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

### From inside the book

Results 1-3 of 72

Page 112

the latter being the expectation value of the exchange mixture in two-body states

with isospin, spin values T and S. For an N = Z even-even nucleus, the Hartree-

Fock field of H, is exactly that of a deformed harmonic

the latter being the expectation value of the exchange mixture in two-body states

with isospin, spin values T and S. For an N = Z even-even nucleus, the Hartree-

Fock field of H, is exactly that of a deformed harmonic

**oscillator**. The exchange ...Page 116

ever just yields an

variation after projection Hartree-Fock calculation reduces to finding the

expectation value of H, in projected states from

varying ...

ever just yields an

**oscillator**with a different 6- and v-deformation. Thus thevariation after projection Hartree-Fock calculation reduces to finding the

expectation value of H, in projected states from

**oscillator**intrinsic states withvarying ...

Page 120

Amplitude of the spherical-

amplitudes of Xo plus 2ho excited states in the deformed

Shown as a function of deformation 6. The shape consistent deformation is

shown by the ...

Amplitude of the spherical-

**oscillator**state xo (eq. (4.3) with 0 = 0) and sum ofamplitudes of Xo plus 2ho excited states in the deformed

**oscillator**state X3.Shown as a function of deformation 6. The shape consistent deformation is

shown by the ...

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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