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

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Page 159

+ 2 +" 7 12 90 p 6 90 - LANG and LECOUTEUR [32] have made a correction to

the equation of state E*=(to/6) goto —t by considering that g, Ag, ; a = (to/6)g, is

called the

+ 2 +" 7 12 90 p 6 90 - LANG and LECOUTEUR [32] have made a correction to

the equation of state E*=(to/6) goto —t by considering that g, Ag, ; a = (to/6)g, is

called the

**level**density parameter. 3'2.**Levels**of angular momentum ...Page 164

Then one can calculate the ground-state energy E, by summing all energy

The state density is derived with the usual formalism of the grand partition

function, the energy of the single-particle

with m ...

Then one can calculate the ground-state energy E, by summing all energy

**levels**.The state density is derived with the usual formalism of the grand partition

function, the energy of the single-particle

**level**being defined as eone – m + köwith m ...

Page 167

yrast

corresponding angular momentum. It is very easy to calculate E. – = J(J -- 1) hos2

.f.a. for a rigid rotor. However the result can only be taken as a qualitative ...

yrast

**levels**puts a limitation for the formation of a compound nucleus with thecorresponding angular momentum. It is very easy to calculate E. – = J(J -- 1) hos2

.f.a. for a rigid rotor. However the result can only be taken as a qualitative ...

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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