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Search: Author = K.Nakayama

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2019NA18      Phys.Rev. C 100, 035208 (2019)


Explicit derivation of the completeness condition in pseudoscalar meson photoproduction

doi: 10.1103/PhysRevC.100.035208
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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
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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
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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
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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
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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
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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
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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
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2012HA20      Phys.Rev. C 85, 064001 (2012)

H.Haberzettl, K.Nakayama

Gauge-invariant formulation of NN → NNγ

doi: 10.1103/PhysRevC.85.064001
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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
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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
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2011HA27      Phys.Rev. C 83, 065502 (2011)

H.Haberzettl, F.Huang, K.Nakayama

Dressing the electromagnetic nucleon current

doi: 10.1103/PhysRevC.83.065502
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1914.

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
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2010DO11      Eur.Phys.J. A 43, 83 (2010)

M.Doring, K.Nakayama

The phase and pole structure of the N*(1535) in πN → πN and γN → πN

doi: 10.1140/epja/i2009-10892-4
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2010NA24      Phys.Rev. C 82, 065201 (2010)

K.Nakayama, F.Huang

Model-independent analysis of p+p → pp(1S0)+γ

doi: 10.1103/PhysRevC.82.065201
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2009NA37      Phys.Rev. C 80, 051001 (2009)

K.Nakayama, H.Haberzettl

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
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2008OH04      Phys.Rev. C 77, 045204 (2008)

Y.Oh, C.M.Ko, K.Nakayama

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
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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
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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
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2006NA11      Phys.Rev. C 73, 045211 (2006)

K.Nakayama, H.Haberzettl

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
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2006NA23      Acta Phys.Slovaca 56, 237 (2006)

K.Nakayama, H.Haberzettl

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
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2006OH01      Phys.Rep. 423, 49 (2006)

Y.Oh, K.Nakayama, T.-S.H.Lee

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
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2005NA33      Phys.Rev. C 72, 034603 (2005)

K.Nakayama, W.G.Love

Spin structure of spin-1/2 baryon and spinless meson production amplitudes in photonic and hadronic reactions

doi: 10.1103/PhysRevC.72.034603
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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
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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
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2004NA19      Phys.Rev. C 69, 065212 (2004)

K.Nakayama, H.Haberzettl

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
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2004NA23      Phys.Rev. C 70, 012201 (2004)

K.Nakayama, W.G.Love

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
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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
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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
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2003TS05      Phys.Rev. C 68, 034612 (2003)

K.Tsushima, K.Nakayama

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
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2003TS07      Nucl.Phys. A721, 633c (2003)

K.Tsushima, K.Nakayama

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
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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
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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
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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
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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
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1999HA23      Phys.Lett. 454B, 176 (1999)

C.Hanhart, K.Nakayama

On the Treatment of NN Interaction Effects in Meson Production in NN Collisions

doi: 10.1016/S0370-2693(99)00377-9
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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
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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
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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)

F.de Jong, K.Nakayama

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
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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
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1995DE41      Phys.Rev. C52, 2377 (1995)

F.de Jong, K.Nakayama

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
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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
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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
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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
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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
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1992HE06      Phys.Rev. C45, 1450 (1992)

V.Herrmann, K.Nakayama

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
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1992HE18      Phys.Rev. C46, 2199 (1992)

V.Herrmann, K.Nakayama

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0213.

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
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1991HE14      Phys.Rev. C44, R1254 (1991)

V.Herrmann, K.Nakayama

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
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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)

V.Herrmann, K.Nakayama

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
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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
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1989NA08      Phys.Rev. C40, 685 (1989)

K.Nakayama, G.F.Bertsch

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
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1989NA19      Phys.Rev. C40, 2520 (1989)

K.Nakayama, G.F.Bertsch

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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0545.

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
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1988NA04      Phys.Rev. C38, 51 (1988)

K.Nakayama, W.G.Love

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
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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
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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
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1987NA15      Phys.Rev.Lett. 59, 1053 (1987)

K.Nakayama, G.Bertsch

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
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1987NA25      Phys.Rev. C36, 1848 (1987)

K.Nakayama, G.F.Bertsch

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
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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
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1986NA15      Phys.Rev. C34, 2190 (1986)

K.Nakayama, G.Bertsch

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1980IS04      J.Phys.Soc.Jpn. 48, 1804 (1980)

K.Isagawa, K.Nakayama, Y.Oda

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
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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0306.

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