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

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Page 21

Thus , the separation between the degenerate orbits that occurs for finite wrot

particular , the K = 1 / 2 orbits exhibit a separation that is linear in wo and the

coefficient ...

Thus , the separation between the degenerate orbits that occurs for finite wrot

**gives**the signaturedependent term in the rotational energy ( see ( 13 ) ) . Inparticular , the K = 1 / 2 orbits exhibit a separation that is linear in wo and the

coefficient ...

Page 316

The choice k = 2

deformation analogous to the hydrodynamical or Tassie model for the density .

The latter is frequently used for electron scattering analyses . When eq . ( 23 ) is ...

The choice k = 2

**gives**the distribution a uniform radial strain , while k = L**gives**adeformation analogous to the hydrodynamical or Tassie model for the density .

The latter is frequently used for electron scattering analyses . When eq . ( 23 ) is ...

Page 326

The choice k = 1

analyses of electron scattering data . ... These prescriptions usually

to the electron inelastic scattering unless data are available for large momentum

...

The choice k = 1

**gives**the Tassie model [ 106 ] , which is frequently used inanalyses of electron scattering data . ... These prescriptions usually

**give**good fitsto the electron inelastic scattering unless data are available for large momentum

...

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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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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