NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = I.Duck Found 17 matches. 1996DU02 Z.Phys. A354, 107 (1996) Octet and Decuplet Magnetic and Axial Couplings from One-Loop Self-Consistent Perturbation Theory NUCLEAR STRUCTURE 1H, 1n; calculated μ. Octet, decuplet wave functions, one-loop self-consistent perturbation theory.
doi: 10.1007/s002180050018
1994DU14 Z.Phys. A350, 71 (1994) Octet-Decuplet Baryon Mass Splittings from Self-Consistent One-Loop Perturbation Theory
doi: 10.1007/BF01285055
1988PA22 Phys.Rev. C38, 2716 (1988) P.V.Pancella, G.S.Mutchler, S.D.Baker, J.W.Kruk, I.M.Duck, M.D.Corcoran, G.C.Phillips, J.M.Clement, J.A.Buchanan, B.W.Mayes, L.S.Pinsky, W.von Witsch, E.Andrade, H.Garcilazo, J.M.Laget Measurement of π+d → Δ++n at Intermediate Energy NUCLEAR REACTIONS 2H(π+, π+p), E at 312-600 MeV/c; measured σ(θ(π), θ(p)) vs pion momentum; deduced σ(θ) for reaction 2H(π+, Δ++).
doi: 10.1103/PhysRevC.38.2716
1983HA11 Phys.Rev. C27, 2742 (1983) A.D.Hancock, R.W.Hackenburg, J.M.Hungerford, B.W.Mayes, L.S.Pinsky, J.C.Allred, T.M.Williams, S.D.Baker, J.A.Buchanan, J.M.Clement, M.Copel, I.M.Duck, G.S.Mutchler, G.P.Pepin, E.A.Umland, G.C.Phillips, M.W.McNaughton, C.Hwang, M.Furic Asymmetries and Cross Sections for the Reaction p(pol) + p → p + π+ + n at 800 MeV NUCLEAR REACTIONS 1H(polarized p, π+p), E=800 MeV; measured σ(θp, σ(π)) vs proton momemtum, analyzing power. Polarized target.
doi: 10.1103/PhysRevC.27.2742
1981HO01 Phys.Rev. C23, 407 (1981) J.H.Hoftiezer, S.D.Baker, J.M.Clement, W.H.Dragoset, I.M.Duck, R.D.Felder, D.M.Judd, G.S.Mutchler, G.P.Pepin, G.C.Phillips, E.A.Umland, J.C.Allred, E.V.Hungerford III, B.W.Mayes, L.S.Pinsky, T.M.Williams, M.Furic, W.von Witsch Reaction πd → pπn in the Δ Resonance Region NUCLEAR REACTIONS 2H(π+, π+p), (π-, π-p), E at 340 MeV/c; measured σ(θp, θ(π), proton momentum). DWIA model, dibaryon resonances.
doi: 10.1103/PhysRevC.23.407
1979HO26 Phys.Lett. 88B, 73 (1979) J.H.Hoftiezer, M.Furic, G.S.Mutchler, I.M.Duck, W.H.Dragoset, J.M.Clement, D.M.Judd, R.D.Felder, G.P.Pepin, W.von Witsch, G.C.Phillips, J.C.Allred, E.V.Hungerford, B.W.Mayes, L.S.Pinsky, T.M.Williams Reaction Mechanisms and Isospin Effects for the π+ + D → p + π+ + n Processes at Pπ = 340 MeV/c NUCLEAR REACTIONS 2H(π+, π+p), (π-, π-p), E at 340 MeV/c; measured σ; deduced reaction mechanism, isospin effects, role of spectator particle.
doi: 10.1016/0370-2693(79)90117-5
1978DU09 Phys.Rev. C18, 887 (1978) I.Duck, K.R.Hogstrom, G.S.Mutchler pd → ndπ+ Reaction Mechanisms NUCLEAR REACTIONS 2H(p, π+n), E=585 MeV; calculated σ.
doi: 10.1103/PhysRevC.18.887
1978HU13 Phys.Rev. C18, 2666 (1978) J.Hudomalj-Gabitzsch, I.M.Duck, M.Furic, G.S.Mutchler, J.M.Clement, R.D.Felder, W.H.Dragoset, G.C.Phillips, J.C.Allred, E.V.Hungerford, B.W.Mayes, L.S.Pinsky, T.M.Williams Production of the Δ++ in the Reaction pp → pπ+n at 800 MeV NUCLEAR REACTIONS 1H(p, p'π+), E=800 MeV; measured σ(Ep', θp, θπ); deduced form factor range parameters, Δ++ intermediate state.
doi: 10.1103/PhysRevC.18.2666
1977DU02 Nucl.Phys. A282, 425 (1977) I.Duck, R.D.Felder, G.S.Mutchler Comparison of Glauber Theory to Final State Interaction Theory for pd Inelastic/Elastic Scattering NUCLEAR REACTIONS 2H(p, p'), (p, p), E=585, 800 MeV; calculated σ(Ep', θ)/σ(θ).
doi: 10.1016/0375-9474(77)90067-7
1977FE06 Nucl.Phys. A280, 308 (1977) R.D.Felder, T.M.Williams, G.S.Mutchler, I.Duck, J.Hudomalj-Gabitzsch, M.Furic, D.Mann, N.D.Gabitzsch, J.M.Clement, G.C.Phillips, T.R.Witten, E.V.Hungerford, M.Warneke, B.W.Mayes, L.Y.Lee, J.C.Allred Final State Interactions in Deuteron Breakup by Protons at 585 and 800 MeV NUCLEAR REACTIONS 2H(p, 2p), E=585, 800 MeV; measured σ(θ); deduced singlet, triplet contributions in pn final state interactions.
doi: 10.1016/0375-9474(77)90607-8
1973BH04 Phys.Lett. 46B, 309 (1973) Pion Production in the Reaction pd → tπ NUCLEAR REACTIONS 2H(p, πt), E=340-670 MeV; calculated σ(E;θ).
doi: 10.1016/0370-2693(73)90126-3
1972DU12 Phys.Rev.Lett. 29, 875 (1972) I.M.Duck, V.Valkovic, G.C.Phillips Off-Energy-Shell Effects in Deuteron-Induced Deuteron Breakup NUCLEAR REACTIONS 2H(d, np), E=6-14 MeV; measured σ(Ed, Ep).
doi: 10.1103/PhysRevLett.29.875
1972VA04 Nucl.Phys. A182, 225 (1972) V.Valkovic, N.Gabitzsch, D.Rendic, I.Duck, G.C.Phillips Coincidence Spectra from d + d → d + p + n and p + d → p + p + n Reactions with Neutron Detection at Zero Degrees NUCLEAR REACTIONS 2H(p, pn), E=10 MeV; 2H(d, np), E=10 MeV; measured σ(Ep, En, θ(n)=0°, θ(p)=15-40°), σ(Ep, En, θ(n)=0°, θ(d)=15-35°).
doi: 10.1016/0375-9474(72)90273-4
1972VA05 Nucl.Phys. A183, 126 (1972) V.Valkovic, I.Duck, W.E.Sweeney, G.C.Phillips Three-Body Break-up in the d+d → d+p+n Reaction NUCLEAR REACTIONS 2H(d, pn), E=6-13 MeV; measured σ(E;Ed, Ep, En, θ=θ(1)=-θ(2)=20°).
doi: 10.1016/0375-9474(72)90934-7
1972VA35 Phys.Lett. 42B, 191 (1972) V.Valkovic, I.M.Duck, G.C.Phillips Coulomb Effects in Deuteron-Induced Deuteron Break-up
doi: 10.1016/0370-2693(72)90057-3
1971VA28 Phys.Rev. C4, 2289 (1971) V.Valkovic, I.M.Duck, W.E.Sweeney, Jr., E.Andrade, G.C.Phillips Nuclear-Deuteron Quasifree Scattering in the Reaction d + d → d + p + n at Low Bombarding Energies NUCLEAR REACTIONS 2H(d, np), E=6-13 MeV; measured σ(E;Ed, En, θ(d), θ(n)), σ(E;Ed, Ep, θ(d), θ(p)).
doi: 10.1103/PhysRevC.4.2289
1970MC25 Nucl.Phys. A157, 417 (1970) Three-Alpha Final State Interactions NUCLEAR REACTIONS 11B(p, α)2α, E=2.65 MeV; measured nothing; analyzed σ(Eα, θ(α)); deduced phase shifts.
doi: 10.1016/0375-9474(70)90223-X
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