NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Y.Fujiwara Found 83 matches. 2019AJ01 Phys.Lett. B 789, 620 (2019) S.Ajimura, H.Asano, G.Beer, C.Berucci, H.Bhang, M.Bragadireanu, P.Buehler, L.Busso, M.Cargnelli, S.Choi, C.Curceanu, S.Enomoto, H.Fujioka, Y.Fujiwara, T.Fukuda, C.Guaraldo, T.Hashimoto, R.S.Hayano, T.Hiraiwa, M.Iio, M.Iliescu, K.Inoue, Y.Ishiguro, T.Ishikawa, S.Ishimoto, K.Itahashi, M.Iwasaki, K.Kanno, K.Kato, Y.Kato, S.Kawasaki, P.Kienle, H.Kou, Y.Ma, J.Marton, Y.Matsuda, Y.Mizoi, O.Morra, T.Nagae, H.Noumi, H.Ohnishi, S.Okada, H.Outa, K.Piscicchia, Y.Sada, A.Sakaguchi, F.Sakuma, M.Sato, A.Scordo, M.Sekimoto, H.Shi, K.Shirotori, D.Sirghi, F.Sirghi, K.Suzuki, S.Suzuki, T.Suzuki, K.Tanida, H.Tatsuno, M.Tokuda, D.Tomono, A.Toyoda, K.Tsukada, O.Vazquez Doce, E.Widmann, T.Yamaga, T.Yamazaki, Q.Zhang, J.Zmeskal "K-pp", a K-bar-meson nuclear bound state, observed in 3He(K-, Λp)n reactions NUCLEAR REACTIONS 3He(K-, Λp), E ∼ 1 GeV; measured reaction products; deduced a distinct peak in the Λp invariant mass spectrum.
doi: 10.1016/j.physletb.2018.12.058
2014FU08 Few-Body Systems 55, 993 (2014) Four-Body Faddeev-Yakubovsky Equations Using Two-Cluster RGM Kernels: Applications to 4N and 4α Systems NUCLEAR STRUCTURE 3H, 3,4He; calculated ground state, α particle energies. Comparison with experimental data.
doi: 10.1007/s00601-014-0818-2
2011FU05 Prog.Theor.Phys.(Kyoto) 125, 957 (2011) Effective-Range Expansion of Neutron-Deuteron Scattering Studied by a Quark-Model Nonlocal Gaussian Potential
doi: 10.1143/PTP.125.957
2011FU06 Prog.Theor.Phys.(Kyoto) 125, 979 (2011) Quark-Model Baryon-Baryon Interaction Applied to Neutron-Deuteron Scattering. III -Breakup Differential Cross Sections- NUCLEAR REACTIONS H(d, 2p), E=16 MeV; 2H(n, 2n), E=8-10.3 MeV; 2H(p, 2p), E<70 MeV; calculated breakup σ(θ, E). Comparison with experimental data.
doi: 10.1143/PTP.125.979
2011FU07 Int.J.Mod.Phys. E20, 847 (2011) Effect of an off-shell transformation of the quark-model NN interaction in the neutron-deuteron scattering
doi: 10.1142/S0218301311018824
2010FU05 Prog.Theor.Phys.(Kyoto) 124, 433 (2010) Quark-Model Baryon-Baryon Interaction Applied to Neutron-Deuteron Scattering. I -Noyes-Kowalski Approach to the AGS Equations -
doi: 10.1143/PTP.124.433
2010KO41 Nucl.Phys. A835, 358c (2010) Quark-model predictions for the ΞN interaction and the implications for Ξ hypernuclei NUCLEAR REACTIONS 12C(K-, K+), E at 1.8 GeV/c; calculated Ξ- hypernucleus production σ(E, θ). Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.218
2009KO13 Phys.Rev. C 79, 054318 (2009) Localized N, Λ, Σ, and Ξ single-particle potentials in finite nuclei calculated with SU6 quark-model baryon-baryon interactions NUCLEAR STRUCTURE 12C, 16O, 28Si, 40Ca, 56Fe, 90Zr; calculated single-particle potentials and point nucleon density distributions using quark-model baryon-baryon interaction and the lowest order Brueckner theory.
doi: 10.1103/PhysRevC.79.054318
2008FU02 Phys.Rev. C 77, 027001 (2008) Y.Fujiwara, Y.Suzuki, M.Kohno, K.Miyagawa Addendum to triton and hypertriton binding energies calculated from SU6 quark-model baryon-baryon interactions NUCLEAR STRUCTURE 3H; calculated binding energies for nucleus and hypernucleus using SU6 model.
doi: 10.1103/PhysRevC.77.027001
2008FU12 Prog.Theor.Phys.(Kyoto) 120, 289 (2008) nα Resonating-Group Calculation with a Quark-Model G-Matrix NN Interaction
doi: 10.1143/PTP.120.289
2008SU01 Phys.Lett. B 659, 160 (2008) Y.Suzuki, H.Matsumura, M.Orabi, Y.Fujiwara, P.Descouvemont, M.Theeten, D.Baye Local versus nonlocal αα interactions in a 3α description of 12C NUCLEAR STRUCTURE 12C; calculated ground and excited 0+ states energies, radii. α-cluster model with non-local forces.
doi: 10.1016/j.physletb.2007.10.033
2007FU02 Nucl.Phys. A784, 161 (2007) Λα, Σα and Ξα potentials derived from the SU6 quark-model baryon-baryon interaction NUCLEAR STRUCTURE 5He; calculated hyperon-nucleus potentials, hypernucleus bound state energies.
doi: 10.1016/j.nuclphysa.2006.12.005
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
2007KO72 Phys.Rev. C 76, 064002 (2007) M.Kohno, R.Okamoto, H.Kamada, Y.Fujiwara Equivalent hyperon-nucleon interactions in low-momentum space
doi: 10.1103/PhysRevC.76.064002
2007SU12 Nucl.Phys. A790, 223c (2007) Y.Suzuki, Y.Fujiwara, W.Horiuchi, H.Matsumura, M.Orabi Dynamics of macroscopic and microscopic three-body systems NUCLEAR STRUCTURE 3H; calculated binding energies. Quark-model interactions. Comparison with data.
doi: 10.1016/j.nuclphysa.2007.03.039
2007TH16 Phys.Rev. C 76, 054003 (2007) M.Theeten, H.Matsumura, M.Orabi, D.Baye, P.Descouvemont, Y.Fujiwara, Y.Suzuki Three-body model of light nuclei with microscopic nonlocal interactions NUCLEAR STRUCTURE 6He, 9Be, 12C; calculated potential functions, phase shifts, charge densities, neutron densities. Compared to experimental energies.
doi: 10.1103/PhysRevC.76.054003
2006KO45 Phys.Rev.C 74, 064613 (2006) M.Kohno, Y.Fujiwara, Y.Watanabe, K.Ogata, M.Kawai Semiclassical distorted-wave model analysis of the (π-, K+)Σ formation inclusive spectrum NUCLEAR REACTIONS 12C, 28Si(π-, K+X), E at 1.2 GeV/c; analyzed hyperon production associated particle spectra, σ(E, θ); deduced hyperon-nucleus potential features.
doi: 10.1103/PhysRevC.74.064613
2006MA52 Nucl.Phys. A776, 1 (2006) H.Matsumura, M.Orabi, Y.Suzuki, Y.Fujiwara Removal of forbidden states in a three-α system NUCLEAR STRUCTURE 12C; calculated ground and excited 0+ states energies, radii. α-cluster model.
doi: 10.1016/j.nuclphysa.2006.07.002
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
2004FU05 Phys.Rev. C 69, 037002 (2004) Case of almost redundant components in 3α Faddeev equations
doi: 10.1103/PhysRevC.69.037002
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
2004FU11 Few-Body Systems 34, 237 (2004) Solving Three-Cluster OCM Equations in the Faddeev Formalism NUCLEAR STRUCTURE 12C; calculated 3α cluster states energies, related features. Orthogonality condition models, Faddeev formalism.
doi: 10.1007/s00601-004-0021-y
2004FU14 Nucl.Phys. A738, 382 (2004) Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki Faddeev Calculation of the Hypertriton in the Quark-Model NN and YN Interactions NUCLEAR STRUCTURE 3H; calculated hypernucleus wave function, binding energy. Three-cluster Fadeev formalism.
doi: 10.1016/j.nuclphysa.2004.04.066
2004FU15 Nucl.Phys. A738, 495 (2004) Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, D.Baye, J.-M.Sparenberg A Consistent 3α and 2αΛ Faddeev Calculation using the 2α RGM Kernel
doi: 10.1016/j.nuclphysa.2004.04.095
2004FU18 Phys.Rev. C 70, 024001 (2004) Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki Faddeev calculation of the hypertriton using the SU6 quark-model nucleon-nucleon and hyperon-nucleon interactions NUCLEAR STRUCTURE 3H; calculated hypertriton binding energy, wave function, related features. Three-cluster Faddeev formalism.
doi: 10.1103/PhysRevC.70.024001
2004FU19 Phys.Rev. C 70, 024002 (2004) Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, D.Baye, J.-M.Sparenberg Faddeev calculation of 3α and ααΛ systems using αα resonating-group method kernels NUCLEAR STRUCTURE 12C; calculated 3α-cluster states energies. 9Be; calculated hypernucleus ground and excited states energies. Faddeev calculations, two-cluster resonating-group method kernels.
doi: 10.1103/PhysRevC.70.024002
2004FU22 Phys.Rev. C 70, 037001 (2004) Y.Fujiwara, M.Kohno, K.Miyagawa, Y.Suzuki, J.-M.Sparenberg Faddeev calculation of 6ΛΛHe using SU6 quark-model baryon-baryon interactions NUCLEAR STRUCTURE 6He; calculated two-Λ hypernucleus binding energy. Faddeev formalism, two-cluster resonating-group method.
doi: 10.1103/PhysRevC.70.037001
2004FU26 Phys.Rev. C 70, 047002 (2004) Y.Fujiwara, M.Kohno, K.Miyagawa, Y.Suzuki Spin-orbit splitting of 9ΛBe excited states studied with the SU6 quark-model baryon-baryon interactions NUCLEAR STRUCTURE 9Be; calculated hypernucleus excited states energies, spin-orbit splitting.
doi: 10.1103/PhysRevC.70.047002
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
2003FU12 Nucl.Phys. A721, 983c (2003) Y.Fujiwara, K.Miyagawa, Y.Suzuki, M.Kohno, H.Nemura Three-Nucleon Bound State in the SU6 Quark Model for the Baryon-Baryon Interaction
doi: 10.1016/S0375-9474(03)01265-X
2003KO45 Phys.Rev. C 68, 034302 (2003) M.Kohno, Y.Fujiwara, Y.Akaishi Brueckner, rearrangement effects in 5ΛHe and 6ΛΛHe NUCLEAR STRUCTURE 5,6He; calculated rearrangement contributions to hypernucleus energy.
doi: 10.1103/PhysRevC.68.034302
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
2002FU12 Prog.Theor.Phys.(Kyoto) 107, 745 (2002) Y.Fujiwara, H.Nemura, Y.Suzuki, K.Miyagawa, M.Kohno Three-Cluster Equation Using the Two-Cluster RGM Kernel
doi: 10.1143/PTP.107.745
2002FU13 Phys.Rev. C66, 021001 (2002) Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, H.Nemura Triton binding energy calculated from the SU6 quark-model nucleon-nucleon interaction NUCLEAR STRUCTURE 2,3H, 3He; calculated binding energies, radii. Fadeev approach, quark-model interaction.
doi: 10.1103/PhysRevC.66.021001
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
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
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
1995FU11 Prog.Theor.Phys.(Kyoto) 93, 357 (1995) Multiconfiguration Resonating-Group Study of the 10-Nucleon System NUCLEAR STRUCTURE 10B; calculated levels. Multi-configuration, multi-channel resonating group method. NUCLEAR REACTIONS 6Li(α, α), E=0-8 MeV; calculated L(π)=2+, phase shifts vs E. Multi-configuration, multi-channel resonating group method.
doi: 10.1143/PTP.93.357
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
1995FU16 Prog.Theor.Phys.(Kyoto) 93, 711 (1995) Reaction Cross Sections in Light Nuclear Systems with the Multiconfiguration Resonating-Group Method NUCLEAR REACTIONS 7Li(n, n), (n, n'), E=9.58-12.2 MeV; 4He(3He, p), (3He, d), E=15.95 MeV; 4He(d, p), E=16.2 MeV; 6Li(n, n'), E=8.57, 12 MeV; 6Li(n, d), (n, t), E=12 MeV; calculated σ(θ). Multi-configuration resonating group method.
doi: 10.1143/ptp/93.4.711
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
1994FU17 Few-Body Systems 16, 91 (1994) Reaction Cross Sections in the Ten-Nucleon System NUCLEAR REACTIONS, ICPND 6Li(α, d), (α, α'), E ≤ 24 MeV; calculated reaction, breakup, total σ(E).
doi: 10.1007/BF01074543
1992FU10 Few-Body Systems 12, 21 (1992) Reaction Mechanisms in the Six-Nucleon System with the Multi-Configuration Resonating-Group Method NUCLEAR REACTIONS, ICPND 4He(d, d), E(cm) ≤ 22 MeV; calculated σ(θ), reaction σ vs E.
doi: 10.1007/BF01080194
1992IT03 J.Phys.Soc.Jpn. 61, 1287 (1992) Y.Itoh, H.Yasuoka, Y.Fujiwara, Y.Ueda, T.Machi, I.Tomeno, K.Tai, N.Koshizuka, S.Tanaka 63Cu(2) Nuclear Spin-Spin Relaxation in YBa2Cu3O(6.98), YBa2(63Cu)3O(7-δ), and YBa2Cu4O8 NUCLEAR MOMENTS 63Cu; measured nuclear quadrupole resonance; deduced 63Cu(2) spin-spin relaxation in YBa2Cu3O(6.98), YBa2(63Cu)3O(7-δ) and YBa2Cu4O8.
doi: 10.1143/JPSJ.61.1287
1991FU01 Phys.Rev. C43, 96 (1991) Multiconfiguration Resonating-Group Study of the Six-Nucleon System with Cluster-Rearrangement and Pseudo-Inelastic Configurations NUCLEAR REACTIONS, ICPND 2H(α, α), E ≤ 24 MeV; calculated phase shifts, σ(θ), σ(E). Multi-configuration resonating group method.
doi: 10.1103/PhysRevC.43.96
1991FU02 Nucl.Phys. A522, 459 (1991) Effects of d + 5He Cluster Configuration in the Seven-Nucleon System NUCLEAR REACTIONS, ICPND 3H(α, α), 6Li(n, n), E ≈ 0-18 MeV; calculated phase shifts, transmission coefficients vs E. 3H(α, n), (α, d), E=threshold-20 MeV; calculated σ(E). 4He(3He, 3He), E=15-95 MeV; 4He(3He, p), (3He, d), E=15-95 MeV; 6Li(n, n), E=8.57, 12 MeV; 6Li(n, n'), E=12 MeV; calculated σ(θ); deduced d+5He cluster role. Resonating group method.
doi: 10.1016/0375-9474(91)90076-I
1990FU01 Phys.Rev. C41, 28 (1990) Multiconfiguration Resonating-Group Theory of 8Li NUCLEAR STRUCTURE 8Li; calculated bound state, resonance energies. Resonating group method, multiple cluster configurations. NUCLEAR REACTIONS 7Li(n, n), E ≈ 0-20 MeV; calculated phase shifts, σ(θ), reaction σ(E). Multiconfiguration resonating group calculation.
doi: 10.1103/PhysRevC.41.28
1989FU03 Phys.Lett. 222B, 311 (1989) Resonating-Group Study of the 6.53 MeV State in 8Li NUCLEAR REACTIONS 7Li(n, n), E(cm)=4-7.5 MeV; calculated phase shifts. 8Li deduced resonance. Multi-configuration resonating group.
doi: 10.1016/0370-2693(89)90313-4
1988FU09 Phys.Rev. C38, 1531 (1988) Y.Fujiwara, Q.K.K.Liu, Y.C.Tang Multiconfiguration Resonating-Group Study of Scattering and Reaction Cross Sections in the Seven-Nucleon System NUCLEAR REACTIONS 4He(t, n), E ≈ 5-25 MeV; calculated σ(θ), reaction σ(E). Multi-configuration resonating group methods.
doi: 10.1103/PhysRevC.38.1531
1987FU01 Nucl.Phys. A462, 621 (1987) RGM Study of the NN Interaction in an Extended Quark Model NUCLEAR STRUCTURE 2H; calculated bound state characteristics. Extended quark model. NUCLEAR REACTIONS 1H(n, n), (p, p), 1n(n, n), E=low; calculated phase shifts, scattering lengths, effective range parameters. Extended quark model.
doi: 10.1016/0375-9474(87)90569-0
1987HE06 Nucl.Phys. A463, 255c (1987) The NN Interaction in a Quark Model with Quark-Antiquark Excitations NUCLEAR REACTIONS 1H(p, p), (n, n), E(cm) ≤ 200 MeV; calculated phase shifts. Quark model.
doi: 10.1016/0375-9474(87)90668-3
1985FU01 Phys.Rev. C31, 342 (1985) Multiconfiguration Resonating-Group Theory of the Seven-Nucleon System with Realistic Cluster Wave Functions NUCLEAR REACTIONS 6Li(n, n), 3H(α, α), E not given; calculated phase shifts vs relative energy. 7Li deduced resonances. Multi-configurational resonating group theory. NUCLEAR STRUCTURE 6Li; calculated different cluster reduced width amplitudes. Multi-configurational resonating group theory.
doi: 10.1103/PhysRevC.31.342
1985FU11 Phys.Rev. C32, 1428 (1985) Cluster Configurations in 7Li NUCLEAR REACTIONS 3H(α, α), E ≈ 1-20 MeV; calculated L=1 phase shifts; deduced cluster configuration dependence. Resonating group method, various cluster configurations. NUCLEAR STRUCTURE 7Li; calculated α+3H cluster separation energies. Resonating group method, various cluster configurations.
doi: 10.1103/PhysRevC.32.1428
1985SH08 Phys.Rev. C31, 2001 (1985) P.N.Shen, Y.C.Tang, Y.Fujiwara, H.Kanada Specific Distortion Effects in the Five-Nucleon System NUCLEAR REACTIONS 3He(d, d), E=0-20 MeV; calculated phase shifts, σ(θ); deduced specific distortion effects. Resonating group formulation.
doi: 10.1103/PhysRevC.31.2001
1984FU04 Phys.Rev. C29, 2025 (1984) n + 6Li System Investigated with the Resonating-Group Method: Effects of channel coupling NUCLEAR REACTIONS 6Li(n, n), E=0-25 MeV; calculated phase shifts vs E; deduced channel coupling effects. Resonanting group method.
doi: 10.1103/PhysRevC.29.2025
1983FU06 Phys.Rev. C27, 2457 (1983) n + 6Li System Investigated with the Resonating-Group Method: Effect of target clustering and charge form factor NUCLEAR STRUCTURE 6Li; calculated charge from factor. Resonating group method, three-cluster formulation. NUCLEAR REACTIONS 6Li(n, n), E=0-50 MeV; calculated phase shifts; 6Li(n, n), E=40 MeV; calculated σ(θ); deduced resonance structure cluster dependence. Resonating group method.
doi: 10.1103/PhysRevC.27.2457
1983FU11 Phys.Rev. C28, 1869 (1983) Channel-Coupling Effects in the Resonating-Group Study of the Seven-Nucleon System NUCLEAR REACTIONS 3H(α, α), E=0-35 MeV; calculated phase shifts. 3H(α, α), E=35 MeV; calculated σ(θ). 4He(t, n), E=5-35 MeV; calculated reaction σ(E). Resonating group method, channel coupling effects.
doi: 10.1103/PhysRevC.28.1869
1983FU19 Phys.Lett. 131B, 261 (1983) Three-Cluster Resonating-Group Method in the Coupled-Channel Formalism NUCLEAR REACTIONS 3H(α, α), 6Li(n, n), E(cm)=7-50 MeV; calculated phase shifts vs E. Three cluster resonating group method, analytical formulation.
doi: 10.1016/0370-2693(83)90494-X
1982LE23 Phys.Rev. C26, 1847 (1982) M.LeMere, Y.Fujiwara, Y.C.Tang, Q.K.K.Liu Detailed Investigation of Exchange Effects in 3He + α and α + 16O Scattering NUCLEAR REACTIONS 3He(α, α), E=16, 30, 60 MeV; 16O(α, α), E=18, 80 MeV; calculated σ(θ); deduced exchange effect role. Resonating group method, antisymmetrization.
doi: 10.1103/PhysRevC.26.1847
1982ST15 Phys.Rev. C26, 2410 (1982) D.J.Stubeda, Y.Fujiwara, Y.C.Tang N + 6Li System with Flexible Cluster Wave Function NUCLEAR REACTIONS 6Li(p, p), E=22.2, 30, 38.9 MeV; 6Li(n, n), E ≤ 48 MeV; calculated σ(θ), phase shifts. Resonating group method, flexible clusters, generator coordinate technique.
doi: 10.1103/PhysRevC.26.2410
1979FU06 Prog.Theor.Phys.(Kyoto) 62, 122 (1979) Cluster-Structure Study of 20Ne by (16O-α)+(12C-8Be) Coupled Channel Orthogonality Condition Model. II NUCLEAR STRUCTURE 20Ne; calculated levels, wave functions, reduced α-widths; deduced rotational band structure. Alpha plus 16O, 8Be plus 12C cluster channel coupling, orthogonality condition. NUCLEAR REACTIONS 16O(α, α), E(cm)=1-12 MeV; calculated phase shifts, Γα, resonance energies. Alpha plus 16O, 8Be plus 12C cluster channel coupling, orthogonality condition.
doi: 10.1143/PTP.62.122
1979FU08 Prog.Theor.Phys.(Kyoto) 62, 138 (1979) Cluster-Structure Study of 20Ne by (16O-α)+(12C-8Be) Coupled Channel Orthogonality Condition Model. III NUCLEAR STRUCTURE 20Ne; deduced α-widths, B(λ). Alpha plus 16O, 8Be plus 12C cluster channel coupling, orthogonality condition. NUCLEAR REACTIONS 16O(α, α), E(cm)=1-18 MeV; calculated phase shifts. Coupling to 8Be plus 12C cluster channel, ortogonality condition.
doi: 10.1143/PTP.62.138
1979FU09 Prog.Theor.Phys.(Kyoto) 61, 1629 (1979) Y.Fujiwara, H.Horiuchi, R.Tamagaki Cluster-Structure Study of 20Ne by (16O-α)+(12C-8Be) Coupled Channel Orthogonality Condition Model. I NUCLEAR STRUCTURE 20Ne; calculated levels, α-, 8Be-reduced width amplitudes; deduced cluster structure of 0+ levels. Alpha plus 12C cluster channel coupling, orthogonality condition.
doi: 10.1143/PTP.61.1629
1976FU09 Progr.Theor.Phys. 56, 154 (1976) A Study on Three-Alpha Structure of 12C in the Faddeev Formalism NUCLEAR STRUCTURE 12C; calculated 3α-structure. Faddeev formalism.
1973FU10 J.Phys.Soc.Jap. 34, 1690 (1973) Y.Fujiwara, M.Nomura, H.Fujiwara Nuclear Magnetic Resonance of V51 in Iron-Rich Fe-V Alloys NUCLEAR MOMENTS 51V; measured nuclear magnetic resonance.
doi: 10.1143/JPSJ.34.1690
1968IS01 Inst. Nucl. Study, Univ. Tokyo, Ann. Rept. 1967, p. 17 (1968) Y.Ishizaki, Y.Saji, T.Suehiro, K.Yuasa, Y.Fujiwara, Y.Yoshida, H.Taketani Levels of 58Cu NUCLEAR STRUCTURE 58Cu; measured not abstracted; deduced nuclear properties.
1964IS01 Inst.Nucl.Study, Univ.Tokyo, Annual Rept., p.11 (1964); NP-15772 Y.Ishizaki, Y.Saji, H.Yamaguchi, Y.Fujiwara, B.Saeki, K.Yuasa, K.Okano, N.Yoshimura, T.Aizawa Direct (p, n) Reaction in Medium Weight Nuclei NUCLEAR STRUCTURE 56Co, 58Cu, 55Fe, 52Mn, 88Y, 80Br, 94Nb, 90Nb, 89Zr; measured not abstracted; deduced nuclear properties.
Back to query form |