Neutron Induced Reactions: Proceedings of the 4th by P. E. Hodgson (auth.), J. Krištiak, E. Běták (eds.)

By P. E. Hodgson (auth.), J. Krištiak, E. Běták (eds.)

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Additional info for Neutron Induced Reactions: Proceedings of the 4th International Symposium Smolenice, Czechoslovakia, June 1985

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The initial linear momentum of the excitons is rather high as is seen in Fig. 7 and reduction of the level density 27 occurs because of the small phase space due to the small number of combination with respect to the momentum. After the emission of fast particle in the forward direction, the momentum of residual nucleus is reduced depending on the energy and angle of emitted particle. As a result, the momentum-dependent fac~or of reSidual nucleus becomes much larger than the pre-emission system.

OR and fusion. take place outside the barrier. Thus. there remains no room to introduce the concept of barrier penetration. On the other hand. we remarked above that fission and fusion are inversely related. and for the former concept of barrier penetration is known to be vital. Does this mean that there is something wrong in our understanding of fusion? There is actually no problem. There is not much room to discuss this in detail here. and we want to refer the reader to our recent paper /16/.

In the calculation of Figs. 8 and 9, the initial exciton number is 4-particle 4-hole state (target source emission is negligible as far as forward emission of fast particle is concerned). The excitation energy is about 65 MeV and exciton state till the 8-particle 8-hole state is included in the calculation. The most part of the fast particle is coming from the first 2 steps, as was the case of light ion reaction both for nucleon and alpha emission. The main term of alpha emission is two-particle pick-up type reaction and the next term is the three-particle pick-up term and these two terms domina·te the cross-section.

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