NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = W.M.Kloet Found 36 matches. 2004EL11 Phys.Rev. C 70, 034001 (2004) Relativistic treatment of pion wave functions in the annihilation (p-bar)p → π-π+ NUCLEAR REACTIONS 1H(p-bar, π+π-), E not given; calculated pion wave functions. Constituent quark model.
doi: 10.1103/PhysRevC.70.034001
2004EL12 Phys.Rev. C 70, 034002 (2004) Relativistic effects and angular dependence in the reaction (p-bar)p → π-π+ NUCLEAR REACTIONS 1H(p-bar, π+π-), E=66.7-803.1 MeV; analyzed σ(θ), analyzing power; deduced relativistic effects.
doi: 10.1103/PhysRevC.70.034002
2003EL04 Phys.Rev. C 68, 014003 (2003) B.El-Bennich, W.M.Kloet, B.Loiseau Annihilation range and final-state interaction in (p-bar)p annihilation into π-π+ NUCLEAR REACTIONS 1H(p-bar, π+π-), E at 360-1550 MeV/c; analyzed σ(θ), analyzing powers; deduced role of final-state interactions, other reaction mechanism features.
doi: 10.1103/PhysRevC.68.014003
2000KL01 Phys.Rev. C61, 015501 (2000) Constraints on Vector Meson Photoproduction Spin Observables
doi: 10.1103/PhysRevC.61.015501
2000KL04 Nucl.Phys. A663-664, 425c (2000) Constraints in Vector Meson Photoproduction
doi: 10.1016/S0375-9474(99)00674-0
2000KL08 Nucl.Phys. A675, 325c (2000) Vector Meson Photoproduction - Model Independent Aspects
doi: 10.1016/S0375-9474(00)00275-X
1998KL04 Eur.Phys.J. A 1, 337 (1998) ππ Scattering and the Meson Resonance Spectrum
doi: 10.1007/s100500050067
1998KL05 Nucl.Phys. A631, 538c (1998) Elastic ππ Scattering up to 2 GeV and the Meson Resonance Spectrum
doi: 10.1016/S0375-9474(98)00063-3
1998KL08 Phys.Rev. C58, 1086 (1998) W.M.Kloet, W.-T.Chiang, F.Tabakin Spin Information from Vector-Meson Decay in Photoproduction
doi: 10.1103/PhysRevC.58.1086
1998KL22 Acta Phys.Pol. B29, 3331 (1998) W.M.Kloet, W.-T.Chiang, F.Tabakin Spin Self-Analysis of Photoproduced Meson and Baryon Resonances
1997KL02 Z.Phys. A358, 423 (1997) Comparing the p(bar)p → K-K+ and p(bar)p π-π+ Reactions NUCLEAR REACTIONS 1H(p-bar, X), E at 360-988 MeV/c; analyzed σ(θ), analyzing power vs θ for K-K+-, π-π+-production; deduced partial wave amplitude parameters.
doi: 10.1007/s002180050350
1996KL11 Acta Phys.Pol. B27, 2871 (1996) Comparing (p-bar)p → π-π+ and (p-bar)p → K-K+
1995KL05 Z.Phys. A353, 227 (1995) The ππ S-Wave in the 1 to 2 GeV Region from a ππ, (K-bar)K and ρρ(ωω) Coupled Channel Model
doi: 10.1007/BF01295901
1993BA13 Phys.Rev. C47, 2207 (1993) Left-Right Asymmetry in (p-bar)p → π-π+ NUCLEAR REACTIONS 1H(p-bar, X), E at 497 MeV/c; analyzed σ(θ), analyzing power data. Quark, nucleon exchange models.
doi: 10.1103/PhysRevC.47.2207
1991KL01 Phys.Rev. C43, 1575 (1991) Correlation Between the Elastic NN Phase and the Inelastic Analyzing Power NUCLEAR REACTIONS 1H(polarized p, pπ+), E=0.8 GeV; calculated σ, analyzing power vs proton momentum; deduced 3F3 nucleon-nucleon phase parameter role.
doi: 10.1103/PhysRevC.43.1575
1990FR13 Phys.Rev. C42, 1838 (1990) J.L.Friar, B.F.Gibson, G.Berthold, W.Glockle, Th.Cornelius, H.Witala, J.Haidenbauer, Y.Koike, G.L.Payne, J.A.Tjon, W.M.Kloet Benchmark Solutions for a Model Three-Nucleon Scattering Problem NUCLEAR REACTIONS 2H(n, n), E=4-42 MeV; calculated s-wave scattering parameters. Three-nucleon problem, single model interaction.
doi: 10.1103/PhysRevC.42.1838
1990KL02 Phys.Rev. C41, 2263 (1990) W.M.Kloet, R.R.Silbar, J.A.Tjon Parity-Violating Asymmetry in p(pol)p Scattering at Medium Energies NUCLEAR REACTIONS 1H(p, X), E ≤ 1 GeV; calculated longitudinal asymmetry; deduced parity-violation. Polarized target.
doi: 10.1103/PhysRevC.41.2263
1989SI18 Phys.Rev. C40, 2218 (1989) R.R.Silbar, W.M.Kloet, L.S.Kisslinger, J.Dubach Pion-Exchange Contribution to the Parity-Violating Asymmetry in p(pol)p Scattering NUCLEAR REACTIONS 1H(polarized p, p), E=200-1000 MeV; calculated parity violating asymmetry vs E; deduced pion-exchange contribution.
doi: 10.1103/PhysRevC.40.2218
1987DU03 Nucl.Phys. A466, 573 (1987) J.Dubach, W.M.Kloet, R.R.Silbar NN → NNπ at Intermediate Energies: Predictions of a unitary model NUCLEAR REACTIONS 1H(p, pπ+), (p, pπ0), (n, pπ-), (p, pX), (p, nX), E=800 MeV; calculated σ(Ep, θp, θπ), spin observables, σ(Ep, θp), σ(En, θn). Unitary model.
doi: 10.1016/0375-9474(87)90458-1
1987RI06 Phys.Lett. 197B, 23 (1987) P.J.Riley, M.Bachman, C.L.Hollas, K.H.McNaughton, S.-W.Xu, B.E.Bonner, O.B.Van Dyck, J.McGill, M.W.McNaughton, J.C.Peng, R.R.Silbar, J.Dubach, W.M.Kloet Polarization Observables for the Reaction pp → ppπ0 at 800 MeV NUCLEAR REACTIONS 1H(polarized p, pπ0), E=647, 733, 800 MeV; measured induced polarization, analyzing power, Wolfenstein parameters. Orthogonal beam polarization.
doi: 10.1016/0370-2693(87)90334-0
1986DU01 Phys.Rev. C33, 373 (1986) J.Dubach, W.M.Kloet, R.R.Silbar Nucleon-Nucleon Final-State Interactions in NN → NNπ NUCLEAR REACTIONS 1H(p, pπ+), (polarized p, pπ+), E=800 MeV; calculated σ(θp, θ(π)), spin observables, spin-spin correlation parameter vs proton momentum.
doi: 10.1103/PhysRevC.33.373
1986DU08 Phys.Rev. C34, 944 (1986) J.Dubach, W.M.Kloet, R.R.Silbar, J.A.Tjon, E.van Faassen Model Dependence of Unitary Isobar Model Treatments of NN → NN(π) at Intermediate Energies NUCLEAR REACTIONS 1H(polarized p, π+), E=800 MeV; calculated σ(θp, θ(π)) vs proton momentum, spin observables vs θ; deduced dibaryon resonance role. Unitary isobar model.
doi: 10.1103/PhysRevC.34.944
1985HO16 Phys.Rev.Lett. 55, 29 (1985) C.L.Hollas, K.H.McNaughton, P.J.Riley, Shen-wu Xu, B.E.Bonner, O.B.van Dyck, J.McGill, M.W.McNaughton, J.C.Peng, R.R.Silbar, J.Dubach, W.M.Kloet Wolfenstein Polarization Observables for the Reaction p(pol)p → p(pol)πn at 800 MeV NUCLEAR REACTIONS 1H(polarized p, pπ+), E=650, 733, 800 MeV; measured Wolfenstein polarization parameters, induced polarization, σ(θ1, θ2) vs proton momentum.
doi: 10.1103/PhysRevLett.55.29
1983BH07 Phys.Rev. C28, 2071 (1983) T.S.Bhatia, J.G.J.Boissevain, J.J.Jarmer, R.R.Silbar, J.E.Simmons, G.Glass, J.C.Hiebert, R.A.Kenefick, L.C.Northcliffe, W.B.Tippens, W.M.Kloet, J.Dubach Analyzing Powers and Spin Correlations A(NN) and A(LL) for pp → npπ+ at 650 and 800 MeV NUCLEAR REACTIONS 1H(polarized p, pπ), E=800, 650 MeV; measured analyzing power, spin correlation vs proton momentum. Born approximation calculations.
doi: 10.1103/PhysRevC.28.2071
1983KL01 Nucl.Phys. A392, 271 (1983) Nucleon-Nucleon Resonance Behavior in an Exactly Soluble Model NUCLEAR REACTIONS 1H(p, p), E=0.4-1 GeV; calculated phase shifts, inelasticity parameters. Soluble coupled-channel model.
doi: 10.1016/0375-9474(83)90126-4
1983KL05 Phys.Rev. C27, 2529 (1983) W.M.Kloet, B.F.Gibson, G.J.Stephenson, Jr., E.M.Henley Parity Nonconserving Asymmetry in Neutron-Deuteron and Proton-Deuteron Scattering NUCLEAR REACTIONS 2H(polarized p, p), (polarized n, p), E=14-40 MeV; calculated σ(E), parity nonconserving asymmetry.
doi: 10.1103/PhysRevC.27.2529
1981DU17 Phys.Lett. 106B, 29 (1981) J.Dubach, W.M.Kloet, A.Cass, R.R.Silbar Exclusive Spin-Dependent Pion Production in Medium-Energy Nucleon-Nucleon Collisions: The role of unitarity NUCLEAR REACTIONS 1H(polarized p, π+p), E=800 MeV; calculated asymmetry vs θp, θ(π). Unitarity, relativistic model dynamics.
doi: 10.1016/0370-2693(81)91073-X
1979BO19 Phys.Rev. C20, 879 (1979) D.I.Bonbright, A.M.McDonald, W.T.H.van Oers, J.W.Watson, H.S.Caplan, J.M.Cameron, J.G.Rogers, J.Soukup, W.M.Kloet, C.Stolk, J.A.Tjon Noncoplanar 2H(p, 2p)n Reaction NUCLEAR REACTIONS 2H(p, 2p), E=23.0, 39.5 MeV; measured two types of constant-relative-energy loci. Faddeev calculations, Reid soft-core potentials.
doi: 10.1103/PhysRevC.20.879
1977HA03 Phys.Rev. C15, 404 (1977) Trinucleon Charge Form Factor NUCLEAR STRUCTURE 3He, 3H; calculated charge form factors; pair, recoil exchange currents included; effect of πNN vertex function; dependen ce onn nuclear force; six two-body forces, two three-body forces.
doi: 10.1103/PhysRevC.15.404
1977KL07 Phys.Rev.Lett. 39, 1392 (1977) W.M.Kloet, B.F.Gibson, G.J.Stephenson, Jr., E.M.Henley Parity-Nonconserving Asymmetry in n-d Scattering NUCLEAR REACTIONS 2H(polarized n, X), E=14.4 MeV; calculated weak parity-nonconserving asymmetry in total σ.
doi: 10.1103/PhysRevLett.39.1392
1976KL02 Phys.Lett. 61B, 356 (1976) Recoil and Strong Formfactor Effects in Mesonic Exchange Corrections on the Charge Distribution of 3He and 3H NUCLEAR STRUCTURE 3He, 3H; calculated charge form factors.
doi: 10.1016/0370-2693(76)90587-6
1976WI04 Nucl.Phys. A261, 13 (1976) B.J.Wielinga, J.R.Balder, G.J.F.Blommestijn, R.Van Dantzig, W.M.Kloet, J.A.Tjon, I.Slaus A '4π-Type' Study of the Reaction p(d, pp)n at Ed = 26.5 MeV NUCLEAR REACTIONS 1H(d, d), E=26.5 MeV; measured σ(θ). 1H(d, 2p), E=26.5 MeV; measured σ.
doi: 10.1016/0375-9474(76)90038-5
1975MC04 Phys.Rev.Lett. 34, 488 (1975) A.M.McDonald, D.I.Bonbright, W.T.H.van Oers, J.W.Watson, J.G.Rogers, J.M.Cameron, J.Soukup, W.M.Kloet, J.A.Tjon 2H(p, 2p)n Cross Sections for Constant NN Relative Energies NUCLEAR REACTIONS 2H(p, 2p), E=39.5 MeV; measured pp-coin, Ep, σ.
doi: 10.1103/PhysRevLett.34.488
1974KL04 Phys.Lett. 49B, 419 (1974) Meson Exchange Effects on the Charge Form Factors of the Tri-Nucleon System NUCLEAR STRUCTURE 3H, 3He; calculated charge form factor.
doi: 10.1016/0370-2693(74)90623-6
1974WI18 Lett.Nuovo Cim. 11, 655 (1974) B.J.Wielinga, J.R.Balder, R.Van Dantzig, I.Slaus, W.M.Kloet, J.A.Tjon Where Does the Local-Potential Model Differ from the H(d, 2p)n Data at E = 26.5 MeV NUCLEAR REACTIONS 1H(d, 2p), E=26.5 MeV; measured σ(θ).
doi: 10.1007/BF02763139
1971KL08 Phys.Lett. 37B, 460 (1971) Neutron-Deuteron Scattering with Local Potentials NUCLEAR REACTIONS 2H(n, n), E=14.1 MeV; calculated σ(θ). Pade approximation.
doi: 10.1016/0370-2693(71)90344-3
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