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NSR database version of April 24, 2024.

Search: Author = C.Nakamoto

Found 29 matches.

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2016NA31      Phys.Rev. C 94, 035803 (2016)

C.Nakamoto, Y.Suzuki

Quark-Pauli effects in three octet-baryons

doi: 10.1103/PhysRevC.94.035803
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2000YA18      Phys.Rev. C62, 034319 (2000)

T.Yamada, C.Nakamoto

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1998NA26      Prog.Theor.Phys.(Kyoto) 99, 1001 (1998)

C.Nakamoto, H.Toki

One and Two Baryon Systems in the Chiral Constituent Quark Model

doi: 10.1143/PTP.99.1001
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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