NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = K.Miyagawa Found 45 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
2018MI04 Phys.Rev. C 97, 055209 (2018) K.Miyagawa, J.Haidenbauer, H.Kamada Faddeev approach to the reaction K- d → πΖn at pK = 1 GeV /c NUCLEAR REACTIONS 2H(K-, nπ-Σ+), (K-, nπ+Σ-), (K-, pπ-Σ0), (K-, nπ0Σ0), E at 1 GeV/c; calculated double differential σ(E, θ) by Faddeev-type approach using TW1, VE-dep, and ORB potentials with and without three-step processes. Comparison with preliminary data from E31 experiment performed at J-PARC facility.
doi: 10.1103/PhysRevC.97.055209
2012MI15 Phys.Rev. C 85, 065201 (2012) Precise calculation of the two-step process for K- d → πΣn in the Λ(1405) resonance region
doi: 10.1103/PhysRevC.85.065201
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
2007GA47 Eur.Phys.J. A 32, 61 (2007) A.Gasparyan, J.Haidenbauer, C.Hanhart, K.Miyagawa Λ N scattering length from the reaction γ d → K+ Λ n
doi: 10.1140/epja/i2007-10359-8
2006MI21 Phys.Rev. C 74, 034002 (2006) K.Miyagawa, T.Mart, C.Bennhold, W.Glockle Polarization observables in exclusive kaon photoproduction on the deuteron NUCLEAR REACTIONS 2H(γ, K+X), E=1.3 GeV; calculated σ(E, θ), polarization observables, hyperon production features.
doi: 10.1103/PhysRevC.74.034002
2006SA39 Phys.Rev. C 74, 044004 (2006) A.Salam, K.Miyagawa, T.Mart, C.Bennhold, W.Glockle K0 photoproduction on the deuteron and the extraction of the elementary amplitude NUCLEAR REACTIONS 2H(γ, K0X), E=1.1 GeV; calculated hyperon production associated σ(E, θ), final state interaction effects.
doi: 10.1103/PhysRevC.74.044004
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
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
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
2003MI35 Mod.Phys.Lett. A 18, 290 (2003) K.Miyagawa, T.Mart, C.Bennhold, W.Glockle Electromagnetic K+ production on light nuclei with beam and hyperon recoil polarizations NUCLEAR REACTIONS 2H(γ, K+X), E=1.3 GeV; 2H(e, e'K+X), E=3.2 GeV; calculated σ(E, θ), hyperon recoil polarization, final state interaction effects.
doi: 10.1142/S0217732303010363
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
2001MI31 Nucl.Phys. A691, 64c (2001) K.Miyagawa, H.Yamamura, T.Mart, C.Bennhold, H.Haberzettl, W.Glockle Electromagnetic K+ Production on the Deuteron with Hyperon Recoil Polarization NUCLEAR REACTIONS 2H(γ, K+), E=1.3 GeV; 2H(e, e'K+), E=3.2 GeV; calculated σ(E), σ(θ), hyperon polarization.
doi: 10.1016/S0375-9474(01)01008-9
2000YA01 Phys.Rev. C61, 014001 (2000) H.Yamamura, K.Miyagawa, T.Mart, C.Bennhold, H.Haberzettl, W.Glockle Inclusive K+ and Exclusive K+Y Photoproduction on the Deuteron: Λ- and Σ-Threshold Phenomena NUCLEAR REACTIONS 2H(γ, K+X), E=high; calculated hyperon production associated σ, σ(θ); deduced final state interaction effects.
doi: 10.1103/PhysRevC.61.014001
2000YA13 Nucl.Phys. A670, 293c (2000) H.Yamamura, K.Miyagawa, W.Glockle Final-State Hyperon-Nucleon Interaction in the Inclusive K+ Photoproduction from the Deuteron NUCLEAR REACTIONS 2H(γ, K+), E=1.3 GeV; calculated σ(E, θ); deduced hyperon-nucleon final state interaction effects.
doi: 10.1016/S0375-9474(00)00116-0
1999GO19 Phys.Rev.Lett. 83, 3142 (1999) J.Golak, H.Kamada, K.Miyagawa, H.Witala, W.Glockle Impossibility to Measure the Total Neutron- and Proton-Induced Nonmesonic Decays for Λ3H NUCLEAR STRUCTURE 3H; calculated hypernucleus single-proton, single-neutron nonmesonic decay rates.
doi: 10.1103/PhysRevLett.83.3142
1999MI19 Phys.Rev. C60, 024003 (1999) S-Matrix Poles Near the ΛN and ΣN Thresholds in the Coupled ΛN-ΣN System
doi: 10.1103/PhysRevC.60.024003
1998GL10 Nucl.Phys. A639, 297c (1998) W.Glockle, K.Miyagawa, H.Kamada, J.Golak, H.Witala The Hypertriton and Its Decays NUCLEAR STRUCTURE 3H; calculated hypernucleus wavefunctions, binding energy, decay rates. Fadeev equations.
doi: 10.1016/S0375-9474(98)00287-5
1998GO06 Nucl.Phys. A631, 740c (1998) J.Golak, K.Miyagawa, H.Kamada, H.Witala, W.Glockle, A.Parreno, A.Ramos, C.Bennhold The Nonmesonic Weak Decay of Hypertriton NUCLEAR STRUCTURE 3H; calculated hypernucleus nonmesonic decay rate.
doi: 10.1016/S0375-9474(98)00102-X
1998KA12 Phys.Rev. C57, 1595 (1998) H.Kamada, J.Golak, K.Miyagawa, H.Witala, W.Glockle π-Mesonic Decay of the Hypertriton NUCLEAR STRUCTURE 3H; calculated hypernucleus mesonic decay rate.
doi: 10.1103/PhysRevC.57.1595
1998TO25 Nucl.Phys. A642, 483 (1998) K.Tominaga, T.Ueda, M.Yamaguchi, N.Kijima, D.Okamoto, K.Miyagawa, T.Yamada A One-Boson-Exchange Potential for ΛN, ΛΛ and ΞN Systems and Hypernuclei
doi: 10.1016/S0375-9474(98)00485-0
1998UE01 Prog.Theor.Phys.(Kyoto) 99, 891 (1998) T.Ueda, K.Tominaga, M.Yamaguchi, N.Kijima, D.Okamoto, K.Miyagawa, T.Yamada ΛN and ΛΛ Interactions in an OBE Model and Hypernuclei NUCLEAR STRUCTURE 6He, 10Be, 13B; calculated ΛΛ-hypernuclei separation energies. OBE model of ΛN, ΛΛ interactions.
doi: 10.1143/PTP.99.891
1997GO04 Phys.Rev. C55, 2196 (1997); Erratum Phys.Rev. C56, 2892 (1997) J.Golak, K.Miyagawa, H.Kamada, H.Witala, W.Glockle, A.Parreno, A.Ramos, C.Bennhold Nonmesonic Weak Decay of the Hypertriton NUCLEAR STRUCTURE A=3; calculated hypertriton nonmesonic weak decay rate. Three-body Faddeev equations.
doi: 10.1103/PhysRevC.55.2196
1997KA77 Physica C282-287, 2063 (1997) K.Kanoda, K.Miyagawa, A.Kawamoto 13C and 1H NMR Study of Vortex Dynamics in a Layered Organic Superconductor at Selective Nuclear Sites NUCLEAR MOMENTS 1H, 13C; measured NMR, relaxation rates; deduced superconductor characteristics.
doi: 10.1016/S0921-4534(97)01131-3
1997MI06 Nucl.Phys. A614, 535 (1997) K.Miyagawa, H.Kamada, W.Glockle Faddeev Equations for the Ξ NN - ΛΛN System
doi: 10.1016/S0375-9474(96)00479-4
1995KA11 Phys.Rev.Lett. 74, 3455 (1995) A.Kawamoto, K.Miyagawa, Y.Nakazawa, K.Kanoda 13C NMR Study of Layered Organic Superconductors Based on BEDT-TTF Molecules NUCLEAR MOMENTS 13C; measured NMR; deduced electronic phases of layered organic superconductors.
doi: 10.1103/PhysRevLett.74.3455
1995KA38 Phys.Rev.Lett. 75, 3587 (1995) A.Kawamoto, K.Miyagawa, Y.Nakazawa, K.Kanoda Kawamoto et al. Reply: NUCLEAR MOMENTS 13C; analyzed, commented on NMR data interpretations. Layered organic superconductors.
doi: 10.1103/PhysRevLett.75.3587
1995MI06 Nucl.Phys. A585, 169c (1995) Hypertriton Calculations with Meson-Theoretical Hyperon-Nucleon Interactions
doi: 10.1016/0375-9474(94)00561-Z
1995MI12 Phys.Rev. C51, 2905 (1995) K.Miyagawa, H.Kamada, W.Glockle, V.Stoks Properties of the Bound (Lambda)(Σ)NN System and Hyperon-Nucleon Interactions NUCLEAR STRUCTURE 3H; A=3; calculated deuteron overlap functions for triton, hypertriton. Faddeev equations, realistic NN-, Nijmegen hypertriton-nucleon interactions.
doi: 10.1103/PhysRevC.51.2905
1994GO47 J.Phys.Soc.Jpn. 63, 3494 (1994) T.Goto, S.Kazama, K.Miyagawa, T.Fukase 63/65Cu/139La-NMR Study on Antiferromagnetic Ordering in High-T(c) Oxides La(2-x)Sr(x)CuO4(x ≈ 0.115) and La(2-x)Ba(x)CuO4(x ≈ 0.125) NUCLEAR MOMENTS 63,65Cu, 139La; measured NMR, high T(c) La(2-x)Sr(x)CuO4, La(2-x)Ba(x)CuO4 oxides; deduced antiferromagnetic ordering evidence.
doi: 10.1143/JPSJ.63.3494
1993MI21 Phys.Rev. C48, 2576 (1993) Hypertriton Calculation with Meson-Theoretical Nucleon-Nucleon and Hyperon-Nucleon Interactions NUCLEAR STRUCTURE A=3; calculated hypertriton binding energy features. Faddeev calculations, (lambda)NN-, ΣNN-coupled systems.
doi: 10.1103/PhysRevC.48.2576
1989MI20 Prog.Theor.Phys.(Kyoto) 82, 329 (1989) Phenomenological Separable N-12C Interaction with Correct Energy-Dependence in Positive and Negative Energy Regions NUCLEAR REACTIONS 12C(n, n), E ≤ 80 MeV; calculated phase shifts vs E. 12C(polarized n, n), E=40 MeV; calculated σ(θ), A(θ); deduced potential. Phenomenological separable model.
doi: 10.1143/PTP.82.329
1987MI06 Nucl.Phys. A463, 411c (1987) K.Miyagawa, T.Ueda, T.Sawada, S.Takagi Multi Three-Cluster Coupling Model of Nuclear Reactions NUCLEAR REACTIONS 4He(d, d), (polarized d, d), E=56 MeV; 2H(α, 3He), E=166 MeV; calculated σ(θ), analyzing power; deduced multi-cluster coupling effects. Cluster coupling model.
doi: 10.1016/0375-9474(87)90683-X
1986MI23 Nucl.Phys. A459, 93 (1986) K.Miyagawa, T.Ueda, T.Sawada, S.Takagi Multi Three-Cluster Coupling Model of Nuclear Reactions NUCLEAR REACTIONS 4He(polarized d, d), E=56 MeV; calculated σ(θ), vector analyzing power; 2H(α, 3He), E=166 MeV; calculated σ(θ). Multi three-cluster coupling model.
doi: 10.1016/0375-9474(86)90058-8
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