## Proceedings of the International School of Physics "Enrico Fermi.", Volume 62N. Zanichelli, 1976 - Nuclear physics |

### From inside the book

Results 1-3 of 45

Page 79

C) the same as B) but with the addition of a

between neutrons and protons. In all cases we have isospin zero, so the

occupation of orbitals is the same for neutrons as for protons. In case A) we

would expect ...

C) the same as B) but with the addition of a

**quadrupole**-**quadrupole**interactionbetween neutrons and protons. In all cases we have isospin zero, so the

occupation of orbitals is the same for neutrons as for protons. In case A) we

would expect ...

Page 86

For transitions and moments for T = 0 states, one sees that the electric-

an enhancement factor e = 1 + m, + m, . Thus with the usual assumption ma = m,

= m = 0.5 ...

For transitions and moments for T = 0 states, one sees that the electric-

**quadrupole**operator is simply proportional to the mass**quadrupole**operator withan enhancement factor e = 1 + m, + m, . Thus with the usual assumption ma = m,

= m = 0.5 ...

Page 377

On the other hand, one could seek the possibility to depend on the

giant resonance. This seems to have advantages over E1 capture due to

following reasons: i) For a system composed of two heavy ions, the dipole

moment is ...

On the other hand, one could seek the possibility to depend on the

**quadrupole**giant resonance. This seems to have advantages over E1 capture due to

following reasons: i) For a system composed of two heavy ions, the dipole

moment is ...

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### Contents

Gruppo fotografico dei partecipanti al Corso fuori testo | 1 |

Simple ideas on reaction mechanisms | 19 |

B BUCK Nuclearstructure information from severalnucleon | 29 |

Copyright | |

39 other sections not shown

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### Common terms and phrases

alpha amplitude angle angular distribution angular momentum approximation C+*C calculation centre-of-mass co-ordinates collision compound nucleus configurations continuum core corresponding Coulomb barrier coupling cross-section curve decay deformation DWBA effective eigenstates elastic scattering emission excitation energy excitation functions exit channel experimental fission form factor fragments gamma-rays ground-state Hamiltonian Hartree-Fock heavy ions heavy-ion high-spin incident energy isospin isotopes kinetic energy Lett level density mass matrix elements measured molecular moment of inertia neutron Nucl nuclear nuclei nucleons observed obtained operator optical potential orbits oscillator parameter particle peak Phys projectile proton quadrupole quasi-atom quasi-bound region renormalization residual interaction resonances rotational band shell model shown in Fig shows single-particle spectra spectroscopic spectrum spherical spherical-shell model spin structure sudden approximation target tion transfer reactions transition two-proton transfer values wave function width X-rays Y-ray yrast