion and the application of manybody | 99 |

T Ep icson The compound nucleus and the random phase approximation | 142 |

Copyright | |

1 other sections not shown

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### Common terms and phrases

amplitude approximation assume calculated closed shells coefficients commutation compound configuration consider corresponding coupling cross-section define deformed describe determined diagonal dipole dipole strength discuss eigenfunctions eigenstate eigenvalues electron equation excitation energy expectation value experimental factor force gives Green's function ground Hamiltonian harmonic oscillator Hartree-Fock hermitian adjoint hole hyperfine-structure intrinsic irreducible representation isobaric spin isospin isotope shift large number lecture levels linear magnetic matrix elements Ml transitions Mottelson multipole neutron nuclear charge distribution nucleon nucleus number of particles obtained one-particle operator operator F optical potential orbitals orthogonal pair parameters particle-hole interaction perturbation theory Phys physical problem proton quadrupole qualitative quantum number quasi-particle random relation residual interaction resonant rotation rotation group scattering self-consistent shell-model shown single-particle solution spectrum spherical symmetry time-dependent tion total angular momentum two-body two-particle unperturbed variation vector vibrations wave function wave-functions width y-ray zero