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

### From inside the book

Results 1-3 of 72

Page 240

73 for [ 633 7 / 2 ] - [ 624 9 / 2 ] one gets the value of the

seventh column of table II , from the comparison of the calculated matrix elements

with the measured B ( E2 ) values . Experimental B ( E2 ) values are taken from

ref .

73 for [ 633 7 / 2 ] - [ 624 9 / 2 ] one gets the value of the

**factor**n shown in theseventh column of table II , from the comparison of the calculated matrix elements

with the measured B ( E2 ) values . Experimental B ( E2 ) values are taken from

ref .

Page 249

+ w3 ) ) may be neglected in the estimate of gle ) , but they must be included in

the evaluation of both g ) and D ( or the reduction

strength ) . Without inclusion of the AN = 2 excitation modes , both the Migdal

term ...

+ w3 ) ) may be neglected in the estimate of gle ) , but they must be included in

the evaluation of both g ) and D ( or the reduction

**factor**of the Coriolis couplingstrength ) . Without inclusion of the AN = 2 excitation modes , both the Migdal

term ...

Page 502

However , because an assumed form

model dependent , and a superposition of other multipoles may yield a similar

pattern . A more important disadvantage is the very large continuous background

which ...

However , because an assumed form

**factor**enters into the calculation , it ismodel dependent , and a superposition of other multipoles may yield a similar

pattern . A more important disadvantage is the very large continuous background

which ...

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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