## Nuclear Structure and Heavy-ion Dynamics: Varenna on Lake Como, Villa Monastero, 27 July-6 August 1982, Volume 87 |

### From inside the book

Results 1-3 of 49

Page 196

The distance between the two reactants in a collision is such a

. The second class of

sometimes they are referred to as the « bath » ) . Their coupling to the collective ...

The distance between the two reactants in a collision is such a

**degree of freedom**. The second class of

**degrees of freedom**is the « internal » ( microscopic ) set (sometimes they are referred to as the « bath » ) . Their coupling to the collective ...

Page 275

The change of the relative momentum ( ur ) is given by a conservative force ( -

V V ( r ) ) plus a friction force ( - yr ) which describes the energy loss due to the

coupling to the internal

( the ...

The change of the relative momentum ( ur ) is given by a conservative force ( -

V V ( r ) ) plus a friction force ( - yr ) which describes the energy loss due to the

coupling to the internal

**degrees of freedom**plus a rapidly fluctuating force 8F ( t )( the ...

Page 276

This is necessary to obtain equilibration in internal

scale which is smaller than the one for collective variables . 2 . – Macroscopic

variables . 2 ' 1 . Shape

This is necessary to obtain equilibration in internal

**degrees of freedom**on a timescale which is smaller than the one for collective variables . 2 . – Macroscopic

variables . 2 ' 1 . Shape

**degrees of freedom**. – If the relative velocity of the two ...### What people are saying - Write a review

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### Contents

Introduction | 3 |

Relation with the collective model | 12 |

A FAESSLER Competition between collective and singlepar | 30 |

Copyright | |

36 other sections not shown

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### Common terms and phrases

alignment analysis angle angular distributions angular momentum approximation assumed asymmetry average band barrier beam calculated channel collective collisions component compound consider contributions corresponding coupling cross-section curve decay defined deformation dependence described detector determined direct discussed effect elements emission energy equations evaporation excitation excitation energy expected experiment experimental expression Figure fission fluctuations force fragment function fusion given heavy heavy-ion increase indicated inelastic interaction Legnaro Lett light limit mass mean measured method modes motion neutron Nucl nuclear nuclei nucleons observed obtained operator pairs parameters particles Phys polarization possible potential predictions present probability Q-value reaction region relative residues respectively rotational scattering shape shell shows similar space spectra spin statistical strength structure surface tion trajectory transfer transitions values width y-ray