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

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Page 164

... t ) and assume that we can parameterise them in terms of a few variables u ; ( t ) , i.e. ( 39 ) yn ( e , t ) — 4 , ( u ( t ) , « ) . The set of

... t ) and assume that we can parameterise them in terms of a few variables u ; ( t ) , i.e. ( 39 ) yn ( e , t ) — 4 , ( u ( t ) , « ) . The set of

**parameters**u ; ( t ) are time dependent and the Lagrangian is now of the form ( 40 ) ...Page 242

+ The matrix elements ( 15a ) vanish for Ug = U , ( e.g. , the decoupling

+ The matrix elements ( 15a ) vanish for Ug = U , ( e.g. , the decoupling

**parameter**in K = 1 bands ) , while they are ... element is largest for the diagonal matrix elements ( such as the ones appeared in decoupling**parameters**) .Page 397

Hence it is possible to make the linearization approximation that the di are constants , solve for the new 2bme and spe , and then iterate this procedure until a stable solution of Hamiltonian

Hence it is possible to make the linearization approximation that the di are constants , solve for the new 2bme and spe , and then iterate this procedure until a stable solution of Hamiltonian

**parameters**is obtained .### What people are saying - Write a review

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### Contents

Rotational degrees of freedom Deformation and | 3 |

86 | 8 |

the framework of a course such as the present The topics selected by | 10 |

Copyright | |

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addition angular momentum appears approximation associated backbending band calculated closed collective compared comparison components configurations consider 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 motion neutron Nucl nuclear nuclei nucleons observed obtained operator orbits oscillator pairing parameters particle particular peak Phys physical possible potential predictions present processes proton 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 strong structure surface symmetry theory tion transfer transition values vibrational wave functions