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

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Page 369

pronounced angular dependence of the intensities. It is because the initial states

are strongly aligned (m & 0) and the alignment is kept till the end of cascades.

**Angular distribution**of gamma-rays. – The prompt gamma-rays usually show apronounced angular dependence of the intensities. It is because the initial states

are strongly aligned (m & 0) and the alignment is kept till the end of cascades.

Page 436

quasi-elastic ) and « deep inelastic transfers) are also clearly shown by the

...

**Angular distributions**. – The two mechanisms occurring in these reactions (i.e.quasi-elastic ) and « deep inelastic transfers) are also clearly shown by the

**angular distributions**. T T T I r— H- T T + T 208 *oco .208Pb 288 MeV | 0 O Cu |-|-f...

Page 509

In the case of H.I. the angular momentum involved is quite high. For example in

the ... Under these conditions the Y-ray

with the formula - W(0) = 1 + x, A. P. (cos()) + ox, A. P. (cos 0). The coefficients or

...

In the case of H.I. the angular momentum involved is quite high. For example in

the ... Under these conditions the Y-ray

**angular distribution**has to be analysedwith the formula - W(0) = 1 + x, A. P. (cos()) + ox, A. P. (cos 0). The coefficients or

...

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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