166 research outputs found

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

    Get PDF
    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 Îł\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

    Search for the Θ+\Theta^{+} pentaquark via the π−p→K−X\pi^-p\to K^-X reaction at 1.92 GeV/cc

    Get PDF
    The Θ+\Theta^+ pentaquark baryon was searched for via the π−p→K−X\pi^-p\to K^-X reaction in a missing-mass resolution of 1.4 MeV/c2c^2(FWHM) at J-PARC. π−\pi^- meson beams were incident on the liquid hydrogen target with the beam momentum of 1.92 GeV/cc. No peak structure corresponding to the Θ+\Theta^+ mass was observed. The upper limit of the production cross section averaged over the scattering angle of 2∘^{\circ} to 15∘^{\circ} in the laboratory frame was obtained to be 0.26 ÎŒ\mub/sr in the mass region of 1.51−-1.55 GeV/c2c^2.The upper limit of the Θ+\Theta^+ decay width using the effective Lagrangian approach was obtained to be 0.72 MeV/c2c^2 and 3.1 MeV/c2c^2 for JΘP=1/2+J^P_{\Theta}=1/2^+ and JΘP=1/2−J^P_{\Theta}=1/2^-, respectively.Comment: 5 pages, 3 figures, 1 tabl

    Search for Λ6^6_\LambdaH hypernucleus by the 6^6Li(π−,K+)(\pi^-,K^+) reaction at pπ−p_{\pi^-} = 1.2 GeV/cc

    Get PDF
    We have carried out an experiment to search for a neutron-rich hypernucleus, Λ6^6_{\Lambda}H, by the 6^6Li(π−,K+\pi^-,K^+) reaction at pπ−p_{\pi^-} =1.2 GeV/cc. The obtained missing mass spectrum with an estimated energy resolution of 3.2 MeV (FWHM) showed no peak structure corresponding to the Λ6^6_{\Lambda}H hypernucleus neither below nor above the Λ4^4_{\Lambda}H+2n+2n particle decay threshold. An upper limit of the production cross section for the bound Λ6^6_{\Lambda}H hypernucleus was estimated to be 1.2 nb/sr at 90% confidence level.Comment: 6 pages, 5 figures, published versio

    Acute Insulin Stimulation Induces Phosphorylation of the Na-Cl Cotransporter in Cultured Distal mpkDCT Cells and Mouse Kidney

    Get PDF
    The NaCl cotransporter (NCC) is essential for sodium reabsorption at the distal convoluted tubules (DCT), and its phosphorylation increases its transport activity and apical membrane localization. Although insulin has been reported to increase sodium reabsorption in the kidney, the linkage between insulin and NCC phosphorylation has not yet been investigated. This study examined whether insulin regulates NCC phosphorylation. In cultured mpkDCT cells, insulin increased phosphorylation of STE20/SPS1-related proline-alanine-rich kinase (SPAK) and NCC in a dose-dependent manner. This insulin-induced phosphorylation of NCC was suppressed in WNK4 and SPAK knockdown cells. In addition, Ly294002, a PI3K inhibitor, decreased the insulin effect on SPAK and NCC phosphorylation, indicating that insulin induces phosphorylation of SPAK and NCC through PI3K and WNK4 in mpkDCT cells. Moreover, acute insulin administration to mice increased phosphorylation of oxidative stress-responsive kinase-1 (OSR1), SPAK and NCC in the kidney. Time-course experiments in mpkDCT cells and mice suggested that SPAK is upstream of NCC in this insulin-induced NCC phosphorylation mechanism, which was confirmed by the lack of insulin-induced NCC phosphorylation in SPAK knockout mice. Moreover, insulin administration to WNK4 hypomorphic mice did not increase phosphorylation of OSR1, SPAK and NCC in the kidney, suggesting that WNK4 is also involved in the insulin-induced OSR1, SPAK and NCC phosphorylation mechanism in vivo. The present results demonstrated that insulin is a potent regulator of NCC phosphorylation in the kidney, and that WNK4 and SPAK are involved in this mechanism of NCC phosphorylation by insulin

    Isoscaling in central Sn+Sn collisions at 270 MeV/u

    Full text link
    Experimental information on fragment emissions is important in understanding the dynamics of nuclear collisions and in the development of transport model simulating heavy-ion collisions. The composition of complex fragments emitted in the heavy-ion collisions can be explained by statistical models, which assume that thermal equilibrium is achieved at collision energies below 100 MeV/u. Our new experimental data together with theoretical analyses for light particles from Sn+Sn collisions at 270 MeV/u, suggest that the hypothesis of thermal equilibrium breaks down for particles emitted with high transfer momentum. To inspect the system's properties in such limit, the scaling features of the yield ratios of particles from two systems, a neutron-rich system of 132Sn+124Sn{}^{132}\mathrm{Sn}+{}^{124}\mathrm{Sn} and a nearly symmetric system of 108Sn+112Sn{}^{108}\mathrm{Sn}+{}^{112}\mathrm{Sn}, are examined in the framework of the statistical multifragmentation model and the antisymmetrized molecular dynamics model. The isoscaling from low energy particles agree with both models. However the observed breakdown of isoscaling for particles with high transverse momentum cannot be explained by the antisymmetrized molecular dynamics model

    Search for the pentaquark at J-PARC

    Get PDF
    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 ÎŒb/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

    Constraining nucleon effective masses with flow and stopping observables from the Sπ\piRIT experiment

    Full text link
    Properties of the nuclear equation of state (EoS) can be probed by measuring the dynamical properties of nucleus-nucleus collisions. In this study, we present the directed flow (v1v_1), elliptic flow (v2v_2) and stopping (VarXZ) measured in fixed target Sn + Sn collisions at 270 AMeV with the Sπ\piRIT Time Projection Chamber. We perform Bayesian analyses in which EoS parameters are varied simultaneously within the Improved Quantum Molecular Dynamics-Skyrme (ImQMD-Sky) transport code to obtain a multivariate correlated constraint. The varied parameters include symmetry energy, S0S_0, and slope of the symmetry energy, LL, at saturation density, isoscalar effective mass, ms∗/mNm_{s}^*/m_{N}, isovector effective mass, mv∗/mNm_{v}^{*}/m_{N} and the in-medium cross-section enhancement factor η\eta. We find that the flow and VarXZ observables are sensitive to the splitting of proton and neutron effective masses and the in-medium cross-section. Comparisons of ImQMD-Sky predictions to the Sπ\piRIT data suggest a narrow range of preferred values for ms∗/mNm_{s}^*/m_{N}, mv∗/mNm_{v}^{*}/m_{N} and η\eta

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

    Full text link
    The pentaquark Θ+\Theta^+ has been searched for via the π−p→K−X\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 ÎŒ\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 1/2−1/2^-, respectively.Comment: 12 pages, 9 figures; published versio
    • 

    corecore