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

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Page 131

The Green's function can, as we shall see, be expressed as a sum of products of

to, ...

The Green's function can, as we shall see, be expressed as a sum of products of

**wave functions**; by restricting our attention to the « 34 » component of the one-**wave function**, we have been considering only its dependence on the other two (to, ...

Page 168

The

whole nucleus and taking the proper ... Pif max [8] applied the generating

procedure to the internal

shell region.

The

**wave function**which is an eigenfunction of J is obtained by rotating thewhole nucleus and taking the proper ... Pif max [8] applied the generating

procedure to the internal

**wave functions**calculated by Nilssox [9] for the first p-shell region.

Page 169

Again the agreement between the

generating procedure and those calculated in intermediate coupling is very good.

We see that the two different methods of calculation give very nearly the same ...

Again the agreement between the

**wave functions**calculated by Redlich with thegenerating procedure and those calculated in intermediate coupling is very good.

We see that the two different methods of calculation give very nearly the same ...

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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