NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = K.Nakayama Found 83 matches. 2019NA18 Phys.Rev. C 100, 035208 (2019) Explicit derivation of the completeness condition in pseudoscalar meson photoproduction
doi: 10.1103/PhysRevC.100.035208
2017WA34 Phys.Rev. C 96, 035206 (2017) A.C.Wang, W.L.Wang, F.Huang, H.Haberzettl, K.Nakayama Nucleon resonances in γp → K*+Λ NUCLEAR REACTIONS 1H(γ, K*+Λ), E=1850-3850 MeV; analyzed high-precision differential σ(θ, E) data from the CLAS Collaboration at Jefferson National Accelerator facility using effective Lagrangian approach in the tree-level approximation; deduced model parameters in five different fits, total σ(E), and photon beam asymmetry.
doi: 10.1103/PhysRevC.96.035206
2015JA03 Phys.Rev. C 91, 065208 (2015) B.C.Jackson, Y.Oh, H.Haberzettl, K.Nakayama K-bar + N → K + Ξ reaction and S = -1 hyperon resonances
doi: 10.1103/PhysRevC.91.065208
2015RO14 Eur.Phys.J. A 51, 70 (2015) D.Ronchen, M.Doring, H.Haberzettl, J.Haidenbauer, U.-G.Meissner, K.Nakayama Eta photoproduction in a combined analysis of pion- and photon-induced reactions
doi: 10.1140/epja/i2015-15070-7
2014JA04 Phys.Rev. C 89, 025206 (2014) B.C.Jackson, Y.Oh, H.Haberzettl, K.Nakayama Model-independent aspects of the reaction K(bar) + N → K + Κ
doi: 10.1103/PhysRevC.89.025206
2014RO13 Eur.Phys.J. A 50, 101 (2014), Erratum Eur.Phys.J. A 51, 63 (2015) D.Ronchen, M.Doring, F.Huang, H.Haberzettl, J.Haidenbauer, C.Hanhart, S.Krewald, U.-G.Meissner, K.Nakayama Photocouplings at the pole from pion photoproduction NUCLEAR REACTIONS 1H(γ, π0), (γ, π+), E≈1.08-2.35 GeV; calculated, analyzed σ, σ(θ), beam asymmetry, target asymmetry using semi-phenomenological approach with dynamical CC model; deduced photocoupling resonance parameters from the fit to the data.
doi: 10.1140/epja/i2014-14101-3
2013HU02 Phys.Rev. C 87, 054004 (2013) F.Huang, H.Haberzettl, K.Nakayama Combined analysis of η' production reactions: γN → η'N, NN → NNη', and πN → η'N
doi: 10.1103/PhysRevC.87.054004
2013RO13 Eur.Phys.J. A 49, 44 (2013) D.Ronchen, M.Doring, F.Huang, H.Haberzettl, J.Haidenbauer, C.Hanhart, S.Krewald, U.-G.Meissner, K.Nakayama Coupled-channel dynamics in the reactions πN → πN, ηN, KΛ, KΣ
doi: 10.1140/epja/i2013-13044-5
2012HA20 Phys.Rev. C 85, 064001 (2012) Gauge-invariant formulation of NN → NNγ
doi: 10.1103/PhysRevC.85.064001
2012HU02 Phys.Rev. C 85, 054003 (2012) F.Huang, M.Doring, H.Haberzettl, J.Haidenbauer, C.Hanhart, S.Krewald, U.-G.Meissner, K.Nakayama Pion photoproduction in a dynamical coupled-channels model
doi: 10.1103/PhysRevC.85.054003
2012NA08 Phys.Rev. C 85, 042201 (2012) K.Nakayama, Y.Oh, H.Haberzettl Model-independent determination of the parity of Ξ hyperons
doi: 10.1103/PhysRevC.85.042201
2011HA27 Phys.Rev. C 83, 065502 (2011) H.Haberzettl, F.Huang, K.Nakayama Dressing the electromagnetic nucleon current
doi: 10.1103/PhysRevC.83.065502
2011JO03 Phys.Rev. C 83, 054001 (2011) A.Johansson, H.Haberzettl, K.Nakayama, C.Wilkin Measurement and analysis of the pp → ppγ reaction at 310 MeV NUCLEAR REACTIONS 1H(p, 2pγ), E=310 MeV; measured proton spectra, angular distribution of protons and bremsstrahlung photons, two-proton momenta, total σ, σ(Eγ, θ), proton-proton timing correlations, forward-backward symmetry. Comparison with Habersettl-Nakayama theoretical model. Promice-Wasa facility.
doi: 10.1103/PhysRevC.83.054001
2011KA14 Phys.Rev. C 83, 055201 (2011) J.Ka Shing Man, Y.Oh, K.Nakayama Role of high-spin hyperon resonances in the reaction of γp → K+K+Ξ-
doi: 10.1103/PhysRevC.83.055201
2010DO11 Eur.Phys.J. A 43, 83 (2010) The phase and pole structure of the N*(1535) in πN → πN and γN → πN
doi: 10.1140/epja/i2009-10892-4
2010NA24 Phys.Rev. C 82, 065201 (2010) Model-independent analysis of p+p → pp(1S0)+γ
doi: 10.1103/PhysRevC.82.065201
2009NA37 Phys.Rev. C 80, 051001 (2009) Interaction current in pp → ppγ NUCLEAR REACTIONS p(p, pγ), E=190 MeV; analyzed σ(θ) and analyzing powers using gauge-invariant relativistic meson exchange model approach. Nucleon-nucleon bremsstrahlung reaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.051001
2008OH04 Phys.Rev. C 77, 045204 (2008) Nucleon and Δ resonances in KΣ(1385) photoproduction from nucleons NUCLEAR REACTIONS p(γ, K+), E=1.6-3.8 GeV; analyzed resonances, cross sections, σ(θ), photon asymmetry for Σ0(1385).
doi: 10.1103/PhysRevC.77.045204
2007OH05 Nucl.Phys. A790, 498c (2007) Y.Oh, H.Haberzettl, K.Nakayama Photoproduction of Cascade Baryon NUCLEAR REACTIONS 1H(γ, 2K+X), E≈2-5 GeV; calculated total σ for Ξ-production. Relativistic meson exchange model. Comparison with data.
doi: 10.1016/j.nuclphysa.2007.03.133
2006HA43 Phys.Rev. C 74, 045202 (2006) H.Haberzettl, K.Nakayama, S.Krewald Gauge-invariant approach to meson photoproduction including the final-state interaction NUCLEAR REACTIONS 1H(γ, π0), E=140-400 MeV; calculated σ. 1H(γ, π0), (γ, π+), 1n(γ, π-), E=180, 220, 340, 390 MeV; calculated σ(θ). Gauge-invariant approach, comparison with data.
doi: 10.1103/PhysRevC.74.045202
2006NA11 Phys.Rev. C 73, 045211 (2006) Analyzing η' photoproduction data on the proton at energies of 1.5-2.3 GeV NUCLEAR REACTIONS 1H(γ, pX), E=1.5-2.3 GeV; analyzed η' meson production σ, σ(θ); deduced resonance and mesonic current contributions.
doi: 10.1103/PhysRevC.73.045211
2006NA23 Acta Phys.Slovaca 56, 237 (2006) Photo- and Hadro-production of η' meson NUCLEAR REACTIONS 1H(γ, X), (p, X), E=high; analyzed η'-meson production σ(θ), σ. Relativistic meson exchange model.
2006NA29 Phys.Rev. C 74, 035205 (2006) K.Nakayama, Y.Oh, H.Haberzettl Photoproduction of Ξ off nucleons NUCLEAR REACTIONS 1n, 1H(γ, 2K+X), (γ, 2K0X), (γ, K+K0X), E ≈ 2-5 GeV; calculated Ξ production σ, σ(θ).
doi: 10.1103/PhysRevC.74.035205
2006OH01 Phys.Rep. 423, 49 (2006) Pentaquark Θ+ (1540) production in γN → K(K-bar)N reactions NUCLEAR REACTIONS 1n, 1H(γ, K+K-), E=1-4.5 GeV; calculated σ, invariant mass spectra, pentaquark production features.
doi: 10.1016/j.physrep.2005.10.002
2005NA33 Phys.Rev. C 72, 034603 (2005) Spin structure of spin-1/2 baryon and spinless meson production amplitudes in photonic and hadronic reactions
doi: 10.1103/PhysRevC.72.034603
2005TI03 Phys.Rev. C 71, 035203 (2005) A.I.Titov, H.Ejiri, H.Haberzettl, K.Nakayama Some aspects of Θ+ parity determination in the reaction γN → Θ+ (K-bar) → NK(K-bar) NUCLEAR REACTIONS 1n, 1H(γ, K+K-), E ≈ threshold; calculated pentaquark production associated invariant mass spectra, spin observables. Implications for parity determination discussed.
doi: 10.1103/PhysRevC.71.035203
2004MO08 Phys.Rev. C 69, 025203 (2004) P.Moskal, H.-H.Adam, A.Budzanowski, R.Czyzykiewicz, D.Grzonka, M.Janusz, L.Jarczyk, B.Kamys, A.Khoukaz, K.Kilian, P.Kowina, K.Nakayama, W.Oelert, C.Piskor-Ignatowicz, J.Przerwa, T.Rozek, R.Santo, G.Schepers, T.Sefzick, M.Siemaszko, J.Smyrski, S.Steltenkamp, A.Taschner, P.Winter, M.Wolke, P.Wustner, W.Zipper Experimental study of pp η dynamics in the pp → pp η reaction NUCLEAR REACTIONS 1H(p, pX), E at 2.027 GeV/c; measured η-meson production associated invariant mass spectra, σ(θ), σ; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.69.025203
2004NA19 Phys.Rev. C 69, 065212 (2004) Consistent analysis of the reactions γp → pη' and pp → ppη' NUCLEAR REACTIONS 1H(γ, pX), E=1.49-2.44 GeV; 1H(p, p'X), E ≈ threshold; analyzed η' meson production σ(θ); deduced resonance energies, related features. Relativistic meson exchange model.
doi: 10.1103/PhysRevC.69.065212
2004NA23 Phys.Rev. C 70, 012201 (2004) Spin observables and the determination of the parity of Θ+ in photoproduction reaction NUCLEAR REACTIONS 1H(γ, X), E not given; calculated pentaquark production associated polarization observables.
doi: 10.1103/PhysRevC.70.012201
2004VO07 Phys.Rev.Lett. 92, 202301 (2004) M.Volkerts, J.C.S.Bacelar, M.J.van Goethem, M.N.Harakeh, M.Hoefman, H.Huisman, N.Kalantar-Nayestanaki, S.Kopecky, H.Lohner, J.G.Messchendorp, K.Nakayama, R.W.Ostendorf, S.Schadmand, O.Scholten, H.W.Wilschut Exclusive Measurement of Quasifree Proton-Neutron Bremsstrahlung NUCLEAR REACTIONS 2H(p, np), E=190 MeV; measured En, Ep, bremsstrahlung Eγ, σ(E, θ); deduced proton-neutron bremsstrahlung features.
doi: 10.1103/PhysRevLett.92.202301
2003NA28 Phys.Rev. C 68, 045201 (2003) K.Nakayama, J.Haidenbauer, C.Hanhart, J.Speth Analysis of the reaction pp → ppη near threshold NUCLEAR REACTIONS 1H(p, p'X), E ≈ threshold; analyzed η meson production associated invariant mass spectra, σ, σ(θ), Ay(θ); deduced partial wave amplitudes, resonance features.
doi: 10.1103/PhysRevC.68.045201
2003TS05 Phys.Rev. C 68, 034612 (2003) Near-threshold ω and φ meson productions in pp collisions NUCLEAR REACTIONS 1H(p, p'X), E ≈ threshold; calculated ω and φ meson production σ, σ(θ), resonance effects. Relativistic effective Lagrangian.
doi: 10.1103/PhysRevC.68.034612
2003TS07 Nucl.Phys. A721, 633c (2003) Near-threshold ω-meson production in proton-proton collisions: With or without resonance excitations? NUCLEAR REACTIONS 1H(p, pX), (π-, X), E ≈ threshold; calculated ω meson production σ, σ(θ); deduced resonance contributions.
doi: 10.1016/S0375-9474(03)01140-0
2002NA11 Phys.Rev. C65, 045210 (2002) K.Nakayama, J.Speth, T.-S.H.Lee η Meson Production in NN Collisions NUCLEAR REACTIONS 1H(p, X), (n, X), E ≈ threshold; calculated η meson production σ, σ(θ), Ay(θ). Relativistic meson exchange model, comparison with data.
doi: 10.1103/PhysRevC.65.045210
2001NA03 Phys.Rev. C63, 015201 (2001) K.Nakayama, J.Haidenbauer, J.Speth The Reactions pn → dω and pn → dφ Near Threshold NUCLEAR REACTIONS 1H(n, dX), E ≈ threshold; calculated ω, φ meson production σ, σ(θ). Relativistic meson-exchange model.
doi: 10.1103/PhysRevC.63.015201
2001NA25 Nucl.Phys. A689, 402c (2001) K.Nakayama, J.Haidenbauer, J.Speth The Reactions pn → dω and pn → d0 and the Role of the OZI Rule NUCLEAR REACTIONS 1H(n, X), E ≈ threshold; calculated φ, ω meson production σ. Relativistic meson-exchange model.
doi: 10.1016/S0375-9474(01)00865-X
2000NA02 Phys.Rev. C61, 024001 (2000) K.Nakayama, H.F.Arellano, J.W.Durso, J.Speth η' Meson Production in Proton-Proton Collisions NUCLEAR REACTIONS 1H(p, pX), E ≈ threshold; calculated pion, η-, η'-meson production σ; deduced contributions. Relativistic meson exchange model. Comparisons with data.
doi: 10.1103/PhysRevC.61.024001
1999HA23 Phys.Lett. 454B, 176 (1999) On the Treatment of NN Interaction Effects in Meson Production in NN Collisions
doi: 10.1016/S0370-2693(99)00377-9
1999NA38 Phys.Rev. C60, 055209 (1999) K.Nakayama, J.W.Durso, J.Haidenbauer, C.Hanhart, J.Speth φ-Meson Production in Proton-Proton Collisions NUCLEAR REACTIONS 1H(p, pX), E=2.85 MeV; calculated φ-meson production associated σ(θ); deduced reaction mechanism features. Relativistic meson-exchange model. Comparisons with data.
doi: 10.1103/PhysRevC.60.055209
1998NA11 Phys.Rev. C57, 1580 (1998) K.Nakayama, A.Szczurek, C.Hanhart, J.Haidenbauer, J.Speth Production of ω Mesons in Proton-Proton Collisions NUCLEAR REACTIONS 1H(p, p'X), E=1890-2200 MeV; calculated ω-meson σ(θ), production σ; deduced off-shell effects. Comparison with data. Meson exchange model.
doi: 10.1103/PhysRevC.57.1580
1998NA31 Acta Phys.Pol. B29, 2519 (1998) K.Nakayama, S.Krewald, J.Speth Possible Role of the ρN Coupling in Pion Photo-Production
1996DE46 Phys.Lett. 385B, 33 (1996) The Influence of Negative-Energy States on Proton-Proton Bremsstrahlung NUCLEAR REACTIONS 1H(p, γ), E not given; analyzed bremsstrahlung associated σ(θ1, θ2, θ), analyzing power; deduced need to include all diagrams to investigate negative energy states. Spectator model based T-matrix.
doi: 10.1016/0370-2693(96)00863-5
1995DE17 Phys.Rev. C51, 2334 (1995) F.de Jong, K.Nakayama, T.-S.H.Lee Proton-Proton Bremsstrahlung Below and Above Pion Threshold: Influence of the Δ isobar NUCLEAR REACTIONS 1H(p, γ), (polarized p, γ), E=280-800 MeV; analyzed σ(θ1, θ2, θ), analyzing power vs (θ1, θ2, θ) data; deduced Δ excitation role. Coupled-channels model.
doi: 10.1103/PhysRevC.51.2334
1995DE41 Phys.Rev. C52, 2377 (1995) Effects of Meson-Decay Diagrams in Proton-Proton Bremsstrahlung NUCLEAR REACTIONS 1H(p, γX), E=280, 550 MeV; calculated bremsstrahlung σ(θ1, θ2, θ), analyzing power θ1, θ2, θ; deduced meson-decay diagrams role.
doi: 10.1103/PhysRevC.52.2377
1995HE03 Nucl.Phys. A582, 568 (1995) V.Herrmann, K.Nakayama, O.Scholten, H.Arellano Proton-Proton Bremsstrahlung and the Off-Shell Behavior of the NN Interaction NUCLEAR REACTIONS 1H(polarized p, γ), E=280 MeV; calculated bremsstrahlung σ(θ), polarization observables, σ(θ1, θ2); deduced NN-interaction off-shell behavior features.
doi: 10.1016/0375-9474(94)00474-2
1994DE35 Phys.Lett. 333B, 1 (1994) F.de Jong, K.Nakayama, V.Herrmann, O.Scholten The Δ-Isobar and Proton-Proton Bremsstrahlung NUCLEAR REACTIONS 1H(p, γ), E=280 MeV; calculated σ(θ1, θ2, θγ), analyzing power vs θγ bremsstrahlung; deduced Δ-isobar role.
doi: 10.1016/0370-2693(94)90998-9
1994HA02 Phys.Rev. C49, 420 (1994) O.Hashimoto, H.Hamagaki, T.Kobayashi, K.Nakayama, Y.Shida, I.Tanihata, O.Yamakawa, N.Yoshikawa, S.Nagamiya, J.A.Bistirlich, K.M.Crowe, T.J.Humanic, M.Justice, J.O.Rasmussen, Y.-W.Xu Projectile Rapidity Pions in 775 MeV/nucleon 139La + 12C and 139La + 139La Reactions NUCLEAR REACTIONS 139La, 12C(139La, X), E=775 MeV/nucleon; measured projectile (fragment)(π-)-coin; deduced pion peak position, width. Participant-spectator interaction.
doi: 10.1103/PhysRevC.49.420
1993KR20 Phys.Lett. 319B, 393 (1993) F.Krmpotic, A.Mariano, T.T.S.Kuo, K.Nakayama Projected Linear Response Theory for Charge-Exchange Excitations and Double Beta Decay RADIOACTIVITY 76Ge(2β); calculated 2β-decay matrix element vs particle-particle coupling constant. Projected RPA, charge exchange excitations.
doi: 10.1016/0370-2693(93)91740-E
1992HE06 Phys.Rev. C45, 1450 (1992) Comparison of Nucleon-Nucleon Potential Models in Proton-Proton Bremsstrahlung NUCLEAR REACTIONS 1H(polarized p, γ), E=280 MeV; calculated σ(θ1, θ2, θ), analyzing power. Relativistic approach, pp-bremsstrahlung.
doi: 10.1103/PhysRevC.45.1450
1992HE18 Phys.Rev. C46, 2199 (1992) Relativistic Effects in Proton-Proton Bremsstrahlung NUCLEAR REACTIONS 1H(p, γ), (polarized p, γ), E=100, 280 MeV; calculated bremsstrahlung σ(θ1, θ2, θ), analyzing power; deduced rescattering role. Proton-proton bremsstrahlung, relativistic effects.
doi: 10.1103/PhysRevC.46.2199
1992NA06 Phys.Rev. C45, 2039 (1992) Hard Photon Production in Proton-Deuteron Reactions at Intermediate Energies NUCLEAR REACTIONS 2H(p, γ), E=195-200 MeV; calculated bremsstrahlung σ(θγ, Eγ). Meson exchange potential model.
doi: 10.1103/PhysRevC.45.2039
1991AR03 Phys.Rev. C43, 1875 (1991) H.F.Arellano, F.A.Brieva, W.G.Love, K.Nakayama Comparison of Nucleon-Nucleon Potential Models in a Full-Folding Description of Elastic Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 300, 400 MeV; analyzed σ(θ), polarization observables data; deduced effective nucleon-nucleon potential dependence. Nonrelativistic full-folding model analysis.
doi: 10.1103/PhysRevC.43.1875
1991BA26 Phys.Rev. C44, 93 (1991) F.T.Baker, L.Bimbot, R.W.Fergerson, C.Glashausser, A.Green, O.Hausser, K.Hicks, K.Jones, C.A.Miller, M.Vetterli, R.Abegg, D.Beatty, B.Bonin, B.Castel, X.Y.Chen, V.Cupps, C.Djalali, R.Henderson, K.P.Jackson, R.Jeppesen, K.Nakayama, S.K.Nanda, R.Sawafta, S.Yen Spin Decomposition of the Responses of 44Ca and 48Ca to 300 MeV Protons NUCLEAR REACTIONS 44Ca(polarized p, p'), E=290 MeV; 48Ca(polarized p, p'), E=318 MeV; measured σ(θ, Ep), analyzing power, spin-flip σ(θ). 44,48Ca deduced giant, spin resonance strength distributions.
doi: 10.1103/PhysRevC.44.93
1991HE01 Phys.Rev. C43, 394 (1991) V.Herrmann, J.Speth, K.Nakayama Nucleon-Nucleon Bremsstrahlung at Intermediate Energies NUCLEAR REACTIONS 1H(n, pγ), E=200 MeV; 1H(p, γ), E=10-600 MeV; calculated σ(θ1, θ2, θγ); deduced nucleon-nucleon bremsstrahlung role.
doi: 10.1103/PhysRevC.43.394
1991HE14 Phys.Rev. C44, R1254 (1991) Spin Observables in pp Bremsstrahlung and Off-Shell Effects of the NN Interaction NUCLEAR REACTIONS 1H(polarized p, γ), E=280 MeV; calculated bremsstrahlung spin polarization observables.
doi: 10.1103/PhysRevC.44.R1254
1990AR31 J.Phys.(Paris), Colloq.C-6, 603 (1990) H.F.Arellano, W.E.Love, K.Nakayama, F.A.Brieva Off-Shell Effects of Nucleon-Nucleon Potential Models on Proton-Nucleus Elastic Scattering Observables NUCLEAR REACTIONS 40Ca(polarized p, p), E=200 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ.
1990HE29 Phys.Lett. 251B, 6 (1990) Probing Off-Shell Effects with Proton-Proton Bremsstrahlung NUCLEAR REACTIONS 1H(p, γ), E=280 MeV; analyzed bremsstrahlung σ(θ1, θ2, θγ), analyzing power vs θ; deduced off-shell effects role.
doi: 10.1016/0370-2693(90)90222-R
1989NA04 Phys.Rev. C39, 1475 (1989) High-Energy Photons in Neutron-Proton and Proton-Nucleus Collisions NUCLEAR REACTIONS 1H(n, γ), E=200, 150 MeV; 9Be(p, γ), E=140 MeV; calculated bremsstrahlung σ(θ(γ), E(γ)).
doi: 10.1103/PhysRevC.39.1475
1989NA08 Phys.Rev. C40, 685 (1989) Potential Model Calculation of Energetic Photon Production from Heavy Ion Collisions NUCLEAR REACTIONS 12C(12C, γX), E=84 MeV/nucleon; 208Pb(14N, X), E=40 MeV/nucleon; 154Sm(12C, X), E=10 MeV/nucleon; calculated σ(θ, Eγ) bremsstrahlung. Potential model calculation.
doi: 10.1103/PhysRevC.40.685
1989NA19 Phys.Rev. C40, 2520 (1989) Hard Photons in Proton-Nucleus Collisions NUCLEAR REACTIONS 107Ag, 159Tb(p, γ), E=168 MeV; 197Au(p, γ), E=72 MeV; calculated bremsstrahlung σ(θγ, E). First chance nucleon-nucleon collision mechanism.
doi: 10.1103/PhysRevC.40.2520
1989YO03 Phys.Rev. C39, 2090 (1989) H.Yokota, S.Igarashi, K.Hama, T.Mori, T.Katsumi, K.Nakayama, K.Ichimaru, R.Chiba, K.Nakai, J.Chiba Direct (π+, pd) Cross Sections for Light Nuclei NUCLEAR REACTIONS 6,7Li, C(π+, pd), E=70, 130, 165 MeV; measured σ(θp, θd); deduced quasifree π+t → pd σ.
doi: 10.1103/PhysRevC.39.2090
1989YO05 Phys.Rev. C40, 270 (1989) H.Yokota, S.Igarashi, K.Hama, T.Mori, T.Katsumi, K.Ichimaru, K.Nakayama, R.Chiba, K.Nakai, J.Chiba Inclusive (π+, p) and (π+, pp) Cross Sections for Light Nuclei in the Resonance Energy Region NUCLEAR REACTIONS 6,7Li, C(π+, pX), (π+, 2p), E=70, 130, 165 MeV; measured σ(θ), σ(θp1, θp2); deduced effective numbers of quasideuteron.
doi: 10.1103/PhysRevC.40.270
1989YO07 Phys.Rev. C40, 1069 (1989) H.Yokota, S.Igarashi, K.Hama, T.Mori, T.Katsumi, K.Ichimaru, K.Nakayama, R.Chiba, K.Nakai, J.Chiba Broad Component of the (π+, pp) Angular Correlation NUCLEAR REACTIONS 6Li, 12C(π+, 2p), (π-, 2p), E=165 MeV; measured σ(θ1, θ2); deduced σ(θ) ratio, reaction mechanism.
doi: 10.1103/PhysRevC.40.1069
1988BA06 Phys.Rev. C37, 1350 (1988) F.T.Baker, L.Bimbot, R.W.Fergerson, C.Glashausser, K.Jones, A.Green, K.Nakayama, S.Nanda Using the (p(pol), p(pol)') Reaction to Study ΔS = 0 Giant Resonances NUCLEAR REACTIONS 40Ca(polarized p, p'), E=318 MeV; measured σ(θp', Ep'). 40Ca deduced ΔS=0 multipole transition strength distribution, EWSR.
doi: 10.1103/PhysRevC.37.1350
1988BA44 Nucl.Phys. A485, 46 (1988) E.Bauer, F.Krmpotic, K.Nakayama On the Description of the Giant Resonances within an RPA Formalism with Good Isospin NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated giant resonances, Gamow-Teller transition strengths. Charge-independent hamiltonian.
doi: 10.1016/0375-9474(88)90521-0
1988NA04 Phys.Rev. C38, 51 (1988) Effective Interaction for Nucleon-Nucleus Scattering Based on a One-Boson-Exchange Model NUCLEAR REACTIONS 90Zr(p, p), E=121.5 MeV; 12C(polarized p, p), E=200 MeV; 48Ca(polarized p, n), E=134 MeV; 28Si(p, p'), E=134 MeV; calculated σ(θ), analyzing power vs θ.
doi: 10.1103/PhysRevC.38.51
1987LO13 Phys.Rev.Lett. 59, 1401 (1987) W.G.Love, K.Nakayama, M.A.Franey Isovector Couplings for Nucleon Charge-Exchange Reactions at Intermediate Energies NUCLEAR REACTIONS 14C(p, n), E=60-450 MeV; calculated σ(θ=0°) vs E; deduced nucleon-nucleon interaction isovector component features.
doi: 10.1103/PhysRevLett.59.1401
1987NA14 Nucl.Phys. A470, 573 (1987) K.Nakayama, S.Drozdz, S.Krewald, J.Speth Quasiparticle Relativistic G-Matrix Interaction NUCLEAR STRUCTURE 208Pb, 16O, 40Ca; calculated breathing mode 0+ state energy, B(λ). Relativistic G-matrix.
doi: 10.1016/0375-9474(87)90588-4
1987NA15 Phys.Rev.Lett. 59, 1053 (1987) Comment on ' Can an Isovector Dipole Mode of Nuclear Collective Motion Give a Signature Duplicating That of an Isoscalar Mode ( Question ) ' NUCLEAR REACTIONS 116Sn(α, α'), E=15.6 MeV; calculated σ(θ). 116Sn deduced isovector dipole excitation role.
doi: 10.1103/PhysRevLett.59.1053
1987NA25 Phys.Rev. C36, 1848 (1987) Ultradipole Photons in Low-Energy Heavy-Ion Reactions NUCLEAR REACTIONS, MECPD 154Sm(α, Xγ), 148Sm(3He, Xγ), E=27 MeV; analyzed σ(θ) vs Eγ. One-dimensional potential approach.
doi: 10.1103/PhysRevC.36.1848
1986NA03 Phys.Rev. C33, 1002 (1986) K.Nakayama, H.Yokota, K.Ichimaru, Y.Takahata, F.Suekane, R.Chiba, K.Nakai, I.Arai, H.Enyo, S.Sasaki, T.Nagae, M.Sekimoto Pion Absorption on Nuclei at 65 MeV NUCLEAR REACTIONS C, 27Al, Cu, Ta(π+, p), (π-, p), (π+, d), (π-, d), (π+, 2p), (π-, 2p), (π+, np), (π-, np), E=65 MeV; measured σ(θ), pp-, nn- correlations; deduced nucleon-nucleon pair pion absorption σ ratio.
doi: 10.1103/PhysRevC.33.1002
1986NA15 Phys.Rev. C34, 2190 (1986) High Energy Photon Production in Nuclear Collisions NUCLEAR REACTIONS 1n(p, pγ), E=40, 100, 120, 140 MeV; 9Be(p, pγ), E=140 MeV; 208Pb(14N, 14Nγ), E=40 MeV/nucleon; calculated bremsstrahlung probability, rate, Eγ, Iγ, γ(θ), σ(θ(γ), E(γ)), σ. Infinite, semi-infinite nuclear matter approximations.
doi: 10.1103/PhysRevC.34.2190
1986YO05 Phys.Lett. 175B, 23 (1986) H.Yokota, K.Nakayama, K.Ichimaru, Y.Takahata, F.Suekane, R.Chiba, K.Nakai, I.Arai, H.Enyo, S.Sasaki, T.Nagae, M.Sekimoto Deuteron Emission from Pion Absorption at T(π) = 65 MeV NUCLEAR REACTIONS C, 27Al, Cu, Ta(π+, d), (π-, d), (π+, p), (π+, 2p), (π+, pd), E=65 MeV; measured σ(θ), σ(θ1, θ2); deduced pion absorption mechanism.
doi: 10.1016/0370-2693(86)90324-2
1986YO06 Phys.Rev.Lett. 57, 807 (1986) H.Yokota, K.Nakayama, K.Ichimaru, T.Katsumi, T.Mori, S.Igarashi, K.Hama, R.Chiba, K.Nakai, J.Chiba, H.Enyo, S.Sasaki, T.Nagae, M.Sekimoto Pion Absorption on T = 1 Nucleon Pairs at T(π) = 70 MeV NUCLEAR REACTIONS 6,7Li(π+, np), (π-, np), E=70 MeV; measured np(θ); deduced σ(θ), two-nucleon absorption component.
doi: 10.1103/PhysRevLett.57.807
1984NA26 Phys.Lett. 148B, 399 (1984) K.Nakayama, S.Krewald, J.Speth Test of the Nuclear Matter G-Matrix Interaction in Nuclear Structure Calculations NUCLEAR STRUCTURE 16O; calculated levels, Γ, B(λ). 208Pb; calculated levels, B(λ). G-matrix, one-boson exchange model.
doi: 10.1016/0370-2693(84)90726-3
1984SC04 Nucl.Phys. A414, 67 (1984) H.R.Schelin, E.Farrelly Pessoa, W.R.Wylie, E.W.Cybulska, K.Nakayama, L.M.Fagundes, R.A.Douglas The 12C(d, n)13N Reaction between E(d) = 7.0 and 13.0 MeV NUCLEAR REACTIONS 12C(d, n), E=7, 9.1, 13 MeV; measured σ(En), σ(E), absolute σ(θ). 12C(d, n), E=10.6-13 MeV; measured σ(E). 13N levels deduced S. Hauser-Feshbach reduction factors. Tof. DWBA analysis.
doi: 10.1016/0375-9474(84)90497-4
1983FU20 Nucl.Instrum.Methods 217, 441 (1983) Y.Fujita, K.Nakayama, M.Fujiwara, S.Morinobu, T.Yamazaki, H.Ikegami Two-Dimensional Focal Plane Counter with Induction Readout NUCLEAR REACTIONS 48Ca(p, p'), 50Cr(p, d), E=65 MeV; measured σ(Ep'), σ(Ed). Two-dimensional gas proportional counter, large dispersion spectrograph, induction readout.
doi: 10.1016/0167-5087(83)90753-6
1983KR08 Nucl.Phys. A399, 478 (1983) F.Krmpotic, K.Nakayama, A.Pio Galeao Giant First-Forbidden Resonances NUCLEAR STRUCTURE 90,91,92,94,96Zr, 93Nb, 94,96,97,98Mo, 112,116,120,122,124Sn, 208Pb; calculated E1 resonance, first-forbidden giant resonance, energy splitting, isospin character, Gamow-Teller resonance characteristics. Schematic model.
doi: 10.1016/0375-9474(83)90259-2
1983SH49 Nucl.Phys. A408, 525 (1983) T.A.Shibata, K.Nakai, H.En'yo, S.Sasaki, M.Sekimoto, I.Arai, K.Nakayama, K.Ichimaru, H.Nakamura-Yokota, R.Chiba Particle Production in the Target-Rapidity Region from Hadron-Nucleus Reactions at Several GeV NUCLEAR REACTIONS C(p, π-), C(p, π+), C(π+, π-), C(π+, π+), 12C(p, x), 12C(π+, x), Cu(p, π-), Cu(p, π+), Cu(p, x), Cu(π+, π-), Cu(π+, π+), Cu(π+, x), Pb(p, π-), Pb(p, π+), Pb(p, x), Pb(π+, π-), Pb(π+, π+), Pb(π+, x), E=747 MeV-12 GeV; measured products, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry O0597.
doi: 10.1016/0375-9474(83)90244-0
1983YO04 Phys.Rev.Lett. 51, 1530 (1983) H.Yokota, K.Nakayama, K.Ichimaru, Y.Takahata, F.Suekane, R.Chiba, K.Nakai, E.Arai, H.Enyo, S.Sasaki, T.Nagae, M.Sekimoto Isospin Dependence of Pion Absorption by Light Nuclei NUCLEAR REACTIONS C, 27Al(π+, p), (π-, p), (π+, 2p), (π+, np), E=65 MeV; measured σ(θ) ratio, integrated two-nucleon yield ratios, pp(θ), pn(θ); deduced pion absorption mechanism.
doi: 10.1103/PhysRevLett.51.1530
1982NA12 Phys.Lett. 114B, 217 (1982) K.Nakayama, A.Pio Galeao, F.Krmpotic On the Energetics of the Gamow-Teller Resonances NUCLEAR STRUCTURE 90,91,92,94Zr, 93Nb, 94,96,97,98,100Mo, 112,116,120,122,124Sn, 169Tm, 208Pb; analyzed Gamow-Teller, Fermi resonance energy difference systematics; deduced spin, isospin interaction, effective axial vector coupling constants dependence. TDA, schematic residual force.
doi: 10.1016/0370-2693(82)90480-4
1980IS04 J.Phys.Soc.Jpn. 48, 1804 (1980) Isobaric Analogue Resonances in 27Al Studied with the 26Mg(p, p) and 26Mg(p, γ) Reactions NUCLEAR REACTIONS 26Mg(p, p), E=1.9-4 MeV; measured σ(E, θ); 26Mg(p, γ), E=1.6-3.95 MeV; measured σ(E, Eγ, θ). 27Al deduced IAR, J, π, Γ, Coulomb energy differences, S. Enriched target.
doi: 10.1143/JPSJ.48.1804
1980KO09 J.Phys.Soc.Jpn. 48, 720 (1980) S.Koh, K.Nakayama, M.Tsuda, T.Hayashi, Y.Tanaka, Y.Oda 26Mg(d, p)27Mg Reactions at 3.1 and 3.5 MeV NUCLEAR REACTIONS 26Mg(d, p), E=3.1, 3.5 MeV; measured σ(Ep, θ). 27Mg deduced levels, L, S. DWBA, Hauser-Feshbach analysis, shell model. Enriched target.
doi: 10.1143/JPSJ.48.720
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