NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of May 19, 2024.

Search: Author = M.Kohno

Found 81 matches.

Back to query form



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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2020KO23      Phys.Rev. C 102, 024611 (2020)

M.Kohno

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
Citations: PlumX Metrics


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

M.Kohno

Ξ hyperons in the nuclear medium described by chiral NLO interactions

doi: 10.1103/PhysRevC.100.024313
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2018KO10      Phys.Rev. C 97, 035206 (2018)

M.Kohno

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
Citations: PlumX Metrics


2018KO25      Phys.Rev. C 98, 054617 (2018)

M.Kohno

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2015KO21      Prog.Theor.Exp.Phys. 2015, 123D02 (2015)

M.Kohno

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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

M.Kohno

Λ, Σ, and Ξ hyperons in neutron matter

doi: 10.1016/j.nuclphysa.2013.02.003
Citations: PlumX Metrics


2013KO36      Phys.Rev. C 88, 064005 (2013), Erratum Phys.Rev. C 96, 059903 (2017)

M.Kohno

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2012KO44      Phys.Rev. C 86, 061301 (2012)

M.Kohno

Strength of reduced two-body spin-orbit interaction from a chiral three-nucleon force

doi: 10.1103/PhysRevC.86.061301
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2010KO03      Phys.Rev. C 81, 014003 (2010)

M.Kohno

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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


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
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


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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


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
Citations: PlumX Metrics


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
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


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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


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


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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


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
Citations: PlumX Metrics


1993KO44      Phys.Rev. C48, 3122 (1993)

M.Kohno

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
Citations: PlumX Metrics


1992KO22      Prog.Theor.Phys.(Kyoto) 88, 537 (1992)

M.Kohno

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1988KO13      Phys.Rev. C38, 584 (1988)

M.Kohno

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1983KO08      J.Phys.(London) G9, L85 (1983)

M.Kohno

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1983KO32      Nucl.Phys. A410, 349 (1983)

M.Kohno

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


Back to query form