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

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Page 5

sion of a length to the power minus three-halves (LTP), and this is no surprise, for

the square of p can be interpreted as a

when it is integrated over the whole

sion of a length to the power minus three-halves (LTP), and this is no surprise, for

the square of p can be interpreted as a

**probability**density which adds up to 1when it is integrated over the whole

**space**(1.3) six vo) – 1. In the case of plane ...Page 153

... l values and to calculate the number of states for the particle a' in the phase

reaction (a'-CN) in the volume V is given by Xoses,(v/V), where v is the velocity =

k(hlu).

... l values and to calculate the number of states for the particle a' in the phase

**space**volume 47 Vp” dp/h” = =VKodk/27t", ... The**probability**for the inversereaction (a'-CN) in the volume V is given by Xoses,(v/V), where v is the velocity =

k(hlu).

Page 201

Moreover, because the necessity of dissipating also a large amount of angular

momentum, gammarays are emitted. iii) The

particle is governed by the

by ...

Moreover, because the necessity of dissipating also a large amount of angular

momentum, gammarays are emitted. iii) The

**probability**for emitting a givenparticle is governed by the

**space**phase volume and by the level density, but notby ...

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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 | |

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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