## Proceedings of the International School of Physics "Enrico Fermi.", Volume 62N. Zanichelli, 1976 - Nuclear physics |

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Page 107

What we must

effective Hamiltonian is only part of the real kinetic - energy operator — the

remaining part is absorbed in the effective residual interaction . Thus , although

one cannot ...

What we must

**consider**however is that the kinetic - energy operator of theeffective Hamiltonian is only part of the real kinetic - energy operator — the

remaining part is absorbed in the effective residual interaction . Thus , although

one cannot ...

Page 115

It was soon realized however that one must

one is to understand spectra . Now , instead of trying to

residual interaction , we choose at first only that part that contributes towards the

...

It was soon realized however that one must

**consider**the residual interaction ifone is to understand spectra . Now , instead of trying to

**consider**the whole of theresidual interaction , we choose at first only that part that contributes towards the

...

Page 124

( 5.96 ) In

only the renormalization to the matrix elements of the ( 80 ) -representation , i.e.

we

( 5.96 ) In

**considering**the renormalization of the full potential ve we**consider**firstonly the renormalization to the matrix elements of the ( 80 ) -representation , i.e.

we

**consider**only the states | a80L ) . We put a label a in the state to remind ...### What people are saying - Write a review

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### Contents

Introduction | 1 |

Generator coordinate DWBA for heavy ions | 8 |

Simple ideas on reaction mechanisms | 19 |

Copyright | |

44 other sections not shown

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### Common terms and phrases

angle angular distribution angular momentum approximation assumed average band barrier calculation channel cluster collision complete compound nucleus configurations consider core corresponding Coulomb coupling cross-section curve decay defined deformation depends described direct discussed distance effective elastic scattering emission emitted example excitation energy excitation function expected experimental experiments expression factor final fission fragments given gives Hamiltonian Hartree-Fock heavy ions higher integral interaction interesting internal level density levels mass matrix elements means measured mechanism neutron nuclear nucleons observed obtained operator optical orbital oscillator parameter particle Phys possible potential present probability projectile reaction region relative residual resonances respectively rotational scattering shape shell model shown simple single-particle space spectra spectrum structure surface theory tion transfer transition values wave function X-rays yrast