Nuclear structure and heavy-ion dynamics: Varenna on Lake Como, Villa Monastero, 27 July-6 August 1982 |
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Page 5
The oscillator Hamiltonian is then given by (1) fitted* <!, + -&» = ha>(d+-d~) +-h(o,
i„ = (- l)"d-„ . pi l The collective Hamiltonian with any potential can be expressed in
terms of the d-boson operators d+, d^ and its solutions obtained in this boson ...
The oscillator Hamiltonian is then given by (1) fitted* <!, + -&» = ha>(d+-d~) +-h(o,
i„ = (- l)"d-„ . pi l The collective Hamiltonian with any potential can be expressed in
terms of the d-boson operators d+, d^ and its solutions obtained in this boson ...
Page 13
If the potential of the collective Hamiltonian has a minimum at 0, y0 = 0, rotational
bands with L(L + 1) energy dependence arise only to the extent that rotation-
vibration interaction can be ignored. Deviations from L(L + 1) dependence and
the ...
If the potential of the collective Hamiltonian has a minimum at 0, y0 = 0, rotational
bands with L(L + 1) energy dependence arise only to the extent that rotation-
vibration interaction can be ignored. Deviations from L(L + 1) dependence and
the ...
Page 530
a two-body boson Hamiltonian in the corresponding s-d space can be sufficient
to do the job. A simple way of looking at the problem is to try to exploit the
possibility of mapping the pair r onto a boson y and of describing the ground-
state ...
a two-body boson Hamiltonian in the corresponding s-d space can be sufficient
to do the job. A simple way of looking at the problem is to try to exploit the
possibility of mapping the pair r onto a boson y and of describing the ground-
state ...
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Contents
Introduction | 3 |
Relation with the collective model | 12 |
A Faesslee Competition between collective and singlepar | 30 |
Copyright | |
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a-particle alignment amplitude angle angular distributions angular momentum anisotropy approximation band barrier beam bombarding energy boson calculated Casimir operator classical trajectory coincidence collisions component compound nucleus configuration corresponding Coulomb Coulomb barrier coupling cross-section curve decay deep inelastic deformation degrees of freedom detector dissipation edited effect eigenstates ejectiles emission equations evaporation excitation energy excitation functions exit channel experimental Fermi Fermi surface fermion fission fluctuations fragment spin given Hamiltonian incomplete fusion inertia interaction kinetic energy Lett matrix elements measured momenta neutron neutron emission Nucl nuclear nuclei nucleons observed obtained orbital pairing parameters particles phase space Phys polarization potential probability projectile proton Q-value quadrupole quantum number quasi-particle region residual resonance rotational saddle point scattering shape shell model shown in fig shows single-particle spectra spectrum statistical structure target tion transfer transitions values velocity width y-ray yrast zero