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

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Page 10

There are only three parameters in the 06 Hamiltonian , those that multiply Q ' Q '

and the scalar products of the k = 1 and k = 3 generators with themselves . In the

There are only three parameters in the 06 Hamiltonian , those that multiply Q ' Q '

and the scalar products of the k = 1 and k = 3 generators with themselves . In the

**present**case ( dt . d ) ( or sts ) do not commute with Q ' Q ' and the single sand d ...Page 182

... reactions between heavy nuclei . 2 . - Quasi - elastic reactions between heavy

ions . In the

as a spectroscopic tool for the study of nuclear properties at low excitation ...

... reactions between heavy nuclei . 2 . - Quasi - elastic reactions between heavy

ions . In the

**present**section , I would like to discuss reactions between heavy ionsas a spectroscopic tool for the study of nuclear properties at low excitation ...

Page 505

V which is in the

collision time is an order of magnitude shorter than the lifetime of the compound

nucleus , which means that the fine structure , statistical fluctuation , is weakly ...

V which is in the

**present**alpha scattering experiment 0 . 8 . 10 - 21 8 . Thus thecollision time is an order of magnitude shorter than the lifetime of the compound

nucleus , which means that the fine structure , statistical fluctuation , is weakly ...

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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