Nuclear structure and heavy-ion dynamics: Varenna on Lake Como, Villa Monastero, 27 July-6 August 1982 |
From inside the book
Results 1-3 of 80
Page 93
can be observed. The y-y correlation experiments have been discussed in detail
many times before [21, 25-27], and we shall, therefore, here only mention a few of
the most significant features which can be recognized and extracted from the ...
can be observed. The y-y correlation experiments have been discussed in detail
many times before [21, 25-27], and we shall, therefore, here only mention a few of
the most significant features which can be recognized and extracted from the ...
Page 135
This is observed to be highly fragmented, consistent with pick-up reaction data [
15]. It is apparent from the (p, n) spectrum shown in fig. 4 and 5 that the lowest d.
hole state contains only a small part of the d} hole strength. It is difficult to define ...
This is observed to be highly fragmented, consistent with pick-up reaction data [
15]. It is apparent from the (p, n) spectrum shown in fig. 4 and 5 that the lowest d.
hole state contains only a small part of the d} hole strength. It is difficult to define ...
Page 242
Projectilelike reaction products are observed with about beam velocity
approximately satisfying the optimum Q-value relation of Siemens et al. [4]. In
contrast to reactions with heavier projectiles and involving more symmetric
nucleus-nucleus ...
Projectilelike reaction products are observed with about beam velocity
approximately satisfying the optimum Q-value relation of Siemens et al. [4]. In
contrast to reactions with heavier projectiles and involving more symmetric
nucleus-nucleus ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
Introduction | 3 |
Relation with the collective model | 12 |
A Faesslee Competition between collective and singlepar | 30 |
Copyright | |
33 other sections not shown
Other editions - View all
Common terms and phrases
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