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

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Page 114

The

. 15 ) cannot be basis states according to rule I ) , but only intermediate states .

The quantities Šiem are the amplitudes of the

The

**physical**states are to be written as ( 6 . 16 ) Iqm ) = figmini = 1 ; m , 1 ) , as ( 6. 15 ) cannot be basis states according to rule I ) , but only intermediate states .

The quantities Šiem are the amplitudes of the

**physical**state in the different ...Page 117

On the other hand , the agreement between the exact and the nuclear - field -

theoretical results shows that the effects of those spurious states are eliminated

from all the matrix elements associated with

follows ...

On the other hand , the agreement between the exact and the nuclear - field -

theoretical results shows that the effects of those spurious states are eliminated

from all the matrix elements associated with

**physical**observables . In whatfollows ...

Page 120

13 ) Vi + 1 1 and ( 7 . 14 ) G + ( E – £m - V ) - , the result ( 1 . 3 ) can be directly

utilized . Thus 2 43 ( 7 . 15 ) E - Em — V = F ( E ) - 1W , - E n = is the dispersion

relation fixing the energies Egm of the

...

13 ) Vi + 1 1 and ( 7 . 14 ) G + ( E – £m - V ) - , the result ( 1 . 3 ) can be directly

utilized . Thus 2 43 ( 7 . 15 ) E - Em — V = F ( E ) - 1W , - E n = is the dispersion

relation fixing the energies Egm of the

**physical**states . There is one equation for...

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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