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

### From inside the book

Results 1-3 of 18

Page 64

(0, y,) , where n is the radial

and lTIm the appropriate spherical harmonic. The eigenvalues and eigenstate

can ...

(0, y,) , where n is the radial

**quantum number**, I the orbital momentum**quantum****number**and m the magnetic**quantum number**. N.1 is a normalization constantand lTIm the appropriate spherical harmonic. The eigenvalues and eigenstate

can ...

Page 84

To obtain the wave function we must project out states which have L and M as

good

accomplished by choosing (6.6) yi((J/0*O if 1<M. The

been ...

To obtain the wave function we must project out states which have L and M as

good

**quantum numbers**: (6.5) ipLM(afi)KeA) ... Elliot has shown that this isaccomplished by choosing (6.6) yi((J/0*O if 1<M. The

**quantum number**A hasbeen ...

Page 169

(k is the

calculated by Nilsson (and transformed from the ģi,ģi4 to the jm scheme). Again

the agreement between the wave functions calculated by Redlich with the

generating ...

(k is the

**quantum number**related to ;',) xk, yk and zk are different from thosecalculated by Nilsson (and transformed from the ģi,ģi4 to the jm scheme). Again

the agreement between the wave functions calculated by Redlich with the

generating ...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### 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

### Other editions - View all

### 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