NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = K.Kubodera Found 75 matches. 2014PA37 Int.J.Mod.Phys. E23, 1430010 (2014) S.Pastore, F.Myhrer, K.Kubodera An update of muon capture on hydrogen NUCLEAR REACTIONS 1,2H(μ-, X), E not given; analyzed available data; deduced parameters for capture rate. Chiral perturbation theory.
doi: 10.1142/S0218301314300100
2013PA40 Phys.Rev. C 88, 058501 (2013) S.Pastore, F.Myhrer, K.Kubodera Muon capture rate on hydrogen and the values of gA and gπNN
doi: 10.1103/PhysRevC.88.058501
2013RA07 Phys.Rev. C 87, 055501 (2013) Ordinary muon capture in hydrogen reexamined
doi: 10.1103/PhysRevC.87.055501
2012RA11 Phys.Rev. C 85, 045502 (2012), Erratum Phys.Rev. C 86, 039903 (2012) Radiative corrections to antineutrino-proton scattering at low energies
doi: 10.1103/PhysRevC.85.045502
2011AD03 Rev.Mod.Phys. 83, 195 (2011) E.G.Adelberger, A.Garcia, R.G.H.Robertson, K.A.Snover, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, D.Bemmerer, A.Junghans, D.Bemmerer, A.Junghans, C.A.Bertulani, K.-W.Chen, H.Costantini, P.Prati, M.Couder, E.Uberseder, M.Wiescher, R.Cyburt, B.Davids, S.J.Freedman, M.Gai, D.Gazit, L.Gialanella, G.Imbriani, U.Greife, M.Hass, W.C.Haxton, T.Itahashi, K.Kubodera, K.Langanke, D.Leitner, M.Leitner, P.Vetter, L.Winslow, L.E.Marcucci, T.Motobayashi, A.Mukhamedzhanov, R.E.Tribble, F.M.Nunes, T.-S.Park, R.Schiavilla, E.C.Simpson, C.Spitaleri, F.Strieder, H.-P.Trautvetter, K.Suemmerer, S.Typel Solar fusion cross sections. II. The pp chain and CNO cycles NUCLEAR REACTIONS 2H(p, γ), 3He(3He, 2p), (α, γ), (p, e), 7Be, 12C, 14N, 15N, 17O(p, γ), 15N, 16,17,18O(p, α), E<3 MeV; analyzed and evaluated experimental data; deduced recommended values and uncertainties.
doi: 10.1103/RevModPhys.83.195
2011AN16 Phys.Rev. C 83, 064002 (2011) S.-I.Ando, Y.-H.Song, C.H.Hyun, K.Kubodera Spin polarization in γd → (n-pol)p at low energies with a pionless effective field theory NUCLEAR REACTIONS 2H(γ, n), E<30 MeV; calculated spin up/down differential cross sections, neutron polarization as function of incident energy and angle, σ(E, θ). Pionless effective field theory with dibaryon fields (dEFT) framework. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.064002
2010NA04 Phys.Rev. C 81, 035502 (2010) S.X.Nakamura, T.Sato, T.-S.H.Lee, B.Szczerbinska, K.Kubodera Dynamical model of coherent pion production in neutrino-nucleus scattering NUCLEAR REACTIONS 12C(π-, X), E=75-275 MeV; calculated total cross section. 12C(π+, π+), E=40, 80 MeV; 12C(π-, π-), E=120, 180, 230, 280 MeV; 12C(γ, π0), E=173 MeV; 12C(γ, π0), E(cm)=200, 290, 350 MeV; calculated σ(θ) of differential cross section. 12C(ν, X), E=0.2-1.5 GeV; calculated σ, pion and muon momentum distributions. Microscopic dynamical model describing neutrino-induced coherent pion production. Comparisons with experimental data.
doi: 10.1103/PhysRevC.81.035502
2009KI06 Phys.Rev. C 80, 015206 (2009) Y.Kim, T.Sato, F.Myhrer, K.Kubodera Two-pion-exchange and other higher-order contributions to the pp → ppπ0 reaction NUCLEAR REACTIONS p(p, p)pπ0, E not given; calculated contributions to the threshold reaction amplitude with the use of the momentum coupling scheme (MCS) in the plane-wave approximation and in the frozen kinematics approximation (FKA). Comparison with the Weinberg scheme.
doi: 10.1103/PhysRevC.80.015206
2007GA32 Phys.Rev. C 76, 014005 (2007) A.Gardestig, K.Kubodera, F.Myhrer Comparison of the heavy-fermion and Foldy-Wouthuysen formalisms at third order
doi: 10.1103/PhysRevC.76.014005
2007KI14 Nucl.Phys. A792, 249 (2007) Y.Kim, K.Kubodera, D.-P.Min, F.Myhrer, M.Rho The effect of kaon condensation on quark-antiquark condensate in dense matter
doi: 10.1016/j.nuclphysa.2007.05.005
2007KI18 Phys.Lett. B 657, 187 (2007) Y.Kim, T.Sato, F.Myhrer, K.Kubodera Two-pion-exchange contributions to the pp → ppπ0 reaction
doi: 10.1016/j.physletb.2007.10.023
2007SZ03 Phys.Lett. B 649, 132 (2007) B.Szczerbinska, T.Sato, K.Kubodera, T.-S.H.Lee Neutrino-nucleus reactions in the delta resonance region NUCLEAR REACTIONS 12C(ν, X), (e, X), E=1, 1.1 GeV; calculated e-, μ energy spectra, σ(θ, Q2). Sato-Lee model.
doi: 10.1016/j.physletb.2007.03.046
2006AN03 Phys.Lett. B 633, 253 (2006) Neutron-neutron fusion NUCLEAR REACTIONS 1n(n, d), E≤thermal; calculated σ and electron energy spectra. Pionless effective field theory.
doi: 10.1016/j.physletb.2005.11.085
2006KI01 Phys.Rev. C 73, 025202 (2006) Y.Kim, I.Danchev, K.Kubodera, F.Myhrer, T.Sato Use of Vlow-k in a chiral-perturbation-theory description of the pp → ppπ0 reaction NUCLEAR REACTIONS 1H(p, p'π0), E=280-320 MeV; calculated σ. Chiral perturbation theory, comparison with data.
doi: 10.1103/PhysRevC.73.025202
2006KU20 Nucl.Phys. B(Proc.Supp.) S159, 21 (2006) K.Kubodera, S.Nakamura, T.Sato Neutrino-nucleus reactions in the energy range 1-100 MeV
doi: 10.1016/j.nuclphysbps.2006.08.023
2006SA36 Nucl.Phys. B(Proc.Supp.) S159, 141 (2006) T.Sato, B.Szczerbinska, K.Kubodera, T.-S.H.Lee Dynamical model of electroweak pion production in the resonance region NUCLEAR REACTIONS 1H(e, e'π+), (e, e'π0), (ν, eπ+), (ν, μ-π+), E ≈ 1-1.4 GeV; calculated σ(Q2).
doi: 10.1016/j.nuclphysbps.2006.08.030
2005AL36 Phys.Rev. C 72, 038201 (2005) W.P.Alvarez, K.Kubodera, F.Myhrer Comparison of the extended linear σ model and chiral perturbation theory
doi: 10.1103/PhysRevC.72.038201
2005GU24 J.Res.Natl.Inst.Stand.Technol. 110, 315 (2005) V.Gudkov, K.Kubodera, F.Myhrer Radiative Corrections for Neutron Decay and Search for New Physics RADIOACTIVITY 1n(β-); calculated radiative corrections.
doi: 10.6028/jres.110.046
2005KO06 Phys.Rev. C 71, 028201 (2005) S.Kondratyuk, K.Kubodera, F.Myhrer Ratio of the proton electromagnetic form factors from meson dressing NUCLEAR STRUCTURE 1H; calculated electromagnetic form factor ratio. Dressed K-matrix model, comparison with data.
doi: 10.1103/PhysRevC.71.028201
2004AN13 Phys.Lett. B 595, 250 (2004) S.Ando, H.W.Fearing, V.Gudkov, K.Kubodera, F.Myhrer, S.Nakamura, T.Sato Neutron beta-decay in effective field theory RADIOACTIVITY 1n(β-); calculated T1/2, angular correlation coefficients, radiative corrections. Effective field theory.
doi: 10.1016/j.physletb.2004.06.037
2004KI20 Prog.Theor.Phys.(Kyoto) 112, 289 (2004) Fixed-Point Analysis of the Low-Energy Constants in the Pion-Nucleon Chiral Lagrangian
doi: 10.1143/PTP.112.289
2004KO25 Nucl.Phys. A736, 339 (2004) S.Kondratyuk, K.Kubodera, F.Myhrer, O.Scholten The Adler-Weisberger and Goldberger-Miyazawa-Oehme sum rules as probes of constraints from analyticity and chiral symmetry in dynamical models for pion-nucleon scattering
doi: 10.1016/j.nuclphysa.2004.03.003
2004KU29 Ann.Rev.Nucl.Part.Sci. 54, 19 (2004) The Solar hep Process
doi: 10.1146/annurev.nucl.54.070103.181239
2004TS09 Phys.Lett. B 602, 60 (2004) K.Tsuji, S.Nakamura, T.Sato, K.Kubodera, F.Myhrer Neutrino magnetic moment contribution to the neutrino-deuteron reaction NUCLEAR REACTIONS 2H(ν, ν'n), E=2.4-20.0 MeV; calculated breakup σ, effect of neutrino magnetic moment.
doi: 10.1016/j.physletb.2004.09.064
2003AN03 Phys.Lett. B 555, 49 (2003) S.Ando, Y.H.Song, T.-S.Park, H.W.Fearing, K.Kubodera Solar-neutrino reactions on deuteron in effective field theory NUCLEAR REACTIONS 2H(ν, ep), (ν-bar, e+n), (ν, ν'p), (ν-bar, ν-bar'p), E=spectrum; calculated σ for solar neutrinos. Effective field theory.
doi: 10.1016/S0370-2693(03)00046-7
2003GU16 J.Phys.(London) G29, 2597 (2003) Solar neutrinos, SNO and neutrino-deuteron reactions
doi: 10.1088/0954-3899/29/11/011
2003KO55 Phys.Rev. C 68, 044001 (2003) S.Kondratyuk, K.Kubodera, F.Myhrer In-medium meson properties and field transformations
doi: 10.1103/PhysRevC.68.044001
2003NA32 Nucl.Phys. A721, 549c (2003) S.Nakamura, T.Sato, S.Ando, T.-S.Park, F.Myhrer, V.Gudkov, K.Kubodera Neutrino-deuteron reactions at solar neutrino energies NUCLEAR REACTIONS 2H(ν, ep), (ν, νn), E=5, 10, 20 MeV; calculated σ. 2H(ν, X), E=0-20 MeV; calculated total charged-current σ.
doi: 10.1016/S0375-9474(03)01121-7
2003PA19 Phys.Rev. C 67, 055206 (2003) T.-S.Park, L.E.Marcucci, R.Schiavilla, M.Viviani, A.Kievsky, S.Rosati, K.Kubodera, D.-P.Min, M.Rho Parameter-free effective field theory calculation for the solar proton-fusion and hep processes NUCLEAR REACTIONS 1H, 3He(p, e+ν), E=low; calculated threshold astrophysical S-factors, dependence on cutoff parameters. Effective field theory.
doi: 10.1103/PhysRevC.67.055206
2002AN08 Phys.Rev. C65, 048501 (2002) S.-I.Ando, F.Myhrer, K.Kubodera Ordinary and Radiative Muon Capture in Liquid Hydrogen Reexamined NUCLEAR REACTIONS 1H(μ, ν), E at rest; analyzed ordinary and radiative capture rates.
doi: 10.1103/PhysRevC.65.048501
2002AN10 Phys.Lett. 533B, 25 (2002) S.Ando, T.-S.Park, K.Kubodera, F.Myhrer The μ-d Capture Rate in Effective Field Theory NUCLEAR REACTIONS 2H(μ-, ν), E at rest; calculated capture rate vs final-state energy. Heavy baryon chiral perturbation theory.
doi: 10.1016/S0370-2693(02)01619-2
2002NA19 Nucl.Phys. A707, 561 (2002) S.Nakamura, T.Sato, S.Ando, T.-S.Park, F.Myhrer, V.Gudkov, K.Kubodera Neutrino-Deuteron Reactions at Solar Neutrino Energies NUCLEAR REACTIONS 2H(ν, ep), (ν, νp), E=1.5-20.0 MeV; calculated σ. Effective field theory.
doi: 10.1016/S0375-9474(02)00993-4
2001AN01 Phys.Rev. C63, 015203 (2001) S.-I.Ando, F.Myhrer, K.Kubodera Capture Rate and Neutron Helicity Asymmetry for Ordinary Muon Capture on Hydrogen NUCLEAR REACTIONS 1H(μ-, ν), E at rest; calculated muon capture rate, neutron helicity asymmetry. Heavy-baryon chiral perturbation theory. ATOMIC PHYSICS, Mesic-atoms 1H(μ-, ν), E at rest; calculated muon capture rate, neutron helicity asymmetry. Heavy-baryon chiral perturbation theory.
doi: 10.1103/PhysRevC.63.015203
2001NA08 Phys.Rev. C63, 034617 (2001); Erratum Phys.Rev. C 73, 049904 (2006) S.Nakamura, T.Sato, V.Gudkov, K.Kubodera Neutrino Reactions on the Deuteron NUCLEAR REACTIONS 2H(ν, νp), (ν, ep), (ν, e+n), E=2-170 MeV; calculated σ, σ(E), σ(θ). Phenomenological Lagrangian approach.
doi: 10.1103/PhysRevC.63.034617
2001PA17 Nucl.Phys. A684, 101c (2001) T.-S.Park, K.Kubodera, D.-P.Min, M.Rho Effective Field Theory for Nuclei: Confronting fundamental questions in astrophysics
doi: 10.1016/S0375-9474(01)00494-8
2000DM02 Nucl.Phys. A663-664, 465c (2000) V.Dmitrasinovic, K.Kubodera, F.Myhrer, T.Sato A Next-to-Next-to-Leading-Order pp → ppπ0 Transition Operator in Chiral Perturbation Theory NUCLEAR REACTIONS 1H(p, pπ0), E not given; calculated next-to-leading-order S-wave amplitude.
doi: 10.1016/S0375-9474(99)00632-6
2000KU17 Nucl.Phys. A670, 103c (2000) Chiral Symmetry in Nuclei
doi: 10.1016/S0375-9474(00)00079-8
2000PA03 Phys.Lett. 472B, 232 (2000) T.-S.Park, K.Kubodera, D.-P.Min, M.Rho Effective Field Theory Approach to n(pol) + p(pol) → d + γ at Threshold NUCLEAR REACTIONS 1H(polarized n, γ), E not given; calculated polarization observables. Effective field theory, polarized target.
doi: 10.1016/S0370-2693(99)01438-0
1999DM03 Phys.Lett. 465B, 43 (1999) V.Dmitrasinovic, K.Kubodera, F.Myhrer, T.Sato A Next-to-Next-to-Leading-Order pp → ppπ0 Transition Operator in Chiral Perturbation Theory NUCLEAR REACTIONS 1H(p, pπ0), E ≈ threshold; calculated transition operators, corrections. Chiral perturbation theory.
doi: 10.1016/S0370-2693(99)01075-8
1999PA05 Nucl.Phys. A646, 83 (1999) T.-S.Park, K.Kubodera, D.-P.Min, M.Rho The Power of Effective Field Theories in Nuclei: The deuteron, NN scattering and electroweak processes NUCLEAR REACTIONS 1H(p, e+), (n, γ), E=low; calculated phase shifts, matrix elements; deduced pion role, cut-off parameter. Effective field theory.
doi: 10.1016/S0375-9474(98)00614-9
1998AD12 Rev.Mod.Phys. 70, 1265 (1998) E.G.Adelberger, S.M.Austin, J.B.Bahcall, A.B.Balantekin, G.Bogaert, L.S.Brown, L.Buchmann, F.E.Cecil, A.E.Champagne, L.de Braeckeleer, C.A.Duba, S.R.Elliott, S.J.Freedom, M.Gai, G.Goldring, C.R.Gould, A.Gruzinov, W.C.Haxton, K.M.Heeger, E.Henley, C.W.Johnson, M.Kamionkowski, R.W.Kavanagh, S.E.Koonin, K.Kubodera, K.Langanke, T.Motobayashi, V.Pandharipande, P.Parker, R.G.H.Robertson, C.Rolfs, R.F.Sawyer, N.Shaviv, T.D.Shoppa, K.A.Snover, E.Swanson, R.E.Tribble, S.Turck-Chieze, J.F.Wilkerson Solar Fusion Cross Sections NUCLEAR REACTIONS 7Be, 12,13C, 15N, 16,17,18O(p, γ), 14,15N, 17,18O(p, α), 7Li(d, p), 3He(p, e+), (α, γ), (3He, 2p), 1H(p, e+), E=low; compiled, analyzed S-factor data, calculations; deduced implications for solar neutrino flux calculations.
doi: 10.1103/RevModPhys.70.1265
1998ME02 Phys.Lett. 416B, 36 (1998) T.Meissner, F.Myhrer, K.Kubodera Radiative Muon Capture by a Proton in Chiral Perturbation Theory NUCLEAR REACTIONS 1H(μ-, nγ), E not given; analyzed radiative muon capture rate; deduced pseudoscalar coupling related features. Chiral perturbation theory.
doi: 10.1016/S0370-2693(97)01330-0
1998PA21 Phys.Rev. C58, R637 (1998) T.-S.Park, K.Kubodera, D.-P.Min, M.Rho Effective Field Theory for Low-Energy Two-Nucleon Systems NUCLEAR REACTIONS 1H(n, γ), E(cm) < 220 MeV; calculated phase shift, M1 transition amplitude; deduced little cutoff dependence. Effective field theory.
doi: 10.1103/PhysRevC.58.R637
1997SA42 Phys.Rev. C56, 1246 (1997) T.Sato, T.-S.H.Lee, F.Myhrer, K.Kubodera Chiral Perturbation Theory and the pp → ppπ0 Reaction Near Threshold NUCLEAR REACTIONS 1H(p, p'X), E=280-320 MeV; analyzed pion production σ(E); deduced rescattering term contribution enhancement. Chiral perturbation theory, momentum-space representation.
doi: 10.1103/PhysRevC.56.1246
1996PA10 Phys.Rev. C53, 1519 (1996) B.-Y.Park, F.Myhrer, J.R.Morones, T.Meissner, K.Kubodera Chiral Perturbation Approach to the pp → ppπ0 Reaction Near Threshold NUCLEAR REACTIONS 1H(p, pπ0), E ≈ threshold; calculated σ. Chiral perturbation approach.
doi: 10.1103/PhysRevC.53.1519
1994KU24 Nucl.Phys. A577, 393c (1994) Heavy-Baryon Chiral Perturbation Theory Applied to Axial-Charge Exchange Currents NUCLEAR STRUCTURE A=16-208; calculated loop correction related parameters. Two-body exchange current, heavy-baryon chiral perturbation theory.
doi: 10.1016/0375-9474(94)90886-9
1994KU48 Int.J.Mod.Phys. E3, 101 (1994) Neutrino-Nucleus Reactions NUCLEAR REACTIONS 2H(ν, X), E=2-170 MeV; compiled, reviewed reaction σ, other aspects, other ν-induced reactions data analyses.
doi: 10.1142/S0218301394000048
1994PA31 Nucl.Phys. A579, 381 (1994) T.-S.Park, I.S.Towner, K.Kubodera Nuclear Matrix Elements of Axial-Charge Exchange Currents Derived in Heavy-Fermion Chiral Perturbation Theory NUCLEAR STRUCTURE A=16-208; calculated impulse approximation, meson exchange contributions to current ratio. Heavy-fermion chiral perturbation theory, shell model.
doi: 10.1016/0375-9474(94)90914-8
1993KU29 Hyperfine Interactions 78, 3 (1993) Non-Nucleonic Degrees of Freedom in Weak Nuclear Currents
doi: 10.1007/BF00568113
1993TA14 Nucl.Phys. A556, 601 (1993) S.Takeuchi, F.Myhrer, K.Kubodera Maximum Asymmetry Phenomena in (p-bar)p → π-π+ and (p-bar)p → K-K+ Reactions NUCLEAR REACTIONS 1H(p-bar, p-bar), E at 988, 1550 MeV/c; calculated σ(θ), polarization. 1H(p-bar, X), E at 988, 1550 MeV/c; calculated σ(θ), asymmetry vs θ for (K-K+), (π-π+) production; deduced helicity-flip, helicity-nonflip amplitudes role.
doi: 10.1016/0375-9474(93)90472-A
1992DO03 Phys.Rev. C45, 1988 (1992) Astrophysical Neutrino Reactions on the Deuteron NUCLEAR REACTIONS 2H(ν, X), (ν-bar, X), E=4-150 MeV; calculated charge, axial current, total σ.
doi: 10.1103/PhysRevC.45.1988
1991KU18 Phys.Rev.Lett. 67, 3479 (1991) Axial-Charge Transitions in Heavy Nuclei and In-Medium Effective Chiral Lagrangians NUCLEAR STRUCTURE A=205-212; analyzed first forbidden β-decay related axial-charge matrix enhancement; deduced hadron scaling evidence. Effective Lagrangian, chiral, scale QCD invariances.
doi: 10.1103/PhysRevLett.67.3479
1990FU03 Phys.Rev. C41, 1359 (1990) M.Fukugita, Y.Kohyama, K.Kubodera, T.Kuramoto Reaction Cross Sections for ν13C → e-13N and ν13C → ν'13C(*) for Low Energy Neutrinos NUCLEAR REACTIONS 13C(ν, e-), E < 20 MeV; calculated σ, σ(E, θ); deduced counting rates for the solar 8B neutrinos.
doi: 10.1103/PhysRevC.41.1359
1990KU07 Nucl.Phys. A512, 711 (1990) T.Kuramoto, M.Fukugita, Y.Kohyama, K.Kubodera Neutrino-Induced Reaction Cross Sections at Intermediate Energies for Chlorine and Water Detectors NUCLEAR REACTIONS 37Cl(ν, X), E ≤ 300 MeV; 16O(ν, X), (ν-bar, X), E ≤ 300 MeV; calculated σ(E) for X=e, μ.
doi: 10.1016/0375-9474(90)90232-B
1990TA22 Phys.Rev. C42, 1694 (1990) N.Tatara, Y.Kohyama, K.Kubodera Weak Interaction Processes on Deuterium: Muon capture and neutrino reactions NUCLEAR REACTIONS 2H(μ-, 2n), E at rest; calculated muon capture rate; deduced σ for (ν+d) reaction. ATOMIC PHYSICS, Mesic-Atoms 2H(μ-, 2n), E at rest; calculated muon capture rate; deduced σ for (ν+d) reaction.
doi: 10.1103/PhysRevC.42.1694
1989FU02 Astrophys.J. 337, L59 (1989) M.Fukugita, Y.Kohyama, K.Kubodera, T.Kuramoto Reaction Cross Section for ' Solar Flare Neutrinos ' with 37Cl and 16O Targets NUCLEAR REACTIONS 37Cl(ν, e-), 16O(ν, e-X), E=50-200 MeV; calculated σ(E).
doi: 10.1086/185378
1989YA12 Nucl.Phys. A500, 429 (1989) T.Yamaguchi, K.Tsushima, Y.Kohyama, K.Kubodera Semi-Leptonic Beta-Decay Form Factors and Magnetic Moments of Octet Baryons: Recoil effects and center-of-mass corrections in the cloudy bag model including gluonic effects RADIOACTIVITY 1n; calculated semi-leptonic β-decay form factors. Cloudy bag model. NUCLEAR STRUCTURE 1n, 1H; calculated μ. Cloudy bag model.
doi: 10.1016/0375-9474(89)90222-4
1988FU08 Phys.Lett. 212B, 139 (1988) M.Fukugita, Y.Kohyama, K.Kubodera Neutrino Reaction Cross Sections on 12C Target NUCLEAR REACTIONS 12C(ν, ν'), (ν-bar, ν-bar'), E=30-100 MeV; calculated reaction σ(E).
doi: 10.1016/0370-2693(88)90513-8
1988TS05 Nucl.Phys. A489, 557 (1988) K.Tsushima, T.Yamaguchi, Y.Kohyama, K.Kubodera Weak Interaction Form Factors and Magnetic Moments of Octet Baryons: Chiral bag model with gluonic effects NUCLEAR STRUCTURE 1n, 1H; calculated μ, weak interaction form factors.
doi: 10.1016/0375-9474(88)90111-X
1987KO10 Phys.Lett. 186B, 255 (1987) Y.Kohyama, K.Oikawa, K.Tsushima, K.Kubodera Weak-Current Form Factors of Octet Baryons in the Volume-Type Cloudy Bag Model RADIOACTIVITY 1n(β-); calculated vector, axial current form factors. MIT, cloudy bag, SU(3) model.
doi: 10.1016/0370-2693(87)90290-5
1986NO04 Nucl.Phys. A453, 645 (1986) S.Nozawa, K.Kubodera, H.Ohtsubo Exchange Currents and Cofiguration-Mixing Effects in the 16O(0+) - 16N(0-) Transitions NUCLEAR STRUCTURE 16N, 16O; calculated β-decay, μ capture rates; deduced exchange currents, configuration mixing effects roles.
doi: 10.1016/0375-9474(86)90256-3
1986NO11 J.Phys.Soc.Jpn. 55, 2636 (1986) S.Nozawa, Y.Kohyama, T.Kaneta, K.Kubodera Exchange Currents in the Neutrino-Deuteron Reactions and the Solar Neutrino Problem NUCLEAR REACTIONS 2H(ν, e-p), (ν-bar, e+n), E < 15 MeV; calculated average σ; deduced possible exchange current effects. Impulse approximation.
doi: 10.1143/JPSJ.55.2636
1985NO10 Prog.Theor.Phys.(Kyoto) 74, 926 (1985) S.Nozawa, K.Kubodera, H.Ohtsubo, H.Nishimura Further Study of the 16O(0+) - 16N(0-) Transitions NUCLEAR STRUCTURE 16N, 16O; calculated μ-capture to β-decay rate vs range parameter; deduced nonsoft pion exchange role.
doi: 10.1143/PTP.74.926
1984FU14 Phys.Lett. 149B, 451 (1984) Energetic Neutrons from Muon Capture by a Heavy Nucleus NUCLEAR REACTIONS 165Ho(μ-, n), E at rest; analyzed σ(En). Energetic neutrons, nuclear Fermi motion.
doi: 10.1016/0370-2693(84)90364-2
1984NO03 Phys.Lett. 140B, 11 (1984) S.Nozawa, Y.Kohyama, K.Kubodera The 0+ - 0- Transitions in the A = 16 System and Meson-Exchange Currents NUCLEAR STRUCTURE A=16; calculated β-, muon capture transition rates connecting 0+, 0- states. Meson exchange effects, inclusion of highly excited configurations, first-order perturbation.
doi: 10.1016/0370-2693(84)91037-2
1983KI06 Phys.Rev. D27, 2765 (1983) Double-Positron Decay, Positron-Emitting K Capture, and Double K Capture RADIOACTIVITY 136Ce, 130Ba, 124Xe, 106Cd, 96Ru, 58Ni(β+β+); calculated T1/2 for two-neutrino, neutrinoless double β+-decay, K-capture, double K-capture processes; deduced two-neutrino, double K-capture channel dominance.
doi: 10.1103/PhysRevD.27.2765
1983NO12 Prog.Theor.Phys.(Kyoto) 70, 892 (1983) S.Nozawa, Y.Kohyama, K.Kubodera Weak Processes in the A = 12 Nuclei with Finite Momentum Transfer RADIOACTIVITY 12N(β-); analyzed form factors associated with ft value, asymmetry coefficient, shape factor data analysis; deduced scaling deviations parametrization, neutrino reaction relevance to test CVC. NUCLEAR REACTIONS 12C(μ-, ν), E at rest; 12C(e, e'), E not given; analyzed axial, weak magnetism form factor scaling in data analysis; deduced elementary particle treatment limitations. Impulse approximation.
doi: 10.1143/PTP.70.892
1982NO05 Prog.Theor.Phys.(Kyoto) 67, 1240 (1982) S.Nozawa, Y.Kohyama, K.Kubodera Exchange Currents for the Time Component of Axial Currents - A = 2 Nucclear System as a Test Case - NUCLEAR STRUCTURE A=2; calculated axial current time component exchange contributions; deduced tensor interaction role. One soft pion exchange model.
doi: 10.1143/PTP.67.1240
1980OK01 Phys.Lett. 90B, 45 (1980) Determination of Upper Limits to Second-Class Currents RADIOACTIVITY A=8-20; analyzed β-decay data; deduced second-class current upper limits.
doi: 10.1016/0370-2693(80)90047-7
1978TO09 Phys.Lett. 76B, 259 (1978) Energy Dependent ft-Value and B(M1) in 8Be NUCLEAR STRUCTURE 8Be; calculated β, γ decay to 2+ level.
doi: 10.1016/0370-2693(78)90781-5
1977KU20 Progr.Theor.Phys. 57, 1599 (1977) Feeding of 8Be via β- and γ-Transitions NUCLEAR STRUCTURE 8Be; analyzed feeding of first 2+ level by β, γ.
doi: 10.1143/PTP.57.1599
1976NI05 Progr.Theor.Phys. 56, 986 (1976) Pion-Nucleus Charge-Exchange Reaction NUCLEAR REACTIONS 13C(π+, π0), E=40-240 MeV; calculated total σ(E).
doi: 10.1143/PTP.56.986
1975KU03 Phys.Lett. 55B, 380 (1975) Negative-Pion Capture by 4He NUCLEAR REACTIONS 4He(π-, X); analyzed data; deduced reaction mechanism.
doi: 10.1016/0370-2693(75)90364-0
1975KU20 Phys.Lett. 58B, 402 (1975) K.Kubodera, H.Ohtsubo, Y.Horikawa Energy-Dependent Anisotropy of Beta-Rays and Second-Class Currents RADIOACTIVITY 12B, 12N; analyzed data on energy dependence of β-asymmetry; polarized nuclei.
doi: 10.1016/0370-2693(75)90571-7
1970SU13 Progr.Theoret.Phys. 44, 617 (1970) The Hartree-Fock Model of the Li6 Nucleus NUCLEAR STRUCTURE 6Li; calculated binding energy, rms radius, B(E2), charge form factor. Projected Hartree-Fock model.
doi: 10.1143/PTP.44.617
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