## Proceedings of the International School of Physics "Enrico Fermi.", Volume 69N. Zanichelli, 1977 - Nuclear physics |

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Page 144

To make the slabs move , one must impose an initial condition on the total wave

function , multiplying the static total wave function by a phase exp [ imvZ ] , with Z

the center - of -

To make the slabs move , one must impose an initial condition on the total wave

function , multiplying the static total wave function by a phase exp [ imvZ ] , with Z

the center - of -

**mass**co - ordinate , Z = { xi , M the total**mass**M = mA , and v the ...Page 403

Hence , comparisons of calculated and experimental total binding energies are

most meaningful in situations where the model Hamiltonian has some a priori

significance or where the range of

Hence , comparisons of calculated and experimental total binding energies are

most meaningful in situations where the model Hamiltonian has some a priori

significance or where the range of

**masses**considered is large enough to allow ...Page 515

Since such quantities as the effective

very sensitive to the choice of the interaction , comparison with experiment will

enable us to discriminate between different possible parametrizations of the

effective ...

Since such quantities as the effective

**mass**or the nuclear compressibility arevery sensitive to the choice of the interaction , comparison with experiment will

enable us to discriminate between different possible parametrizations of the

effective ...

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### Contents

A BOHR Some aspects of rotational motion | 3 |

B R MOTTELSON Elementary excitations in the nucleus | 42 |

R BÉs and R A BROGLIA Nuclear superfluidity | 55 |

Copyright | |

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### Common terms and phrases

addition angular momentum appears approximation associated backbending band calculated closed collective compared comparison components configurations considered contributions corresponding coupling cross-sections deformation density dependence describe determined discussed distribution effects electron equations estimate evidence example excitation energy expected experiment experimental expression fact factor field given gives ground Hamiltonian hole included increase indicate inertia interaction Lett levels limit mass matrix elements measured modes moments motion neutron Nucl nuclear nuclei nucleons observed obtained operator orbits oscillator pairing parameters particle particular peak Phys physical possible potential predictions present processes protons quadrupole reaction region relation relative resonance respect rotational rule scattering seen shape shell model shown in fig shows simple single single-particle space spectra spectrum strength structure surface symmetry theory tion transfer transition values vibrational wave functions