1983
DOI: 10.1007/bf01419519
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Two-component exciton model

Abstract: The exciton model of nuclear reactions with the distinguishability of protons and neutrons explicitly included is discussed. The Pauli master equation and transition rates in this two-component formulation are given. Both the simple considerations and actual calculations show that the two-component model exhibits new features and modifies conclusions of the one-component formulation. The ratio of the proton to neutron preequilibrium emissions in proton induced reactions decreases twice to three times when comp… Show more

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Cited by 47 publications
(25 citation statements)
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“…For a neutron ejectile of energy E the rate is given by [14] where σ k,inv is the inverse reaction cross section (calculated within the optical model framework) and E * is the total excitation energy of the system. The calculated probability for pre-equilibrium neutron emission is shown in the upper panel of Fig.…”
Section: Multichance Fissionmentioning
confidence: 99%
“…For a neutron ejectile of energy E the rate is given by [14] where σ k,inv is the inverse reaction cross section (calculated within the optical model framework) and E * is the total excitation energy of the system. The calculated probability for pre-equilibrium neutron emission is shown in the upper panel of Fig.…”
Section: Multichance Fissionmentioning
confidence: 99%
“…Some consequences of their proposal are also discussed by Gupta [5]. It appears, however, that the approach of [4] and [5-1 brings along serious mathematical and numerical complications. Although theoretically very interesting, this approach is therefore not very suitable for introduction into routine pre-equilibrium calculations.…”
Section: Introductionmentioning
confidence: 92%
“…In Sect. 4 we discuss some related observations on the meaning of the effective mfp values occurring in exciton models. Section5 summarizes our conclusions.…”
Section: Introductionmentioning
confidence: 98%
See 1 more Smart Citation
“…5) The energy range of interest is 100 keV-200 MeV because atmospheric neutrons are very abundant in this energy range. 12) The physics of DHORIN is mainly based on the 2D-exciton model, 13) the Hauser-Feshbach formulation 14) and the generalized evaporation model. 15) The main advantage of this code is that it is able to calculate all the needed quantities (cross sections, level densities and transmission coefficients) for all nucleus that have to be treated during a reaction.…”
Section: Monte Carlo Simulations With Dhorinmentioning
confidence: 99%