## Nuclear structure and heavy-ion dynamics: Varenna on Lake Como, Villa Monastero, 27 July-6 August 1982 |

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Page 256

the complete-fusion reaction for which the

slower than the total reaction

for fusion has been exceeded. If one, therefore, introduces an « effective critical ...

the complete-fusion reaction for which the

**cross**-**section**still keeps rising, thoughslower than the total reaction

**cross**-**section**, after the critical angular momentumfor fusion has been exceeded. If one, therefore, introduces an « effective critical ...

Page 270

Whereas the break-up fusion models are dynamical models, the sum rule model

is a static model that deals with the partition of

assumed that fusion and incomplete fusion are the only processes that occur for ...

Whereas the break-up fusion models are dynamical models, the sum rule model

is a static model that deals with the partition of

**cross**-**sections**. In this model it isassumed that fusion and incomplete fusion are the only processes that occur for ...

Page 393

2), the differential

QE

damped component at 6 MeV/nucleon and by far dominant at 13.5 MeV/nucleon.

2), the differential

**cross**-**section**is strongly forward peaked. The angle-integratedQE

**cross**-**section**, excluding elastic scattering, is comparable to that of thedamped component at 6 MeV/nucleon and by far dominant at 13.5 MeV/nucleon.

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### Contents

Introduction | 3 |

Relation with the collective model | 12 |

A Faesslee Competition between collective and singlepar | 30 |

Copyright | |

33 other sections not shown

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### 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