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

### From inside the book

Results 1-3 of 35

Page 24

Hartree-Fock method for singular

the two-body

simple H-F wave function becomes a poor approximation; as an illustration of this

, ...

Hartree-Fock method for singular

**forces**. Reaction matrix. 31. Preliminaries. - Ifthe two-body

**force**i>(l, 2) is singular, as actual nuclear**forces**seem to be, thesimple H-F wave function becomes a poor approximation; as an illustration of this

, ...

Page 67

Kurath treated all lp shell nuclei. The agreement with experimental data was

reasonably good. It should be noted that as the number of particles in the shell

increases the I s

shell ...

Kurath treated all lp shell nuclei. The agreement with experimental data was

reasonably good. It should be noted that as the number of particles in the shell

increases the I s

**force**strength must be increased. Elliott and Flower treated ld-2sshell ...

Page 104

We shall see that this is approximately true for the low-lying vibrations, so that

one needs consider only a quadrupole

vibrations, etc. Secondly, we should note that for the case of zero-range

which ...

We shall see that this is approximately true for the low-lying vibrations, so that

one needs consider only a quadrupole

**force**while working with quadrupolevibrations, etc. Secondly, we should note that for the case of zero-range

**forces**(which ...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### 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

### Other editions - View all

### 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