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

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Results 1-3 of 54

Page 99

States with one pair

r = - n , pairs , the states with one pair

quanta are of the form ( n . tit . + 1 , 11 ; TT , ) and can be obtained by acting ...

States with one pair

**addition**and several pair removal modes . For a system withr = - n , pairs , the states with one pair

**addition**quantum and several pair removalquanta are of the form ( n . tit . + 1 , 11 ; TT , ) and can be obtained by acting ...

Page 101

Transitions involving proton

same isospin as the ground state are also given in fig . 15 . Two strong states

have been observed in some nuclei . One of these states is the proton pairing

vibration ...

Transitions involving proton

**addition**phonons and leading to states with thesame isospin as the ground state are also given in fig . 15 . Two strong states

have been observed in some nuclei . One of these states is the proton pairing

vibration ...

Page 105

For the Fe pair

experimental ratios are 1 : 1 . 3 : 1 . 9 , while the theoretical ratios are 1 : 2 : 3 .

The Cr pair

with ...

For the Fe pair

**addition**band ( 4Fe → A + 2Fe ( gs ) ; A = 54 , 56 and 58 ) theexperimental ratios are 1 : 1 . 3 : 1 . 9 , while the theoretical ratios are 1 : 2 : 3 .

The Cr pair

**addition**band intensity ratio on the other hand is 1 : 2 , which agreeswith ...

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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