NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.Bennhold Found 95 matches. 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
2005LA12 Eur.Phys.J. A 24, 275 (2005) R.Lawall, J.Barth, C.Bennhold, K.-H.Glander, S.Goers, J.Hannappel, N.Jopen, F.Klein, E.Klempt, T.Mart, D.Menze, M.Ostrick, E.Paul, I.Schulday, W.J.Schwille, F.W.Wieland, C.Wu Measurement of the reaction γp → K0∑+ at photon energies up to 2.6 GeV NUCLEAR REACTIONS 1H(γ, Σ+K0), E=0.9-2.6 GeV; measured σ, σ(θ), polarization. Tagged photons. Comparison with model predictions.
doi: 10.1140/epja/i2005-10002-x
2005LE23 Nucl.Phys. A754, 248c (2005) Baryon resonances and pentaquarks on the lattice
doi: 10.1016/j.nuclphysa.2004.12.072
2005PA38 Nucl.Phys. A754, 127c (2005) A.Parreno, C.Bennhold, B.R.Holstein An EFT for the weak ΛN interaction NUCLEAR STRUCTURE 5He, 11B, 12C; analyzed hypernucleus decay rates, related features; deduced parameters. Effective field theory framework.
doi: 10.1016/j.nuclphysa.2005.01.008
2005RA18 Nucl.Phys. A754, 202c (2005) A.Ramos, E.Oset, C.Bennhold, D.Jido, J.A.Oller, U.-G.Meissner Dynamical generation of hyperon resonances
doi: 10.1016/j.nuclphysa.2005.01.003
2004PA39 Phys.Rev. C 70, 051601 (2004) A.Parreno, C.Bennhold, B.R.Holstein ΛN → NN weak interaction in effective-field theory NUCLEAR STRUCTURE 5He, 11B, 12C; calculated hypernucleus weak decay rates, related observables.
doi: 10.1103/PhysRevC.70.051601
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
2003PA47 Nucl.Phys. A721, 967c (2003) A.Parreno, A.Ramos, G.Garbarino, C.Bennhold Λ- and ΛΛ-hypernuclear decay predictions in a OME model. NUCLEAR STRUCTURE 5,6He, 12C; calculated hypernucleus decay widths. Meson-exchange model, comparison with data.
doi: 10.1016/S0375-9474(03)01261-2
2003RA47 Nucl.Phys. A721, 711c (2003) Low-lying Jp = 1/2- resonances from chiral unitary dynamics
doi: 10.1016/S0375-9474(03)01163-1
2002KA67 Phys.Rev. C 66, 065206 (2002) S.S.Kamalov, L.Tiator, D.Drechsel, R.A.Arndt, C.Bennhold, I.I.Strakovsky, R.L.Workman Dispersion relation analysis of neutral pion photoproduction and electroproduction at threshold NUCLEAR REACTIONS 1H(γ, π0), (e, e'π0), E ≈ threshold; analyzed data; deduced multipole contributions. Dispersion relation analysis.
doi: 10.1103/PhysRevC.66.065206
2002PA03 Phys.Rev. C65, 015205 (2002) A.Parreno, A.Ramos, C.Bennhold Novel Weak Decays in Doubly Strange Systems NUCLEAR STRUCTURE 6He; calculated ΛΛ hypernucleus partial weak decay rates.
doi: 10.1103/PhysRevC.65.015205
2002ZH06 Phys.Rev. C65, 032201 (2002) Q.Zhao, J.S.Al-Khalili, C.Bennhold Contributions of Vector Meson Photoproduction to the Gerasimov-Drell-Hearn Sum Rule NUCLEAR REACTIONS 1n, 1H(γ, X), E=1-6 GeV; calculated ω and ρ meson production σ, σ(θ), contributions to sum rule.
doi: 10.1103/PhysRevC.65.032201
2001BA92 Nucl.Phys. A691, 374c (2001) J.Barth, C.Bennhold, W.Braun, J.Ernst, K.H.Glander, S.Goers, J.Hannappel, N.Jopen, H.Kalinowsky, F.Klein, E.Klempt, A.Kozela, R.Lawall, J.Link, T.Mart, D.Menze, W.Neuerburg, M.Ostrick, E.Paul, H.van Pee, I.Schulday, W.-J.Schwille, J.Smyrski, U.Thoma, R.Wedemeyer, B.Wiegers, F.W.Wieland, J.Wisskirchen New Results on η and η' Photoproduction with SAPHIR at ELSA NUCLEAR REACTIONS 1H(γ, X), E=0.7-2.6 GeV; measured η and η' meson production σ, σ(θ).
doi: 10.1016/S0375-9474(01)01059-4
2001HA22 Nucl.Phys. A684, 475c (2001) H.Haberzettl, C.Bennhold, T.Mart Gauge-Invariant Description of Photo- and Electroproduction of Mesons with Extended Nucleons Applied to Kaon Production NUCLEAR REACTIONS 1H(γ, K+), (e, e'K+), E=high; calculated hyperon production associated σ(θ). Gauge-invariant approach, off-shell form factors discussed. Comparisons with data.
doi: 10.1016/S0375-9474(01)00510-3
2001LE40 Nucl.Phys. A695, 237 (2001) F.X.Lee, T.Mart, C.Bennhold, H.Haberzettl, L.E.Wright Quasifree Kaon Photoproduction on Nuclei NUCLEAR REACTIONS 1n, 1H(γ, K+), (γ, K0), E=1.6-2.2 GeV; calculated hyperon production σ, σ(θ), asymmetry, recoil polarization. 12C(γ, K+X), (γ, K0X), E=1.4 GeV; calculated hyperon production σ(θ), Ay(θ), final-state interaction effects.
doi: 10.1016/S0375-9474(01)01098-3
2001MA36 Nucl.Phys. A684, 502c (2001) T.Mart, S.Sumowidagdo, D.Kusno, C.Bennhold, H.Haberzettl Kaon Photoproduction on the Nucleon: Overview of some applications
doi: 10.1016/S0375-9474(01)00477-8
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
2001ZH36 Phys.Rev. C64, 052201 (2001) Q.Zhao, J.S.Al-Khalili, C.Bennhold Quark Model Predictions for K* Photoproduction on the Proton NUCLEAR REACTIONS 1H(γ, X), E=1.8-3.4 GeV; calculated K* vector meson production σ, σ(θ). Quark model.
doi: 10.1103/PhysRevC.64.052201
2000KA04 Phys.Rev. C61, 024319 (2000) S.Karataglidis, P.J.Dortmans, K.Amos, C.Bennhold Alternative Evaluations of Halos in Nuclei NUCLEAR REACTIONS 1H(6He, 6He), (8He, 8He), E=72 MeV/nucleon; 1H(9Li, 9Li), (11Li, 11Li), E=62 MeV/nucleon; 6Li(γ, π+), E=200 MeV; calculated σ(θ). 6,8He, 9,11Li deduced halo features. Microscopic folding model, comparison with data. NUCLEAR STRUCTURE 6,8He, 9,11Li; calculated levels, J, π, radii, neutron density profiles. Shell model, comparison with data.
doi: 10.1103/PhysRevC.61.024319
2000MA02 Phys.Rev. C61, 012201 (2000) Evidence for a Missing Nucleon Resonance in Kaon Photoproduction NUCLEAR REACTIONS 1H(γ, K+X), E(cm)=1.6-2.2 GeV; analyzed hyperon production associated σ, σ(θ), asymmetry; deduced possible resonance.
doi: 10.1103/PhysRevC.61.012201
2000PA29 Nucl.Phys. A670, 257c (2000) A.Parreno, C.Bennhold, A.Ramos Decay of Hypernuclei NUCLEAR STRUCTURE 12C; calculated hypernucleus decay observables.
doi: 10.1016/S0375-9474(00)00108-1
2000PA65 Acta Phys.Hung.N.S. 11, 397 (2000) A.Parreno, C.Bennhold, A.Ramos, M.Zarei Decay of Single- and Double-Λ Hypernuclei NUCLEAR STRUCTURE 5He, 11B, 12C; calculated hypernuclei non-mesonic and baryonic decay widths and branching ratios. Comparison with data.
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
1999LE35 Phys.Rev. C60, 034605 (1999) F.X.Lee, C.Bennhold, S.S.Kamalov, L.E.Wright Higher Nucleon Resonances in Exclusive (γ, πN) Reactions on Nuclei NUCLEAR REACTIONS 12C(γ, π-p), (γ, π+n), (γ, π0p), (γ, π0n), E=200-1200 MeV; calculated σ, σ(θ), photon asymmetry; deduced final state interaction, medium modification effects, resonance contributions.
doi: 10.1103/PhysRevC.60.034605
1999PA15 Phys.Rev. C59, 2122 (1999) A.Parreno, A.Ramos, N.G.Kelkar, C.Bennhold Weak Strangeness Production Reaction pn → pΛ in a One-Boson-Exchange Model NUCLEAR REACTIONS 1n(p, X), E at 900-1200 MeV/c; calculated hyperon production σ, σ(θ); deduced sensitivity to hyperon-nucleon interaction. One-meson exchange model.
doi: 10.1103/PhysRevC.59.2122
1999TI09 Phys.Rev. C60, 035210 (1999) L.Tiator, D.Drechsel, G.Knochlein, C.Bennhold Analysis of Resonance Multipoles from Polarization Observables in η Photoproduction NUCLEAR REACTIONS 1H(γ, X), E=716-1050 MeV; analyzed η production σ(θ), polarization observables; deduced resonance multipole parameters, branching ratios.
doi: 10.1103/PhysRevC.60.035210
1998BE59 Nucl.Phys. A639, 209c (1998) C.Bennhold, S.Goers, J.Barth, W.Braun, R.Burgwinkel, J.Ernst, K.H.Glander, J.Hannappel, N.Jopen, H.Kalinowsky, U.Kirch, F.Klein, F.J.Klein, E.Klempt, A.Kozela, R.Lawall, Z.Li, J.Link, T.Mart, D.Menze, W.Neuerburg, M.Paganetti, E.Paul, H.van Pee, R.Plotzke, M.Schumacher, W.J.Schwille, F.Smend, J.Smyrski, H.-N.Tran, M.Q.Tran, F.Wehnes, B.Wiegers, F.W.Wieland, J.Wisskirchen K0-Σ+ Photoproduction with SAPHIR NUCLEAR REACTIONS 1H(γ, K0), E=1.0-1.6 GeV; measured hyperon production σ(θ), σ. Model comparisons.
doi: 10.1016/S0375-9474(98)00275-9
1998BE60 Nucl.Phys. A639, 227c (1998) C.Bennhold, F.X.Lee, T.Mart, L.E.Wright Kaon Electromagnetic Production on Nuclei NUCLEAR REACTIONS 12C(γ, K+X)11B, E=1.4 GeV; calculated hyperon production σ(θ); deduced reaction mechanism features. Quasifree kinematics.
doi: 10.1016/S0375-9474(98)00278-4
1998ER03 Nucl.Phys. A639, 213c (1998) J.Ernst, H.Jungst, H.Kalinowsky, E.Klempt, J.Link, H.van Pee, R.Plotzke, J.Barth, W.Braun, R.Burgwinkel, K.H.Glander, S.Goers, J.Hannappel, N.Jopen, U.Kirch, F.Klein, F.-J.Klein, R.Lawall, D.Menze, W.Neuerburg, M.Paganetti, E.Paul, W.-J.Schwille, M.Q.Tran, F.Wehnes, B.Wiegers, F.W.Wieland, J.Wisskirchen, M.Schumacher, F.Smend, H.-N.Tran, A.Kozela, J.Smyrski, C.Bennhold First Results of η' Photoproduction with SAPHIR NUCLEAR REACTIONS 1H(γ, X), E=1.5-2.5 GeV; measured preliminary η' production σ.
doi: 10.1016/S0375-9474(98)00276-0
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
1998HA32 Phys.Rev. C58, R40 (1998) H.Haberzettl, C.Bennhold, T.Mart, T.Feuster Gauge-Invariant Tree-Level Photoproduction Amplitudes with Form Factors
doi: 10.1103/PhysRevC.58.R40
1998KA06 Phys.Rev.Lett. 80, 1614 (1998) Probing Proton Halos Through Pion Photoproduction NUCLEAR REACTIONS 17O(γ, π-), E=200 MeV; calculated σ(θ); deduced 17F proton halo dependence.
doi: 10.1103/PhysRevLett.80.1614
1998MA20 Nucl.Phys. A631, 765c (1998) T.Mart, D.Kusno, C.Bennhold, L.Tiator, D.Drechsel Photoproduction of the Hypertriton NUCLEAR REACTIONS 3He(γ, X), E=1500-2200 MeV; calculated kaon production σ(θ); deduced hypertriton production features. Fadeev equations.
doi: 10.1016/S0375-9474(98)00106-7
1998MA57 Nucl.Phys. A639, 237c (1998) Kaon and Hyperon Form Factors in Kaon Electroproduction on the Nucleon NUCLEAR REACTIONS 1n, 1H(e, e'K0), 1H(e, e'K+), E not given; calculated hyperon production associated response functions.
doi: 10.1016/S0375-9474(98)00279-6
1998MA59 Nucl.Phys. A640, 235 (1998) T.Mart, L.Tiator, D.Drechsel, C.Bennhold Electromagnetic Production of the Hypertriton NUCLEAR REACTIONS 3He(γ, K+), E=1500-2200 MeV; calculated hypernucleus production σ(θ); deduced Fermi motion effects, other reaction mechanism features. Impulse approximation.
doi: 10.1016/S0375-9474(98)00441-2
1998PA29 Nucl.Phys. A639, 333c (1998) A.Parreno, A.Ramos, C.Bennhold, K.Maltman Violation of the ΔI = 1/2 Rule in the Nonmesonic Weak Decay of Λ Hypernuclei NUCLEAR STRUCTURE 12C; calculated hypernucleus weak decay observables; deduced ΔI=3/2 contributions.
doi: 10.1016/S0375-9474(98)00292-9
1998PA30 Phys.Lett. 435B, 1 (1998) A.Parreno, A.Ramos, C.Bennhold, K.Maltman Violation of the ΔI = 1/2 Rule in the Nonmesonic Weak Decay of Hypernuclei NUCLEAR STRUCTURE 12C; calculated hypernucleus decay observables; deduced sensitivity to ΔI=3/2 amplitudes.
doi: 10.1016/S0370-2693(98)00832-6
1998RA23 Nucl.Phys. A639, 307c (1998) A.Ramos, A.Parreno, C.Bennhold, E.Oset, L.L.Salcedo, M.J.Vincente-Vacas Non-Mesonic Weak Decay of Λ Hypernuclei NUCLEAR STRUCTURE 12C, 16O, 20Ne, 40Ca, 56Fe, 89Y, 208Pb; calculated hypernuclei mesonic, one-, two-nucleon induced decay rates. 12C; calculated neutron spectra, proton spectra from hypernucleus decay. 208Pb; calculated proton, neutron multiplicities from hypernucleus decay.
doi: 10.1016/S0375-9474(98)00288-7
1998TR06 Phys.Lett. 445B, 20 (1998) M.Q.Tran, J.Barth, C.Bennhold, M.Bockhorst, W.Braun, A.Budzanowski, G.Burbach, R.Burgwinkel, J.Ernst, K.H.Glander, S.Goers, B.Guse, K.-M.Haas, J.Hannappel, K.Heinloth, K.Honscheid, T.Jahnen, N.Jopen, H.Jungst, H.Kalinowsky, U.Kirch, F.J.Klein, F.Klein, E.Klempt, D.Kostrewa, A.Kozela, R.Lawall, L.Lindemann, J.Link, J.Manns, T.Mart, D.Menze, H.Merkel, R.Merkel, W.Neuerburg, M.Paganetti, E.Paul, R.Plotzke, U.Schenk, J.Scholmann, I.Schulday, M.Schumacher, P.Schutz, W.J.Schwille, F.Smend, J.Smyrski, W.Speth, H.N.Tran, H.van Pee, W.Vogel, R.Wedemeyer, F.Wehnes, B.Wiegers, F.W.Wieland, J.Wisskirchen, A.Wolf, and the SAPHIR Collaboration Measurement of γp → K+ Λ and γp → K+Σ0 at Photon Energies up to 2 GeV NUCLEAR REACTIONS 1H(γ, K+X), E=0.8-2 GeV; measured Λ, Σ0 hyperon production σ(θ), σ, polarizations. Tagged photons.
doi: 10.1016/S0370-2693(98)01393-8
1998ZH29 Phys.Lett. 436B, 42 (1998) ω and ρ Photoproduction with an Effective Quark Model Lagrangian NUCLEAR REACTIONS 1n, 1H(γ, X), E=1-5 GeV; analyzed ρ-, ω-meson production σ; deduced intermediate resonance contributions, polarization observables role. Effective quark model Lagrangian.
doi: 10.1016/S0370-2693(98)00894-6
1998ZH31 Phys.Rev. C58, 2393 (1998) Vector Meson Photoproduction with an Effective Lagrangian in the Quark Model
doi: 10.1103/PhysRevC.58.2393
1997ES05 Phys.Rev. C56, 2607 (1997) M.A.Espy, J.M.O'Donnell, B.Davis, D.Dehnhard, J.L.Langenbrunner, B.Larson, M.Palarczyk, C.M.Riedel, K.Wick, S.Blanchard, G.R.Burleson, W.R.Gibbs, B.Lail, B.Nelson, B.K.Park, Q.Zhao, W.J.Cummings, P.P.J.Delheij, B.K.Jennings, O.Hausser, R.Henderson, D.Thiessen, E.Brash, M.K.Jones, B.Brinkmoller, K.Maeda, F.Merrill, C.L.Morris, S.Penttila, D.Swenson, D.Tupa, C.Bennhold, S.S.Kamalov Asymmetries for Elastic Scattering of π- from Polarized 3He atΔ Resonance Energies NUCLEAR REACTIONS 3He(π+, π+), E=142, 180, 256 MeV; 3He(π-, π-), E=180 MeV; measured σ(θ); deduced asymmetries, Δ-n spin-spin interaction. Optically pumped spin polarized target, large acceptance spectrometer. Model comparisons.
doi: 10.1103/PhysRevC.56.2607
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
1997KA01 Phys.Rev. C55, 88 (1997) S.S.Kamalov, L.Tiator, C.Bennhold Elastic Pion Scattering on the Deuteron in a Multiple Scattering Model NUCLEAR REACTIONS 2H(π+, π+), E=65-324; calculated σ(θ), tensor analyzing power vs θ, other polarization observables. Multiple scattering model, polarized target.
doi: 10.1103/PhysRevC.55.88
1997KA02 Phys.Rev. C55, 98 (1997) S.S.Kamalov, L.Tiator, C.Bennhold Coherent π0 and η Photoproduction on the Deuteron NUCLEAR REACTIONS 2H(γ, π0), E=139-151 MeV; calculated reduced σ, σ(θ) vs E, photon asymmetry, vector, tensor analyzing power vs θ. 2H(γ, X), E=675 MeV; calculated η production σ(θ). Polarized target, coupled-channels approach in momentum space.
doi: 10.1103/PhysRevC.55.98
1997LE02 Phys.Rev. C55, 318 (1997) F.X.Lee, C.Bennhold, L.E.Wright Quasifree Pion Electroproduction from Nuclei in the Δ Region NUCLEAR REACTIONS 1H(e, e'X), E not given; calculated quasifree pion production associated σ vs k2, W. 12C(e, e'X), E not given; calculated quasifree pion production associated differential σ. Plane, distorted wave impulse approximation.
doi: 10.1103/PhysRevC.55.318
1997PA18 Phys.Rev. C56, 339 (1997) A.Parreno, A.Ramos, C.Bennhold Weak Decay of Hypernuclei NUCLEAR STRUCTURE A=5; A=11; A=12; calculated ΛN to NN decay rate of 5He(Λ), 11B(Λ), 12C(Λ) hypernuclei. Shell model, realistic short-range correlations.
doi: 10.1103/PhysRevC.56.339
1996ES04 Phys.Rev.Lett. 76, 3667 (1996) M.A.Espy, D.Dehnhard, C.M.Edwards, M.Palarczyk, J.L.Langenbrunner, B.Davis, G.R.Burleson, S.Blanchard, W.R.Gibbs, B.Lail, B.Nelson, B.K.Park, Q.Zhao, W.J.Cummings, P.P.J.Delheij, B.K.Jennings, R.Henderson, O.Hausser, D.Thiessen, E.Brash, M.K.Jones, B.Larson, B.Brinkmoller, K.Maeda, C.L.Morris, J.M.O'Donnell, S.Penttila, D.Swenson, D.Tupa, C.Bennhold, S.S.Kamalov Asymmetries for Elastic Scattering of π+ from Polarized 3He and the Δ-Neutron Spin-Spin Interaction NUCLEAR REACTIONS 3He(π+, π+), E=142-256 MeV; measured energy spectra, asymmetry vs θ; deduced Δ-n spin-spin interaction role. Polarized target.
doi: 10.1103/PhysRevLett.76.3667
1996KA29 Phys.Rev. C54, 1863 (1996) S.Karataglidis, K.Amos, C.Bennhold, L.Tiator Large Basis Shell Model Analysis of 14N(γ, π+)14C(g.s) Reaction NUCLEAR REACTIONS 14N(γ, π+), E=173 MeV; calculated σ(θ); deduced need for improved elementary pion production process. Shell model wave functions.
doi: 10.1103/PhysRevC.54.1863
1996LE11 Nucl.Phys. A603, 345 (1996) F.X.Lee, L.E.Wright, C.Bennhold, L.Tiator Quasi-Free η Photoproduction from Nuclei NUCLEAR REACTIONS 12C, 40Ca(γ, X), E=680-800 MeV; calculated σ(θp, θ(η), E(η)), photon asymmetry. DWIA.
doi: 10.1016/0375-9474(96)80006-D
1996MA83 Acta Phys.Pol. B27, 3167 (1996) Electromagnetic Production of Kaons on the Nucleon
1995BE17 Nucl.Phys. A585, 313c (1995) C.Bennhold, L.Tiator, S.S.Kamalov The Nucleon Strangeness Content and the (Eta)NN Coupling NUCLEAR REACTIONS 1H(γ, X), E ≤ 750 MeV; calculated σ(E). 1H(γ, X), E=752 MeV; calculated eta production σ(θ), recoil polarization; deduced (eta NN) coupling related features.
doi: 10.1016/0375-9474(94)00583-9
1995KA37 Phys.Rev.Lett. 75, 1288 (1995) S.S.Kamalov, L.Tiator, C.Bennhold Two-Body Mechanisms in Pion Photoproduction on the Trinucleon NUCLEAR REACTIONS 3He(γ, π+), E=300, 400, 500 MeV; analyzed σ(θ); deduced two-body mechanisms role.
doi: 10.1103/PhysRevLett.75.1288
1995MA09 Phys.Rev. C51, R1074 (1995) T.Mart, C.Bennhold, C.E.Hyde-Wright Constraints on Coupling Constants Through Charge Σ Photoproduction NUCLEAR REACTIONS 1n, 1H(γ, X), E=1-2 GeV; analyzed Σ+, Σ- production σ(E) data; deduced Born coupling constants. Phenomenological models.
doi: 10.1103/PhysRevC.51.R1074
1995MA32 Phys.Rev. C51, 2534 (1995) S.K.Matthews, W.J.Briscoe, C.Bennhold, B.L.Berman, R.W.Caress, K.S.Dhuga, S.N.Dragic, S.S.Kamalov, N.J.Nicholas, M.F.Taragin, L.Tiator, S.J.Greene, D.B.Barlow, B.M.K.Nefkens, C.Pillai, J.W.Price, L.D.Isenhower, M.E.Sadler, I.Slaus, I.Supek Elastic Scattering of Pions from 3H and 3He into the Backward Hemisphere NUCLEAR REACTIONS 3He, 3H(π+, π+), E=142-256 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.51.2534
1995PA36 Phys.Rev. C52, R1768 (1995); Erratum Phys.Rev. C54, 1500 (1996) A.Parreno, A.Ramos, C.Bennhold Role of the ρ Meson in the Nonmesionic Hypernuclear Decay NUCLEAR STRUCTURE A=12; calculated ρ-, π-exchange contribution to (Λ)N-, NN-decay rate in hypernucleus 12C(Λ); deduced ρ-exchange central potential role.
doi: 10.1103/PhysRevC.52.R1768
1995RA05 Nucl.Phys. A585, 375c (1995) Non Mesonic Hypernuclear Decay in a Weak Meson Exchange Model NUCLEAR STRUCTURE A=12; calculated nonmesonic rate, Γn/Γp, asymmetry parameter, hypernucleus. A=5; A=11; calculated asymmetry parameter, hypernucleus.
doi: 10.1016/0375-9474(94)00616-U
1994LE20 Phys.Rev. C50, R1283 (1994) F.X.-D.Lee, L.E.Wright, C.Bennhold Exclusive Pion Radiative Capture from Nuclei in the Δ Region NUCLEAR REACTIONS 16O(π+, p), E=160, 220 MeV; analyzed σ(Eγ, θγ, Ep) data; deduced 16O(γ, π-p) reaction implications. Nonlocal DWIA.
doi: 10.1103/PhysRevC.50.R1283
1994RA24 Nucl.Phys. A577, 287c (1994) Weak Decay of Polarized (Lambda) Hypernuclei NUCLEAR STRUCTURE A=12; calculated hypernucleus 12C(lambda) decay Γn/Γp, asymmetry parameter. Relativistic model, nonmesonic lambda hypernuclei decay.
doi: 10.1016/0375-9474(94)90869-9
1994TI06 Nucl.Phys. A580, 455 (1994) L.Tiator, C.Bennhold, S.S.Kamalov The (Eta)NN Coupling in Eta Photoproduction NUCLEAR REACTIONS 1H(γ, X), E=708-780 MeV; calculated σ(θ), σ(E) for eta production, polarization observables. Effective lagrangian approach.
doi: 10.1016/0375-9474(94)90909-1
1993KA06 Phys.Rev. C47, 941 (1993) S.S.Kamalov, L.Tiator, C.Bennhold Pion Interaction with the Trinucleon Up to the Eta Production Threshold NUCLEAR REACTIONS 3He(π+, π+), (π-, π-), E=100-500 MeV; calculated σ(θ), asymmetry vs θ. 2H(π+, π+), E=180-300 MeV; calculated σ(θ). 3He(π-, X), E=555-680 MeV; calculated σ(θ), target asymmetry vs θ for eta production. 3He(π-, π0), E=100-500 MeV; calculated target asymmetry vs θ.
doi: 10.1103/PhysRevC.47.941
1993LI21 Phys.Rev. C48, 816 (1993) Exclusive Quasifree Pion Photoproduction on Complex Nuclei in the Δ Region NUCLEAR REACTIONS 12C(γ, π-p), E=380 MeV; 16O(γ, π-p), E=360 MeV; calculated σ(Ep, θp, θπ), photon asymmetry. DWIA, momentum space.
doi: 10.1103/PhysRevC.48.816
1992BE02 Phys.Rev. C45, 947 (1992) C.Bennhold, A.Ramos, D.A.Aruliah, U.Oelfke Nonmesonic Weak Decay of the Hypertriton NUCLEAR STRUCTURE A=3; calculated hypertriton nonmesonic decay; deduced (lambda-deuteron) bound system role, decay rate compared to free lambda-decay.
doi: 10.1103/PhysRevC.45.947
1992BE13 Nucl.Phys. A540, 621 (1992) C.Bennhold, B.K.Jennings, L.Tiator, S.S.Kamalov The Asymmetry in π-3He Scattering NUCLEAR REACTIONS 3He(π+, π+), E=100-260 MeV; analyzed asymmetry data. Optical potential, realistic Faddeev wave functions, polarized target.
doi: 10.1016/0375-9474(92)90176-K
1992BE16 Phys.Rev. C45, 3017 (1992) Partial Transitions in the Nonmesonic Decay of Hypernuclei NUCLEAR STRUCTURE A=12; calculated nonmesonic partial, total decay rates of 12C(lambda). Hypernuclei, partial transitions.
doi: 10.1103/PhysRevC.45.3017
1992BE41 Phys.Rev. C46, 2456 (1992) C.Bennhold, L.Tiator, S.S.Kamalov, R.Mach Electromagnetic and Pion-Nuclear Reactions on 15N NUCLEAR REACTIONS 15N(π+, π0), E=30, 48 MeV; calculated σ(θ). 15N(γ, π-), E=170 MeV; calculated σ(θ). 15N(e, e), E not given; calculated M1 form factor; deduced higher configurations role. Shell model.
doi: 10.1103/PhysRevC.46.2456
1992BE59 Nucl.Phys. A547, 79c (1992) Photo- and Electroproduction of Strangeness NUCLEAR REACTIONS 1H(γ, K+), E=0.9-3 GeV; calculated σ(E), lambda polarization. 28Si, 56Fe, 89Y, 16O(γ, K+), E=1.5 GeV; calculated σ(θ), lambda polarization. 2H(γ, K+), E=1.5 GeV; 2H(γ, K0p), E not given; calculated σ(θ(K), θp, p(p)). 1H(e, e'K+), E not given; calculated σ. Different phenomenological approaches.
doi: 10.1016/0375-9474(92)90712-S
1992KA31 Nucl.Phys. A547, 599 (1992) S.S.Kamalov, L.Tiator, C.Bennhold Polarization Observables in Pion Photoproduction on 3He NUCLEAR REACTIONS 3He(γ, π+), E=200-500 MeV; calculated σ(θ), photon asymmetry, polarization observables vs θ. Three-body Faddeev amplitude, nonlocal coupled-channels framework.
doi: 10.1016/0375-9474(92)90653-2
1992KO02 Phys.Rev. C45, 230 (1992) D.Koetsier, K.Amos, L.Tiator, C.Bennhold, L.E.Wright Photopion Cross Sections and Mass 14 Structures NUCLEAR REACTIONS 14N(γ, π+), E=173, 200 MeV; calculated σ(θ); deduced core polarization effects role.
doi: 10.1103/PhysRevC.45.230
1992LI04 Phys.Rev. C45, 2011 (1992) Kaon Photoproduction on the Neutron Using Deuterium NUCLEAR REACTIONS 2H(γ, X), E=1.5 GeV; calculated σ(θp, θ(K)) vs proton, kaon momentum. Impulse approximation, kaon photoproduction.
doi: 10.1103/PhysRevC.45.2011
1992RA16 Nucl.Phys. A544, 703 (1992) A.Ramos, E.van Meijgaard, C.Bennhold, B.K.Jennings Asymmetries in the Weak Decay of Polarized Hypernuclei NUCLEAR STRUCTURE A=5, 11, 12; calculated hypernuclei decay rates, polarization observables. Relativistic model, nonmesonic weak decay.
doi: 10.1016/0375-9474(92)90538-U
1992RA32 Nucl.Phys. A547, 103c (1992) A.Ramos, C.Bennhold, E.van Meijgaard, B.K.Jennings Proton Asymmetry in the Weak Decay of Polarized Hypernuclei NUCLEAR STRUCTURE A=12; calculated proton polarization following hypernuclear decay. Relativistic model.
doi: 10.1016/0375-9474(92)90715-V
1991BE01 Phys.Rev. C43, 775 (1991) Electromagnetic Production of Polarization in Hypernuclei NUCLEAR REACTIONS 16O(γ, K+), E=1.1-2 GeV; 28Si, 56Fe, 89Y(γ, K+), E=1.5 GeV; calculated σ(θ), polarization vs θ for hypernuclei production.
doi: 10.1103/PhysRevC.43.775
1991BE14 Phys.Rev. C43, 2742 (1991) C.Bennhold, L.Tiator, A.M.Bernstein, S.S.Kamalov 0+ - 0+ Transition in Charged Photopion Reactions NUCLEAR REACTIONS 14C(γ, π-), E=200 MeV; calculated σ(θ); deduced non-spin-flip term role in 0+ → 0+ transition.
doi: 10.1103/PhysRevC.43.2742
1991BE22 Nucl.Phys. A530, 625 (1991) Coherent and Incoherent (eta)-Photoproduction from Nuclei NUCLEAR REACTIONS 4He, 12C, 40Ca(γ, X), E < 800 MeV; 12C, 10B, 6Li(γ, X), E=650 MeV; calculated coherent, incoherent eta production σ(θ). DWIA.
doi: 10.1016/0375-9474(91)90772-X
1991KA18 Phys.Lett. 259B, 410 (1991) S.S.Kamalov, C.Bennhold, R.Mach 2p-Shell Admixtures in Pion Single Charge Exchange on 13C NUCLEAR REACTIONS 13C(π+, π0), E=30-240; calculated σ(θ). 2p-shell admixtures.
doi: 10.1016/0370-2693(91)91648-F
1991KA32 Few-Body Systems 10, 143 (1991) S.S.Kamalov, L.Tiator, C.Bennhold Pion Photoproduction on 3He Including Final-State Interaction NUCLEAR REACTIONS 3He(π+, π+), (π-, π-), E=50, 100 MeV; calculated σ(θ). 3He(π+, π+), (π-, π-), E=200 MeV; calculated spin-flip, nonspin-flip σ(θ). Faddeev wave functions, full nonlocal DWIA.
doi: 10.1007/BF01076291
1991LA09 Phys.Rev.Lett. 67, 3356 (1991) B.Larson, O.Hausser, E.J.Brash, C.Chan, A.Rahav, C.Bennhold, P.P.J.Delheij, R.S.Henderson, B.K.Jennings, A.Mellinger, D.Ottewell, A.Trudel, M.C.Vetterli, D.M.Whittal, S.Ram, L.Tiator, S.S.Kamalov Asymmetries in Elastic Scattering of 100 MeV π+ from a Polarized 3He Target NUCLEAR REACTIONS 3He(π+, π+), E=100 MeV; measured σ(θ), analyzing power. Full nonlocal DWIA, realistic three-body Faddeev wave functions. Polarized target.
doi: 10.1103/PhysRevLett.67.3356
1991RA21 Phys.Lett. 264B, 233 (1991) A.Ramos, C.Bennhold, E.van Meijgaard, B.K.Jennings Non-Mesonic Weak Decay of 12C(Lambda) NUCLEAR STRUCTURE A=12; calculated hypernuclear nonmesonic decay rate. Relativistic model.
doi: 10.1016/0370-2693(91)90340-V
1990BE12 Phys.Lett. 238B, 31 (1990) E0 Suppression in Pion Photoproduction on 13C NUCLEAR REACTIONS 13C(γ, π-), E ≈ 160-320 MeV; calculated pion photoproduction σ(θ) vs E; deduced E0 suppression features.
doi: 10.1016/0370-2693(90)92095-Z
1990BE21 Phys.Lett. 243B, 13 (1990) Low-Energy Eta Photoproduction from Nucleons and Nuclei NUCLEAR REACTIONS 1H(γ, X), E=750, 800 MeV; 4He(γ, X), E=650 MeV; calculated eta production σ(θ). 4He, 12C, 40Ca(γ, X), E=600-740 MeV; calculated eta production σ(E).
doi: 10.1016/0370-2693(90)90947-5
1990BE24 Phys.Rev. C42, 464 (1990) Comment on ' Wave Function of 14N ' NUCLEAR REACTIONS 14N(γ, π+), E=173, 200 MeV; 14N(e, e'), E not given; calculated σ(θ), M1 form factors. Phenomenological vs shell model wave functions.
doi: 10.1103/PhysRevC.42.464
1990BE30 Phys.Rev. C42, 775 (1990) Radiative Kaon Capture on Nuclei NUCLEAR REACTIONS 16O(K-, γ), E at 800 MeV/c; calculated σ(θ). Feynman diagrams, elementary operator.
doi: 10.1103/PhysRevC.42.775
1990BE45 Nucl.Phys. A519, 805 (1990) The E0 Transition in Pion Photoproduction and Radiative Pion Capture on 13C NUCLEAR REACTIONS 13C(γ, π-), E=160-320 MeV; calculated σ(θ) vs E. 13C(π+, γ), E=115.5 MeV; calculated σ(θ). Nonlocal DWIA, extended shell model space. NUCLEAR STRUCTURE 13C; calculated magnetic form factor. Extended shell model space.
doi: 10.1016/0375-9474(90)90436-P
1990BE49 Can.J.Phys. 68, 1270 (1990) C.Bennhold, L.Tiator, L.E.Wright Low-Energy Pion Photoproduction from p-Shell Nuclei NUCLEAR REACTIONS 6Li, 10B(γ, π+), E=200 MeV; 14N(γ, π+), E=173 MeV; calculated σ(θ(π)). Improved DWIA, Feynman diagram based production operator.
doi: 10.1139/p90-183
1990SO06 Nucl.Phys. A517, 473 (1990) K.C.So, K.Min, L.Y.Murphy, E.J.Winhold, M.Yamazaki, P.Yergin, R.W.Gothe, B.Schoch, C.Bennhold, L.Tiator, S.J.Hall, J.D.Kellie, I.J.D.MacGregor, R.O.Owens, D.Branford Spin-Isospin Excitation in 12C(γ, π+)12B(*) using Tagged Photons NUCLEAR REACTIONS 12C(γ, π+), E=176-182 MeV; measured σ(Eπ, θπ); deduced photopion production σ(θ). 12B deduced levels. Natural target, tagged photon beam.
doi: 10.1016/0375-9474(90)90212-5
1989BE02 Phys.Rev. C39, 927 (1989) Kaon Photoproduction from Nuclei in a Relativistic Nuclear Model NUCLEAR REACTIONS 40Ca, 208Pb(γ, K+), E=1.2 GeV; calculated σ(θ). Relativistic DWIA.
doi: 10.1103/PhysRevC.39.927
1989BE11 Phys.Rev. C39, 1944 (1989) Electromagnetic Production of Σ Hypernuclei NUCLEAR REACTIONS 1H(γ, K+), E=1.157, 1.45 GeV; calculated σ(θ). 1H(γ, K+), E=1-2 GeV; calculated σ(E).
doi: 10.1103/PhysRevC.39.1944
1989KO32 Nuovo Cim. 102A, 193 (1989) K+(Lambda) Photoproduction Amplitudes Incorporating Absorptive Effects and Hypernuclear Formation NUCLEAR REACTIONS 1H(γ, K+), E=0.9-3 GeV; calculated σ(E). 16O(γ, K+), E=1.3 GeV; calculated σ(θ); deduced Lambda photoproduction amplitudes.
doi: 10.1007/BF02735106
1989TA04 Phys.Rev. C39, 741 (1989) Absorptive Effects in K+(Lambda) Photoproduction on Nucleons and Nuclei NUCLEAR REACTIONS 16O(γ, K+), E=1.3 GeV; calculated hypernuclear formation σ(θ).
doi: 10.1103/PhysRevC.39.741
1989TI02 Nucl.Phys. A501, 751 (1989) L.Tiator, C.Bennhold, R.Neuhausen Inelastic Electron Scattering and Pion Photoproduction on 12C NUCLEAR REACTIONS 12C(e, e'), E=350 MeV; measured σ(E, θ); deduced form factors, nuclear structure coefficients, 12C(γ, π+) reaction σ(θ). Non-local DWIA.
doi: 10.1016/0375-9474(89)90159-0
1988YA10 Phys.Rev. C38, 923 (1988) Yanhe Jin, L.E.Wright, C.Bennhold, D.S.Onley 14C Beta Decay and the 14N M1 Form Factors NUCLEAR REACTIONS 14N(e, e'), E not given; calculated M1 transition form factors. Relativistic wave functions. NUCLEAR STRUCTURE 14C(β-); calculated β-decay rate. Relativistic wave functions.
doi: 10.1103/PhysRevC.38.923
1987BE11 Phys.Rev. C36, 438 (1987) Pseudovector versus Pseudoscalar Theory in Kaon Photoproduction from Nucleons and Nuclei NUCLEAR REACTIONS 12C(γ, K+), E=2 GeV; calculated σ(θ) for 12B level; deduced pseudovector, pseudoscalar coupling constants.
doi: 10.1103/PhysRevC.36.438
1987BE14 Phys.Lett. 191B, 11 (1987) Relativistic Effects in Kaon Photoproduction from 12C NUCLEAR REACTIONS 12C(K-, γ), E=1.5, 2 GeV; calculated 12B formation σ(θ). Relativistic impulse approximation.
doi: 10.1016/0370-2693(87)91312-8
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