NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Picklesimer Found 24 matches. 1995PI18 Few-Body Systems 19, 47 (1995) A.Picklesimer, R.A.Rice, R.Brandenburg Δ Degrees of Freedom in Trinuclei with the Argonne V28Q Model NUCLEAR STRUCTURE 3H; calculated Δ degrees of freedom contribution to binding energy. Different models.
doi: 10.1007/s006010050017
1992CH41 Nuovo Cim. 105A, 1149 (1992) Off-Shell and Medium Effects on the Electromagnetic Nucleon Current NUCLEAR REACTIONS 40Ca(e, e'p), E=210, 425 MeV; 16O(e, e'p), E=135, 200 MeV; calculated longitudinal, transverse response functions. Off-shell, medium effects on electromagnetic nucleon current.
doi: 10.1007/BF02730873
1992PI03 Phys.Rev. C45, 547 (1992) A.Picklesimer, R.A.Rice, R.Brandenburg Δ Degrees of Freedom in Trinuclei. II. The Hannover ΔΔ Model NUCLEAR STRUCTURE 3H; calculated binding energy; deduced Δ-, ΔΔ- degrees of freedom role. Hannover ΔΔ-force model.
doi: 10.1103/PhysRevC.45.547
1992PI05 Phys.Rev.Lett. 68, 1484 (1992) A.Picklesimer, R.A.Rice, R.Brandenburg Trinuclear Δ Components and the Triton Binding Energy NUCLEAR STRUCTURE 3H; calculated binding energy; deduced trinuclear Δ components contribution. Hannover, Argonne force models.
doi: 10.1103/PhysRevLett.68.1484
1992PI16 Phys.Rev. C46, 1178 (1992) A.Picklesimer, R.A.Rice, R.Brandenburg Δ Degrees of Freedom in Trinuclei. V. Exotic Contributions NUCLEAR STRUCTURE 3H; calculated binding energy. Exotic channels.
doi: 10.1103/PhysRevC.46.1178
1991PI08 Phys.Rev. C44, 1359 (1991) A.Picklesimer, R.A.Rice, R.Brandenburg Δ Degrees of Freedom in Trinuclei: The Hannover one-Δ model NUCLEAR STRUCTURE 3H; calculated binding energy. Explicit Δ in triton.
doi: 10.1103/PhysRevC.44.1359
1989CH25 Phys.Rev. C40, 790 (1989) C.R.Chinn, A.Picklesimer, J.W.van Orden Final-State Interactions and Relativistic Effects in the Quasielastic (e, e') Reaction NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated longitudinal, transverse response functions. Final state interactions, relativistic effects.
doi: 10.1103/PhysRevC.40.790
1989CH33 Phys.Rev. C40, 1159 (1989) C.R.Chinn, A.Picklesimer, J.W.Van Orden Quasielastic (e, e') Sum Rule Saturation NUCLEAR REACTIONS 40Ca(e, e'X), E not given; calculated Coulomb sum rule saturation. Microscopic Green's function doorway formalism.
doi: 10.1103/PhysRevC.40.1159
1989PI07 Phys.Rev. C40, 290 (1989) Polarization Response Functions and the (e(pol), e'p(pol)) Reaction NUCLEAR REACTIONS 16O(polarized e, e'p), E=135 MeV; calculated longitudinal, transverse response functions. Polarized nucleon, relativistic, nonrelativistic treatments.
doi: 10.1103/PhysRevC.40.290
1988BR03 Phys.Rev. C37, 781 (1988) R.A.Brandenburg, G.S.Chulick, Y.E.Kim, D.J.Klepacki, R.Machleidt, A.Picklesimer, R.M.Thaler Nuclear Charge Symmetry Breaking and the 3H-3He Binding Energy Difference NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference; deduced charge asymmetric contributions.
doi: 10.1103/PhysRevC.37.781
1988BR05 Phys.Rev. C37, 1245 (1988) R.A.Brandenburg, G.S.Chulick, R.Machleidt, A.Picklesimer, R.M.Thaler Essential Mechanisms in the Triton Binding NUCLEAR STRUCTURE 3H; calculated binding energy. Effective energy dependent central potential.
doi: 10.1103/PhysRevC.37.1245
1988BR22 Phys.Rev. C38, 1397 (1988) R.A.Brandenburg, G.S.Chulick, R.Machleidt, A.Picklesimer, R.M.Thaler Mesic Retardation and the Triton Binding Energy NUCLEAR STRUCTURE 3H; analyzed binding energy estimates; deduced mesic retardation role.
doi: 10.1103/PhysRevC.38.1397
1988CH12 Phys.Rev. C37, 1549 (1988) G.S.Chulick, Ch.Elster, R.Machleidt, A.Picklesimer, R.M.Thaler Neutron-Proton Scattering Observables at 325 MeV, the ϵ1 Parameter, and the Tensor Force NUCLEAR REACTIONS 1H(polarized n, n), E=325 MeV; calculated polarization observables; deduced tensor force role.
doi: 10.1103/PhysRevC.37.1549
1987CO26 Phys.Rev.Lett. 59, 1267 (1987) T.D.Cohen, J.W.Van Orden, A.Picklesimer Medium-Modified Form Factors, Relativistic Dynamics, and the (e, e'p) Reaction NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated transverse to longitudinal response function ratio. DWIA.
doi: 10.1103/PhysRevLett.59.1267
1985AA02 Phys.Rev. C32, 231 (1985) B.Aas, M.V.Hynes, A.Picklesimer, P.C.Tandy, R.M.Thaler Spin Observables in Elastic Proton Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=500, 650, 318 MeV; calculated analyzing power, spin rotation function, spin variables vs θ. Relativistic, nonrelativistic approach.
doi: 10.1103/PhysRevC.32.231
1985HY01 Phys.Rev. C31, 1438 (1985) M.V.Hynes, A.Picklesimer, P.C.Tandy, R.M.Thaler Relativistic (Dirac Equation) Effects in Microscopic Elastic Scattering Calculations NUCLEAR REACTIONS 40Ca(polarized p, p), E=500, 181, 650 MeV; 16O(polarized p, p), E=180, 318, 500, 135 MeV; calculated σ(θ), analyzing power spin rotation parameter vs θ. First-order multiple scattering model, relativistic extension.
doi: 10.1103/PhysRevC.31.1438
1985PI10 Phys.Rev. C32, 1312 (1985) A.Picklesimer, J.W.Van Orden, S.J.Wallace Final State Interactions and Relativistic Effects in the (e(pol), e'p) Reaction NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated response functions for Ep=135 MeV. Relativistic effects, final state interactions, DWIA.
doi: 10.1103/PhysRevC.32.1312
1985PI14 Phys.Lett. 163B, 311 (1985) A.Picklesimer, P.C.Tandy, J.A.Tjon Dynamical Model of (p-bar)-Nucleus Elastic Scattering NUCLEAR REACTIONS 12C, 40Ca(p-bar, p-bar), E=180 MeV; calculated σ(θ). Nonrelativistic, Dirac first-order potentials.
doi: 10.1016/0370-2693(85)90287-4
1984HY01 Phys.Rev.Lett. 52, 978 (1984) M.V.Hynes, A.Picklesimer, P.C.Tandy, R.M.Thaler Characteristic Dirac Signature in Elastic Proton Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=500, 300 MeV; 16O(polarized p, p), E=135, 500 MeV; calculated σ(θ), analyzing power vs θ.
doi: 10.1103/PhysRevLett.52.978
1984PI05 Phys.Rev. C29, 1582 (1984) A.Picklesimer, P.C.Tandy, R.M.Thaler, D.H.Wolfe Off-Shell and Nonlocal Effects in Proton-Nucleus Elastic Scattering NUCLEAR REACTIONS 16O(polarized p, p), E=135 MeV; 12C(polarized p, p), E=200 MeV; 40Ca(polarized p, p), E=300 MeV; calculated σ(θ), analyzing power vs θ; deduced off-shell, nonlocal effects. First-order nonrelativisitic microscopic optical potential.
doi: 10.1103/PhysRevC.29.1582
1984PI17 Phys.Rev. C30, 1861 (1984) A.Picklesimer, P.C.Tandy, R.M.Thaler, D.H.Wolfe Momentum Space Approach to Microscopic Effects in Elastic Proton Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=181, 500 MeV; 16O(polarized p, p), E=135, 318 MeV; calculated σ(θ), analyzing power, spin rotation function vs θ. Nonrelativistic, microscopic optical potential, momentum space approach.
doi: 10.1103/PhysRevC.30.1861
1980PE11 Phys.Lett. B95, 166 (1980) F.Petrovich, W.G.Love, A.Picklesimer, G.E.Walker, E.R.Siciliano Differences in the Structure of Isoscalar and Isovector Stretched Excitations in 24Mg and 28Si NUCLEAR REACTIONS 24Mg, 28Si(p, p'), E=135 MeV; analyzed σ(θ). 24Mg, 28Si levels deduced isospin dependence of S, stretched configurations.
doi: 10.1016/0370-2693(80)90461-X
1978PI01 Phys.Rev. C17, 237 (1978) Spin-Dependent N-N t Matrix for Intermediate Energy Nucleon-Nucleus Reactions NUCLEAR REACTIONS 16O(p, p'), E=156 MeV; 28Si(p, p'), E=134 MeV; calculated σ(θ). Nucleon-nucleon transition matrix from two-body data.
doi: 10.1103/PhysRevC.17.237
1977AD04 Phys.Rev.Lett. 38, 1387 (1977) G.S.Adams, A.D.Bacher, G.T.Emery, W.P.Jones, R.T.Kouzes, D.W.Miller, A.Picklesimer, G.E.Walker Excitation of High-Spin 'Particle-Hole' States in 28Si and 24Mg by Inelastic Proton Scattering at Large Momentum Transfer NUCLEAR REACTIONS 24Mg, 28Si(p, p'), E=135 MeV; measured σ(Ep', θ). 24Mg, 28Si deduced resonances, J, π, T.
doi: 10.1103/PhysRevLett.38.1387
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