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

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Page 51

In such cases one could, in principle, analyse by proper experiments the intensity

of a number of various

In such cases one could, in principle, analyse by proper experiments the intensity

of a number of various

**multipoles**in ... A success in accounting for this particular**multipole**moment should not be taken to mean that other**multipole**moments ...Page 68

Suppose that particle 2 is in a state ip1m. The potential seen by particle 1 which

is produced by particle 2 is (2.1) fyMHr,,) V1m(2)dr,= 17(1). This potential is not

spherically symmetric as follows by expanding V(r12) in

Suppose that particle 2 is in a state ip1m. The potential seen by particle 1 which

is produced by particle 2 is (2.1) fyMHr,,) V1m(2)dr,= 17(1). This potential is not

spherically symmetric as follows by expanding V(r12) in

**multipole**parts: (2.2) ...Page 157

This noncentral interaction is usually expanded in

. ... The highest

k = 3 and 4 are the highest magnetic and electric ones, respectively, detected, ...

This noncentral interaction is usually expanded in

**multipoles**[1] of orders k (1) ffu. ... The highest

**multipole**interaction k is limited by the smaller value 2/ or 2J, andk = 3 and 4 are the highest magnetic and electric ones, respectively, detected, ...

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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