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

### From inside the book

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Page 84

... then recalculate h hoping for some convergence. In practice the Hartree-Fock

single-particle states (i, j, ...) are often

single-particle states (x, B, ...) usually chosen to be those of a spherical oscillator.

... then recalculate h hoping for some convergence. In practice the Hartree-Fock

single-particle states (i, j, ...) are often

**represented**in terms of a complete set ofsingle-particle states (x, B, ...) usually chosen to be those of a spherical oscillator.

Page 194

For a nucleus with no angular momentum the fission barrier is

For some value of J the rotational energy E. = Joh”/2.9 is larger in the spherical

shape than in the deformed shape since the momentum of inertia J., is smaller for

...

For a nucleus with no angular momentum the fission barrier is

**represented**by B,.For some value of J the rotational energy E. = Joh”/2.9 is larger in the spherical

shape than in the deformed shape since the momentum of inertia J., is smaller for

...

Page 206

... 5O - IOO 15O 200 |CO 150 2OO 250 EcM (MeV) EcM (MeV) Fig. 34. —

Complete-fusion cross-section vs. kinetic energy for two systems: a) (*Ar-I-77Se),

b) ("Ar-i-lo"Sb). Experimental values of ocesatà" in h” units are

triangles.

... 5O - IOO 15O 200 |CO 150 2OO 250 EcM (MeV) EcM (MeV) Fig. 34. —

Complete-fusion cross-section vs. kinetic energy for two systems: a) (*Ar-I-77Se),

b) ("Ar-i-lo"Sb). Experimental values of ocesatà" in h” units are

**represented**bytriangles.

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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