NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = M.Kohno Found 81 matches. 2024KO03 Phys.Rev. C 109, 024003 (2024) Contributions of 2π exchange, 1π exchange, and contact three-body forces in NNLO chiral effective field theory to 3ΛH
doi: 10.1103/PhysRevC.109.024003
2023KA18 Phys.Rev. C 108, 024004 (2023) Faddeev calculation of 3ΛH incorporating the 2π-exchange ΛNN interaction NUCLEAR STRUCTURE 3H; calculated binding energies for Λ hypernuclei, hypertriton separation energies with and without 2π-exchange ΛNN 3-baryon force. Faddeev calculations of hypertriton performed, incorporating 2π-exchange ΛNN three-baryon force.
doi: 10.1103/PhysRevC.108.024004
2022KO27 Phys.Rev. C 106, 054004 (2022) Partial-wave expansion of ΛNN three-baryon interactions in chiral effective field theory NUCLEAR STRUCTURE 2H; calculated s- and d-wave functions in momentum space, folding potential of ΛNN hypernuclei. Partial-wave decomposition of three-body forces concerning the relevant Jacobi momenta, which allows to systematically treat the higher-rank spin and angular-momentum tensor-product structure.
doi: 10.1103/PhysRevC.106.054004
2021KO38 Prog.Theor.Exp.Phys. 2021, 103D04 (2021) Ξ hypernuclear states predicted by next-to-leading-order chiral baryon-baryon interactions NUCLEAR STRUCTURE 56Fe; calculated the Ξ levels, level phase and atomic shifts, single-particle potential and levels, rms radii, J, π. Chiral NLOΞN interactions with a cutoff scale.
doi: 10.1093/ptep/ptab115
2020KO23 Phys.Rev. C 102, 024611 (2020) Comparison between optical-model potentials in G-matrix folding method and improved local-density approximation method NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(p, p), E=65, 100 MeV; analyzed experimental data for σ(E, θ) for microscopic optical-model potentials (OMP) using two methods: G-matrix folding method, and an improved local-density approximation (LDA) method; discussed comparison and analytical relationship between the two approaches.
doi: 10.1103/PhysRevC.102.024611
2019KO14 Phys.Rev. C 100, 024313 (2019) Ξ hyperons in the nuclear medium described by chiral NLO interactions
doi: 10.1103/PhysRevC.100.024313
2019MI17 Phys.Rev. C 100, 034310 (2019) T.Miyagi, T.Abe, M.Kohno, P.Navratil, R.Okamoto, T.Otsuka, N.Shimizu, S.R.Stroberg Ground-state properties of doubly magic nuclei from the unitary-model-operator approach with chiral two- and three-nucleon forces NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground-state energies, root-mean square (rms) radii, charge radii. Unitary-model-operator approach (UMOA), with similarity renormalization group (SRG) evolved nucleon-nucleon (NN) and three-nucleon (3N) interactions based on chiral effective field theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.034310
2018KO10 Phys.Rev. C 97, 035206 (2018) Single-particle potential of the Λ hyperon in nuclear matter with chiral effective field theory NLO interactions including effects of YNN three-baryon interactions
doi: 10.1103/PhysRevC.97.035206
2018KO25 Phys.Rev. C 98, 054617 (2018) Pauli rearrangement potential for a scattering state with the nucleon-nucleon interaction in chiral effective field theory NUCLEAR REACTIONS 40Ca(p, p), (n, n), E=65, 100 MeV; calculated momentum and energy dependence of the Pauli rearrangement potential in symmetric nuclear matter as function of Fermi momenta, relation between the energy and the momentum in symmetric nuclear matter, radial dependence of the real part of the optical model potential, lowest-order potential, and Pauli rearrangement potential using a local density approximation in chiral effective field theory (ChEFT) with NN and 3N interactions. Comparison with other theoretical predictions.
doi: 10.1103/PhysRevC.98.054617
2017MI16 Phys.Rev. C 96, 024609 (2017) K.Minomo, M.Kohno, K.Yoshida, K.Ogata Probing three-nucleon-force effects via (p, 2p) reactions NUCLEAR REACTIONS 40Ca(p, 2p)39K, E=148.2, 150 MeV; calculated triple differential cross sections as a function of the recoil momentum of the residue, unpolarized in-medium pp cross sections as a function of the relative momentum, with and without three-nucleon-forces, and compared with experimental data. Distorted-wave impulse approximation (DWIA) formalism with a g-matrix interaction based on chiral two- and three-nucleon forces.
doi: 10.1103/PhysRevC.96.024609
2016MI03 Phys.Rev. C 93, 014607 (2016), Erratum Phys.Rev. C 96, 059906 (2017) Microscopic coupled-channels calculations of nucleus-nucleus scattering including chiral three-nucleon-force effects NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=30, 85 MeV; 16O(16O, 16O), (16O, 16O'), E=44, 70 MeV; calculated differential σ(E, θ), for elastic and inelastic scattering with and without the chiral three-nucleon force (3NF) effects. Microscopic coupled-channels method. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.014607
2015KO21 Prog.Theor.Exp.Phys. 2015, 123D02 (2015) Nuclear saturation in lowest-order Brueckner theory with two- and three-nucleon forces in view of chiral effective field theory
doi: 10.1093/ptep/ptv166
2015TO12 Phys.Rev. C 92, 024618 (2015), Erratum Phys.Rev. C 96, 059905 (2017) M.Toyokawa, M.Yahiro, Ta.Matsumoto, Ko.Minomo, K.Ogata, M.Kohno Microscopic calculations based on chiral two- and three-nucleon forces for proton- and 4He-nucleus scattering NUCLEAR REACTIONS 40Ca, 58Ni, 208Pb(p, p'), E=65 MeV; 58Ni, 208Pb(α, α'), E=72 MeV; calculated differential σ(θ) using standard Brueckner-Hartree-Fock (BHF) method and the g-matrix folding model, the g matrix evaluated from chiral two-nucleon force (2NF) of N3LO and chiral three-nucleon force (3NF) of NNLO; deduced effects of chiral three-nucleon force (3NF) on proton and α scattering. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.024618
2015TO18 J.Phys.(London) G42, 025104 (2015); Corrigenda J.Phys.(London) G44, 079502 (2017) M.Toyokawa, K.Minomo, M.Kohno, M.Yahiro Roles of chiral three-nucleon forces in nucleon-nucleus scattering NUCLEAR REACTIONS 12C, 16O, 24Mg, 40Ca, 58Ni, 90Zr, 208Pb(p, p), E=65 MeV; calculated σ(θ), vector analyzing powers. Comparison with experimental data.
doi: 10.1088/0954-3899/42/2/025104
2014MI22 Phys.Rev. C 90, 051601 (2014), Erratum Phys.Rev. C 96, 059904 (2017) K.Minomo, M.Toyokawa, M.Kohno, M.Yahiro Effects of a chiral three-nucleon force on nucleus-nucleus scattering NUCLEAR REACTIONS 12C(12C, 12C), E=85 MeV/nucleon; 16C(16C, 16C), E=70 MeV/nucleon; calculated folding potential, differential σ(θ); deduced effects of next-to-next-to leading order (NNLO) chiral three-nucleon force (3NF). Brueckner-Hartree-Fock method and the g-matrix folding model. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.051601
2013KO21 Nucl.Phys. A914, 427c (2013) Λ, Σ, and Ξ hyperons in neutron matter
doi: 10.1016/j.nuclphysa.2013.02.003
2013KO36 Phys.Rev. C 88, 064005 (2013), Erratum Phys.Rev. C 96, 059903 (2017) Nuclear and neutron matter G-matrix calculations with a chiral effective field theory potential including effects of three-nucleon interactions
doi: 10.1103/PhysRevC.88.064005
2012KO27 Phys.Rev. C 86, 014317 (2012) 4He energies and radii calculated by the coupled-cluster method with a many-body average potential NUCLEAR STRUCTURE 4He; calculated ground state energies, rms radii. Coupled-cluster method (CCM) calculations with AV18 and CD-Bonn interactions. Contribution of the three-nucleon force to the ground-state energy.
doi: 10.1103/PhysRevC.86.014317
2012KO44 Phys.Rev. C 86, 061301 (2012) Strength of reduced two-body spin-orbit interaction from a chiral three-nucleon force
doi: 10.1103/PhysRevC.86.061301
2011OG12 J.Phys.:Conf.Ser. 312, 082008 (2011) K.Ogata, T.Matsumoto, S.Hashimoto, K.Minomo, T.Egami, Y.Iseri, M.Kohno, S.Chiba, C.A.Bertulani, Y.R.Shimizu, M.Kamimura, M.Yahiro Status of breakup reaction theory NUCLEAR REACTIONS 7Li(d, γ), (d, n), (d, p), E=10-50 MeV; calculated σ. 90Zr(p, p), E=65, 800 MeV; calculated dσ with and without Brieva-Rook localization. 208Pb(8B, X), E=250 MeV/nucleon; calculated breakup σ including relativistic corrections. 209Bi(6He, 6He), E=22.5 MeV; calculated σ with and without breakup effects, B(E1) strength distribution. Three- and four-body CDCC.
doi: 10.1088/1742-6596/312/4/082008
2010KO02 Prog.Theor.Phys.(Kyoto) 123, 157 (2010) Ξ-Nucleus Potential and (K-, K+) Inclusive Spectrum at Ξ-Production Threshold Region
doi: 10.1143/PTP.123.157
2010KO03 Phys.Rev. C 81, 014003 (2010) Comparative study of hyperon-nucleon interactions in a quark model and in chiral effective field theory by low-momentum equivalent interactions and G matrices
doi: 10.1103/PhysRevC.81.014003
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
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
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
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
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
2002OG04 Nucl.Phys. A703, 152 (2002) K.Ogata, Y.Watanabe, S.Weili, M.Kohno, M.Kawai Semiclassical Distorted Wave Model Analysis of the Complete Set of Spin Transfer Coefficients for Multistep Direct (p, nx) at 350 MeV NUCLEAR REACTIONS 40Ca(p, p'X), E=392 MeV; calculated σ(E, θ). 12C, 40Ca(p, nX), E=346 MeV; calculated σ(E, θ), spin transfer coefficients. Semiclassical distorted wave model, multistep processes, several nucleon-nucleon forces compared.
doi: 10.1016/S0375-9474(01)01339-2
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
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
2000SU03 Nucl.Phys. A665, 92 (2000) K.Suzuki, R.Okamoto, M.Kohno, S.Nagata Exact Treatment of the Pauli Exclusion Operator in Nuclear Matter Calculation
doi: 10.1016/S0375-9474(99)00399-1
1999OG12 Phys.Rev. C60, 054605 (1999); Erratum Phys.Rev. C63, 019902 (2001) K.Ogata, M.Kawai, Y.Watanabe, W.Sun, M.Kohno Theoretical Modification on Semiclassical Distorted Wave Model and Its Application to the Study of Spin Observables NUCLEAR REACTIONS 90Zr(p, p'X), (p, nX), E=160 MeV; 58Ni(p, p'X), E=80 MeV; calculated σ(E, θ), spin observables. Extended semiclassical distorted wave model, comparisons with data.
doi: 10.1103/PhysRevC.60.054605
1999SU15 Phys.Rev. C60, 064605 (1999); Erratum Phys.Rev. C63, 019903 (2001) W.Sun, Y.Watanabe, M.Kohno, K.Ogata, M.Kawai Semiclassical Distorted Wave Model with Wigner Transform of One-Body Density Matrix NUCLEAR REACTIONS 90Zr(p, p'X), E=80, 160 MeV; calculated σ(E, θ); deduced target nucleon momentum effects. Semiclassical distorted wave model, finite range single particle potential. Comparison with data, other models.
doi: 10.1103/PhysRevC.60.064605
1999WA07 Phys.Rev. C59, 2136 (1999); Erratum Phys.Rev. C63, 019901 (2001) Y.Watanabe, R.Kuwata, W.Sun, M.Higashi, H.Shinohara, M.Kohno, K.Ogata, M.Kawai Semiclassical Distorted Wave Model Analysis of Multistep Direct (p, p'x) and (p, nx) Reactions to the Continuum NUCLEAR REACTIONS 90Zr(p, p'X), (p, nX), E=80, 120, 160 MeV; 58Ni(p, p'X), E=65, 120 MeV; 209Bi(p, p'X), E=62 MeV; calculated σ(E, θ); deduced role of three-step processes. Extended semiclassical distorted wave model. Comparison with data, other models.
doi: 10.1103/PhysRevC.59.2136
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
1998KO21 Phys.Rev. C57, 3495 (1998) M.Kohno, M.Higashi, Y.Watanabe, M.Kawai In-Medium Nucleon-Nucleon Cross Sections from Nonrelativistic Reaction Matrices in Nuclear Matter
doi: 10.1103/PhysRevC.57.3495
1993KO44 Phys.Rev. C48, 3122 (1993) Description of Proton Elastic Scattering on 6,7,9,11Li with Microscopic Effective Interaction NUCLEAR REACTIONS 6,7,9,11Li(p, p), E ≈ 60 MeV; calculated σ(θ). Microscopic effective interaction.
doi: 10.1103/PhysRevC.48.3122
1992KO22 Prog.Theor.Phys.(Kyoto) 88, 537 (1992) Widths of Hypernuclear Lambda and Σ Single-Particle States NUCLEAR STRUCTURE 40Ca; calculated hypernuclear single-particle states widths.
doi: 10.1143/ptp/88.3.537
1990KO36 Nucl.Phys. A519, 755 (1990) Pion-Induced (Eta) Production on Nuclei NUCLEAR REACTIONS 12C, 16O(π+, pX), E at 800 MeV/c; calculated eta production σ(θ, E). DWIA, Green function method.
doi: 10.1016/0375-9474(90)90434-N
1989KO32 Nuovo Cim. 102A, 193 (1989) K+(Lambda) Photoproduction Amplitudes Incorporating Absorptive Effects and Hypernuclear Formation NUCLEAR REACTIONS 1H(γ, K+), E=0.9-3 GeV; calculated σ(E). 16O(γ, K+), E=1.3 GeV; calculated σ(θ); deduced Lambda photoproduction amplitudes.
doi: 10.1007/BF02735106
1989KO42 Phys.Lett. 231B, 219 (1989) Low Energy Eta Production in (π+, p) and (γ, p) Reactions on 12C NUCLEAR REACTIONS 12C(π+, p), E at 800 MeV/c; 12C(γ, p), E=800 MeV; calculated eta production σ(θ) vs E. Green's function method, phenomenological spreading potential.
doi: 10.1016/0370-2693(89)90202-5
1989TA04 Phys.Rev. C39, 741 (1989) Absorptive Effects in K+(Lambda) Photoproduction on Nucleons and Nuclei NUCLEAR REACTIONS 16O(γ, K+), E=1.3 GeV; calculated hypernuclear formation σ(θ).
doi: 10.1103/PhysRevC.39.741
1988KO13 Phys.Rev. C38, 584 (1988) Proton Distortion Effects and Meson Exchange Current Contributions in the (e, e'p) Reaction NUCLEAR REACTIONS 12C(e, e'p), E not given; calculated transverse to longitudinal response ratio; deduced proton distortion role.
doi: 10.1103/PhysRevC.38.584
1987HA40 Phys.Lett. 199B, 17 (1987) R.Hausmann, P.B.Siegel, W.Weise, M.Kohno Coupled Channel Calculation of Σ-Hypernuclear Spectra from 12C, 16O and 6Li Targets NUCLEAR REACTIONS 6Li, 12C, 16O(K-, π+), E=713 MeV/c; calculated σ(E(π+), θ(π+)). DWIA.
doi: 10.1016/0370-2693(87)91455-9
1987KO30 Nucl.Phys. A470, 609 (1987) M.Kohno, R.Hausmann, P.Siegel, W.Weise Σ- Hypernuclear Spectra from (K-, π+) Inclusive Reactions NUCLEAR REACTIONS 12C(K-, K-), E at 800 MeV/c; calculated σ(θ). 12C, 16O(K-, π+), E at 450 MeV/c; 12C(K-, π-), E at rest; calculated missing mass spectra.
doi: 10.1016/0375-9474(87)90589-6
1986KO12 Nucl.Phys. A454, 429 (1986) Proton-Antiproton Scattering and Annihilation into Two Mesons NUCLEAR REACTIONS 1H(p-bar, p-bar), (p-bar, n-bar), E at 200-700 MeV/c; calculated total, elastic, inelastic σ.
doi: 10.1016/0375-9474(86)90098-9
1985MA37 J.Phys.(London) G11, L151 (1985) L.Mathelitsch, K.Schwarz, H.F.K.Zingl, M.Kohno Mesion and Relativistic Corrections to Electromagnetic Form Factors of the Deuteron NUCLEAR REACTIONS 2H(e, e), E not given; calculated magnetic form factor, structure function vs momentum transfer.
doi: 10.1088/0305-4616/11/9/003
1984HA28 Nucl.Phys. A420, 399 (1984) Nucleonic Versus Nuclear Spin-Isospin Polarization: A study of the 48Ca and 88Sr M1 form factors NUCLEAR REACTIONS 48Ca, 88Sr(e, e'), E not given; calculated M1 form factors; deduced isobar-hole, nucleon-hole interaction relative strength role. Nuclear, isobar-hole polarizations, meson exchange current effects, isovector spin transition quenching.
doi: 10.1016/0375-9474(84)90665-1
1984KO06 Phys.Lett. 137B, 10 (1984) M.Kohno, D.W.L.Sprung, S.Nagata, N.Yamaguchi Incident Energy Dependence of the Effective Interaction and Radius of the Optical Model Potential NUCLEAR REACTIONS 40Ca(p, p), E=30.3 MeV; calculated σ(θ), proton polarization; deduced effective interaction incident energy dependence. Microscopic optical model.
doi: 10.1016/0370-2693(84)91095-5
1983KO08 J.Phys.(London) G9, L85 (1983) Mesonic and Relativistic Corrections to the Deuteron Charge Radius and Quadrupole Moment NUCLEAR STRUCTURE 2H; calculated quadrupole moment, charge radius correction factors. Mesonic, relativistic effects, Paris potential wave function.
doi: 10.1088/0305-4616/9/1/013
1983KO11 Nucl.Phys. A397, 1 (1983) Elastic Scattering of Protons and Neutrons on 48Ca by the Density-Dependent Hartree-Fock Field NUCLEAR REACTIONS 40Ca(p, p), E=10.37, 14.51, 30.3, 40 MeV; 40Ca(n, n), E=7.91, 14.1, 20, 26 MeV; calculated σ(θ), P(θ). Self-consistent, density-dependent Hartree-Fock field real potential, phenomenological imaginary potential.
doi: 10.1016/0375-9474(83)90075-1
1983KO32 Nucl.Phys. A410, 349 (1983) Density-Dependent Hartree-Fock Response Functions in Quasi-Elastic Electron Scattering on 12C and Related Sum Rules NUCLEAR REACTIONS 12C(e, e'), E=180, 220, 500 MeV; calculated σ(θ, E(e')), longitudinal, transverse response functions. Density-dependent forces, Hartree-Fock approximation.
doi: 10.1016/0375-9474(83)90631-0
1982KO15 Phys.Rev. C26, 297 (1982) Quenching of the Electromagnetic M1 Strength Due to the First Order Mesonic and Ground State Correlation Effects NUCLEAR STRUCTURE 12C, 48Ca, 90Zr, 208Pb; calculated M1 transition strength. Ground state correlation, isobar-hole excitation, meson exchange currents.
doi: 10.1103/PhysRevC.26.297
1982KO22 Can.J.Phys. 60, 1193 (1982) On the Quenching of the Spin Flip Excitation Strength due to the Isobar-Hole Excitation Process NUCLEAR STRUCTURE 12C, 48Ca, 90Zr, 208Pb; calculated M1 transition strength; deduced quenching effect mass dependence. Isobar-hole excitation, perturbation theory, Hartree-Fock wave functions.
doi: 10.1139/p82-163
1982MO20 Nucl.Phys. A388, 525 (1982) F.H.Molzahn, M.Kohno, D.W.L.Sprung, X.Campi The Local Fermi Momentum and Effective Nuclear Interactions NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 132Sn, 140Ce, 208Pb; calculated charge radius, nucleon binding energy, incompressibility, nucleon removal energies. 40Ca, 208Pb; calculated charge density. Hartree-Fock method, local Fermi momentum approximation, Skyrme type effective interactions.
doi: 10.1016/0375-9474(82)90475-4
1982SU08 Prog.Theor.Phys.(Kyoto) 68, 690 (1982) Collective 1+ Δ- Hole States NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated collective 1+ states. Isobar-hole excitation.
doi: 10.1143/PTP.68.690
1981SE06 Prog.Theor.Phys.(Kyoto) 65, 204 (1981) Nuclear Binding Mechanism and Structure of Neutron-Rich Be and B Isotopes by Molecular-Orbital Model NUCLEAR STRUCTURE 8,9,10,11,12,13,14,15,16Be, 9,10,11,12,13,14,15,16,17B; calculated levels, binding energy. Molecular-orbital model, density-dependent effective interactions.
doi: 10.1143/PTP.65.204
1979KO18 Prog.Theor.Phys. 61, 1065 (1979) Isoscalar Giant Resonances and Landau Parameters with Density-Dependent Effective Interactions NUCLEAR STRUCTURE 16O, 40Ca; calculated isoscalar giant monopole, quadrupole collective energies. Density-dependent effective interactions.
doi: 10.1143/PTP.61.1065
1979KO29 Prog.Theor.Phys.Suppl No.65, 200 (1979) M.Kohno, S.Nagata, N.Yamaguchi Chapter VII. Hartree-Fock Calculations of Nuclear Bulk Properties with Density- and Starting-Energy-Dependent Effective Interaction NUCLEAR STRUCTURE 12Be, 16,22O, 40,48Ca; calculated p, n density distributions, differences of rms, radii. Density-, energy-dependent effective interactions, Hartree-Fock method. NUCLEAR REACTIONS 16O(e, e), E=374.5 MeV; 40Ca(e, e), E=249.3, 496.8 MeV; 48Ca(e, e), E=250, 500 MeV; calculated σ(θ). DWBA analysis, charge distributions from Hartree-Fock calculations.
doi: 10.1143/PTPS.65.200
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