649 research outputs found

    Equivalent hyperon-nucleon interactions in low-momentum space

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    Equivalent interactions in a low-momentum space for the ΛN\Lambda N, ΣN\Sigma N and ΞN\Xi N interactions are calculated, using the SU6_6 quark model potential as well as the Nijmegen OBEP model as the input bare interaction. Because the two-body scattering data has not been accumulated sufficiently to determine the hyperon-nucleon interactions unambiguously, the construction of the potential even in low-energy regions has to rely on a theoretical model. The equivalent interaction after removing high-momentum components is still model dependent. Because this model dependence reflects the character of the underlying potential model, it is instructive for better understanding of baryon-baryon interactions in the strangeness sector to study the low-momentum space YNYN interactions.Comment: 9 pages, 13 figures, accepted for publication in Phys. Rev.

    Simulation and Design of a Simple and Easy-to-use Small-scale Neutron Source at Kyoto University

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    AbstractA simple and easy-to-use compact neutron source based on a low power level proton accelerator (proton energy 3.5 MeV and 0.35kW beam power) at Kyoto University was designed with the conception of low cost, compact size, high safety and intensive thermal neutron flux via Monte Carlo method with PHITS code. By utilizing (p, n) reactions in a beryllium target coupled to a polyethylene moderator and graphite reflector with a wing configuration, this facility is expected to produce time-averaged thermal neutron fluxes suitable for neutron scattering and development of instrumentation, and play a role in educating students in neutron science and performing research with neutrons. Borated polyethylene (BPE) and ordinary concrete were combined to shield the neutron and photon. By using niobium as target backing and water as cooler, it is promising to cope with the problem of thermal damage and hydrogen embrittlement damage. The sizes of moderator and reflector are optimized to have thermal neutron flux as high as possible, while keeping the low ratio of fast neutron flux to thermal neutron flux. The neutron and gamma dose equivalent rates were evaluated and the current shielding configuration is acceptable

    KˉNN\bar{K}NN quasi-bound state and the KˉN\bar{K}N interaction: coupled-channel Faddeev calculations of the KˉNN−πΣN\bar{K}NN - \pi \Sigma N system

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    Coupled-channel three-body calculations of an I=1/2I=1/2, Jπ=0−J^{\pi}=0^- KˉNN\bar{K}NN quasi-bound state in the KˉNN−πΣN\bar{K}NN - \pi \Sigma N system were performed and the dependence of the resulting three-body energy on the two-body KˉN−πΣ\bar{K}N - \pi \Sigma interaction was investigated. Earlier results of binding energy BK−pp∼50−70B_{K^-pp} \sim 50 -70 MeV and width ΓK−pp∼100\Gamma_{K^-pp} \sim 100 MeV are confirmed [N.V. Shevchenko {\it et al.}, Phys. Rev. Lett. {\bf 98}, 082301 (2007)]. It is shown that a suitably constructed energy-independent complex KˉN\bar{K}N potential gives a considerably shallower and narrower three-body quasi-bound state than the full coupled-channel calculation. Comparison with other calculations is made.Comment: 22 pages, 7 figures, 4 tables; minor corrections, accepted for publication in Phys. Rev.

    Measurement of the π−\pi^- decay width of Λ5^5_\LambdaHe

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    We have precisely measured Λ→pπ−\Lambda \to p\pi^- decay width of \5LHe and demonstrated significantly larger α\alpha -Λ\Lambda overlap than expected from the central repulsion α\alpha-Λ\Lambda potential, which is derived from YNG \Lambda$-nucleon interaction.Comment: 4 pages, 3 figure

    Proton asymmetry in non-mesonic weak decay of light hypernuclei

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    We have obtained the decay asymmetry parameters in non-mesonic weak decay of polarized Lambda-hypernuclei by measuring the proton asymmetry. The polarized Lambda-hypernuclei, 5_Lambda-He, 12_Lambda-C, and 11_Lambda-B, were produced in high statistics via the (pi^+,k^+) reaction at 1.05 GeV/c in the forward angles. Preliminary analysis shows that the decay asymmetry parameters are very small for these s-shell and p-shell hypernuclei.Comment: 4pages, 4figures, International Conference on Hypernuclear and Strange Particle Physics (HYP2003
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