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

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Page 143

The stationary HF solutions have a trivial time dependence

y ( r , t ) = exp [ - iɛnt ] or ( r ) , where the stationary single - particle functions are

The stationary HF solutions have a trivial time dependence

**given**by ( h = 1 ) ( 3 )y ( r , t ) = exp [ - iɛnt ] or ( r ) , where the stationary single - particle functions are

**given**by ht " on ( r ) = EnQn ( r ) . These stationary HF equations are nonlinear ...Page 375

In a

L = 2 level ( d - bosons ) . In the ground states of vibrational nuclei , all bosons

are in the L = 0 level . The first excited J = 2 level is obtained by raising one of ...

In a

**given**nucleus , N bosons can be either in the L = 0 level ( s - bosons ) or in aL = 2 level ( d - bosons ) . In the ground states of vibrational nuclei , all bosons

are in the L = 0 level . The first excited J = 2 level is obtained by raising one of ...

Page 477

As Ê is a straight line , the iterative procedure to determine õ for a

) , correspondingly for Z and ( 10 ) , can be replaced by an interpolation between

different I to obtain the smooth energy for

As Ê is a straight line , the iterative procedure to determine õ for a

**given**I from ( 9) , correspondingly for Z and ( 10 ) , can be replaced by an interpolation between

different I to obtain the smooth energy for

**given**1 . The shell energy is then for a ...### 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 |

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