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

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Page 107

indices explicitly on the creation and annihilation operators, and to use Clebsch-

Gordan coefficients to combine the functions to total spin (

Thus {11) \phLSTy = 2 (— l)'" m"(— 1 )»-"•(— 1)*-»< • ». mi - (hm,l9- mo | LML) ...

indices explicitly on the creation and annihilation operators, and to use Clebsch-

Gordan coefficients to combine the functions to total spin (

**isospin**) zero or unity.Thus {11) \phLSTy = 2 (— l)'" m"(— 1 )»-"•(— 1)*-»< • ». mi - (hm,l9- mo | LML) ...

Page 167

It is a well-known fact that the ^'-coupling shell model works much better for states

with maximum

been shown [1-3] that most of the energy levels with anormal parity in the first ...

It is a well-known fact that the ^'-coupling shell model works much better for states

with maximum

**isospin**T than for states with lower**isospin**. For example it hasbeen shown [1-3] that most of the energy levels with anormal parity in the first ...

Page 171

... deformation for states with maximum

states with lower

providing me with his unpublished work and for helpful discussions. Thanks are

also due ...

... deformation for states with maximum

**isospin**T is much smaller than that forstates with lower

**isospins**. * * * I would like to thank Prof. C. A. Levinson forproviding me with his unpublished work and for helpful discussions. Thanks are

also due ...

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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 | |

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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