NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = S.Cooper Found 52 matches. 2003CO08 Nucl.Phys. A723, 45 (2003) Data-to-potential inversion for tensor polarized deuterons scattered from 4He NUCLEAR REACTIONS 4He(polarized d, d), E=4-13 MeV; analyzed σ(θ), analyzing powers; deduced potential. Iterative perturbative procedure.
doi: 10.1016/S0375-9474(03)01082-0
2000CO22 Nucl.Phys. A677, 187 (2000) S.G.Cooper, V.I.Kukulin, R.S.Mackintosh, V.N.Pomerantsev An Inversion Procedure for Coupled-Channel Scattering: Determining the deuteron-nucleus tensor interaction NUCLEAR REACTIONS 58Ni(d, d'), E=56 MeV; 4He(d, d'), E=8-13 MeV; 56Fe(d, d'), E=30 MeV; calculated scattering potential. 4He(d, d'), E=10 MeV; calculated σ(θ), analyzing powers. S-matrix to potential inversion procedure, coupled channels approach.
doi: 10.1016/S0375-9474(00)00309-2
1999CO11 Phys.Rev. C59, 2361 (1999) S.G.Cooper, V.I.Kukulin, R.S.Mackintosh, V.N.Pomerantsev Spin 1 Inversion: A Majorana tensor force for deuteron alpha scattering NUCLEAR REACTIONS 4He(polarized d, d'), E ≈ 10 MeV; analyzed σ(θ), tensor analyzing powers; deduced tensor interaction. S-matrix to potential inversion.
doi: 10.1103/PhysRevC.59.2361
1999KU21 Yad.Fiz. 62, No 7, 1187 (1999); Phys.Atomic Nuclei 62, 1114 (1999) V.I.Kukulin, V.N.Pomerantsev, S.G.Cooper, R.S.Mackintosh Majorana Tensor FOrce for Deuteron-Nucleus Interactions NUCLEAR REACTIONS 4He(d, d), E not given; analyzed data; deduced parity-dependent tensor component in internucleus interaction. Coupled-channel inversion technique.
1999MA02 Nucl.Phys. A645, 399 (1999) R.S.Mackintosh, S.G.Cooper, V.I.Kukulin Determination of 6Li-4He Interaction from Multi-Energy Scattering Data NUCLEAR REACTIONS 4He(polarized 6Li, 6Li), E=19.6, 27.7, 37.5 MeV; analyzed σ(θ), vector analyzing power vs theta; deduced interaction potential. Energy dependent components, Majorana terms.
doi: 10.1016/S0375-9474(98)00623-X
1999SH12 Phys.Rev.Lett. 82, 1109 (1999) R.W.Shaw, J.P.Young, S.P.Cooper, O.F.Webb Spontaneous Ultraviolet Emission from 233Uranium/229Thorium Samples RADIOACTIVITY 233U(α); measured photon spectrum; deduced N2 electric discharge origin of ultraviolet emission.
doi: 10.1103/PhysRevLett.82.1109
1998CO17 Phys.Rev. C58, R31 (1998) S.G.Cooper, V.I.Kukulin, R.S.Mackintosh, E.V.Kuznetsova New Technique for Phase Shift Analysis: Multienergy Solution of Inverse Scattering Problem NUCLEAR REACTIONS 4He(polarized d, d), E=3-12 MeV; analyzed σ(θ), iT11(θ); deduced phase shifts. Direct inversion from multienergy data to potentials.
doi: 10.1103/PhysRevC.58.R31
1998KU12 Phys.Rev. C57, 2462 (1998) V.I.Kukulin, V.N.Pomerantsev, S.G.Cooper, S.B.Dubovichenko Improved d + 4He Potentials by Inversion: The tensor force and validity of the double folding model NUCLEAR REACTIONS 4He(d, X), E not given; calculated interaction potentials; deduced double folding model validity.
doi: 10.1103/PhysRevC.57.2462
1998MA48 J.Phys.(London) G24, 1599 (1998) Using Inverse Scattering Methods to Study Inter-Nucleus Potentials NUCLEAR REACTIONS 4He(polarized d, d), E=3-11.5 MeV; calculated σ(θ), iT11(θ). Iterative-perturbative method, applications to exotic nuclei discussed.
doi: 10.1088/0954-3899/24/8/039
1997CO09 Nucl.Phys. A618, 87 (1997) Energy-Dependent Inversion of p + 16O Scattering Data NUCLEAR REACTIONS 16O(polarized p, p), E=27.3-46.1 MeV; analyzed σ(θ), analyzing power data. Iterative procedures, energy-dependent inversion procedures.
doi: 10.1016/S0375-9474(97)00055-9
1997CO27 Nucl.Phys. A626, 715 (1997) Antisymmetry and Channel Coupling Contributions to the Absorption for p + α/d + 3He NUCLEAR REACTIONS 4He(p, p), 3He(d, d), E not given; calculated interaction potentials; deduced channel coupling contributions.
doi: 10.1016/S0375-9474(97)00476-4
1997MA24 J.Phys.(London) G23, 565 (1997) The Energy Dependence of the Nucleon-Nucleus Potential NUCLEAR REACTIONS 16O(n, n), E=4-20 MeV; 40Ca(n, n), E=12-20 MeV; calculated nucleon-nucleus potential vs E; deduced energy-dependent inversion procedure related features. Comparison between different approaches.
doi: 10.1088/0954-3899/23/5/009
1997MA63 Nucl.Phys. A625, 651 (1997) Deuteron-α Interaction by Inversion of RGM S-Matrix: Determination of spin-orbit potential for spin-one projectile NUCLEAR REACTIONS 4He(d, d), E(cm)=17-55 MeV; calculated potential; deduced spin-orbit role. Iterative-perturbative procedure.
doi: 10.1016/S0375-9474(97)00495-8
1996CO20 Phys.Rev. C54, 3133 (1996) Energy Dependent Potentials Determined by Inversion: The p + α potential up to 65 MeV NUCLEAR REACTIONS 16O(p, p), E not given; calculated zero energy potentials. 4He(p, p), E ≤ 65 MeV; calculated phase shifts vs E; deduced zero energy potentials. Inversion of resonating group methods phase shifts.
doi: 10.1103/PhysRevC.54.3133
1995CO01 Nucl.Phys. A582, 283 (1995) 11Li + 28Si and 11Li + 12C Elastic Scattering Studied by Inversion NUCLEAR REACTIONS 28Si(11Li, 11Li), E=319 MeV; 12C(11Li, 11Li), E=637 MeV; analyzed σ(θ). Inversion technique, two-step phenomenology.
doi: 10.1016/0375-9474(94)00477-5
1995CO18 Nucl.Phys. A592, 338 (1995) Quantitative Contribution of Antisymmetry to the Nucleon-Nucleus Potential NUCLEAR REACTIONS 4He(p, p), E(cm)=50 MeV; 3He(p, p), E(cm)=10-40 MeV; 3H(n, n), E(cm)=14.63-17.25 MeV; 6Li(n, n), E(cm)=8.57, 12 MeV; 16O(n, n), E=10-30 MeV; 40Ca(n, n), E=10, 30 MeV; calculated local equivalent potentials to single configuration RGM S-matricies. Iterative-pertubative inversion techniques.
doi: 10.1016/0375-9474(95)00310-W
1995CO32 Nucl.Instrum.Methods Phys.Res. A354, 408 (1995) P.Colling, A.Nucciotti, C.Bucci, S.Cooper, P.Ferger, M.Frank, U.Nagel, F.Probst, W.Seidel Low-Energy X-Ray Detection in Cryogenic Detectors with Tungsten Thermometers NUCLEAR REACTIONS 27Al, V, Ti(X, X), E=radioactive source; measured fluorescence X-ray spectra; deduced detector resolution, other features. Cryogenic detectors with W thermometers. ATOMIC PHYSICS 27Al, V, Ti(X, X), E=radioactive source; measured fluorescence X-ray spectra; deduced detector resolution, other features. Cryogenic detectors with W thermometers.
doi: 10.1016/0168-9002(94)01080-3
1995LI07 Phys.Rev. C51, 2268 (1995) Application of an Iterative-Perturbative Inversion Potential Model to Capture and Bremsstrahlung Reactions NUCLEAR REACTIONS, ICPND 3He(α, γ), E=0.1-4 MeV; calculated dipole capture σ(E), astrophysical S-factor vs E. 4He(α, γ), E ≈ 6-16 MeV; calculated σ(θ1, θ2) vs E. Iterative-perturbative inversion potential model.
doi: 10.1103/PhysRevC.51.2268
1995MA37 Nucl.Phys. A589, 377 (1995) Exchange Contributions to Nucleus-Nucleus Potentials Deduced from RGM Phase Shifts Using Inversion NUCLEAR REACTIONS 3He(α, α), E(cm)=60 MeV; 16O(α, α), E(cm)=18 MeV; 3H(α, α), E(cm)=20 MeV; calculated resonating group method phase shifts; deduced potentials.
doi: 10.1016/0375-9474(95)00171-V
1994CO08 Phys.Rev. C50, 359 (1994) Potentials by Inversion of 3He + α Phase Shifts and Bound State Energies in 7Be NUCLEAR REACTIONS 4He(3He, 3He), E=2-12 MeV; calculated phase shifts vs E; deduced potential. Inversion techniques. NUCLEAR STRUCTURE 7Be; calculated levels. Single channel resonating group method, potential from inversion techniques.
doi: 10.1103/PhysRevC.50.359
1994CO10 Phys.Rev. C50, 1308 (1994) S.G.Cooper, R.S.Mackintosh, A.Csoto, R.G.Lovas Local 4He-p Potentials from Resonating-Group Method Phase Shifts NUCLEAR REACTIONS 4He(p, p), E ≤ 20 MeV; calculated phase shifts vs E; deduced phase equivalent potentials, local potentials comparison. Multi-channel resonating group method.
doi: 10.1103/PhysRevC.50.1308
1994CO14 Nucl.Phys. A576, 308 (1994) 16O + 16O Elastic Scattering at 350 MeV Studied by Inversion NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; analyzed σ(θ). Two-step method including inversion.
doi: 10.1016/0375-9474(94)90261-5
1994CR02 Phys.Rev. C49, 1091 (1994) R.Crespo, R.C.Johnson, J.A.Tostevin, R.S.Mackintosh, S.G.Cooper Equivalent Local Potentials to Multiple Scattering Calculations of Nucleon-Nucleus Scattering NUCLEAR REACTIONS 16O(p, p), E=100, 135, 200 MeV; calculated local phase equivalent potentials. Multiple scattering expansion of the optical potential.
doi: 10.1103/PhysRevC.49.1091
1994FE03 Phys.Lett. 323B, 95 (1994) P.Ferger, P.Colling, S.Cooper, D.Dummer, M.Frank, U.Nagel, A.Nucciotti, F.Probst, W.Seidel A Massive Cryogenic Particle Detector with Good Energy Resolution RADIOACTIVITY 55Fe(EC); measured X-ray spectra; deduced detector energy resolution. Massive cryogenic particle detector.
doi: 10.1016/0370-2693(94)00043-3
1994RA06 Phys.Rev. C49, 1621 (1994) G.H.Rawitscher, D.Lukaszek, R.S.Mackintosh, S.G.Cooper Local Representation of the Exchange Nonlocality in n-16O Scattering NUCLEAR REACTIONS 16O(n, n), E=20, 50 MeV; analyzed σ(θ). Microscopic folding model, exchange nonlocality local representation.
doi: 10.1103/PhysRevC.49.1621
1993AI02 Nucl.Phys. A561, 285 (1993) S.Ait-Tahar, R.S.Mackintosh, S.G.Cooper Local Representation of a Deep Parity and l-Dependent 16O + 20Ne Potential NUCLEAR REACTIONS 20Ne(16O, 16O), E=24.5 MeV; calculated σ(θ). Interative perturbative inversion method.
doi: 10.1016/0375-9474(93)90154-P
1993AI03 Nucl.Phys. A562, 101 (1993) S.Ait-Tahar, R.S.Mackintosh, S.G.Cooper, T.Wada Energy Dependence of a Local Equivalent Potential for RGM Phase Shifts for 16O + 16O NUCLEAR REACTIONS 16O(16O, 16O), E=30-500 MeV; calculated σ(θ). Local equivalent potential for resonating group method phase shifts.
doi: 10.1016/0375-9474(93)90034-U
1993MA09 Phys.Rev. C47, 1716 (1993) Studying the 16O + 12C Dynamic Polarization Potential by Inversion NUCLEAR REACTIONS 12C(16O, 16O), E=168-311 MeV; calculated σ(θ); deduced dynamic polarization features. Coupled-channels, continuum discretized coupled-channels S-matricies, S(l)-V(r) inversion.
doi: 10.1103/PhysRevC.47.1716
1993MC01 Nucl.Phys. A552, 401 (1993) M.A.McEwan, S.G.Cooper, R.S.Mackintosh Elastic-Scattering Phenomenology by Inversion: (I). 12C + 12C from 140 to 2400 MeV NUCLEAR REACTIONS 12C(12C, 12C), E=0.14-2.4 GeV; calculated σ(θ); deduced potential parameters. Local internuclear potential, two-step procedure.
doi: 10.1016/0375-9474(93)90501-N
1992AI01 Nucl.Phys. A542, 499 (1992) S.Ait-Tahar, S.G.Cooper, R.S.Mackintosh An l-Independent Representation of Deep l-Dependent 16O + 16O Potential NUCLEAR REACTIONS 16O(16O, 16O), E=30-150 MeV; calculated l-independent equivalents of l-dependent potentials.
doi: 10.1016/0375-9474(92)90108-V
1992CO01 Phys.Rev. C45, 770 (1992) S.G.Cooper, M.A.McEwan, R.S.Mackintosh Elastic Scattering Phenomenology by Inversion: 16O on 12C at 608 MeV NUCLEAR REACTIONS 12C(16O, 16O), E=608 MeV; calculated model parameters. Optical model, S-matrix approach, inversion techniques.
doi: 10.1103/PhysRevC.45.770
1991CO05 Phys.Rev. C43, 1001 (1991) Proton-4He Potential Derived from Phase Shifts NUCLEAR REACTIONS 4He(p, p), E=0-23 MeV; analyzed phase shifts; deduced parity dependent potential. Iterative-perturbative inversion analysis.
doi: 10.1103/PhysRevC.43.1001
1990CO11 Nucl.Phys. A511, 29 (1990) Nucleon Wavefunctions for Elastic Scattering in the Presence of Dynamically Induced Non-Locality NUCLEAR REACTIONS 40Ca(p, p), E=30.3 MeV; 48Ca(p, p), E=65 MeV; calculated dynamic polarization potential.
doi: 10.1016/0375-9474(90)90025-H
1990CO15 Nucl.Phys. A513, 373 (1990) The O + Pb Interaction Near the Coulomb Barrier NUCLEAR REACTIONS 208Pb(16O, 16O), E=80-102 MeV; calculated interaction potential parameters. Inversion procedure.
doi: 10.1016/0375-9474(90)90103-S
1990CO29 Nucl.Phys. A517, 285 (1990) S-Matrix to Potential Inversion of Low-Energy α-12C Phase Shifts NUCLEAR REACTIONS 12C(α, α), E < inelastic threshold; calculated phase shift vs E.
doi: 10.1016/0375-9474(90)90036-L
1990CO38 Z.Phys. A337, 357 (1990) An l-Independent Representation of a Majorana Potential NUCLEAR REACTIONS 20Ne(α, α), E=54.1 MeV; calculated σ(θ). S-matrix equivalent to parity dependent potential.
1989CO11 Phys.Rev. C40, 502 (1989) p-4He Scattering: Inversion of phase shifts at 64.9 MeV NUCLEAR REACTIONS 4He(p, p), E=64.9 MeV; analyzed phase shift; deduced Schrodinger, Dirac potentials parameters.
doi: 10.1103/PhysRevC.40.502
1989MA25 Nucl.Phys. A494, 123 (1989) Studing the Heavy-Ion Dynamic Polarization Potential NUCLEAR REACTIONS 12C(16O, 16O), E=139.2 MeV; calculated potential parameters. Dynamic polarization potential.
doi: 10.1016/0375-9474(89)90201-7
1988KE06 Phys.Rev. C38, 2461 (1988) Comment on ' Model Wave Functions for the Deuteron ' NUCLEAR STRUCTURE 2H; analyzed deuteron wave function model; deduced tensor potential role.
doi: 10.1103/PhysRevC.38.2461
1988MA05 Nucl.Phys. A476, 287 (1988) R.S.Mackintosh, S.G.Cooper, A.A.Ioannides Apparent Emissive Effects in Local Optical Potentials NUCLEAR REACTIONS 16O(p, p), E=34.1 MeV; calculated real, imaginary potentials; deduced emissive effect role.
doi: 10.1016/0375-9474(88)90485-X
1988MA30 Nucl.Phys. A483, 173 (1988) R.S.Mackintosh, A.A.Ioannides, S.G.Cooper Stationary State Currents in Nuclear Reactions: Rotational coupling in alpha-particle scattering NUCLEAR REACTIONS 20Ne(α, α), E=104 MeV; calculated potentials. Stationary state currents.
doi: 10.1016/0375-9474(88)90530-1
1988MA31 Nucl.Phys. A483, 195 (1988) R.S.Mackintosh, A.A.Ioannides, S.G.Cooper Stationary State Currents in Proton Scattering: Alternative representation of ' emissive ' potentials NUCLEAR REACTIONS 16O, 40Ca(p, p), E=34.1 MeV; calculated potentials. Stationary state currents.
doi: 10.1016/0375-9474(88)90531-3
1987CO27 Nucl.Phys. A472, 101 (1987) S.G.Cooper, R.S.Mackintosh, A.A.Ioannides Systematics of the Pickup Contribution to the Nucleon-Nucleus Interaction NUCLEAR REACTIONS 40Ca(p, p), (n, n), E=30.3-65 MeV; 48Ca(p, p), (n, n), E=65 MeV; calculated potential parameters. 48Ca(polarized p, p), E=65 MeV; calculated σ(θ), analyzing power vs θ. Finite-range coupled reaction channel model.
doi: 10.1016/0375-9474(87)90222-3
1987MA39 Nucl.Phys. A472, 85 (1987) R.S.Mackintosh, S.G.Cooper, A.A.Ioannides Do We Understand Deuteron Scattering at all ( Question ): The polarization potential due to mass-three channels NUCLEAR REACTIONS 40Ca(d, d), E=52, 80, 200 MeV; calculated potential parameters, S-matrix elements. Effective local polarization potential.
doi: 10.1016/0375-9474(87)90221-1
1986CO11 J.Phys.(London) G12, 869 (1986) A DWBA Analysis for 14N(7Li, t)18F(*) to Study α Clustering in 18F NUCLEAR REACTIONS 14N(7Li, t), E=36 MeV; calculated σ(θ). 18F levels deduced spectroscopic factors. DWBA, Merchant-Rowley structure model.
doi: 10.1088/0305-4616/12/9/011
1986CO15 J.Phys.(London) G12, 371 (1986) Analysis of the DWBA for (7Li, t) Reactions Producing α-Cluster States in 16O and 20Ne NUCLEAR REACTIONS 16O, 20Ne(7Li, t), E=34, 38 MeV; calculated σ(θ); 16O, 20Ne deduced α-cluster level spectroscopic factors. DWBA analysis.
doi: 10.1088/0305-4616/12/5/004
1986CO17 J.Phys.(London) G12, L291 (1986) S.G.Cooper, M.W.Kermode, L.J.Allen Optical Potential for 12 - 12C Scattering at 1016 MeV Obtained by Inversion NUCLEAR REACTIONS 12C(12C, 12C), E=1016 MeV; calculated potential parameters vs ion-ion separation distance. Inverse scattering method, WKB approximation.
doi: 10.1088/0305-4616/12/12/005
1986KE11 Phys.Lett. 174B, 357 (1986) M.W.Kermode, S.G.Cooper, S.Klarsfeld A Positive Short Range Tensor Model for the Deuteron NUCLEAR STRUCTURE 2H; calculated binding energy, quadrupole moment, rms radius. Positive short range tensor model.
doi: 10.1016/0370-2693(86)91015-4
1982CO20 J.Phys.(London) G8, 1689 (1982) S.G.Cooper, R.Huby, D.Kelvin, J.R.Mines Test of a Theory for Stripping to Unbound Levels with More than One Open Channel NUCLEAR REACTIONS 12C(3He, d), E=36 MeV; calculated σ(θ, Ed). Multi-channel continuum, DWBA.
doi: 10.1088/0305-4616/8/12/011
1976BI05 Phys.Rev.Lett. 36, 942 (1976) J.A.Bistirlich, S.Cooper, K.M.Crowe, F.T.Shively, E.R.Grilly, J.P.Perroud, R.H.Sherman, H.W.Baer, P.Truol Photon Spectrum in Pion Capture on Tritium NUCLEAR REACTIONS 3H(π-, 3nγ), E=200 MeV/c; measured pair spectra; deduced no evidence for bound trineutron. 3H deduced relative capture branching ratio.
doi: 10.1103/PhysRevLett.36.942
1975BA52 Phys.Rev. C12, 921 (1975) H.W.Baer, J.A.Bistirlich, N.de Botton, S.Cooper, K.M.Crowe, P.Truol, J.D.Vergados Excitation of Giant Magnetic and Spin-Isospin Dipole States in Radiative π Capture on 14N and 10B NUCLEAR REACTIONS 10B, 14N(π-, γ); measured γ-spectrum. 10Be, 14C levels deduced γ-branching.
doi: 10.1103/PhysRevC.12.921
1974BA44 Phys.Rev. C10, 1140 (1974) H.W.Baer, J.A.Bistirlich, N.de Botton, S.Cooper, K.M.Crowe, P.Truol, J.D.Vergados Radiative Pion Capture in 209Bi NUCLEAR REACTIONS 209Bi(π-, γ); measured σ(E, Eγ). 209Pb deduced levels, γ-width.
doi: 10.1103/PhysRevC.10.1140
Back to query form Note: The following list of authors and aliases matches the search parameter S.Cooper: , S.G.COOPER, S.P.COOPER |