NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = R.M.Woloshyn Found 31 matches. 2016WO09 Eur.Phys.J. A 52, 273 (2016) Excitations of strange bottom baryons
doi: 10.1140/epja/i2016-16273-0
2007AB20 Eur.Phys.J. A 31, 773 (2007) A.M.Abdel-Rehim, R.Lewis, R.M.Woloshyn, J.M.S.Wu Lattice QCD with a twisted mass term and a strange quark
doi: 10.1140/epja/i2006-10245-y
2003LE03 Phys.Rev. D 67, 013003 (2003) R.Lewis, W.Wilcox, R.M.Woloshyn Nucleon's strange electromagnetic and scalar matrix elements NUCLEAR STRUCTURE 1n, 1H; calculated strangeness matrix elements. Quenched lattice QCD, quenched chiral perturbation theory, comparison with data.
doi: 10.1103/PhysRevD.67.013003
2003LE21 Nucl.Phys. B(Proc.Supp.) S119, 404 (2003) R.Lewis, W.Wilcox, R.M.Woloshyn Strange matrix elements of the nucleon NUCLEAR STRUCTURE 1n, 1H; calculated strangeness form factors.
doi: 10.1016/S0920-5632(03)01568-8
1993BR05 Phys.Rev. C47, 2064 (1993) E.J.Brash, O.Hausser, B.Larson, A.Rahav, P.W.Green, P.P.J.Delheij, R.S.Henderson, U.Oelfke, M.C.Vetterli, D.M.Whittal, R.M.Woloshyn Proton-Induced Nucleon Knockout from Polarized 3He at 220 MeV NUCLEAR REACTIONS 3He(polarized p, 2p), (polarized p, np), E=220 MeV; measured σ(θ1, θ2), analyzing power, spin-correlation parameters; deduced rescattering corrections role. Quasielastic kinematics, high pressure polarized gas target.
doi: 10.1103/PhysRevC.47.2064
1992RA03 Phys.Lett. 275B, 259 (1992) A.Rahav, O.Hausser, C.A.Miller, P.P.J.Delheij, W.P.Alford, T.E.Chupp, K.Ferguson, R.S.Henderson, C.D.P.Levy, K.P.Jackson, J.Mildenberger, B.Morrissette, M.C.Vetterli, R.M.Woloshyn Proton-Induced Nucleon Knockout from Polarized 3He at 290 MeV NUCLEAR REACTIONS 3He(polarized p, 2p), (polarized p, np), E=290 MeV; measured spin correlation parameters, beam-, target-related asymmetries; deduced role of proton spin momentum distribution in 3He. Polarized target.
doi: 10.1016/0370-2693(92)91587-Y
1992RA23 Phys.Rev. C46, 1167 (1992) A.Rahav, O.Hausser, R.M.Woloshyn, T.E.Chupp, P.P.J.Delheij, K.Ferguson, R.Henderson, K.P.Jackson, C.D.P.Levy, J.Mildenberger, C.A.Miller, B.Morrissette, M.C.Vetterli Nucleon Knockout from Polarized 3He by Polarized Protons at 290 MeV NUCLEAR REACTIONS 3He(polarized p, 2p), (polarized p, np), E=290 MeV; measured spin observables, σ(θ1, θ2) vs energy transfer; deduced knockout mechanism evidence. Polarized target. Plane wave impulse approximation.
doi: 10.1103/PhysRevC.46.1167
1991LE05 Phys.Rev. D43, 1659 (1991) D.B.Leinweber, R.M.Woloshyn, T.Draper Electromagnetic Structure of Octet Baryons NUCLEAR STRUCTURE 1H, 1n; calculated μ ratio.
doi: 10.1103/PhysRevD.43.1659
1989WO03 Nucl.Phys. A496, 749 (1989) Polarized Lepton Deep-Inelastic Scattering from Few-Nucleon Targets NUCLEAR STRUCTURE 1H, 1n, 2H, 3He; calculated polarized lepton scattering asymmetries. Carlitz-Kaur model.
doi: 10.1016/0375-9474(89)90122-X
1987IQ02 Phys.Rev. C36, 2442 (1987) M.J.Iqbal, J.Thaler, R.M.Woloshyn Effect of Neutron-Proton Mass Difference on Charge Symmetry Breaking in Neutron-Proton Elastic Scattering NUCLEAR REACTIONS 1H(n, n), E not given; calculated n-p mass difference contribution to charge symmetry breaking.
doi: 10.1103/PhysRevC.36.2442
1984BL02 Phys.Rev. C29, 538 (1984) Quasi-Elastic Scattering of Polarized Electrons on Polarized 3He NUCLEAR REACTIONS 3He(e, e'), E=0.2488, 0.3984, 0.5, 7.26 GeV; calculated σ(θ, E(e')). 3He(polarized e, e'), E=0.25-2.75 GeV; calculated σ(θ, E(e')), asymmetry vs E. Polarized target, longitudinal beam polarization, impulse approximation.
doi: 10.1103/PhysRevC.29.538
1983CH25 Phys.Lett. 127B, 147 (1983) Electro-Disintegration of 2H with Polarized Beam and Target NUCLEAR REACTIONS 2H(polarized e, e'n), (polarized e, e'X), E=1 GeV; calculated electrodisintegration σ(θ(e), θp) vs outgoing electron momentum, asymmetry vs θ; deduced neutron electric form factor dependence. Quasifree, fixed kinematics, longitudinal beam polarization, polarized target.
doi: 10.1016/0370-2693(83)90863-8
1983GR09 J.Phys.(London) G9, 643 (1983) Low-Energy n-p Capture as a Probe of Two-Nucleon Dynamics NUCLEAR REACTIONS 1H(n, γ), E=200 MeV; calculated σ(θ). 1H(polarized n, γ), E=160, 200, 240 MeV; calculated neutron analyzing power, γ linear polarization vs θ. 1H(n, γ), E=120-240 MeV; calculated σ(E). 2H(e, e), E not given; calculated electric form factor. Nonrelativistic potentials, transformed, untransformed Reid soft-core deuteron wave functions.
doi: 10.1088/0305-4616/9/6/009
1982WO05 Nucl.Phys. A384, 401 (1982) A Parton Model for Polarized Electron Scattering on 3He NUCLEAR REACTIONS 3He(polarized e, e), E not given; calculated asymmetry. Polarized target, parton model.
doi: 10.1016/0375-9474(82)90343-8
1981RO03 Phys.Rev. C23, 1671 (1981) G.Roy, L.G.Greeniaus, G.A.Moss, D.A.Hutcheon, R.Liljestrand, R.M.Woloshyn, D.H.Boal, A.W.Stetz, K.Aniol, A.Willis, N.Willis, R.McCamis Inclusive Scattering of Protons on Helium, Nickel, and Tantalum at 500 MeV NUCLEAR REACTIONS 4He, Ni, 181Ta(polarized p, p), E=500 MeV; measured inclusive σ(Ep, θ), analyzing power vs Ep, θ; deduced reaction mechanism. Knockout model.
doi: 10.1103/PhysRevC.23.1671
1981SA01 Phys.Rev. C23, 351 (1981) Isobar-Doorway Model for Coherent π0 Photoproduction NUCLEAR REACTIONS 16O(γ, π0), E=246, 294, 371 MeV; 12C(γ, π0), E=254-368 MeV; 4He(γ, π0), E=240-360 MeV; calculated σ(θ). Optical potential, coherent photoproduction mechanism, isobar doorway.
doi: 10.1103/PhysRevC.23.351
1981SA14 Phys.Rev. C23, 2140 (1981) A.N.Saharia, R.M.Woloshyn, L.S.Kisslinger Pion-Nucleus Optical Potential in the Isobar-Doorway Model NUCLEAR REACTIONS 16O(π+, π+), E=114, 163, 240 MeV; 12C(π-, π-), E=120, 150, 180, 200, 230 MeV; 12C(π+, π+), E=148, 168 MeV; 4He(π-, π-), E=110, 150, 180, 220 MeV; analyzed σ(θ); deduced pion-nucleus optical potential parameters. Isobar doorway model.
doi: 10.1103/PhysRevC.23.2140
1980GR01 Nucl.Phys. A333, 399 (1980) Non-Relativistic Approximations to the Pion Production Operator in 4He(p, nπ+)4He NUCLEAR REACTIONS 4He(p, π+n), E=350, 560 MeV; calculated σ. Coplanar geometry, non-relativistic, fully covariant methods, pseudovector, pseudoscalar coupling emission graphs.
doi: 10.1016/0375-9474(80)90106-2
1980SA04 Phys.Rev. C21, 1111 (1980) Application of the Isobar-Doorway Model to Pion Charge Exchange Reactions NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=150 MeV; calculated σ(θ). 7Li, 13C, 15N, 18O(π+, π0), E=100-200 MeV; calculated σ(E). Isobar-doorway optical potential.
doi: 10.1103/PhysRevC.21.1111
1979BO27 Phys.Rev. C20, 1878 (1979) Direct Knockout Model for Nuclear Fragmentaion NUCLEAR REACTIONS 9Be, 27Al, Ag(p, α), (p, pα), E=300 MeV; calculated double differential σ. Direct knockout model.
doi: 10.1103/PhysRevC.20.1878
1979SA21 Phys.Lett. 84B, 401 (1979) Energy Dependence of the 13C(π+, π0)13N Cross Section NUCLEAR REACTIONS 13C(π+, π0), E=100-200 MeV; calculated σ. Energy dependence of first-order optical potentials varied with isospin.
doi: 10.1016/0370-2693(79)91225-5
1978FR12 Phys.Rev.Lett. 41, 148 (1978) S.Frankel, W.Frati, M.Gazzaly, G.W.Hoffmann, O.Van Dyck, R.M.Woloshyn Analyzing Power in Inclusive Proton-Nucleus Cross Sections. NUCLEAR REACTIONS 6Li, 12C, 181Ta(polarized p, p), (polarized p, X), E=800 MeV; measured A(θ).
doi: 10.1103/PhysRevLett.41.148
1978FR23 Phys.Rev. C18, 1379 (1978) S.Frankel, W.Frati, R.M.Woloshyn, D.Yang Application of Quasi-Two-Body Scaling to p + A → p + X NUCLEAR REACTIONS 181Ta(p, X), E=730 MeV; analyzed data to probe validity of single scattering model, quasi two-body scaling.
doi: 10.1103/PhysRevC.18.1379
1978KA08 Phys.Lett. 74B, 170 (1978) J.Kallne, A.W.Stetz, R.M.Woloshyn Analyzing Power of Inclusive Nuclear Reactions NUCLEAR REACTIONS 12C(polarized p, p'), E=516 MeV; measured A(θ).
doi: 10.1016/0370-2693(78)90544-0
1978WO11 Phys.Rev. C18, 1056 (1978) Neutral Pion Photoproduction in a Phenomenological Isobar Doorway Model NUCLEAR REACTIONS 12C(π-, π-), E=100-200 MeV; 12C(γ, π0), E=240-360 MeV; calculated σ(E).
doi: 10.1103/PhysRevC.18.1056
1978WO13 Nucl.Phys. A306, 333 (1978) Cluster Recoil Mechanism for Inclusive Nuclear Reactions NUCLEAR REACTIONS 6Li, 181Ta(p, p'), E=800 MeV; calculated inclusive σ.
doi: 10.1016/0375-9474(78)90468-2
1977KO26 Phys.Rev. C16, 1968 (1977) Near Threshold Photoproduction of Neutral Pions from the Deuteron NUCLEAR REACTIONS 1,2H(γ, π0), E=threshold-threshold+6 MeV; calculated σ(E).
doi: 10.1103/PhysRevC.16.1968
1977VE05 Phys.Rev. C16, 292 (1977) Threshold π0 Photoproduction from Complex Nuclear Targets NUCLEAR REACTIONS 4He, 6Li(γ, π0); calculated σ(θ).
doi: 10.1103/PhysRevC.16.292
1976KO04 Phys.Lett. 60B, 221 (1976) Threshold Photoproduction of Neutral Pions from Few-Body Targets NUCLEAR REACTIONS 3H, 3He(γ, π0), E=near threshold; calculated σ.
doi: 10.1016/0370-2693(76)90285-9
1976WO01 Phys.Rev. C13, 286 (1976) R.M.Woloshyn, E.J.Moniz, R.Aaron Relativistic Three-Body Calculation of πd Scattering NUCLEAR REACTIONS 2H(π, π), E=80-240 MeV; calculated σ(θ). Relativistic 3-body calculation.
doi: 10.1103/PhysRevC.13.286
1972WO09 Nucl.Phys. A185, 131 (1972) Relativistic Eikonal Approximation and Low-Energy Nucleon-Nucleon Scattering
doi: 10.1016/0375-9474(72)90555-6
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