NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = P.W.Keaton Found 28 matches. 1982HA06 Phys.Rev. C25, 1090 (1982) R.A.Hardekopf, P.W.Keaton, P.W.Lisowski, L.R.Veeser 9Be(3He, p(pol))11B Polarization and Implications for Time-Reversal Invariance NUCLEAR REACTIONS 9Be(3He, p), E=13.6 MeV; measured P(θ); deduced no time reversal invariance violation.
doi: 10.1103/PhysRevC.25.1090
1977DO01 Phys.Rev. C15, 518 (1977) D.C.Dodder, G.M.Hale, N.Jarmie, J.H.Jett, P.W.Keaton, Jr., R.A.Nisley, K.Witte Elastic Scattering of Protons by Helium 4: New Experiments and Analysis NUCLEAR REACTIONS 4He(p, p), E=11-14 MeV; measured σ(E, θ); deduced R-matrix parameters for E=1-17 MeV.
doi: 10.1103/PhysRevC.15.518
1975DA21 Nucl.Instrum.Methods 129, 85 (1975) A Null Technique for Calibrating Polarization Values in πp Scattering NUCLEAR REACTIONS 1H(π+, π+), (π-, π-), E=900 MeV; measured maximum polarization.
doi: 10.1016/0029-554X(75)90115-9
1975HA44 Phys.Rev.Lett. 35, 1623 (1975) R.A.Hardekopf, L.R.Veeser, P.W.Keaton, Jr. Polarization Measurements and Optical-Model Potential for Tritons NUCLEAR REACTIONS 52Cr, 116Sn, 60Ni, 90Zr, 208Pb(polarized t, t), E=15 MeV; measured σ(θ), A(θ).
doi: 10.1103/PhysRevLett.35.1623
1974DO05 Phys.Rev. C10, 571 (1974) T.R.Donoghue, G.G.Ohlsen, N.Jarmie, P.W.Keaton, Jr. Vector and Tensor Analyzing-Power Measurements for 3H(d, d)3H Elastic Scattering NUCLEAR REACTIONS 3H(polarized d, d), E=11.4, 14.4 MeV; measured A(θ).
doi: 10.1103/PhysRevC.10.571
1974GR30 Nucl.Phys. A230, 353 (1974) W.Gruebler, R.A.Hardekopf, D.D.Armstrong, P.W.Keaton, Jr. Angular Distribution of Polarization Transfer in 2H(d, p)3H NUCLEAR REACTIONS 2H(polarized d, p), E=10 MeV; measured polarization p, polarization transfer coefficients.
doi: 10.1016/0375-9474(74)90313-3
1973CA04 Nucl.Phys. A202, 161 (1973) R.F.Casten, E.Cosman, E.R.Flynn, O.Hansen, P.W.Keaton, Jr., N.Stein, R.Stock The 209Pb Single-Neutron States and the l = 4 Levels of 205Pb Studied By the (d, p) Reaction NUCLEAR REACTIONS 204,208Pb(polarized d, p), E=12.3, 15 MeV; measured σ(Ep, θ), A(Ep, θ). 205Pb levels deduced J, π. 209Pb deduced levels, S. Enriched targets.
doi: 10.1016/0375-9474(73)90249-2
1973CA09 Phys.Rev. C7, 1016 (1973) R.F.Casten, P.W.Keaton, Jr., G.P.Lawrence Spin and Parity Determinations in Tungsten Nuclei Using Polarized Deuterons NUCLEAR REACTIONS 182,184,186W(polarized d, p), E=12.08, 15 MeV; measured σ(Ep), vector analyzing power T11(θ). 183,185,187W deduced levels, J, π.
doi: 10.1103/PhysRevC.7.1016
1973CL05 Phys.Rev. C8, 922 (1973) T.B.Clegg, D.D.Armstrong, R.A.Hardekopf, P.W.Keaton, Jr. Polarization Transfer in the 2H(d, p)3H Reaction at theta = 0° NUCLEAR REACTIONS 2H(polarized d, p), E=6-15 MeV, θ=0°; measured polarization transfer(E).
doi: 10.1103/PhysRevC.8.922
1973HA51 Phys.Rev. C8, 1629 (1973) R.A.Hardekopf, D.D.Armstrong, W.Gruebler, P.W.Keaton, Jr., U.Meyer-Berkhout Polarization Transfer in the 3He(d, p)4He Reaction NUCLEAR REACTIONS 3He(d, p), E=4-14 MeV, θ=0°;E=8 MeV, θ=15, 30, 45, 60°; measured polarization transfer coefficients, P(p).
doi: 10.1103/PhysRevC.8.1629
1973KE17 Phys.Rev. C8, 1692 (1973) P.W.Keaton, Jr., D.D.Armstrong Deuteron Optical Potential with a Tensor Term and Breakup NUCLEAR REACTIONS 52Cr, 56Fe, 60Ni, 90Zr, 122Sn, 197Au(polarized d, d), E=15 MeV; calculated σ(θ), analyzing tensors.
doi: 10.1103/PhysRevC.8.1692
1972HA77 Nucl.Instrum.Methods 103, 425 (1972) R.A.Hardekopf, D.D.Armstrong, P.W.Keaton, Jr. Analyzing Power in Si(p, p) below 15 MeV NUCLEAR REACTIONS Si(polarized p, p), E=5-15 MeV; measured analyzing power(E;θ).
doi: 10.1016/0029-554X(72)90410-7
1972KE02 Nucl.Phys. A179, 561 (1972) P.W.Keaton, Jr., D.D.Armstrong, L.R.Veeser, H.T.Fortune, N.R.Roberson Cross-Section and Polarization Measurements for the 12C(t, p)14C Reaction NUCLEAR REACTIONS 12C(t, t), 12C(t, p), 12C(t, p), E=16, 20 MeV; measured σ(θ), P(θ); deduced optical model parameters.
doi: 10.1016/0375-9474(72)90604-5
1972KE17 Phys.Rev.Lett. 29, 880 (1972) P.W.Keaton, Jr., D.D.Armstrong, R.A.Hardekopf, P.M.Kurjan, Y.K.Lee New Method for Determining Polarization Standards in Nuclear Reactions NUCLEAR REACTIONS 4He(polarized p, p), E=12 MeV; measured P(θ), Wolfenstein polarization parameters.
doi: 10.1103/PhysRevLett.29.880
1972OH02 Phys.Rev. C5, 1205 (1972) G.G.Ohlsen, J.L.Gammel, P.W.Keaton, Jr. Description of 4He(d, d)4He Polarization-Transfer Experiments NUCLEAR REACTIONS 4He(d, d), E not given; defined parameters for polarization transfer; generalized wolfenstein parameters.
doi: 10.1103/PhysRevC.5.1205
1972SE23 Ann.Phys.(New York) 74, 250 (1972) J.D.Seagrave, J.C.Hopkins, D.R.Dixon, P.W.Keaton, Jr., E.C.Kerr, A.Niiler, R.H.Sherman, R.K.Walter Elastic Scattering and Polarization of Fast Neutrons by Liquid Deuterium and Tritium NUCLEAR REACTIONS 2,3H(n, n), E < 23 MeV; measured σ(θ). 3H(n, n), E=22.1 MeV; measured pn(θ).
doi: 10.1016/0003-4916(72)90263-1
1971OH04 Phys.Rev.Lett. 27, 599 (1971) G.G.Ohlsen, J.L.McKibben, G.P.Lawrence, P.W.Keaton, Jr., D.D.Armstrong Precise Proton-Polarization Standards Determined with a Lamb-Shift Ion Source Incorporating a Nuclear Spin Filter NUCLEAR REACTIONS 4He(p, p), E=12.03 MeV; measured analyzing power(θ).
doi: 10.1103/PhysRevLett.27.599
1970VE01 Nucl.Phys. A140, 177 (1970) L.R.Veeser, D.D.Armstrong, P.W.Keaton, Jr. Polarization of Tritons Scattered from Hydrogen NUCLEAR REACTIONS H(t, t), E=6.4-9.5 MeV; measured P(E;θ). Natural target.
doi: 10.1016/0375-9474(70)90894-8
1969AR07 Phys.Rev.Letters 23, 135 (1969) D.D.Armstrong, L.L.Catlin, P.W.Keaton, Jr., L.R.Veeser Polarization of 3He Elastically Scattered from 4He NUCLEAR REACTIONS 4He(3He, 3He), E=7.8, 8.3, 8.8, 13 MeV; measured P(θ).
doi: 10.1103/PhysRevLett.23.135
1968KE03 Phys.Rev.Letters 20, 1392 (1968) P.W.Keaton, Jr., D.D.Armstrong, L.R.Veeser Polarization of Tritons Scattered from 4He NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.20.1392
1967BE10 Phys.Rev. 153, 1152 (1967) J.J.Berlijn, P.W.Keaton, Jr., L.Madansky, G.E.Owen, L.Pfeiffer, N.R.Roberson Nuclear Polarization in the B11(d, p)B12 Reaction. I NUCLEAR STRUCTURE 12B, 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.153.1152
1967RI05 Phys.Rev. 154, 287 (1967) E.T.Ritter, P.W.Keaton, Jr., Y.K.Lee, R.R.Stevens, Jr., J.C.Walker Mossbauer Effect Following Coulomb Excitation of Fe57 NUCLEAR STRUCTURE 57Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.154.287
1965GO07 Phys.Rev.Letters 15, 418 (1965) D.A.Goldberg, P.W.Keaton, Jr., Y.K.Lee, L.Madansky, J.C.Walker Mossbauer Effect Resulting from the Reaction Fe56(d, p)Fe57 NUCLEAR STRUCTURE 57Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.15.418
1965LE13 Phys.Rev.Letters 14, 957 (1965) Y.K.Lee, P.W.Keaton, Jr., E.T.Ritter, J.C.Walker Mossbauer Effect from Coulomb-Excited Levels in Fe57 NUCLEAR STRUCTURE 57Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.14.957
1964TI03 Phys.Rev. 135, B892 (1964) R.M.Tisinger, Jr., P.W.Keaton, G.E.Owen Differential cross sections for the reaction B11(d, p) B12 for ED = 1 - 2.6 MeV NUCLEAR REACTIONS 11B(d, p), E=1-2.6 MeV; measured products, 12B, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry F0275.
doi: 10.1103/PhysRev.135.B892
1964WI03 Phys.Rev. 133, B930 (1964) E.H.Willen, P.W.Keaton, G.E.Owen Angular Distributions for the C13(d, n)N14 Reaction NUCLEAR STRUCTURE 13C, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.133.B930
1963KE06 Bull.Am.Phys.Soc. 8, No.4, 291, A10 (1963) P.W.Keaton, L.Madansky, G.E.Owen, R.Roberson Nuclear Polarization of B12 in a (d, p) Reaction NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1962KE18 TID-17720, p.15 (1962) NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
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