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

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Page 77

This technique makes use of an array of small TJal

and the M -distributions are deduced from measured Pnj-fold probabilities, where

p is the number of !NaI

...

This technique makes use of an array of small TJal

**detectors**, as shown in fig. 8,and the M -distributions are deduced from measured Pnj-fold probabilities, where

p is the number of !NaI

**detectors**which fired per event (fold) and n is the number...

Page 139

We have solved the solid-angle problem by building moderately large

15 cm x 15 cm x 100 cm, and using six at a time. The use of such large

requires some form of time compensation, because the flight time variations of ...

We have solved the solid-angle problem by building moderately large

**detectors**,15 cm x 15 cm x 100 cm, and using six at a time. The use of such large

**detectors**requires some form of time compensation, because the flight time variations of ...

Page 140

It also depends on the energy threshold setting of the

can be eliminated by setting the threshold above the highest energy that the wrap

-around neutrons can deposit in the

It also depends on the energy threshold setting of the

**detector**. This backgroundcan be eliminated by setting the threshold above the highest energy that the wrap

-around neutrons can deposit in the

**detector**. Eaising the threshold ...### What people are saying - Write a review

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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