NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Matsuyama Found 20 matches. 2010SU01 Phys.Rev.Lett. 104, 042302 (2010) N.Suzuki, B.Julia-Diaz, H.Kamano, T.-S.H.Lee, A.Matsuyama, T.Sato Disentangling the Dynamical Origin of P11 Nucleon Resonances
doi: 10.1103/PhysRevLett.104.042302
2009JU04 Phys.Rev. C 80, 025207 (2009) B.Julia-Diaz, H.Kamano, T.-S.H.Lee, A.Matsuyama, T.Sato, N.Suzuki Dynamical coupled-channels analysis of 1H(e, e'π)N reactions
doi: 10.1103/PhysRevC.80.025207
2009KA08 Phys.Rev. C 79, 025206 (2009) H.Kamano, B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato Dynamical coupled-channels study of πN → ππN reactions
doi: 10.1103/PhysRevC.79.025206
2009KA39 Phys.Rev. C 80, 065203 (2009) H.Kamano, B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato Double and single pion photoproduction within a dynamical coupled-channels model
doi: 10.1103/PhysRevC.80.065203
2008JU04 Phys.Rev. C 77, 045205 (2008) B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato, L.C.Smith Dynamical coupled-channels effects on pion photoproduction NUCLEAR REACTIONS p(γ, p)π0, E=1154-1632 MeV; calculated cross sections, angular distributions using dynamical coupled-channel model. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.045205
2007JU07 Phys.Rev. C 76, 065201 (2007) B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato Dynamical coupled-channels model of πN scattering in the W ≤ 2 GeV nucleon resonance region NUCLEAR REACTIONS p(π-, π-), (π-, π0), E<2 GeV; analyzed pion-nucleon scattering using dynamical coupled-channel model.
doi: 10.1103/PhysRevC.76.065201
2007MA11 Phys.Rep. 439, 193 (2007) A.Matsuyama, T.Sato, T.-S.H.Lee Dynamical coupled-channel model of meson production reactions in the nucleon resonance region
doi: 10.1016/j.physrep.2006.12.003
1997MA53 Phys.Lett. 408B, 25 (1997) Narrow πNN Resonance
doi: 10.1016/S0370-2693(97)00822-8
1991MA13 Nucl.Phys. A526, 547 (1991) Unitary Meson-Exchange Calculation of the π+d → pp pp π+d Reaction NUCLEAR REACTIONS 2H(π+, 2p), E not given; calculated σ(E); 1H(polarized p, π+), E=400-1200 MeV; calculated σ(E), σ(θ), analyzing power vs θ. Unitary meson exchange model.
doi: 10.1016/0375-9474(91)90432-6
1988MA09 Nucl.Phys. A477, 673 (1988) A Study of Hypernucleus Production by K- Capture at Rest NUCLEAR REACTIONS 4He, 12C, 16O, 40Ca, 90Zr, 208Pb(K-, π+), (K-, π-), E at rest; calculated hypernucleus production probability.
doi: 10.1016/0375-9474(88)90412-5
1987LE20 Phys.Rev. C36, 1459 (1987) Unitary Meson-Exchange πNN Models: NN and πd elastic scattering NUCLEAR REACTIONS 2H(π, π), E=140-300 MeV; calculated σ(θ), vector, tensor analyzing power vs θ.
doi: 10.1103/PhysRevC.36.1459
1986CO20 Nucl.Phys. A460, 699 (1986) The Relativistic Stripping Model of (p, π+) Reactions in the Δ Resonance Region NUCLEAR REACTIONS 16O(p, π+), (polarized p, π+), E=350 MeV; calculated σ(θ), analyzing power vs θ. Relativistic stripping model, isobar resonance region.
doi: 10.1016/0375-9474(86)90532-4
1986MA56 Phys.Rev. C34, 1900 (1986) Unitary Meson-Exchange Calculation of NN → NNπ Reaction NUCLEAR REACTIONS 1H(p, nπ+), E=800 MeV; calculated σ. Unitary meson exchange calculations.
doi: 10.1103/PhysRevC.34.1900
1985LE12 Phys.Rev. C32, 516 (1985) Theory of Mesonic and Dibaryonic Excitations in the πNN System: Derivation of πNN scattering equations NUCLEAR REACTIONS 2H(π, π), E=100-300 MeV; calculated scattering amplitudes. Faddeev type equation, mesonic, dibaryonic, isobar excitations.
doi: 10.1103/PhysRevC.32.516
1985MA08 Phys.Lett. 152B, 42 (1985) A Three-Body Calculation of the π - d Scattering Amplitude by the Spline Method NUCLEAR REACTIONS 2H(π, π), E=140 MeV; calculated elastic, breakup scattering amplitudes. Three-body calculation, spline method.
doi: 10.1016/0370-2693(85)91135-9
1985MA17 Phys.Lett. 154B, 28 (1985) E.L.Mathie, G.R.Smith, E.T.Boschitz, W.Gyles, C.R.Ottermann, S.Mango, J.A.Konter, A.Matsuyama, R.R.Johnson, R.Olszewski First Measurement of iT11 in the Pion-Deuteron Breakup Reaction NUCLEAR REACTIONS 2H(π+, π+p), E=228 MeV; measured σ(θ), iT11(θ), σ(θp, θ(π)) vs proton momentum. Polarized target, kinematically complete experiment.
doi: 10.1016/0370-2693(85)91561-8
1985SA12 Phys.Rev. C31, 1987 (1985) K.Sakamoto, M.Hirata, A.Matsuyama, K.Yazaki Interpretation of the Angular Distribution of the 4He(π-, n)3H Reaction Based on the Δ-Hole Model NUCLEAR REACTIONS 4He(π-, n), E=100-250 MeV; calculated σ(θ). Isobar-hole model, one nucleon momentum distribution.
doi: 10.1103/PhysRevC.31.1987
1984YA04 Phys.Lett. 144B, 177 (1984) T.Yamazaki, T.Ishikawa, K.Yazaki, A.Matsuyama New Light on Hypernuclear Spectroscopy with Stopped K- NUCLEAR REACTIONS 12C, 208Pb(K-, π-), E at rest; calculated pion spectra; deduced deep lying orbitals, spin-orbit doublet evidence in hypernuclei.
doi: 10.1016/0370-2693(84)91798-2
1983HI11 Phys.Lett. 128B, 15 (1983) M.Hirata, K.Masutani, A.Matsuyama, K.Yazaki The 4He(π-, n)3H Reaction in a Δ-Hole Model NUCLEAR REACTIONS 4He(π-, n), E=100, 150, 200 MeV; calculated σ(θ). 2H(π+, p), E=142 MeV; calculated σ(θ), polarization vs θ; deduced isobar-nucleon to nucleon-nucleon transition interaction parameters.
doi: 10.1016/0370-2693(83)90064-3
1981MA15 Nucl.Phys. A364, 477 (1981) Dibaryon Resonance Effects on πd Scattering NUCLEAR REACTIONS 2H(π, π), E=142, 180, 232, 256 MeV; calculated σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced dibaryon resonance effects. Quasibound nucleon-isobar resonances, three-body background amplitudes.
doi: 10.1016/0375-9474(81)90583-2
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