429 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.

    Multiple hadron production in e+e- annihilation induced by heavy primary quarks. New analysis

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    In this paper we present an analysis of the multiple hadron production induced by primary heavy quarks in e+e- annihilation with the account of most complete and corrected experimental data. In the framework of perturbative QCD, new theoretical bounds on the asymptotically constant differences of the multiplicities in processes with light and heavy quarks are given.Comment: 26 pages, 7 figures, to be published in Particles & Nucle

    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

    Quenching of Weak Interactions in Nucleon Matter

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    We have calculated the one-body Fermi and Gamow-Teller charge-current, and vector and axial-vector neutral-current nuclear matrix elements in nucleon matter at densities of 0.08, 0.16 and 0.24 fm−3^{-3} and proton fractions ranging from 0.2 to 0.5. The correlated states for nucleon matter are obtained by operating on Fermi-gas states by a symmetrized product of pair correlation operators determined from variational calculations with the Argonne v18 and Urbana IX two- and three-nucleon interactions. The squares of the charge current matrix elements are found to be quenched by 20 to 25 % by the short-range correlations in nucleon matter. Most of the quenching is due to spin-isospin correlations induced by the pion exchange interactions which change the isospins and spins of the nucleons. A large part of it can be related to the probability for a spin up proton quasi-particle to be a bare spin up/down proton/neutron. We also calculate the matrix elements of the nuclear Hamiltonian in the same correlated basis. These provide relatively mild effective interactions which give the variational energies in the Hartree-Fock approximation. The calculated two-nucleon effective interaction describes the spin-isospin susceptibilities of nuclear and neutron matter fairly accurately. However ≥\geq 3-body terms are necessary to reproduce the compressibility. All presented results use the simple 2-body cluster approximation to calculate the correlated basis matrix elements.Comment: submitted to PR
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