NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = W.B.Kaufmann Found 21 matches. 2005HI11 Phys.Rev. C 71, 065201 (2005) G.E.Hite, W.B.Kaufmann, R.J.Jacob New evaluation of the πNΣ term
doi: 10.1103/PhysRevC.71.065201
1999KA57 Phys.Rev. C60, 055204 (1999) Tests of Current Algebra and Partially Conserved Axial-Vector Current in the Subthreshold Region of the Pion-Nucleon System
doi: 10.1103/PhysRevC.60.055204
1998GI02 Phys.Rev. C57, 784 (1998) Low-Energy Pion-Nucleon Scattering NUCLEAR REACTIONS 1H(π+, π+), (π-, π-), E ≈ 30-90 MeV; analyzed data; deduced pion-nucleon coupling constant, scattering volumes, subthreshold Σ term, off-shell amplitudes. Several data sets used.
doi: 10.1103/PhysRevC.57.784
1998HI03 Phys.Rev. C57, 931 (1998) ππ Scattering Amplitudes in the Subthreshold Region
doi: 10.1103/PhysRevC.57.931
1998NU05 Phys.Rev. C58, 2292 (1998) M.Nuseirat, M.A.K.Lodhi, M.O.El-Ghossain, W.R.Gibbs, W.B.Kaufmann Energy Dependence of Pion Double Charge Exchange NUCLEAR REACTIONS 14C, 42,44,48Ca(π+, π-), E < 250 MeV; calculated σ(E, θ=10°); deduced reaction mechanism possible short-range corrections. Comparison with data.
doi: 10.1103/PhysRevC.58.2292
1997KA08 Phys.Lett. 390B, 18 (1997) ππ Scattering Amplitudes within the Sub-Threshold Triangle
doi: 10.1016/S0370-2693(96)01390-1
1995GI08 Phys.Rev.Lett. 74, 3740 (1995) Isospin Breaking in Low-Energy Pion-Nucleon Scattering NUCLEAR REACTIONS 1H(π+, π+), (π-, π-), (π-, π0), E=30-50 MeV; analyzed amplitudes obtained from data; deduced clear iso-spin breaking indications.
doi: 10.1103/PhysRevLett.74.3740
1992KA35 Phys.Rev. C46, 1474 (1992) W.B.Kaufmann, P.B.Siegel, W.R.Gibbs Deeply Bound Pionic Atoms Via the (π-, p) Reactions NUCLEAR REACTIONS 58Ni(π-, p), E=20-50 MeV; 58Ni(π-, n), E=50 MeV; calculated σ(θ), pion capture of 1s atomic level. Distorted wave impulse approximation, direct capture into atomic level. ATOMIC PHYSICS 58Ni(π-, p), E=20-50 MeV; 58Ni(π-, n), E=50 MeV; calculated σ(θ), pion capture of 1s atomic level. Distorted wave impulse approximation, direct capture into atomic level.
doi: 10.1103/PhysRevC.46.1474
1989GI08 Phys.Lett. 231B, 6 (1989) W.R.Gibbs, W.B.Kaufmann, J.-P.Dedonder The Pion-Nucleus Resonance and Nuclear Translucence NUCLEAR REACTIONS 12C(π, π), E=10-80 MeV; calculated pion-nucleus s-wave phase shift; deduced nuclear translucence effect.
doi: 10.1016/0370-2693(89)90102-0
1989KA27 Phys.Rev. C40, 1729 (1989) K+-Nucleus Total Cross Section Analysis NUCLEAR REACTIONS 2H, 6Li, 12C, 16O, 28Si(K+, X), E at 550-800 MeV/c; analyzed σ extraction methods; deduced corrections.
doi: 10.1103/PhysRevC.40.1729
1989LE11 Phys.Rev. C39, 2356 (1989) M.J.Leitch, H.W.Baer, R.L.Burman, C.L.Morris, J.N.Knudson, J.R.Comfort, D.H.Wright, R.Gilman, S.H.Rokni, E.Piasetzky, Z.Weinfeld, W.R.Gibbs, W.B.Kaufmann 14C(π+, π-)14O Reaction between 19 and 80 MeV NUCLEAR REACTIONS 14C(π+, π-)14O, E=19-80 MeV; measured σ(θ) vs E. 14O deduced double IAS excitation. DWIA, optical model.
doi: 10.1103/PhysRevC.39.2356
1988AU05 Phys.Rev. C38, 1277 (1988) N.Auerbach, W.R.Gibbs, J.N.Ginocchio, W.B.Kaufmann Pion-Nucleus Double Charge Exchange and the Nuclear Shell Model NUCLEAR REACTIONS 42,44,46,48Ca, 46,48,50Ti, 52Cr, 54Fe(π+, π-), E=35, 45, 292 MeV; calculated ground, IAS transition σ(θ). Shell model.
doi: 10.1103/PhysRevC.38.1277
1987KA03 Phys.Rev. C35, 838 (1987) Deser-Goldberger-Baumann-Thirring Formula for π-p Atoms NUCLEAR REACTIONS 1n(π0, π0), E=3.3-6.5 MeV; calculated σ(E). 1H(π-, π-), E not given; calculated scattering lengths. Dester-Goldberger-Baumann-Thirring formula. ATOMIC PHYSICS, Mesic-Atoms 1H; calculated pionic level shifts, widths. Deser-Goldberger-Baumann-Thirring formula.
doi: 10.1103/PhysRevC.35.838
1986KA02 Phys.Lett. 166B, 279 (1986) Line Widths of Antiprotonic Atoms ATOMIC PHYSICS 4He, 6,7Li, 12C, 14N, 16,17,18O, 19F, 23Na, 31P, 32S, 35Cl, 39K, 56Fe, 89Y, Zr, 120Sn, 127I, 138Ba, Pr, 174Yb; calculated antiprotonic atom level widths. Annihilation probabilities on nucleons.
doi: 10.1016/0370-2693(86)90798-7
1985SI09 Phys.Rev. C31, 2184 (1985) P.B.Siegel, W.B.Kaufmann, W.R.Gibbs K+ as a Probe of Partial Deconfinement in Nuclei NUCLEAR REACTIONS 12C, 40Ca(K+, K+), E at 300-800 MeV/c; calculated σ(θ), σ(E), σ(12C)/σ(2H); deduced K+-nucleon interaction, phase shift nucleon size dependence.
doi: 10.1103/PhysRevC.31.2184
1984GI11 Phys.Lett. 145B, 1 (1984) Antiprotonic Atomic Energy Levels via the (p(bar), p) Reaction NUCLEAR REACTIONS 31P(p-bar, p), E=150 MeV; calculated σ(θ). 31P, 19F, 23Na(p-bar, p), E=100 MeV; calculated σ(θ=0°); deduced possible antiprotonic atom level detection. DWIA.
doi: 10.1016/0370-2693(84)90934-1
1984SI13 Phys.Rev. C30, 1256 (1984) P.B.Siegel, W.B.Kaufmann, W.R.Gibbs K+-Nucleus Elastic Scattering and Charge Exchange NUCLEAR REACTIONS 12C, 40Ca(K+, K+), E=446.4, 425, 433, 440 MeV; 13C(K+, K0), E=100-400 MeV; calculated σ(θ), σ(θ) vs E; deduced medium effects. DWIA analysis, multiple scattering theory.
doi: 10.1103/PhysRevC.30.1256
1983KA19 Phys.Rev. C28, 1286 (1983) Nuclear Medium Effects in Pion Elastic Scattering and Charge Exchange NUCLEAR REACTIONS 12C(π+, π+), E=165 MeV; calculated σ(θ). 7Li, 15N, 13C(π+, π0), E=40-240 MeV; calculated σ(0°), σ vs E, σ(θ); deduced binding, Pauli blocking correction effects. Pion-nucleus optical model, three-body approximation.
doi: 10.1103/PhysRevC.28.1286
1976GI01 Phys.Rev.Lett. 36, 85 (1976) W.R.Gibbs, B.F.Gibson, A.T.Hess, G.J.Stephenson, Jr., W.B.Kaufmann Pion Charge-Exchange Scattering from Light Nuclei NUCLEAR REACTIONS 7Li, 10B, 13C(π+, π0); calculated σ(E).
doi: 10.1103/PhysRevLett.36.85
1976GI06 Phys.Rev. C13, 2433 (1976) W.R.Gibbs, B.F.Gibson, A.T.Hess, G.J.Stephenson, Jr., W.B.Kaufmann Elastic Pion-4He Scattering NUCLEAR REACTIONS 4He(π+, π+), (π-, π-), E=24-110 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.13.2433
1974KA07 Phys.Rev. C9, 1340 (1974) W.B.Kaufmann, J.C.Jackson, W.R.Gibbs Charge-Exchange Reactions on Light Nuclei in a Multiple-Scattering Formalism NUCLEAR REACTIONS 18O(π+, π0), E=180 MeV; calculated σ(E); 18O(π+, π-), E=180 MeV; calculated σ(E); 13C(π+, π0), E=30-200 MeV; calculated σ(E); 13C(π+, π0), E=180 MeV; calculated σ(θ); 9Be(π+, π0), E=30-250 MeV; calculated σ(E); 9Be(π+, π-), E=30-250 MeV; calculated σ(E) to T=3/2 final states; 9Be(π+, π0), E=175 MeV; calculated σ(θ) to ground, sum of final states; 9Be(π+, π-), E=175 MeV; calculated σ(θ) to T=3/2 final states; 11B(π+, π0), E=20-250 MeV; calculated σ(E) to ground, sum of final states.
doi: 10.1103/PhysRevC.9.1340
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