By Tony Duff

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29]. 35] coupled with a modified ALICE-91 code. In this approach the Udagwa and Tamura model was used to deduce the spectra of neutrons and protons transferred into the target nucleus (stripping to bound states and breakup-capture in the continuum); these were then assumed to initiate three-quasiparticle cascades. The deuteron cross-section that does not undergo stripping and breakup-capture was assumed to initiate a separate preequilibrium cascade. Detailed calculations were done for deuteron induced reactions on 48Ti in order to 32 empirically select the best initial exciton number to use for deuteron induced reactions.

There are two types of multiple precompound decay which might be considered. Type I results when a nucleus emits more than one exciton from a single exciton hierarchy. g. in a two particle-one-hole configuration, up to two particles could be emitted; in a three particle-two-hole configuration up to three particles could be emitted, etc. ” If the intervening two-body transitions are omitted from this sequence, it becomes type I multiple emission. In the type II sequence for nucleon induced reactions, the leading term would be two particle-two-hole.

For references to the experimental data. 44 Fig. 7. 127I(p,3n)125Xe reaction, an example of a good fit. ALICE-IPPE calculation from Obninsk is shown as a fit to selected data. 11. for references to the experimental data. In this section we discussed the general features of the modeled cross-sections and the quality of fit to the data. We described calculations by four different groups using mostly global parameters. We identified several deficiencies in reaction formalisms used in the calculations.

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A Song of Milarepa 1 - Milarepa and the Geshe in Drin by Tony Duff


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