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

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Page 92

If ya exists such that P0(yo) = Pitilo) = 0 we have no

solution, and one has (8.13) H12P*4x(y0 ...

we want to obtain W from a

...

If ya exists such that P0(yo) = Pitilo) = 0 we have no

**vibration**but a « frozen »solution, and one has (8.13) H12P*4x(y0 ...

**Vibrations**. - In order to get**vibrations**we want to obtain W from a

**vibration**of an intrinsic state in the same way that we...

Page 102

These

existence is intimately bound up with pairing and nuclear superfluidity, so that we

shall leave their discussion until later, where we shall deal with them. Here we

shall ...

These

**vibrations**are relatively difficult to calculate theoretically, and theirexistence is intimately bound up with pairing and nuclear superfluidity, so that we

shall leave their discussion until later, where we shall deal with them. Here we

shall ...

Page 113

Although we have discussed mainly dipole

find higher order

etc.) one finds: 1) the particle-hole interaction is strongest for T =0 states; 2) the ...

Although we have discussed mainly dipole

**vibrations**, in the same way we canfind higher order

**vibrations**. With the ordinary exchange mixtures (R08ENFELD,etc.) one finds: 1) the particle-hole interaction is strongest for T =0 states; 2) the ...

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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