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

### From inside the book

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Page 59

12 the configuration assignment is made on the basis of both energy and parity

considerations. The E2 transition rate should thus be similar to the E'2 in "O and

indeed it is found to be so. Most of the available evidence on E2

...

12 the configuration assignment is made on the basis of both energy and parity

considerations. The E2 transition rate should thus be similar to the E'2 in "O and

indeed it is found to be so. Most of the available evidence on E2

**matrix elements**...

Page 104

• It can be seen that quite a bit of « Raeahology » is, in general, necessary to

evaluate this

**Matrix element**b is (6) - 2 (- 1 )1--""(«im* «m- w„ | iJlf) (- "(!,»/ J„- «, | £3/) (in | F|;m)• It can be seen that quite a bit of « Raeahology » is, in general, necessary to

evaluate this

**matrix elements**in the case of finite-range potential V. We shall, ...Page 150

For small r there is no contradiction between D.I. and random

one should of course make a deliberate separation between the random and

nonrandom part of the compound

For small r there is no contradiction between D.I. and random

**matrix elements**. ...one should of course make a deliberate separation between the random and

nonrandom part of the compound

**matrix element**, as we will see in a moment.### What people are saying - Write a review

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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