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Distribution of Partial Radiation Widths
47
Citations
21
References
1963
Year
EngineeringNuclear PhysicsNuclear DataRadiation ProtectionRadiative TransferExperimental WidthsNuclear MaterialsNuclear DecayRadiation DetectionPhysicsNuclear TheoryNeutron SourceRadiation TransportNeutron TransportNuclear EngineeringExperimental Nuclear PhysicsNatural SciencesPartial WidthsNuclear ExperimentsNeutron ScatteringPartial Radiation Widths
The gamma-ray spectra that result from the capture of neutrons in resonances of ${\mathrm{Hg}}^{199}$, ${\mathrm{Pt}}^{195}$, ${\mathrm{W}}^{183}$, and ${\mathrm{Se}}^{77}$ are measured. A least-squares fitting of the spectra gives relative values of partial widths for various sets of high-energy radiative transitions. These widths are treated as statistical samples drawn from populations governed by a ${\ensuremath{\chi}}^{2}$ distribution with $\ensuremath{\nu}$ degrees of freedom. A technique of hypothesis testing that makes use of Monte Carlo calculations is used to derive unbiased values of $\ensuremath{\nu}$ from the small samples of experimental widths. The over-all result of the analysis is $\ensuremath{\nu}=1.34\ifmmode\pm\else\textpm\fi{}0.33\ifmmode\pm\else\textpm\fi{}0.21$. The previously reported partial radiation widths for resonances of ${\mathrm{Gd}}^{155}$, ${\mathrm{Yb}}^{173}$, ${\mathrm{Hf}}^{177}$, and ${\mathrm{Hg}}^{201}$ are also analyzed. The result is $\ensuremath{\nu}=1.14\ifmmode\pm\else\textpm\fi{}0.44\ifmmode\pm\else\textpm\fi{}0.21$. Thus, both sets of data are in good agreement with the value $\ensuremath{\nu}=1$ that is expected from the Porter-Thomas description of the distribution of the widths associated with a single exit channel.
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