Titlebook: Interacting Bosons in Nuclear Physics; F. Iachello Book 1979 Springer Science+Business Media New York 1979 Boson.electron.neutron.nuclear

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Collective Properties of Nuclear States in the A～ 150 Transitional Region and the Interacting Boson e of the attractive features of the Interacting Boson Model 1, 2 is that it attempts to do just that in a relatively simple and physically transparent way. It is thus of general interest to test this description by carrying out numerical calculations for a number of observables for e.g. a set of iso

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Systematics of Experimental Properties of Low-Lying States in Even Ru and Pd Nuclei. This is clearly reflected in the energy systematics of the positive parity states presented in fig. 1. In this figure only states with highly reliable spin assignments are given. Thus a number of states with positive parity are omitted especially in the energy region 1–2 MeV.

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B(E2)-Values of High Spin States in 158DYllective behavior of a nucleus and becomes a dominant feature at high spins. A definite test of this prediction is the behavior of the B(E2)-values in the ground state band of rotational like nuclei. The SU(3)-approximation predicts in zero order a cutoff-factor (2N-J) (2N+J+3) (J is the nuclear spi

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Shell Model Tests of the Interacting Boson Model Description of Nuclear Collective Motion valence protons and neutrons defined with respect to a major shell closure. The eigenstates of the proton (neutron) systems are assumed to be constructed purely from combining two-particle “bosons” with L = 0 and L = 2 to form many-particle states. The model is capable of handling nuclear systems w

Bombast

Electron Scattering in the Interacting Boson Modele symmetry aspects of the model have been emphasized. It was shown that the Hamiltonian can be expressed in terms of the generators of the SU(6) group, and in special cases in terms of subgroups of SU(6); the application of group theoretical methods then provides an elegant and simple description of

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