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- W2016383905 abstract "The properties of the excited states of ${mathrm{N}}^{13}$ were reinvestigated by applying dispersion theory to the ${mathrm{C}}^{12}(p, p){mathrm{C}}^{12}$ differential cross section reported in the preceding paper. The quantity and accuracy of the data were sufficient to permit extraction of the experimental $S$ wave phase shift up to 1.4 Mev. The remainder of the data was fitted by successive readjustment of the level parameters.The present analysis corroborates the previous momentum and parity assignments but gives somewhat different values for the resonant energies and widths. The level assignments together with the revised widths and resonant energies are as follows: The 0.46-Mev scattering anomaly is due to a virtual ($j=frac{1}{2}, +$) level in the compound nucleus ${mathrm{N}}^{13}$ with ${E}_{r}=2.369$ Mev and $ensuremath{Gamma}=31$ kev. The 1.7-Mev scattering anomaly is the result of two virtual levels, a ($j=frac{3}{2}, ensuremath{-}$) level with ${E}_{r}=3.511$ Mev and $ensuremath{Gamma}=55$ kev and a ($j=frac{5}{2}, +$) level with ${E}_{r}=3.558$ Mev and $ensuremath{Gamma}=61$ kev. ${E}_{r}$ and $ensuremath{Gamma}$ are calculated in the center-of-mass system and ${E}_{r}$ is measured from the ground state of ${mathrm{N}}^{13}$. These new values for ${E}_{r}$ and $ensuremath{Gamma}$ agree quite well with those obtained from the ${mathrm{C}}^{12}(p, ensuremath{gamma}){mathrm{N}}^{13}$ reaction provided it is assumed that the ($j=frac{5}{2}, +$) level does not participate appreciably in the capture process. The values of the reduced widths of the levels indicate that the two even-parity levels arise mainly from single particle excitation, but that the odd-parity level involves appreciable excitation of the core." @default.
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- W2016383905 date "1953-01-15" @default.
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- W2016383905 title "The Excited States of theN13Nucleus" @default.
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- W2016383905 doi "https://doi.org/10.1103/physrev.89.370" @default.
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