NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.A.Cowley Found 86 matches. 2021CO04 Phys.Rev. C 103, 034622 (2021) Sensitivity of analyzing power to distorting potentials in the quasifree reaction 40Ca(p, pα)36Ar at 100 MeV incident energy: Comparison with 9Be and 12C targets NUCLEAR REACTIONS 9Be(polarized p, pα)5He, E=150 MeV; 12C(polarized p, pα)5He, E=100 MeV; analyzed experimental σ(θ), and analyzing-power angular distributions. 40Ca(polarized p, pα)36Ar, E=100 MeV; analyzed experimental analyzing-power angular distributions, and triple differential energy sharing cross section distribution using distorted-wave impulse approximation (DWIA) theory.
doi: 10.1103/PhysRevC.103.034622
2021CO09 Phys.Rev. C 104, 014608 (2021) Contribution to inclusive (p, α) reactions from (p, pα) knockout at incident energies near 100 MeV NUCLEAR REACTIONS 58Ni(p, pα)54Fe, 58Ni, 59Co(p, α), E=100 MeV; 40Ca(p, pα)36Ar, E=101.3 MeV; analyzed experimental σ(θ) distributions in knockout reactions using distorted-wave impulse approximation (DWIA). Comparison with intranuclear cascade (INC) theory calculations.
doi: 10.1103/PhysRevC.104.014608
2019CO10 Int.J.Mod.Phys. E28, 1950050 (2019) Simplistic distorted-wave Born approximation interpretation of the 11Li(p, t)9Li reaction NUCLEAR REACTIONS 1H(11Li, t), E=4.3 MeV; analyzed available data; deduced σ, σ(θ).
doi: 10.1142/S0218301319500502
2018DI15 Int.J.Mod.Phys. E27, 1850091 (2018) S.S.Dimitrova, A.A.Cowley, E.V.Zemlyanaya, K.V.Lukyanov Reaction mechanism of proton-induced pre-equilibrium α-particle emission from medium-mass nuclei at incident energies between 65 and 160 MeV NUCLEAR REACTIONS 197Au, 59Co, 58Ni, 90Zr(p, α), 93Nb(p, 3He), (p, α), E=65-160 MeV; analyzed available data on σ and analyzing power; deduced the competition between pickup and knockout.
doi: 10.1142/S021830131850091X
2016CO04 Phys.Rev. C 93, 034624 (2016) A.A.Cowley, S.S.Dimitrova, E.V.Zemlyanaya, K.V.Lukyanov, J.J.van Zyl Inclusive (p(pol), α) reaction on 59Co at an incident energy of 100 MeV and comparison with the reaction mechanism for 93Nb between 65 and 160 MeV NUCLEAR REACTIONS 59Co(polarized p, α), E=100 MeV; measured Eα, Iα, σ(θ), analyzing powers Ay(θ) at iThemba LABS in Faure. 93Nb(polarized p, α), E=100 MeV; analyzed double-differential cross section and Ay(θ) data. Pickup and knockout processes. DWBA calculations. Comparison with calculations based on statistical multistep pre-equilibrium theory.
doi: 10.1103/PhysRevC.93.034624
2016CO05 Phys.Rev. C 93, 054329 (2016) Predicted isotopic variation in surface α clustering in Sn compared with (d, 6Li) pickup yields NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(d, 6Li), E=33 MeV; analyzed number of α clusters and reduced widths θ2α(s) as function of mass number. Comparison with α-cluster preformation probability predicted by generalized relativistic mean-field model. Discussed need for (p, pα) experiments.
doi: 10.1103/PhysRevC.93.054329
2015VA04 Phys.Rev. C 91, 024614 (2015) J.J.van Zyl, A.A.Cowley, R.Neveling, E.Z.Buthelezi, S.V.Fortsch, J.Mabiala, J.P.Mira, F.Nemulodi, F.D.Smit, G.F.Steyn, J.A.Swartz, I.T.Usman Incident-energy dependence of angular distributions of cross section and analyzing power for the 58Ni (p(pol) 3He) reaction between 80 and 120 MeV NUCLEAR REACTIONS 58Ni(polarized p, 3He)56Co, E=80, 100, 118 MeV; measured 3He spectra, σ(θ), analyzing powers at cyclotron facility of iThemba LABS. 56Co; deduced levels, l-transfers, J, π, spectroscopic factors. Optical model, and macroscopic zero-range distorted-wave Born approximation (DWBA) analyses. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.024614
2014DI02 Phys.Rev. C 89, 034616 (2014) S.S.Dimitrova, A.A.Cowley, J.J.van Zyl, E.V.Zemlyanaya, K.V.Lukyanov Inclusive reaction 93Nb(p(pol), α) at an incident energy of 160 MeV NUCLEAR REACTIONS 93Nb(polarized p, α), E=160 MeV; measured Eα, Iα, double-differential σ(θ), analyzing power Ay(θ), at iThemba Laboratory. Comparison of angular distribution and analyzing power data with DWBA predictions, and with statistical multistep method calculations.
doi: 10.1103/PhysRevC.89.034616
2014DI15 Phys.Rev. C 90, 054604 (2014) S.S.Dimitrova, A.A.Cowley, E.V.Zemlyanaya, K.V.Lukyanov Pre-equilibrium mechanisms in the 93Nb(p, α) inclusive reaction at incident energies from 65 to 160 MeV NUCLEAR REACTIONS 93Nb(polarized p, α), E=100 MeV; measured Eα, Iα, σ(θ), analyzing powers Ay(θ) at iThemba LABS; analyzed previous σ(θ) and Ay(θ) previous data at 65 MeV. Comparison with predictions of statistical multistep direct emission calculations.
doi: 10.1103/PhysRevC.90.054604
2012CO12 Phys.Rev. C 85, 054622 (2012) A.A.Cowley, J.J.van Zyl, S.S.Dimitrova, E.V.Zemlyanaya, K.V.Lukyanov Mechanism of the 93Nb(p, 3He) inclusive reaction at an incident energy of 160 MeV NUCLEAR REACTIONS 93Nb(polarized p, 3He), E=160 MeV; measured 3He spectra, double differential σ(θ), vector analyzing power (VAP) as function of scattering angle, emission energy distribution of VAP. Comparison with a multistep direct theory in which a reaction mechanism based on two-nucleon pickup combined with Distorted Wave Born approximation (DWBA).
doi: 10.1103/PhysRevC.85.054622
2011CO10 Int.J.Mod.Phys. E20, 962 (2011) Quasifree α-cluster knockout from light nuclei NUCLEAR REACTIONS 9Be(p, pα), E=150 MeV; 12C(α, 2α), E=200 MeV; calculated σ(θ), relative occupation. DWIA calculations, comparison with experimental data.
doi: 10.1142/S0218301311019064
2009CO01 Europhys.Lett. 85, 22001 (2009) A.A.Cowley, J.Mabiala, E.Z.Buthelezi, S.V.Fortsch, R.Neveling, F.D.Smit, G.F.Steyn, J.J.van Zyl Analyzing power distribution in the 12C(p, pα)8Be(g.s.) reaction at an incident energy of 100 MeV NUCLEAR REACTIONS 12C(p, pα), E=101 MeV; measured cross section and analyzing power.
doi: 10.1209/0295-5075/85/22001
2009MA21 Phys.Rev. C 79, 054612 (2009) J.Mabiala, A.A.Cowley, S.V.Fortsch, E.Z.Buthelezi, R.Neveling, F.D.Smit, G.F.Steyn, J.J.Van Zyl Analyzing power and cross section distributions of the 12C(p, pα)8Be cluster knockout reaction at an incident energy of 100 MeV NUCLEAR REACTIONS 12C(polarized p, pα)8Be, E=100 MeV; measured particle spectra, (particle)(particle)-coin, σ, σ(θ), vector analyzing powers; deduced energy sharing cross sections with different optical potential model parameters and spectroscopic factors. Distorted-wave impulse approximation (DWIA) analysis.
doi: 10.1103/PhysRevC.79.054612
2008NE04 Phys.Rev. C 77, 037601 (2008); Erratum Phys.Rev. C 78, 069902 (2008) R.Neveling, A.A.Cowley, Z.Buthelezi, S.V.Fortsch, H.Fujita, G.C.Hillhouse, J.J.Lawrie, G.F.Steyn, F.D.Smit, S.M.Wyngaardt, N.T.Botha, L.Mudau, S.S.Ntshangase Analyzing power of the 40Ca(p(pol), pα) reaction at 100 MeV NUCLEAR REACTIONS 40Ca(polarized p, pα), E=100 MeV; measured analyzing powers. comparisons with model calculations. 36Ar; deduced levels, J. DWIA calculations.
doi: 10.1103/PhysRevC.77.037601
2007CO14 Phys.Rev. C 75, 054617 (2007) A.A.Cowley, J.Bezuidenhout, S.S.Dimitrova, P.E.Hodgson, S.V.Fortsch, G.C.Hillhouse, N.M.Jacobs, R.Neveling, F.D.Smit, J.A.Stander, G.F.Steyn, J.J.van Zyl Multistep direct mechanism in the (p(pol), 3He) inclusive reaction on 59Co and 93Nb at incident energies between 100 and 160 MeV NUCLEAR REACTIONS 59Co, 93Nb(polarized p, 3He), E=40-160 MeV; measured σ, angular distributions and analyzing powers. Compared results to model calculations.
doi: 10.1103/PhysRevC.75.054617
2006BU10 Eur.Phys.J. A 28, 193 (2006) E.Z.Buthelezi, F.Cerutti, E.Gadioli, G.F.Steyn, A.Pepe, S.H.Connell, A.A.Cowley Excitation functions of evaporation residues in the interaction of 16O with 103Rh at incident energies up to 400 MeV NUCLEAR REACTIONS 103Rh(16C, X), E=40-400 MeV; measured evaporation residues isotopic production σ, excitation functions. Activation technique, Monte Carlo calculations, Boltzmann Master Equation theory.
doi: 10.1140/epja/i2006-10054-4
2006MA26 Phys.Rev. C 73, 044606 (2006) H.Machner, D.G.Aschman, K.Baruth-Ram, J.Carter, A.A.Cowley, F.Goldenbaum, B.M.Nangu, J.V.Pilcher, E.Sideras-Haddad, J.P.F.Sellschop, F.D.Smit, B.Spoelstra, D.Steyn Isotopic production cross sections in proton-nucleus collisions at 200 MeV NUCLEAR REACTIONS 27Al, 59Co, 197Au(p, X), E=200 MeV; measured intermediate mass fragments isotopic production σ, σ(E, θ).
doi: 10.1103/PhysRevC.73.044606
2005AU05 Phys.Rev. C 71, 064606 (2005) A.Auce, A.Ingemarsson, R.Johansson, M.Lantz, G.Tibell, R.F.Carlson, M.J.Shachno, A.A.Cowley, G.C.Hillhouse, N.M.Jacobs, J.A.Stander, J.J.van Zyl, S.V.Fortsch, J.J.Lawrie, F.D.Smit, G.F.Steyn Reaction cross sections for protons on 12C, 40Ca, 90Zr, and 208Pb at energies between 80 and 180 MeV NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 208Pb(p, X), E=80-180 MeV; 58Ni(p, X), E=81 MeV; measured reaction σ. Comparison with model predictions.
doi: 10.1103/PhysRevC.71.064606
2005BU12 Nucl.Phys. A753, 29 (2005) E.Z.Buthelezi, F.Cerutti, E.Gadioli, G.F.Steyn, S.H.Connell, A.A.Cowley Excitation functions of residues in the interaction of 12C with 103Rh up to an incident energy of 400 MeV NUCLEAR REACTIONS 103Rh(12C, X), E=40-400 MeV; measured evaporation residues isotopic production σ, excitation functions. Activation technique, Monte Carlo calculations, Boltzmann Master Equation theory.
doi: 10.1016/j.nuclphysa.2005.02.126
2004BU09 Nucl.Phys. A734, 553 (2004) E.Z.Buthelezi, E.Gadioli, G.F.Steyn, F.Albertini, C.Birattari, M.Cavinato, F.Cerutti, S.H.Connell, A.A.Cowley, E.Fabrici, E.Gadioli Erba Incomplete fusion of projectile fragments in the interaction of 12C with 103Rh up to 33 MeV per nucleon NUCLEAR REACTIONS 103Rh(12C, X)105Ag/104Ag/101Pd/100Pd/102Rh/99Rh/97Ru/95Ru/95Tc/94Tc/93mMo/90Mo/90Nb/86Zr/87Y, E=70-400 MeV; analyzed excitation functions; deduced reaction mechanism features.
doi: 10.1016/j.nuclphysa.2004.01.103
2003BE62 Eur.Phys.J. A 18, 639 (2003) B.Becker, F.Albertini, E.Gadioli, G.F.Steyn, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, E.Sideras-Haddad Emission of Li, 7, 9Be and B fragments in the interaction of 12C with 93Nb between 200 and 400 MeV NUCLEAR REACTIONS 93Nb(12C, X), E=200-400 MeV; measured intermediate mass fragments σ(E, θ); deduced binary fragmentation contribution, other reaction mechanism features.
doi: 10.1140/epja/i2003-10091-5
2003BU21 J.Radioanal.Nucl.Chem. 258, 649 (2003) E.Z.Buthelezi, K.Aardaneh, G.F.Steyn, E.Gadioli, T.N.Van der Walt, F.Albertini, F.Cerutti, S.H.Connell, A.A.Cowley, F.M.Nortier Isobaric yields and radiochemistry of near-target residues in the interaction of 12C and 16O with 103Rh at an incident energy of 400 MeV NUCLEAR REACTIONS 103Rh(12C, X), (16O, X), E=400 MeV; measured target-like fragments isotopic production σ. Radiochemical separation.
doi: 10.1023/B:JRNC.0000011764.30879.fb
2003GA15 Eur.Phys.J. A 17, 195 (2003) E.Gadioli, G.F.Steyn, F.Albertini, C.Birattari, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, M.Pigni, J.P.F.Sellschop, E.Sideras-Haddad Emission of intermediate-mass fragments in the interaction of 16O with 59Co, 93Nb and 197Au NUCLEAR REACTIONS 59Co, 93Nb, 197Au(16O, X), E=6-25 MeV/nucleon; measured intermediate mass fragment yields, spectra, σ(E, θ); deduced reaction mechanism features.
doi: 10.1140/epja/i2003-10007-5
2003HI06 Phys.Rev. C 67, 064604 (2003) G.C.Hillhouse, J.Mano, A.A.Cowley, R.Neveling Relativistic predictions of exclusive 208Pb(p(pol), 2p)207Tl analyzing powers at an incident energy of 202 MeV NUCLEAR REACTIONS 208Pb(polarized p, 2p), E=202 MeV; calculated analyzing powers. Comparison of finite-range and zero-range approximations, relativistic and nonrelativistic approaches.
doi: 10.1103/PhysRevC.67.064604
2002GA32 Nucl.Phys. A708, 391 (2002) E.Gadioli, G.F.Steyn, C.Birattari, C.Catarisano, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, J.P.F.Sellschop, E.Sideras-Haddad Interplay of Mean Field and Nucleon-Nucleon Interactions in the Production of Carbon Fragments in 16O Induced Reactions at Incident Energies up to 25 MeV/amu NUCLEAR REACTIONS 59Co, 93Nb(16O, X), E=100, 250, 400 MeV; measured carbon fragments spectra, σ(θ); deduced projectile breakup and nucleon coalescence contributions.
doi: 10.1016/S0375-9474(02)01021-7
2002NE12 Phys.Rev. C66, 034602 (2002) R.Neveling, A.A.Cowley, G.F.Steyn, S.V.Fortsch, G.C.Hillhouse, J.Mano, S.M.Wyngaardt Analyzing Power and Cross Section Distributions of the Knockout Reaction 208Pb(p(pol), 2p)207Tl at an Incident Energy of 202 MeV NUCLEAR REACTIONS 208Pb(polarized p, 2p), E=202 MeV; measured Ep, σ(θ), Ay(θ); deduced nucleon-nucleon interaction features. Comparison with model predictions.
doi: 10.1103/PhysRevC.66.034602
2001CA23 Phys.Rev. C63, 057602 (2001) J.Carter, A.A.Cowley, H.Diesener, R.W.Fearick, S.V.Fortsch, J.J.Lawrie, P.von Neumann-Cosel, J.V.Pilcher, A.Richter, K.Schweda, F.D.Smit, G.F.Steyn, S.Strauch Role of Knockout Contributions in Giant Resonance Studies with (p, p'x) Reactions NUCLEAR REACTIONS 48Ca(p, p'n), E=100 MeV; 40Ca(p, 2p), (p, p'α), E=100 MeV; measured proton spectra, σ(θ), angular correlations. Comparison with DWIA calculations.
doi: 10.1103/PhysRevC.63.057602
2001GA47 Eur.Phys.J. A 11, 161 (2001) E.Gadioli, G.F.Steyn, C.Birattari, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, F.M.Nortier, J.P.F.Sellschop, E.Sideras-Haddad Emission of 8Begs in the Interaction of 12C with Nuclei at Incident Energies up to 33 MeV/amu NUCLEAR REACTIONS 59Co, 93Nb, 197Au(12C, X), E=100-400 MeV; measured σ(θ) vs 8Be energy for 8Be emission, break-up and coalescence contributions. Breakup mechanisms discussed.
doi: 10.1007/s100500170082
2001IN03 Nucl.Phys. A696, 3 (2001) A.Ingemarsson, G.J.Arendse, A.Auce, R.F.Carlson, A.A.Cowley, A.J.Cox, S.V.Fortsch, R.Johansson, B.R.Karlson, M.Lantz, J.Peavy, J.A.Stander, G.F.Steyn, G.Tibell Reaction Cross Sections of Intermediate Energy 3He-Particles on Targets from 9Be to 208Pb NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,118,120,124Sn, 208Pb(3He, X), E=96, 138, 167 MeV; measured reaction σ; deduced reaction mechanism features. Comparison with optical model predictions.
doi: 10.1016/S0375-9474(01)01116-2
2001SC25 Phys.Lett. 506B, 247 (2001) K.Schweda, J.Carter, A.A.Cowley, H.Diesener, R.W.Fearick, S.V.Fortsch, J.J.Lawrie, P.von Neumann-Cosel, J.V.Pilcher, A.Richter, F.D.Smit, G.F.Steyn, S.Strauch Low-Energy Isocalar Quadrupole Strength in 40Ca and 48Ca from (p, p'x) Reactions NUCLEAR REACTIONS 40Ca(p, pα), (p, 2p), 48Ca(p, np), E=100 MeV; measured σ(θ). 40,48Ca deduced B(E2) distributions vs excitation energy. Comparison with (e, e') results. DWBA analysis.
doi: 10.1016/S0370-2693(01)00230-1
2000CO28 Phys.Rev. C62, 064604 (2000) A.A.Cowley, G.F.Steyn, Y.Watanabe, T.Noro, K.Tamura, M.Kawabata, K.Hatanaka, H.Sakaguchi, H.Takeda, M.Itoh Inclusive Reaction 40Ca(p, p'x) at an Incident Energy of 392 MeV NUCLEAR REACTIONS 40Ca(p, p'X), E=392 MeV; measured proton spectra, σ(E, θ); deduced reaction mechanism features. Semiclassical distorted wave analysis.
doi: 10.1103/PhysRevC.62.064604
2000CO29 Phys.Rev. C62, 064605 (2000) A.A.Cowley, G.F.Steyn, S.S.Dimitrova, P.E.Hodgson, G.J.Arendse, S.V.Fortsch, G.C.Hillhouse, J.J.Lawrie, R.Neveling, W.A.Richter, J.A.Stander, S.M.Wyngaardt Multistep Direct Mechanism in the (p(pol), 3He) Inclusive Reaction on 59Co and 93Nb at an Incident Energy of 100 MeV NUCLEAR REACTIONS 59Co, 93Nb(polarized p, 3He), E=100 MeV; measured σ(E, θ), Ay(θ); deduced one-step, multistep process contributions, other reaction mechanism features. Comparison with model predictions.
doi: 10.1103/PhysRevC.62.064605
2000GA39 Eur.Phys.J. A 8, 373 (2000) E.Gadioli, M.Cavinato, E.Fabrici, E.Gadioli Erba, R.Bassini, C.Birattari, S.Crippa, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, F.M.Nortier, S.H.Connell, E.Sideras-Haddad, J.P.F.Sellschop, A.A.Cowley Evidence for a Dissipative Friction Mechanism Based on 8Be Fragments from the Interaction of 12C with 59Co NUCLEAR REACTIONS 59Co(12C, 8Be), E=8.3-33.3 MeV/nucleon; measured σ(θ), αα-coin. Effect of projectile break up discussed. Comparison with model predictions.
doi: 10.1007/s100500070089
1999CH50 Nucl.Phys. (Supplement) A654, 1051c (1999) M.B.Chadwick, D.T.L.Jones, G.J.Arendse, A.A.Cowley, W.A.Richter, J.J.Lawrie, R.T.Newman, J.V.Pilcher, F.D.Smit, G.F.Steyn, J.W.Koen, J.A.Stander Nuclear Interaction Cross Sections for Proton Radiotherapy NUCLEAR REACTIONS 12C(p, pX), (p, dX), E=150 MeV; 16O(p, αX), (p, tX), E=200 MeV; measured σ(E, θ). 12C, 16O(p, pX), E=200 MeV; calculated proton spectra, σ(θ). 16O(p, X)7Li/7Be/9Be/10Be/10B/11B/10C/11C/14C/13N/14O/15O, E ≈ 5-250 MeV; calculated production σ.
doi: 10.1016/S0375-9474(00)88598-X
1999GA39 Nucl.Phys. A654, 523 (1999) E.Gadioli, M.Cavinato, E.Fabrici, E.Gadioli Erba, C.Birattari, I.Mica, S.Solia, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, F.M.Nortier, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, A.A.Cowley Alpha Particle Emission in the Interaction of 12C with 59Co and 93Nb at Incident Energies of 300 and 400 MeV NUCLEAR REACTIONS 59Co, 93Nb(12C, αX), E=300, 400 MeV; measured α spectra, σ(Eα, θ); deduced reaction mechanism features.
doi: 10.1016/S0375-9474(00)88492-4
1999ST06 Phys.Rev. C59, 2097 (1999) G.F.Steyn, S.V.Fortsch, A.A.Cowley, J.J.Lawrie, G.J.Arendse, G.C.Hillhouse, J.V.Pilcher, F.D.Smit, R.Neveling α-Clustering Probabilities Extracted from the 12C(α, 2α)8Be Reaction at 200 MeV NUCLEAR REACTIONS 12C(α, 2α), E=200 MeV; measured Eα, αα-coin, σ(E, θ); deduced α-cluster spectroscopic factors. DWIA analysis.
doi: 10.1103/PhysRevC.59.2097
1998CA11 Nucl.Phys. A630, 631 (1998) J.Carter, A.A.Cowley, H.Diesener, R.W.Fearick, S.V.Fortsch, M.N.Harakeh, J.J.Lawrie, S.J.Mills, P.von Neumann-Cosel, R.T.Newman, J.V.Pilcher, A.Richter, K.Schweda, F.D.Smit, G.F.Steyn, S.Strauch, D.M.Whittal Isoscalar Quadrupole Strength in 40Ca from the (p, p'α0) Reaction at E(p) = 100 MeV NUCLEAR REACTIONS 40Ca(p, p'α), E=99.5 MeV; measured σ(θ(p), θ(α), E(x)); deduced α0 channel multipole distribution, isoscalar E2 strength distribution.
doi: 10.1016/S0375-9474(98)00656-3
1998CO13 Phys.Rev. C57, 3185 (1998) A.A.Cowley, G.J.Arendse, R.F.Visser, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, J.V.Pilcher, T.Noro, T.Baba, K.Hatanaka, M.Kawabata, N.Matsuoka, Y.Mizuno, M.Nomachi, K.Takahisa, K.Tamura, Y.Yuasa, H.Sakaguchi, T.Itoh, H.Takeda, Y.Watanabe Rescattering in Knockout Reactions as Manifested in 40Ca(p, p'p'') at an Incident Energy of 392 MeV NUCLEAR REACTIONS 40Ca(p, 2p), E=392 MeV; measured σ(E(p1), E(p2), θ); deduced reaction mechanism. DWIA analysis.
doi: 10.1103/PhysRevC.57.3185
1998ST07 Phys.Rev. C57, 1817 (1998) G.F.Steyn, S.V.Fortsch, A.A.Cowley, S.Karataglidis, R.Lindsay, J.J.Lawrie, F.D.Smit, R.T.Newman Single-Nucleon Transfer to Unbound States in the 4He(α, t)5Li Reaction at Incident Energies of 120, 160, and 200 MeV NUCLEAR REACTIONS 4He(α, t), E=120, 160, 200 MeV; measured σ(Et, θ); deduced cluster-core potential parameters. Comparison with 4He(α, 3He) results.
doi: 10.1103/PhysRevC.57.1817
1997CO05 Phys.Rev. C55, 1843 (1997) A.A.Cowley, G.J.Arendse, G.F.Steyn, J.A.Stander, W.A.Richter, S.S.Dimitrova, P.Demetriou, P.E.Hodgson Inclusive (p, 3He) Reactions on 59Co and 197Au at Incident Energies of 120, 160, and 200 MeV NUCLEAR REACTIONS 59Co, 197Au(p, 3He), E=120, 160, 200 MeV; measured σ(θ) vs E; deduced multi-step mechanisms role. Statistical multi-step direct reaction theory.
doi: 10.1103/PhysRevC.55.1843
1996CO12 Phys.Rev. C54, 778 (1996) A.A.Cowley, G.J.Arendse, J.W.Koen, W.A.Richter, J.A.Stander, G.F.Steyn, P.Demetriou, P.E.Hodgson, Y.Watanabe Inclusive (p, α) Reactions on 27Al, 59Co, and 197Au at Incident Energies of 120, 160, and 200 MeV NUCLEAR REACTIONS 27Al, 59Co, 197Au(p, α), E=120, 160, 200 MeV; measured σ(Eα, θ); deduced higher-step contributions role. Multi-step DWBA analysis.
doi: 10.1103/PhysRevC.54.778
1996RI11 Phys.Rev. C54, 1756 (1996) W.A.Richter, S.W.Steyn, A.A.Cowley, J.A.Stander, J.W.Koen, R.Lindsay, G.C.Hillhouse, R.E.Julies, J.J.Lawrie, J.V.Pilcher, P.E.Hodgson Inclusive (p, p') Reactions on Nuclei in the Mass Range 115 to 181 at Incident Energies from 120 to 200 MeV NUCLEAR REACTIONS 115In, 167Er, 173Yb, 181Ta(p, p'X), E=120, 150, 175, 200 MeV; 141Pr(p, p'X), E=120, 200 MeV; measured inclusive σ(E, θ); deduced reaction mechanism. Statistical multistep direct theory analysis.
doi: 10.1103/PhysRevC.54.1756
1996ST25 Phys.Rev. C54, 2485 (1996) G.F.Steyn, S.V.Fortsch, J.J.Lawrie, F.D.Smit, R.T.Newman, A.A.Cowley, R.Lindsay Single-Nucleon Transfer to Unbound States by Means of the 4He(α, 3He)5He Reaction at 158 and 200 MeV NUCLEAR REACTIONS 4He(α, 3He), E(cm)=158, 200 MeV; measured yield vs E(3He), 3He spectra, σ(θ). 4He(α, α), E(cm)=158, 200 MeV; measured σ(θ); deduced model parameters, strength factor. DWBA analysis.
doi: 10.1103/PhysRevC.54.2485
1995CO25 Phys.Lett. 359B, 300 (1995) A.A.Cowley, G.J.Arendse, J.A.Stander, W.A.Richter Distortion in Proton-Knockout Reactions NUCLEAR REACTIONS 208Pb(p, 2p), E=204 MeV; measured yield vs total energy, σ(θ, Ep). 208Pb deduced proton knock-out spectroscopic factors.
doi: 10.1016/0370-2693(95)01028-O
1994CO16 Phys.Rev. C50, 2449 (1994) A.A.Cowley, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, J.V.Pilcher, F.D.Smit, D.M.Whittal Quasifree Knockout in 9Be(α, 2α)5He at an Incident Energy of 197 MeV NUCLEAR REACTIONS 9Be(α, 2α), E=197 MeV; measured σ(θ1, θ2). 4He(α, α), E=197 MeV; measured σ(θ); deduced dependence of α-clustering probability, model parameters. 9Be deduced spectroscopic factors. DWIA analysis.
doi: 10.1103/PhysRevC.50.2449
1994RI01 Phys.Rev. C49, 1001 (1994) W.A.Richter, A.A.Cowley, G.C.Hillhouse, J.A.Stander, J.W.Koen, S.W.Steyn, R.Lindsay, R.E.Julies, J.J.Lawrie, J.V.Pilcher, P.E.Hodgson Preequilibrium (p, p') Measurements and Calculations for 90Zr and Neighboring Nuclei for Incident Energies up to 200 MeV NUCLEAR REACTIONS 89Y, 90Zr, 92,94,96,98Mo(p, p'), E=120, 160, 200 MeV; measured inclusive σ(E, θ); deduced reaction mechanism. Statistical multi-step, direct theory analysis.
doi: 10.1103/PhysRevC.49.1001
1994VO05 Nucl.Phys. A569, 373c (1994) P.von Neumann-Cosel, H.Diesener, U.Helm, G.Herbert, V.Huck, A.Richter, G.Schrieder, A.Stascheck, A.Stiller, J.Ryckebusch, J.Carter, A.A.Cowley, R.W.Fearick, J.J.Lawrie, S.J.Mills, R.T.Newman, J.V.Pilcher, F.D.Smit, Z.Z.Vilakazi, D.M.Whittal Excitation and Decay of Electric Giant Resonances in the 40Ca(e, e'X) and 40Ca(p, p'X) Reactions NUCLEAR REACTIONS 40Ca(e, e'p), E=57, 78, 183.5 MeV; measured σ(θ(e), Ep). 40Ca(p, p'α), E=99.1 MeV; 40Ca(e, e'α), E=183.5 MeV; measured proton, α-channel decay. 40Ca deduced electric giant resonance decay features.
doi: 10.1016/0375-9474(94)90128-7
1993FO05 Phys.Rev. C48, 743 (1993) S.V.Fortsch, A.A.Cowley, J.J.Lawrie, J.V.Pilcher, F.D.Smit, D.M.Whittal Coincident Proton Emission Induced by 200 MeV Protons on 197Au NUCLEAR REACTIONS 197Au(p, xp), E=200 MeV; measured energy sharing σ(E), pp-coin, σ(θ); deduced quasifree scattering evidence.
doi: 10.1103/PhysRevC.48.743
1992CO04 Phys.Rev. C45, 1745 (1992) A.A.Cowley, P.G.Roos, J.J.Lawrie, F.D.Smit, J.V.Pilcher, S.V.Fortsch, G.F.Steyn, G.C.Hillhouse Quasifree Subthreshold Pion Production in the Reaction 12C(p, dπ+)11B NUCLEAR REACTIONS 12C(p, dπ+), E=223 MeV; measured σ(θπ, θd, Ed); deduced reaction mechanism. DWIA.
doi: 10.1103/PhysRevC.45.1745
1992RI06 Phys.Rev. C46, 1030 (1992) W.A.Richter, A.A.Cowley, R.Lindsay, J.J.Lawrie, S.V.Fortsch, J.V.Pilcher, R.Bonetti, P.E.Hodgson Statistical Multistep Direct Calculations for (p, p') Continuum Spectra up to 200 MeV NUCLEAR REACTIONS 100Mo(p, p'), E=100-200 MeV; measured σ(θ, Ep'). 58Ni, 197Au(p, p'), E=100-200 MeV; analyzed σ(θ, Ep'). Statistical multi-step direct theory.
doi: 10.1103/PhysRevC.46.1030
1992ZU04 Nucl.Instrum.Methods Phys.Res. A321, 219 (1992) A.Zucchiatti, P.Levi Sandri, C.Schaerf, A.A.Cowley, J.V.Pilcher, L.Mazzaschi, M.Anghinolfi, N.Bianchi, L.Casano, P.Corvisiero, A.D'Angelo, E.De Sanctis, G.Gervino, B.Girolami, V.Lucherini, V.Mokeev, V.Muccifora, P.Picozza, E.Polli, A.R.Reolon, G.Ricco, M.Ripani, P.Rossi, M.Sanzone, M.Taiuti Response of BGO Sectors to Protons Up to 170 MeV
doi: 10.1016/0168-9002(92)90391-G
1991CO03 Phys.Rev. C43, 678 (1991) A.A.Cowley, A.van Kent, J.J.Lawrie, S.V.Fortsch, D.M.Whittal, J.V.Pilcher, F.D.Smit, W.A.Richter, R.Lindsay, I.J.van Heerden, R.Bonetti, P.E.Hodgson Preequilibrium Proton Emission Induced by 80 and 120 MeV Protons Incident on 90Zr NUCLEAR REACTIONS 90Zr(p, p'), E=80, 120 MeV; measured σ(Ep', θp'); deduced reaction mechanism, effective interaction strength. Phenomenological parametrization.
doi: 10.1103/PhysRevC.43.678
1991CO13 Phys.Rev. C44, 329 (1991) A.A.Cowley, J.J.Lawrie, G.C.Hillhouse, D.M.Whittal, S.V.Fortsch, J.V.Pilcher, F.D.Smit, P.G.Roos Quasifree Knockout in 16O(p, 2p)15N at an Incident Energy of 151 MeV NUCLEAR REACTIONS 16O(p, 2p), E=151 MeV; measured σ(E1, E2, θ1, θ2). 15N levels deduced spectroscopic factors. DWIA analysis.
doi: 10.1103/PhysRevC.44.329
1991FO01 Phys.Rev. C43, 691 (1991) S.V.Fortsch, A.A.Cowley, J.J.Lawrie, D.M.Whittal, J.V.Pilcher, F.D.Smit Continuum Protons from 58Ni(p, p') at Incident Energies between 100 and 200 MeV NUCLEAR REACTIONS 58Ni(p, p'), E=100-200 MeV; measured σ(Ep', θp'); deduced reaction mechanism, quasifree knockout contribution.
doi: 10.1103/PhysRevC.43.691
1990CO14 Z.Phys. A336, 189 (1990) A.A.Cowley, S.V.Fortsch, J.J.Lawrie, D.M.Whittal, F.D.Smit, J.V.Pilcher Continuum Protons from the Inclusive Reaction 197Au(p, p') at Incident Energies between 100 and 200 MeV NUCLEAR REACTIONS 197Au(p, p'X), E=100-200 MeV; measured σ(θp, Ep). Kalbach systematics analysis. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0511. 1990CO31 Europhys.Lett. 13, 37 (1990) A.A.Cowley, S.V.Fortsch, J.J.Lawrie, J.V.Pilcher, F.D.Smit, D.M.Whittal Importance of Nucleon-Nucleon Scattering in the Interaction of Protons with 197Au at 200 MeV NUCLEAR REACTIONS 197Au(p, 2p), E=200 MeV; measured σ(θ1, θ2, E1); deduced reaction mechanism. DWIA analysis.
doi: 10.1209/0295-5075/13/1/007
1990LA12 Phys.Rev. C42, 778 (1990) J.J.Lawrie, D.M.Whittal, A.A.Cowley Continuum Analyzing Power for 4He(p(pol), p') at 100 MeV NUCLEAR REACTIONS 4He(polarized p, p'), E=100 MeV; calculated analyzing power vs θ; deduced reaction mechanism. DWIA analysis.
doi: 10.1103/PhysRevC.42.778
1990WH01 Phys.Rev. C42, 309 (1990) D.M.Whittal, A.A.Cowley, J.V.Pilcher, S.V.Fortsch, F.D.Smit, J.J.Lawrie Quasifree Knockout of Charged Particles from 4He with 100 MeV Protons NUCLEAR REACTIONS 4He(p, 2p), (p, pd), (p, pt), (p, p3He), E=100 MeV; measured quasifree σ(E1, θ1, θ2). Spectroscopic factors. DWIA analysis.
doi: 10.1103/PhysRevC.42.309
1989CO17 Phys.Rev. C40, 1950 (1989) A.A.Cowley, J.V.Pilcher, J.J.Lawrie, D.M.Whittal Protons of 200 MeV Incident on 12C. II. Quasifree Proton Knockout NUCLEAR REACTIONS 12C(p, 2p), E=200 MeV; measured σ(E1, E2, θ1, θ2). 11B levels deduced spectroscopic factors. DWIA analysis.
doi: 10.1103/PhysRevC.40.1950
1989PI12 Phys.Rev. C40, 1937 (1989) J.V.Pilcher, A.A.Cowley, D.M.Whittal, J.J.Lawrie Protons of 200 MeV Incident on 12C. I. Coincident Proton Emission from the Continuum NUCLEAR REACTIONS 12C(p, 2p), E=200 MeV; measured σ(E1, E2, θ1, θ2); deduced relation to inelastic scattering.
doi: 10.1103/PhysRevC.40.1937
1988CO02 Phys.Lett. 201B, 196 (1988) A.A.Cowley, J.V.Pilcher, J.J.Lawrie, D.M.Whittal Coincident Proton Emission from the Continuum Induced by 200 MeV Protons on 12C NUCLEAR REACTIONS 12C(p, 2p), E=200 MeV; measured σ(Ep1, θp1, Ep2, θp2), σ(Ep1, θp1, θp2). Detector telescopes. Model calculations.
doi: 10.1016/0370-2693(88)90211-0
1988FO06 Nucl.Phys. A485, 258 (1988) S.V.Fortsch, A.A.Cowley, J.V.Pilcher, D.M.Whittal, J.J.Lawrie, J.C.van Staden, E.Friedland Continuum Yields from 12C(p, p') at Incident Proton Energies of 90 and 200 MeV NUCLEAR REACTIONS 12C(p, p'), E=90, 200 MeV; measured σ(E, E', θ). 12C deduced spectroscopic factors. Natural target. Comparison with quasifree knockout model.
doi: 10.1016/0375-9474(88)90101-7
1987SA01 Phys.Rev. C35, 333 (1987) C.Samanta, N.S.Chant, P.G.Roos, A.Nadasen, A.A.Cowley 16O(α, αp) and 40Ca(α, αp) Reactions at 139.2 MeV Incident Energy NUCLEAR REACTIONS 16O, 40Ca(α, pα), E=139.2 MeV; measured σ(θα, Eα, θp). 39K, 15N levels deduced spectroscopic factors. ΔE-E telescopes. DWIA calculations.
doi: 10.1103/PhysRevC.35.333
1986LA28 Z.Phys. A325, 175 (1986) J.J.Lawrie, A.A.Cowley, D.M.Whittal, S.J.Mills, W.R.McMurray Resonances in Low Energy Elastic Scattering of α-Particles from 28Si NUCLEAR REACTIONS 28Si(α, α), E=5-12 MeV; measured σ(Eα), σ(E), σ(θ). 32S deduced no quasimolecular resonance evidence. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0658. 1986SA24 Phys.Rev. C34, 1610 (1986) C.Samanta, N.S.Chant, P.G.Roos, A.Nadasen, J.Wesick, A.A.Cowley Tests of the Factorized Distorted Wave Impluse Approximation for (p, 2p) Reactions NUCLEAR REACTIONS 40Ca, 16O(p, 2p), E=76.1, 101.3 MeV; measured σ(θ1, θ2, Ep1). 39K, 15N levels deduced L, spectroscopic factors. ΔE-E telescopes. DWIA analysis.
doi: 10.1103/PhysRevC.34.1610
1985WE12 Phys.Rev. C32, 1474 (1985) J.S.Wesick, P.G.Roos, N.S.Chant, C.C.Chang, A.Nadasen, L.Rees, N.R.Yoder, A.A.Cowley, S.J.Mills, W.W.Jacobs 2H, 3,4He(p(pol), p') and 3,4He(p(pol), d') Continuum Yields for 100 and 150 MeV Protons NUCLEAR REACTIONS 2H, 3,4He(polarized p, p'), 3,4He(polarized p, d), E=100, 150 MeV; measured inclusive σ(θ), analyzing power vs θ; deduced reaction mechanism. DWIA analysis.
doi: 10.1103/PhysRevC.32.1474
1983CI02 Phys.Rev. C27, 1360 (1983) G.Ciangaru, C.C.Chang, H.D.Holmgren, A.Nadasen, P.G.Roos, A.A.Cowley, S.Mills, P.P.Singh, M.K.Saber, J.R.Hall Continuum Spectrum in the Quasifree (p, 2p) Scattering NUCLEAR REACTIONS 58Ni(p, 2p), E=198 MeV; measured σ(θ1, E2, θ2, E2); deduced reaction mechanism. DWIA calculations, quasifree particle rescattering effect.
doi: 10.1103/PhysRevC.27.1360
1982SA24 Phys.Rev. C26, 1379 (1982) C.Samanta, N.S.Chant, P.G.Roos, A.Nadasen, A.A.Cowley Discrepancy between Proton- and Alpha-Induced Cluster Knockout Reactions on 16O NUCLEAR REACTIONS 16O(p, pd), (p, pt), E=101.3 MeV; 16O(α, dα), (α, tα), (α, 3Heα), E=139.2 MeV; measured σ(E1, E2, θ1, θ2). 14,13N, 13C levels deduced L, S. DWIA analysis.
doi: 10.1103/PhysRevC.26.1379
1981NA03 Phys.Rev. C23, 2353 (1981) A.Nadasen, P.G.Roos, N.S.Chant, A.A.Cowley, C.Samanta, J.Wesick 40Ca(p, pα)36Ar Reaction in a Noncoplanar Geometry NUCLEAR REACTIONS 40Ca(p, pα), E=101.3 MeV; measured σ(θp, θα, Ep). 40Ca level deduced Sα. DWIA analysis.
doi: 10.1103/PhysRevC.23.2353
1980CO17 Phys.Rev. C22, 2633 (1980) A.A.Cowley, C.C.Chang, H.D.Holmgren Forward-Angle Proton Spectra in the Continuum from the 58Ni(p, xp) Reaction at 100 MeV NUCLEAR REACTIONS 58Ni(p, xp), E=100 MeV; measured σ(θ, Ep); deduced quasi-free nucleon-nucleon scattering effects.
doi: 10.1103/PhysRevC.22.2633
1980CO19 Phys.Rev.Lett. 45, 1930 (1980) A.A.Cowley, C.C.Chang, H.D.Holmgren, J.D.Silk, D.L.Hendrie, R.W.Koontz, P.G.Roos, C.Samanta, J.R.Wu Energy Dissipation Process for 100-MeV Protons and the Nucleon-Nucleon Interactions in Nuclei NUCLEAR REACTIONS 58Ni(p, 2p), E=100 MeV; measured pp-coin, σ(Ep1, Ep2, θ1, θ2); deduced reaction mechanism, energy dissipation process. DWIA analysis, quasifree scattering.
doi: 10.1103/PhysRevLett.45.1930
1979CO15 Nucl.Phys. A325, 83 (1979) A Study of Fluctuations in the Large-Angle Excitation Functions of the Reaction 21Ne(3He, α)20Ne (g.s.) And the Elastic Scattering of α-Particles from 20Ne NUCLEAR REACTIONS 20Ne(α, α), E=25.8, 27.0, 31 MeV; 21Ne(3He, α), E=8-14 MeV; calculated σ(E); deduced reaction mechanism causing correlated fluctuations in σ.
doi: 10.1016/0375-9474(79)90153-2
1978CO06 Phys.Rev. C17, 1322 (1978) Modified Optical Potential for Elastic α Scattering: Folding Potentials and Energy Dependence NUCLEAR REACTIONS 40Ca, 58Ni(α, α), E=140 MeV; 90Zr(α, α), E=40-140 MeV; calculated σ(θ). Modified optical potential.
doi: 10.1103/PhysRevC.17.1322
1978CO10 J.Phys.(London) G4, L149 (1978) A.A.Cowley, S.J.Mills, G.Heymann Correlation between the Forward-Angle Yield of the Reaction 16O(α, d)18F (Ex = 1.125 MeV) and Anomalous Large-Angle Elastic Scattering in 16O(α, α)16O NUCLEAR REACTIONS 16O(α, d), E=28.0-33.6 MeV; measured σ(E, θ) to lowest 5+ level in 18O. Natural solid target, DWBA analysis.
doi: 10.1088/0305-4616/4/6/009
1978CO11 Nucl.Phys. A301, 429 (1978) A.A.Cowley, J.C.van Staden, S.J.Mills, P.M.Cronje, G.Heymann, G.F.Burdzik Large-Angle Elastic Scattering of α-Particles from 20Ne and 22Ne NUCLEAR REACTIONS 20,22Ne(α, α), E=24.6-31.7 MeV; measured σ(E;θ), θ=13°-177°; deduced Regge-pole parameters. Enriched targets.
doi: 10.1016/0375-9474(78)90059-3
1978WA05 Phys.Rev. C17, 1315 (1978) N.S.Wall, A.A.Cowley, R.C.Johnson, A.M.Kobos Modified Optical Potential for the Elastic Scattering of Complex Particles NUCLEAR REACTIONS 40Ca, 58Ni, 90Zr(3He, 3He), (α, α); calculated modified optical potential.
doi: 10.1103/PhysRevC.17.1315
1977CO07 Phys.Rev. C15, 1650 (1977) A.A.Cowley, P.G.Roos, N.S.Chant, R.Woody, III, H.D.Holmgren, D.A.Goldberg (p, d3He) Reaction as a Quasifree Reaction Process NUCLEAR REACTIONS 6,7Li, 9Be, 12C(p, d3He), E=100 MeV; measured σ(Ed, E(3He), θ); deduced absolute Sα for double quasifree angle pairs.
doi: 10.1103/PhysRevC.15.1650
1977RO02 Phys.Rev. C15, 69 (1977) P.G.Roos, N.S.Chant, A.A.Cowley, D.A.Goldberg, H.D.Holmgren, R.Woody, III Absolute Spectroscopic Factors from the (p, pα) Reaction at 100 MeV on 1p-Shell Nuclei NUCLEAR REACTIONS 6,7Li, 9Be, 12C(p, pα), E=100 MeV; measured σ(Ep, Eα, θ). 6,7Li, 9Be, 12C deduced Sα. Coplanar geometry, DWIA analysis.
doi: 10.1103/PhysRevC.15.69
1975RO27 Nucl.Phys. A255, 187 (1975) P.G.Roos, S.M.Smith, V.K.C.Cheng, G.Tibell, A.A.Cowley, R.A.J.Riddle The (p, d) Reaction at 65 MeV NUCLEAR REACTIONS 12C, 14N, 16O, 40Ca, 90Zr(p, d), E=65 MeV; measured σ(Ed, θ). 11C, 13N, 15O, 39Ca, 89Zr levels deduced S.
doi: 10.1016/0375-9474(75)90157-8
1974CO08 Nucl.Phys. A220, 429 (1974) A.A.Cowley, P.G.Roos, H.G.Pugh, V.K.C.Cheng, R.Woody, III A Comparison of the 3He(p, 2p)d and 3He(p, pd)p Reactions NUCLEAR REACTIONS 3He(p, 2p), (p, pd), E=65, 85, 100 MeV; measured σ(Ep1, Ep2, θ), σ(Ep, Ed, θ); deduced reaction mechanism.
doi: 10.1016/0375-9474(74)90126-2
1974CO28 Nucl.Phys. A229, 256 (1974) A.A.Cowley, P.M.Cronje, G.Heymann, S.J.Mills, J.C.van Staden Diffraction Scattering of α-Particles from Even Isotopes of Ni at Backward Angles NUCLEAR REACTIONS 58,60,62,64Ni(α, α), (α, α'), Eα=24.3-32.3 MeV; measured σ(E;θ), θ=15-179degrees; deduced optical model parameters. 58,60,62,64Ni levels deduced β(L).
doi: 10.1016/0375-9474(74)90787-8
1973PU02 Phys.Lett. 46B, 192 (1973) H.G.Pugh, P.G.Roos, A.A.Cowley, V.K.C.Cheng, R.Woody The (p, 2p) Reaction on 2H, 3He and 4He NUCLEAR REACTIONS 2H, 3He, 4He(p, 2p), E=65, 85, 100 MeV; measured σ(Ep).
doi: 10.1016/0370-2693(73)90681-3
1973SM03 Nucl.Phys. A207, 273 (1973) S.M.Smith, G.Tibell, A.A.Cowley, D.A.Goldberg, H.G.Pugh, W.Reichart, N.S.Wall The (α, α), (α, α') and (α, 3He) Reactions on 12C at 139 MeV NUCLEAR REACTIONS 12C(α, α), (α, α'), (α, 3He), E=139 MeV; measured σ(Eα, θ), σ(E(3He), θ). 12C deduced optical potential, inelastic transition strengths, 13C deduced spectroscopic strengths.
doi: 10.1016/0375-9474(73)90347-3
1970CO13 Nucl.Phys. A146, 465 (1970) Regge Pole Analysis of the Elastic Scattering of α-Particles from 16O NUCLEAR REACTIONS 16O(α, α), E=25.4-32.2 MeV; measured σ(E;θ); deduced Regge pole parameters. Natural target.
doi: 10.1016/0375-9474(70)90740-2
1969CO19 Phys.Letters 30B, 618 (1969) Cluster-Model Interpretation of Resonances in α-Particle Elastic Scattering NUCLEAR REACTIONS 16O(α, α), E = 25-32 MeV; measured σ(E;θ). 20Ne deduced resonances, level-width. Cluster model interpretation.
doi: 10.1016/0370-2693(69)90074-4
1966CO24 Nucl.Phys. 86, 363(1966) A.A.Cowley, G.Heymann, R.L.Keizer, M.J.Scott Elastic and Inelastic Scattering of 15.8 MeV Deuterons NUCLEAR REACTIONS Be, C, O, Al, S(d, d), (d, d'), E = 15.8 MeV; measured σ(Ed', θ). Natural targets.
doi: 10.1016/0029-5582(66)90544-X
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