412 research outputs found

    The \gamma-ray production in neutral-current neutrino oxygen interaction in the energy range above 100 MeV

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    We calculate the cross section of the gamma-ray production from neutral-current neutrino-oxygen quasi-elastic interaction, ν+16ˆO→ν+p+15N∗\nu+\^{16}O \rightarrow \nu +p+^{15}N*, or ν+16O→ν+n+15O∗\nu+^{16}O \rightarrow \nu+n+^{15}O*, in which the residual nuclei (15N* or 15O*) lead to the gamma-ray emission with gamma-ray energy >6 MeV at the branching ratio of 41%. Above 200 MeV, this cross section dominates over that of gamma-ray production from the inelastic reaction, ν+16O−>ν+16O∗\nu+^{16}O->\nu+^{16}O*. In the present calculation, spectral function and the spectroscopic factors of 1p1/2,1p3/2and1s1/21p_{1/2}, 1p_{3/2} and 1s_{1/2} states are essential. The gamma-ray production is dominated by the deexcitation of 1p3/21p_{3/2} state of the residual nucleus

    Superdeformation and clustering in 40^{40}Ca studied with Antisymmetrized Molecular Dynamics

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    Deformed states in 40^{40}Ca are investigated with a method of antisymmetrized molecular dynamics. Above the spherical ground state, rotational bands arise from a normal deformation and a superdeformation as well as an oblate deformation. The calculated energy spectra and E2E2 transition strengths in the superdeformed band reasonably agree to the experimental data of the superdeformed band starting from the 03+0^+_3 state at 5.213 MeV. By the analysis of single-particle orbits, it is found that the superdeformed state has particle-hole nature of an 8p8p-8h8h configuration. One of new findings is parity asymmetric structure with 12^{12}C+28^{28}Si-like clustering in the superdeformed band. We predict that 12^{12}C+28^{28}Si molecular bands may be built above the superdeformed band due to the excitation of inter-cluster motion. They are considered to be higher nodal states of the superdeformed state. We also suggest negative-parity bands caused by the parity asymmetric deformation.Comment: 13 figures, submitted to Phys. Rev.

    Alpha clustering and weak coupling in the A=90 region

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    From the viewpoint of a unified description of cluster structure and scattering in the A=90 region, Îą\alpha scattering from 89^{89}Y is investigated. Îą\alpha clustering and weak coupling in 93^{93}Nb is discussed.Comment: 8 pages, 4 figure

    Nuclear corrections of parton distribution functions

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    We report global analysis results of experimental data for nuclear structure-function ratios F_2^A/F_2^{A'} and proton-nucleus Drell-Yan cross-section ratios sigma_{DY}^{pA}/sigma_{DY}^{pA'} in order to determine optimum parton distribution functions (PDFs) in nuclei. An important point of this analysis is to show uncertainties of the distributions by the Hessian method. The results indicate that the uncertainties are large for gluon distributions in the whole x region and for antiquark distributions at x>0.2. We provide a code for calculating any nuclear PDFs at given x and Q^2 for general users. They can be used for calculating high-energy nuclear reactions including neutrino-nucleus interactions, which are discussed at this workshop.Comment: 1+6 pages, LaTeX, 10 eps files, espcrc2.sty, to be published in Nucl. Phys. B Supplements, Proceedings of the Third International Workshop on Neutrino-Nucleus Interactions in the Few GeV Region (NuInt04), Gran Sasso, Italy, March 17-21, 2004. Nuclear PDF library is available at http://hs.phys.saga-u.ac.jp/nuclp.htm

    Deformed Base Antisymmetrized Molecular Dynamics and its Application to ^{20}Ne

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    A new theoretical framework named as deformed base antisymmetrized molecular dynamics that uses the localized triaxially deformed Gaussian as the single particle wave packet is presented. The model space enables us to describe sufficiently well the deformed mean-field structure as well as the cluster structure and their mixed structure within the same framework. The improvement over the original version of the antisymmetrized molecular dynamics which uses the spherical Gaussian is verified by the application to 20Ne^{20}{\rm Ne} nucleus. The almost pure α+16Og.s\alpha + ^{16}{\rm O_{g.s}} cluster structure of the KπK^\pi=0−0^- band, the distortion of the cluster structure in the KπK^\pi=01+0^+_1 band and the dominance of the deformed mean-field structure of the KπK^\pi=2−2^- band are confirmed and their observed properties are reproduced. Especially, the intra-band E2 transition probabilities in KπK^\pi=01+0^+_1 and 2−2^- bands are reproduced without any effective charge. Since it has been long known that the pure α+16Og.s.\alpha + ^{16}{\rm O}_{g.s.} cluster model underestimates the intra-band E2E2 transitions in the KπK^\pi=01+0^+_1 band by about 30%, we consider that this success is due to the sufficient description of the deformed mean-field structure in addition to the cluster structure by the present framework. From the successful description of 20Ne^{20}{\rm Ne}, we expect that the present framework presents us with a powerful approach for the study of the coexistence and interplay of the mean-field structure and the cluster structure

    Tracking Performance of the Scintillating Fiber Detector in the K2K Experiment

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    The K2K long-baseline neutrino oscillation experiment uses a Scintillating Fiber Detector (SciFi) to reconstruct charged particles produced in neutrino interactions in the near detector. We describe the track reconstruction algorithm and the performance of the SciFi after three years of operation.Comment: 24pages,18 figures, and 1 table. Preprint submitted to NI
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