NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = C.Nakamoto Found 29 matches. 2016NA31 Phys.Rev. C 94, 035803 (2016) Quark-Pauli effects in three octet-baryons
doi: 10.1103/PhysRevC.94.035803
2007FU03 Prog.Part.Nucl.Phys. 58, 439 (2007) Y.Fujiwara, Y.Suzuki, C.Nakamoto Baryon-baryon interactions in the SU6 quark model and their applications to light nuclear systems
doi: 10.1016/j.ppnp.2006.08.001
2005FU05 Nucl.Phys. A754, 43c (2005) Y.Fujiwara, C.Nakamoto, M.Kohno, Y.Suzuki, K.Miyagawa Interactions between octet baryons in the SU6 quark model and their applications to light hypernuclei NUCLEAR STRUCTURE 3H, 6He, 9Be; calculated hypernucleus ground and excited states energies. Three-cluster Fadeev formalism.
doi: 10.1016/j.nuclphysa.2005.02.001
2004FU10 Nucl.Phys. A737, 243 (2004) Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, C.Nakamoto A Realistic Baryon-Baryon Interaction in the SU6 Quark Model and its Applications to Few-Baryon Systems
doi: 10.1016/j.nuclphysa.2004.03.083
2004FU31 Prog.Theor.Phys.(Kyoto), Suppl. 156, 17 (2004) Y.Fujiwara, C.Nakamoto, Y.Suzuki, M.Kohno, K.Miyagawa Quark-Model Baryon-Baryon Interaction and Its Applications to Hypernuclei NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, radii. 3H, 6He, 9Be; calculated hypernucleus ground and excited states energies. Quark-model baryon-baryon interaction.
doi: 10.1143/PTPS.156.17
2002FU01 Phys.Rev. C65, 014002 (2002) Y.Fujiwara, T.Fujita, M.Kohno, C.Nakamoto, Y.Suzuki Resonating-Group Study of Baryon-Baryon Interactions for the Complete Baryon Octet: NN interaction NUCLEAR REACTIONS 1H(n, X), (p, X), E ≤ 800 MeV; calculated phase shifts. Unified framework of resonating-group method for baryon-baryon interactions. NUCLEAR STRUCTURE 2H; calculated binding energy, radius, μ, quadrupole moment. Unified framework of resonating-group method for baryon-baryon interactions.
doi: 10.1103/PhysRevC.65.014002
2001FU16 Phys.Rev. C64, 054001 (2001) Y.Fujiwara, M.Kohno, C.Nakamoto, Y.Suzuki Interactions between Octet Baryons in the SU6 Quark Model NUCLEAR REACTIONS 1H(Ξ-, Ξ-), (Ξ-, X), E at 0-1000 MeV/c; calculated total σ. Resonating group method, spin-flavor SU6 quark model.
doi: 10.1103/PhysRevC.64.054001
2001NA35 Nucl.Phys. A691, 238c (2001) C.Nakamoto, Y.Fujiwara, Y.Suzuki ΞN Interaction in the SU6 Quark Model
doi: 10.1016/S0375-9474(01)01036-3
2000FU06 Prog.Theor.Phys.(Kyoto) 103, 755 (2000) Y.Fujiwara, M.Kohno, T.Fujita, C.Nakamoto, Y.Suzuki Lippmann-Schwinger Resonating-Group Formalism for NN and YN Interactions in an SU6 Quark Model NUCLEAR REACTIONS 1n, 1H(polarized p, p), E=400-800 MeV; calculated σ(θ), polarization. Resonating group method, SU(6) quark model, comparisons with data.
doi: 10.1143/PTP.103.755
2000FU08 Nucl.Phys. A674, 493 (2000) Y.Fujiwara, M.Kohno, T.Fujita, C.Nakamoto, Y.Suzuki Single-Particle Spin-Orbit Strengths of the Nucleon and Hyperons by SU6 Quark-Model
doi: 10.1016/S0375-9474(00)00177-9
2000FU17 Prog.Theor.Phys.(Kyoto) 104, 1025 (2000) Y.Fujiwara, M.Kohno, C.Nakamoto, Y.Suzuki G-Matrix Equation in the Quark-Model Resonating-Group Method for Baryon-Baryon Interaction
doi: 10.1143/PTP.104.1025
2000KO26 Nucl.Phys. A670, 319c (2000) M.Kohno, Y.Fujiwara, T.Fujita, C.Nakamoto, Y.Suzuki Single-Particle Spin-Orbit Potentials of the Λ and Σ Hyperons Based on the Quark-Model G-Matrix
doi: 10.1016/S0375-9474(00)00122-6
2000KO28 Nucl.Phys. A674, 229 (2000) M.Kohno, Y.Fujiwara, T.Fujita, C.Nakamoto, Y.Suzuki Hyperon Single-Particle Potentials Calculated from SU6 Quark-Model Baryon-Baryon Interactions
doi: 10.1016/S0375-9474(00)00164-0
2000NA14 Nucl.Phys. A670, 315c (2000) C.Nakamoto, Y.Fujiwara, Y.Suzuki Dependence of the H-Particle Mass on the Effective Meson-Exchange Potentials in a Quark Model
doi: 10.1016/S0375-9474(00)00121-4
2000NE04 Prog.Theor.Phys.(Kyoto) 103, 929 (2000) H.Nemura, Y.Suzuki, Y.Fujiwara, C.Nakamoto Study of Light Λ- and λΛ-Hypernuclei with the Stochastic Variational Method and Effective ΛN Potentials NUCLEAR STRUCTURE 3,4H, 4,5,6He; calculated hypernucleus radii, separation and excitation energies, related features. Stochastic variational method.
doi: 10.1143/PTP.103.929
2000YA18 Phys.Rev. C62, 034319 (2000) Structure of Light S = -2 Nuclei and Hyperon Mixing NUCLEAR STRUCTURE 6He, 10Be, 13B; calculated S=-2 hypernuclei binding energies, hyperon mixing. Several models compared.
doi: 10.1103/PhysRevC.62.034319
1999NE07 Prog.Theor.Phys.(Kyoto) 101, 981 (1999) H.Nemura, Y.Suzuki, Y.Fujiwara, C.Nakamoto Quark Pauli Effects on the Binding Energies os s-Shell Λ Hypernuclei NUCLEAR STRUCTURE 5He, 9Li, 9Be, 9B; calculated hypernucleus binding energies; deduced Pauli principle effects. Stochastic variational method.
doi: 10.1143/PTP.101.981
1998FU02 Nucl.Phys. A629, 190c (1998) Y.Fujiwara, T.Fujita, C.Nakamoto, Y.Suzuki Unified Description of NN and YN Interaction in the SU6 Quark Model
doi: 10.1016/S0375-9474(97)00685-4
1998FU10 Nucl.Phys. A639, 41c (1998) Y.Fujiwara, T.Fujita, C.Nakamoto, Y.Suzuki, M.Kohno Baryon-Baryon Interaction in a Quark Model
doi: 10.1016/S0375-9474(98)00250-4
1998FU15 Prog.Theor.Phys.(Kyoto) 100, 931 (1998) T.Fujita, Y.Fujiwara, C.Nakamoto, Y.Suzuki Scattering Observables of the NN and YN Interactions in the SU6 Quark Model NUCLEAR REACTIONS 1H(n, n), E=50-310 MeV; 1H(p, p), E=50-213 MeV; calculated σ(θ), polarization. Quark model, comparison with data, hyperon-nucleon scattering discussed.
doi: 10.1143/PTP.100.931
1998FU16 Prog.Theor.Phys.(Kyoto) 100, 957 (1998) Y.Fujiwara, T.Fujita, C.Nakamoto, Y.Suzuki Inelastic Capture Ratio at Rest and Low-Energy Cross Sections of Σ-p Scattering in the SU6 Quark Model NUCLEAR REACTIONS 1H(Σ+, X), (Σ-, X), E at 120-200 MeV/c; calculated σ. Quark model, resonating group method.
doi: 10.1143/PTP.100.957
1998NA26 Prog.Theor.Phys.(Kyoto) 99, 1001 (1998) One and Two Baryon Systems in the Chiral Constituent Quark Model
doi: 10.1143/PTP.99.1001
1998NA28 Nucl.Phys. A639, 51c (1998) C.Nakamoto, Y.Fujiwara, Y.Suzuki Baryon-Baryon Interaction with S = -2 in the SU6 Quark Model
doi: 10.1016/S0375-9474(98)00251-6
1996FU09 Phys.Rev.Lett. 76, 2242 (1996) Y.Fujiwara, C.Nakamoto, Y.Suzuki Unified Description of NN and YN Interactions in a Quark Model with Effective Meson-Exchange Potentials NUCLEAR REACTIONS 1H(X, X), E at ≤ 1 GeV/c; analyzed Σ+, Σ-, Λ elastic, charge-exchange σ(E). Unified description of NN, YN interactions, effective meson-exchange potentials, quark model.
doi: 10.1103/PhysRevLett.76.2242
1996FU21 Phys.Rev. C54, 2180 (1996) Y.Fujiwara, C.Nakamoto, Y.Suzuki Effective Meson-Exchange Potentials in the SU6 Quark Model for NN and YN Interactions NUCLEAR REACTIONS 1H(X, X), E at ≤ 1 GeV/c; calculated phase shifts, σ for Σ+ scattering. SU6 quark model for nucleon-nucleon, hyperon-nucleon interactions, effective meson-exchange potentials. NUCLEAR STRUCTURE 2H; calculated binding energy, rms radius, quadrupole moment, μ, D-state probability, D- to S-state ratio. Resonating group method.
doi: 10.1103/PhysRevC.54.2180
1996FU25 Prog.Theor.Phys.(Kyoto) 96, 463 (1996) T.Fujita, Y.Fujiwara, C.Nakamoto, Y.Suzuki, T.Yamamoto, R.Tamagaki Scattering Observables of NN Interaction in the SU6 Quark Model NUCLEAR REACTIONS 1H(n, n), (p, p), E ≤ 350 MeV; analyzed σ vs E, σ(θ), polarization observables. Quark SU6 model.
doi: 10.1143/PTP.96.463
1995FU14 Prog.Theor.Phys.(Kyoto) 94, 215 (1995) Y.Fujiwara, C.Nakamoto, Y.Suzuki RGM Study of the Hyperon-Nucleon Interaction in the SU6 Quark Model. I - Analysis of NN and Σ+p Systems - NUCLEAR REACTIONS 1H(X, X), E at ≤ 1 GeV/c; calculated total Σ+p σ(E). Resonating group method, SU6 quark model.
doi: 10.1143/PTP.94.215
1995FU15 Prog.Theor.Phys.(Kyoto) 94, 353 (1995) Y.Fujiwara, C.Nakamoto, Y.Suzuki RGM Study of the Hyperon-Nucleon Interaction in the SU6 Quark Model. II - Analysis of ΛN-ΣN(I = 1/2) Coupled-Channel System -
doi: 10.1143/PTP.94.353
1995NA30 Prog.Theor.Phys.(Kyoto) 94, 65 (1995) C.Nakamoto, Y.Suzuki, Y.Fujiwara Central Force of the Hyperon-Nucleon Interaction in the SU6 Quark Model
doi: 10.1143/ptp/94.1.65
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