26 research outputs found

    Observation of Spin-Dependent Charge Symmetry Breaking in ΛN\Lambda N Interaction: Gamma-Ray Spectroscopy of Λ4^4_{\Lambda }He

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    The energy spacing between the ground-state spin doublet of Λ4^4_\Lambda He(1+^+,0+^+) was determined to be 1406±2±21406 \pm 2 \pm 2 keV, by measuring γ\gamma rays for the 1+0+1^+ \to 0^+ transition with a high efficiency germanium detector array in coincidence with the 4^4He(K,π)(K^-,\pi^-) Λ4^4_\Lambda He reaction at J-PARC. In comparison to the corresponding energy spacing in the mirror hypernucleus Λ4^4_\Lambda H, the present result clearly indicates the existence of charge symmetry breaking (CSB) in ΛN\Lambda N interaction. It is also found that the CSB effect is large in the 0+0^+ ground state but is by one order of magnitude smaller in the 1+1^+ excited state, demonstrating that the ΛN\Lambda N CSB interaction has spin dependence

    High-resolution search for the Θ+\Theta^{+} pentaquark via a pion-induced reaction at J-PARC

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    The pentaquark Θ+\Theta^+ has been searched for via the πpKX\pi^-p \to K^-X reaction with beam momenta of 1.92 and 2.01 GeV/cc at J-PARC. A missing mass resolution of 2 MeV (FWHM) was achieved but no sharp peak structure was observed. The upper limits on the production cross section averaged over the scattering angle from 2^{\circ} to 15^{\circ} in the laboratory frame were found to be less than 0.28 μ\mub/sr at the 90\% confidence level for both the 1.92- and 2.01-GeV/cc data. The systematic uncertainty of the upper limits was controlled within 10\%. Constraints on the Θ+\Theta^+ decay width were also evaluated with a theoretical calculation using effective Lagrangian. The present result implies that the width should be less than 0.36 and 1.9 MeV for the spin-parity of 1/2+1/2^+ and 1/21/2^-, respectively.Comment: 12 pages, 9 figures; published versio

    Search for the pentaquark at J-PARC

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    We have been searching for the Θ^+ pentaquark via the π^−p→K^−X reaction at the J-PARC hadron facility. No peak structure was observed in the missing mass spectrum obtained at 1.92 GeV/c beam momentum. The upper limit for the production cross section averaged over the scattering angle from 2° to 15° in the laboratory frame was derived to be 0.26 μb/sr. In order to make a more stringent constraint we have also performed a measurement at 2.0 GeV/c. Present analysis status of this new data is reported

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