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

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Page 314

13 - 15 . ) The Bu so

( 6 ) . This limit is often estimated by using R = 1 . 2A fm in eq . ( 6 ) , although

sometimes the empirical ( p2L - ? ) of the proton distribution (

electron ...

13 - 15 . ) The Bu so

**obtained**are then compared to the EWSR limit given by eq .( 6 ) . This limit is often estimated by using R = 1 . 2A fm in eq . ( 6 ) , although

sometimes the empirical ( p2L - ? ) of the proton distribution (

**obtained**fromelectron ...

Page 377

The same expression would result for the state ( s * ) " 10 ) , where st is a boson

creation operator , by using that part of the IBA Hamiltonian relevant for

vibrational nuclei ( 39 ) Vosts + } Astst88 . The result ( 29 ) was

shell model ...

The same expression would result for the state ( s * ) " 10 ) , where st is a boson

creation operator , by using that part of the IBA Hamiltonian relevant for

vibrational nuclei ( 39 ) Vosts + } Astst88 . The result ( 29 ) was

**obtained**from ashell model ...

Page 397

Thus after

again

was utilized to

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 ...### What people are saying - Write a review

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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 |

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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