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

### From inside the book

Results 1-3 of 11

Page 68

Owing to the Pauli principle, the nucleons will in general not be in

symmetric orbits. Suppose that particle 2 is in a state ip1m. The potential seen by

particle 1 which is produced by particle 2 is (2.1) fyMHr,,) V1m(2)dr,= 17(1).

Owing to the Pauli principle, the nucleons will in general not be in

**spherical**symmetric orbits. Suppose that particle 2 is in a state ip1m. The potential seen by

particle 1 which is produced by particle 2 is (2.1) fyMHr,,) V1m(2)dr,= 17(1).

Page 98

... the

decreases. R E F E R E X CES [1] A. Mottelson in Many-Particles Problems, Les

Houches. [2] J. P. Elliott: Proc. Hoy. Soc., A 245, 128, 562 (1958). [3] G. Racah:

Princeton ...

... the

**spherical**shape which probably deepens as the range of the forcedecreases. R E F E R E X CES [1] A. Mottelson in Many-Particles Problems, Les

Houches. [2] J. P. Elliott: Proc. Hoy. Soc., A 245, 128, 562 (1958). [3] G. Racah:

Princeton ...

Page 101

In

momenta and parity. Some of these, in which the neutrons and protons move

together, lie very low in energy. Others, such as the giant dipole resonance

excited ...

In

**spherical**nuclei one can have vibrations, corresponding to all possible angularmomenta and parity. Some of these, in which the neutrons and protons move

together, lie very low in energy. Others, such as the giant dipole resonance

excited ...

### 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