NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = R.R.Silbar Found 31 matches. 2012GO02 Phys.Rev. C 85, 015203 (2012) Charmed mesons have no discernible color-Coulomb attraction
doi: 10.1103/PhysRevC.85.015203
2008GO16 Phys.Rev. C 77, 065203 (2008) Effect of pion exchange in a relativistic quark model of baryons
doi: 10.1103/PhysRevC.77.065203
2002GO29 Phys.Rev. D66, 056001 (2002) A.S.Goldhaber, T.Goldman, R.R.Silbar Effect of hadron dynamics on the proton lifetime NUCLEAR STRUCTURE 1H; calculated hadron dynamics effects on decay rate.
doi: 10.1103/PhysRevD.66.056001
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
1989SH26 Phys.Rev. C40, 2203 (1989) R.L.Shypit, D.V.Bugg, A.H.Sanjari, D.M.Lee, M.W.McNaughton, R.R.Silbar, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis Spin Dependence of pp → npπ+ from 492 to 796 MeV NUCLEAR REACTIONS 1H(polarized p, pπ+), E=492-796 MeV; measured spin correlation parameters; deduced no dibaryon evidence. Longitudinally polarized target.
doi: 10.1103/PhysRevC.40.2203
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
1988SH06 Phys.Rev.Lett. 60, 901 (1988) R.L.Shypit, D.V.Bugg, D.M.Lee, M.W.McNaughton, R.R.Silbar, N.M.Stewart, A.S.Clough, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis Evidence against Broad Dibaryons NUCLEAR REACTIONS 1H(polarized p, π+n), E=492-796 MeV; measured spin correlation parameters; deduced no broad dibaryons. Isobar analysis.
doi: 10.1103/PhysRevLett.60.901
1988SH09 Nucl.Phys. A477, 541 (1988) R.L.Shypit, D.V.Bugg, D.M.Lee, M.W.McNaughton, R.R.Silbar, N.M.Stewart, A.S.Clough, C.L.Hollas, K.H.McNaughton, P.Riley, C.A.Davis A(SL), A(LL) and A(N0) for NN → πD at 492, 729 and 796 MeV NUCLEAR REACTIONS 1H(polarized p, π+), E=492-796 MeV; measured spin correlation parameters A(LL), A(SL), A(N0). Longitudinally polarized propanediol target.
doi: 10.1016/0375-9474(88)90404-6
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
1985MI04 Phys.Rev.Lett. 54, 1237 (1985) C.Milner, M.Barlett, G.W.Hoffmann, S.Bart, R.E.Chrien, P.Pile, P.D.Barnes, G.B.Franklin, R.Grace, H.S.Plendl, J.F.Amann, T.S.Bhatia, T.Kozlowski, J.C.Peng, R.R.Silbar, H.A.Thiessen, C.Glashausser, J.A.McGill, R.Hackenburg, E.V.Hungerford, R.L.Stearns Observation of Lambda-Hypernuclei in the Reaction 12C(π+, K+)12C(Lamdba) NUCLEAR REACTIONS 12C(π+, K+), E at 716, 728 MeV/c; measured σ(θ); deduced 12C hypernuclear levels.
doi: 10.1103/PhysRevLett.54.1237
1985SI26 J.Phys.(Paris), Colloq.C-2, 389 (1985) Theoretical Aspects of the Nucleon-Nucleon Workshop NUCLEAR REACTIONS 1H(p, π+n), E=0.3-1.4 GeV; analyzed σ(Ep, θp, θπ), asymmetry data. 1H(p, n), E=800 MeV; analyzed spin transfer coefficient data.
1984SI03 Phys.Rev. C29, 1116 (1984); Erratum Phys.Rev.C30, 1365 (1984) Isospin Dependence of Pion Absorption on Nucleon Pairs NUCLEAR REACTIONS 3,4He(π-, pn), (π+, 2p), E at rest to resonance; calculated σ(θ), ratio; deduced nucleon pair absorption isospin dependence. Unitary isobar model.
doi: 10.1103/PhysRevC.29.1116
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
1982LO11 Phys.Rev. C26, 586 (1982) D.G.Long, M.M.Sternheim, R.R.Silbar Simplified Intranuclear Cascade Approach to Inclusive (p, π-xn) Reaction near Threshold NUCLEAR REACTIONS 209Bi(p, xnπ-), E=175-220 MeV; calculated σ(E) inclusive. Intranuclear cascade model, nucleon, pion charge exchange.
doi: 10.1103/PhysRevC.26.586
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
1981ST14 Phys.Rev. C24, 574 (1981) (π, πn) Puzzle above the (3, 3) Resonance NUCLEAR REACTIONS 12C(π+, πp), (π+, πn), (π-, πp), (π-, πn), E=40-1000 MeV; calculated σ(π+)/σ(π-). Impulse approximation, Pauli principle, Fermi motion, pion production corrections, final state effects.
doi: 10.1103/PhysRevC.24.574
1980SH02 Nucl.Phys. A333, 461 (1980) T.C.Sharma, L.W.Swenson, K.S.Krane, P.Varghese, D.K.McDaniels, H.A.Thiessen, N.Tanaka, R.R.Silbar, M.Greenfield, C.F.Moore Proton Yields from Quasielastic Pion Scattering on 27Al and 208Pb NUCLEAR REACTIONS 27Al, 208Pb(π+, π+p), (π-, π-p), E=255 MeV; measured σ(Ep, θp); deduced σ ratio. Semi-classical nucleon charge exchange model.
doi: 10.1016/0375-9474(80)90110-4
1980ST07 Phys.Rev. C21, 1974 (1980) Interpretation of Quasielastic Pion Scattering Coincidence Experiments NUCLEAR REACTIONS 12C, 27Al, 208Pb(π+, π+p), (π-, π-p), E=180, 190, 255 MeV; analyzed pion-nucleon coin data. Impulse approximation, recoil nucleon charge exchange.
doi: 10.1103/PhysRevC.21.1974
1979KR14 Phys.Rev. C20, 1873 (1979) K.S.Krane, T.C.Sharma, L.W.Swenson, D.K.McDaniels, P.Varghese, B.E.Wood, R.R.Silbar, H.D.Wohlfahrt, C.A.Goulding Energetic Charged-Particle Spectrum Following μ- Capture by Nuclei NUCLEAR REACTIONS Al, Cu, Pb(μ-, X), E=0; measured charged-particle spectrum, σ(E).
doi: 10.1103/PhysRevC.20.1873
1977SI01 Phys.Rev. C15, 371 (1977) R.R.Silbar, J.N.Ginocchio, M.M.Sternheim Dramatic Nuclear Structure Effects in (π, πN) Reactions NUCLEAR REACTIONS 11B, 12C, 16,17,18O, 19F, 31P, 58,60,62,64Ni, 64,66,68,70Zn(π, X), E ≈ 190 MeV; calculated pion induced nucleon knockout σ.
doi: 10.1103/PhysRevC.15.371
1977SI03 Phys.Rev. C15, 1158 (1977) Neutron Removal from 7Li by π± NUCLEAR REACTIONS 7Li(π+, π+n), (π+, π+p), E=50-290 MeV; calculated nucleon charge exchange probabilities.
doi: 10.1103/PhysRevC.15.1158
1977ST27 Phys.Rev. C16, 2059 (1977) Neutron and Proton Knockout from 19F and 27Al by Negative Pions NUCLEAR REACTIONS 19F, 27Al(π-, π-n), (π-, π-p), (π-, π0n), E=200 MeV; calculated neutron/proton knockout.
doi: 10.1103/PhysRevC.16.2059
1975SI10 Phys.Rev. C11, 1610 (1975) Quasielastic Pion Scattering in the (3, 3) Resonance Region NUCLEAR REACTIONS 12C, 63Cu, 208Pb(π, π'), E=100-400 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.11.1610
1975SI18 Phys.Rev. C12, 341 (1975) (π, πN) Puzzle: Effects of Pion Charge Exchange NUCLEAR REACTIONS 12C(π+, X), (π-, X), E=50-300 MeV; calculated pion charge exchange.
doi: 10.1103/PhysRevC.12.341
1974SP07 Phys.Rev. C10, 2215 (1974) D.A.Sparrow, M.M.Sternheim, R.R.Silbar Semiclassical Model for Pion Production by Neutrons on Nuclei NUCLEAR REACTIONS Al, Cu, Pb(p, π+), (p, π-), (n, π+), (n, π-), (p, γ), (n, γ); calculated σ.
doi: 10.1103/PhysRevC.10.2215
1973SI23 Phys.Rev. C8, 492 (1973) Nuclear Effects in the Production of π+ and π- by Protons on Nuclei NUCLEAR REACTIONS 27Al, 63Cu, 208Pb(p, π+), (p, π-); measured nothing, calculated production σ of π+, π-.
doi: 10.1103/PhysRevC.8.492
1972SI24 Phys.Rev. C6, 764 (1972) Model Dependence of Pion-Nucleus Total Cross Sections
doi: 10.1103/PhysRevC.6.764
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