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NSR database version of May 19, 2024.

Search: Author = M.Kohno

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2024KO03      Phys.Rev. C 109, 024003 (2024)

M.Kohno, H.Kamada, K.Miyagawa

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
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2023KA18      Phys.Rev. C 108, 024004 (2023)

H.Kamada, M.Kohno, K.Miyagawa

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
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2022KO27      Phys.Rev. C 106, 054004 (2022)

M.Kohno, H.Kamada, K.Miyagawa

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
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2021KO38      Prog.Theor.Exp.Phys. 2021, 103D04 (2021)

M.Kohno, K.Miyagawa

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
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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
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2019KO14      Phys.Rev. C 100, 024313 (2019)


Ξ hyperons in the nuclear medium described by chiral NLO interactions

doi: 10.1103/PhysRevC.100.024313
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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
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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
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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
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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
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2016MI03      Phys.Rev. C 93, 014607 (2016), Erratum Phys.Rev. C 96, 059906 (2017)

K.Minomo, M.Kohno, K.Ogata

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
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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
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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
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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
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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
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2013KO21      Nucl.Phys. A914, 427c (2013)


Λ, Σ, and Ξ hyperons in neutron matter

doi: 10.1016/j.nuclphysa.2013.02.003
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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
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2012KO27      Phys.Rev. C 86, 014317 (2012)

M.Kohno, R.Okamoto

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
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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
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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
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2010KO02      Prog.Theor.Phys.(Kyoto) 123, 157 (2010)

M.Kohno, S.Hashimoto

Ξ-Nucleus Potential and (K-, K+) Inclusive Spectrum at Ξ-Production Threshold Region

doi: 10.1143/PTP.123.157
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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
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2010KO41      Nucl.Phys. A835, 358c (2010)

M.Kohno, Y.Fujiwara, Y.Suzuki

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
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2009KO13      Phys.Rev. C 79, 054318 (2009)

M.Kohno, Y.Fujiwara

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
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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
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2008FU12      Prog.Theor.Phys.(Kyoto) 120, 289 (2008)

Y.Fujiwara, M.Kohno, Y.Suzuki

nα Resonating-Group Calculation with a Quark-Model G-Matrix NN Interaction

doi: 10.1143/PTP.120.289
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2007FU02      Nucl.Phys. A784, 161 (2007)

Y.Fujiwara, M.Kohno, Y.Suzuki

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
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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
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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
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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
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2004FU05      Phys.Rev. C 69, 037002 (2004)

Y.Fujiwara, Y.Suzuki, M.Kohno

Case of almost redundant components in 3α Faddeev equations

doi: 10.1103/PhysRevC.69.037002
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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
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2004FU11      Few-Body Systems 34, 237 (2004)

Y.Fujiwara, M.Kohno, Y.Suzuki

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1990KO36      Nucl.Phys. A519, 755 (1990)

M.Kohno, H.Tanabe

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
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1989KO32      Nuovo Cim. 102A, 193 (1989)

M.Kohno, H.Tanabe, C.Bennhold

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
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1989KO42      Phys.Lett. 231B, 219 (1989)

M.Kohno, H.Tanabe

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
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1989TA04      Phys.Rev. C39, 741 (1989)

H.Tanabe, M.Kohno, C.Bennhold

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
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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
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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
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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
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1986KO12      Nucl.Phys. A454, 429 (1986)

M.Kohno, W.Weise

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
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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
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1984HA28      Nucl.Phys. A420, 399 (1984)

A.Harting, M.Kohno, W.Weise

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
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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
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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
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1983KO11      Nucl.Phys. A397, 1 (1983)

M.Kohno, D.W.L.Sprung

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
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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
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1982KO15      Phys.Rev. C26, 297 (1982)

M.Kohno, D.W.L.Sprung

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
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1982KO22      Can.J.Phys. 60, 1193 (1982)

M.Kohno, D.W.L.Sprung

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
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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
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1982SU08      Prog.Theor.Phys.(Kyoto) 68, 690 (1982)

T.Suzuki, M.Kohno

Collective 1+ Δ- Hole States

NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated collective 1+ states. Isobar-hole excitation.

doi: 10.1143/PTP.68.690
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1981SE06      Prog.Theor.Phys.(Kyoto) 65, 204 (1981)

M.Seya, M.Kohno, S.Nagata

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
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1979KO18      Prog.Theor.Phys. 61, 1065 (1979)

M.Kohno, K.Ando

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
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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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