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

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Page 68

The squared PA strength simply shows how much each state contains of the

threehole configuration (30), since (PA)* is just 2(2J + 1) times the intensity of this

component which is listed in the fourth column. The

much ...

The squared PA strength simply shows how much each state contains of the

threehole configuration (30), since (PA)* is just 2(2J + 1) times the intensity of this

component which is listed in the fourth column. The

**ground**-**state**strength ismuch ...

Page 164

The excitation energy of the system is E* = E – Eo (Eo is the

Let N denote the number of particles and n the number of particles occupying the

partially filled shell when the system is in the

The excitation energy of the system is E* = E – Eo (Eo is the

**groundstate**energy).Let N denote the number of particles and n the number of particles occupying the

partially filled shell when the system is in the

**ground state**. The number of ...Page 332

This means that the ground and the high-lying molecular bands would be entirely

distinct, as shown in Fig. 40. Consequently, no state of the

band would contain any (or at least not a significant) admixture of the "O+"O ...

This means that the ground and the high-lying molecular bands would be entirely

distinct, as shown in Fig. 40. Consequently, no state of the

**ground**-**state**rotationalband would contain any (or at least not a significant) admixture of the "O+"O ...

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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