314 research outputs found

    What Do s- and p-Wave Neutron Average Radiative Widths Reveal

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    A first observation of two resonance-like structures at mass numbers 92 and 112 in the average capture widths of the p-wave neutron resonances relative to the s-wave component is interpreted in terms of a spin-orbit splitting of the 3p single-particle state into P{sub 3/2} and P{sub 1/2} components at the neutron separation energy. A third structure at about A = 124, which is not correlated with the 3p-wave neutron strength function, is possibly due to the Pygmy Dipole Resonance. Five significant results emerge from this investigation: (i) The strength of the spin-orbit potential of the optical-model is determined as 5.7 {+-} 0.5 MeV, (ii) Non-statistical effects dominate the p-wave neutron-capture in the mass region A = 85 - 130, (iii) The background magnitude of the p-wave average capture-width relative to that of the s-wave is determined as 0.50 {+-} 0.05, which is accounted for quantitatively in tenns of the generalized Fermi liquid model of Mughabghab and Dunford, (iv) The p-wave resonances arc partially decoupled from the giant-dipole resonance (GDR), and (v) Gamma-ray transitions, enhanced over the predictions of the GDR, are observed in the {sup 90}Zr - {sup 98}Mo and Sn-Ba regions

    Investigation of the fundamental constants stability based on the reactor Oklo burn-up analysis

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    The burn-up for SC56-1472 sample of the natural Oklo reactor zone 3 was calculated using the modern Monte Carlo codes. We reconstructed the neutron spectrum in the core by means of the isotope ratios: 147^{147}Sm/148^{148}Sm and 176^{176}Lu/175^{175}Lu. These ratios unambiguously determine the spectrum index and core temperature. The effective neutron absorption cross section of 149^{149}Sm calculated using this spectrum was compared with experimental one. The disagreement between these two values allows to limit a possible shift of the low laying resonance of 149^{149}Sm even more . Then, these limits were converted to the limits for the change of the fine structure constant α\alpha. We found that for the rate of α\alpha change the inequality ∣δα˙/α∣≤5⋅10−18|\delta \dot{\alpha}/\alpha| \le 5\cdot 10^{-18} is fulfilled, which is of the next higher order than our previous limit.Comment: 16 pages, 7 figure

    Test of nuclear level density inputs for Hauser-Feshbach model calculations

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    The energy spectra of neutrons, protons, and alpha-particles have been measured from the d+59Co and 3He+58Fe reactions leading to the same compound nucleus, 61$Ni. The experimental cross sections have been compared to Hauser-Feshbach model calculations using different input level density models. None of them have been found to agree with experiment. It manifests the serious problem with available level density parameterizations especially those based on neutron resonance spacings and density of discrete levels. New level densities and corresponding Fermi-gas parameters have been obtained for reaction product nuclei such as 60Ni,60Co, and 57Fe

    Enhanced radiative strength in the quasi-continuum of 117Sn

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    Radiative strength functions of 117Sn has been measured below the neutron separation energy using the (3He,3He'gamma) reactions. An increase in the slope of the strength functions around E_gamma= 4.5 MeV indicates the onset of a resonance-like structure, giving a significant enhancement of the radiative strength function compared to standard models in the energy region 4.5 <= E_gamma <= 8.0 MeV. For the first time, the functional form of this resonance-like structure has been measured in an odd tin nucleus below neutron threshold in the quasi-continuum region.Comment: 4 pages, 3 figure

    Evidence for the pair-breaking process in 116,117Sn

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    The nuclear level densities of 116,117Sn below the neutron separation energy have been determined experimentally from the (3He,alpha gamma) and (3He,3He gamma') reactions, respectively. The level densities show a characteristic exponential increase and a difference in magnitude due to the odd-even effect of the nuclear systems. In addition, the level densities display pronounced step-like structures that are interpreted as signatures of subsequent breaking of nucleon pairs.Comment: 7 pages, 5 figures, accepted for publication in Phys. Rev. C, 22 December 200

    Precision Measurement of the n-3He Incoherent Scattering Length Using Neutron Interferometry

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    We report the first measurement of the low-energy neutron-3^3He incoherent scattering length using neutron interferometry: bi′=(−2.512±0.012statistical±0.014systematic)b_i' = (-2.512\pm 0.012{statistical}\pm0.014{systematic}) fm. This is in good agreement with a recent calculation using the AV18+3N potential. The neutron-3^3He scattering lengths are important for testing and developing nuclear potential models that include three nucleon forces, effective field theories for few-body nuclear systems, and neutron scattering measurements of quantum excitations in liquid helium. This work demonstrates the first use of a polarized nuclear target in a neutron interferometer.Comment: 4 figure
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