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

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Page 166

The wave function in this case is a function of two parameters , p and q , and the

exp [ ip ] | Ý ) . If we define the operator Á = exp [ - ipQ ] H exp [ ip ] , we see that

this ...

The wave function in this case is a function of two parameters , p and q , and the

**Hamiltonian**is ( 48 ) H ( p , q ) = ( ( p , q ) | H | ¥ ( p , q ) ) = ( Ý ( ) sexp [ - ipQ ] Hexp [ ip ] | Ý ) . If we define the operator Á = exp [ - ipQ ] H exp [ ip ] , we see that

this ...

Page 395

The message of the preceding discussion of the one - body part of the shell

model

constitutes the fundamental problem to be solved in carrying out a calculation .

Techniques ...

The message of the preceding discussion of the one - body part of the shell

model

**Hamiltonian**has been that the determination of the two - body partconstitutes the fundamental problem to be solved in carrying out a calculation .

Techniques ...

Page 397

Thus after obtaining H as described above , this new

again obtain a full set of eigenvectors YNT . ... One of the

was utilized to obtain the results to be discussed in the following pages was

obtained by ...

Thus after obtaining H as described above , this new

**Hamiltonian**is used toagain obtain a full set of eigenvectors YNT . ... One of the

**Hamiltonians**whichwas utilized to obtain the results to be discussed in the following pages was

obtained by ...

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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