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

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Page 392

of that

discussed next ) , evaluating the many - particle matrix elements H , NJT , and

diagonalizing the resulting H matrix to get the eigenvectors YnJt and their ...

of that

**space**, choosing the proper Hamiltonian operator for the**space**( to bediscussed next ) , evaluating the many - particle matrix elements H , NJT , and

diagonalizing the resulting H matrix to get the eigenvectors YnJt and their ...

Page 393

The number of 2bme is arrived at by determining all Pauli - allowed two - body

states in the

coupled J and T . ( The Hamiltonian is assumed to conserve J and T . ) It is an

almost ...

The number of 2bme is arrived at by determining all Pauli - allowed two - body

states in the

**space**and combining all pairs which have the same two - particlecoupled J and T . ( The Hamiltonian is assumed to conserve J and T . ) It is an

almost ...

Page 395

Here , the effective Hamiltonian for use in a particular model

in so far as is possible a priori from the information available from study of the two

- nucleon problem [ 23 - 25 ) . The problems inherent in this type of procedure ...

Here , the effective Hamiltonian for use in a particular model

**space**is calculatedin so far as is possible a priori from the information available from study of the two

- nucleon problem [ 23 - 25 ) . The problems inherent in this type of procedure ...

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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 | |

28 other sections not shown

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### Common terms and phrases

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