Nuclear structure and heavy-ion dynamics: Varenna on Lake Como, Villa Monastero, 27 July-6 August 1982 |
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Page 37
This can be understood by the residual interaction. The particle-hole interaction
is repulsive and of short range. If we take the zero- B 10 12 14 16 18 20 a-nguLar
momentum I Fig. 5. - Energy difference EI+1 — E, of the odd-even angular ...
This can be understood by the residual interaction. The particle-hole interaction
is repulsive and of short range. If we take the zero- B 10 12 14 16 18 20 a-nguLar
momentum I Fig. 5. - Energy difference EI+1 — E, of the odd-even angular ...
Page 114
Varenna on Lake Como, Villa Monastero, 27 July-6 August 1982 L. Moretto, R. A.
Ricci, Società italiana di fisica. The pairing and residual interaction parameters
deduced for «M«Yb are given in table II. It is seen that this analysis gives a very ...
Varenna on Lake Como, Villa Monastero, 27 July-6 August 1982 L. Moretto, R. A.
Ricci, Società italiana di fisica. The pairing and residual interaction parameters
deduced for «M«Yb are given in table II. It is seen that this analysis gives a very ...
Page 407
Eotational bands of the heavy fragments dominate the y-ray spectra recorded
with a Ge(Li) detector in coincidence with the light fragments. Using known decay
schemes, one may extract from the coincidence yields i) the distribution of
residual ...
Eotational bands of the heavy fragments dominate the y-ray spectra recorded
with a Ge(Li) detector in coincidence with the light fragments. Using known decay
schemes, one may extract from the coincidence yields i) the distribution of
residual ...
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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