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

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Page 60

Theoretical considerations of {a. Let us now see to what extent we can

understand the numerical values of the magnetic moment operator. First, a word

about the operator itself. \t is denned as that

linear term ...

Theoretical considerations of {a. Let us now see to what extent we can

understand the numerical values of the magnetic moment operator. First, a word

about the operator itself. \t is denned as that

**vector**which is the coefficient of thelinear term ...

Page 97

... in the SU2 scheme. The above equation is only approximate and P^y) was

determined by projecting the

-space defined by the 6

... in the SU2 scheme. The above equation is only approximate and P^y) was

determined by projecting the

**vector**^V(i, j)0(y ; 1, 2, 3, 4) onto the incomplete sub-space defined by the 6

**vectors**: d d2 ~ d 0, -=-&, 0, L*4>, L>0, L* — 0 . dy dy' ...Page 146

This

an energy interval of ~100 keV. The resonant states are orthogonal and provide a

set of base

This

**vector**is projected out on a subspace of resonant states i, say resonances inan energy interval of ~100 keV. The resonant states are orthogonal and provide a

set of base

**vectors**for this**vector**space. The statement that they have nothing ...### 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