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Inelastic Neutron Scattering Near Threshold
40
Citations
11
References
1965
Year
EngineeringNuclear PhysicsNuclear DataCross SectionsNuclear MaterialsNuclear DecayHigh-energy Nuclear ReactionPhysicsNuclear SecurityNuclear TheoryNeutron SourceAtomic PhysicsNeutron Inelastic ScatteringNeutron TransportNuclear EngineeringNuclear AstrophysicsExperimental Nuclear PhysicsReaction WidthsNatural SciencesApplied PhysicsNuclear ExperimentsNeutron Scattering
Cross sections for the production of excited states by neutron inelastic scattering were measured as a function of bombarding energy from 0 to 300 keV above threshold for the first two excited states of ${\mathrm{Fe}}^{56}$, the first two excited states of ${\mathrm{Cu}}^{63}$, the first excited state of ${\mathrm{Zr}}^{90}$, the first two excited states of ${\mathrm{Ba}}^{138}$, and the first three excited states of ${\mathrm{Ce}}^{140}$. Neutron-beam energy resolution was 10-20 keV. Inelastic-scattering events were counted by detecting gamma rays from the excited states. When the number of open channels for compound-nucleus decay is small, (a condition which exists near threshold for exciting low-lying states) fluctuations of reaction widths about their average values reduce the inelastic-scattering cross section from that predicted by the Hauser-Feshbach equation by as much as 50%. This correction was evaluated, assuming a Porter-Thomas distribution of widths. Good agreement was found between experimental cross sections and the modified Hauser-Feshbach equation in all but two cases.
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