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

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Page 95

Because if it did then this component would admix strongly into the

we would no longer have a paeketlike

possible therefore to expand the dependence on y into Taylor series and keep ...

Because if it did then this component would admix strongly into the

**solution**andwe would no longer have a paeketlike

**solution**with y's clustered around y0. It ispossible therefore to expand the dependence on y into Taylor series and keep ...

Page 139

Construction of rotating

moment of inertia, eq. (56.5), it is useful to actually construct the rotating Hartree-

Fock

another ...

Construction of rotating

**solutions**. Although one has an expression for themoment of inertia, eq. (56.5), it is useful to actually construct the rotating Hartree-

Fock

**solution**in the linear approximation. This**solution**is closely related toanother ...

Page 154

Therefore there seems very likely that the state determined as a

will contain a large admixture of a spurious state. If this is the case the

eq. (1) will note be able to describe properly a /?- vibration. Keeping this ...

Therefore there seems very likely that the state determined as a

**solution**of eq. (1)will contain a large admixture of a spurious state. If this is the case the

**solution**ofeq. (1) will note be able to describe properly a /?- vibration. Keeping this ...

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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