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

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Page 200

If we replace the distribution f(K) by the

K. and g(J) by the

parameter can be expressed as p = J./4K., and appears in the expression of ...

If we replace the distribution f(K) by the

**average**value of a Gaussian distributionK. and g(J) by the

**average**value of a linear distribution J., the**average**anisotropyparameter can be expressed as p = J./4K., and appears in the expression of ...

Page 454

We shall consider two particular properties of fragment excitation energies, which

show typical statistical aspects of the scission process. a)

In 1965 LANG [9] performed an accurate analysis of the neutron cascade ...

We shall consider two particular properties of fragment excitation energies, which

show typical statistical aspects of the scission process. a)

**Average**temperature.In 1965 LANG [9] performed an accurate analysis of the neutron cascade ...

Page 455

from formulae (4), (5), (6) we obtain the

the

for *U slow-neutron fission and *U fission induced by 13 MeV protons [10, 11].

from formulae (4), (5), (6) we obtain the

**average**temperature T corresponding tothe

**average**excitation energy U. Figures 1 and 2 show the values of T obtainedfor *U slow-neutron fission and *U fission induced by 13 MeV protons [10, 11].

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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