NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = R.de Swiniarski Found 63 matches. 2000BA18 Phys.Rev. C61, 037302 (2000) F.T.Baker, L.Bimbot, G.Edwards, C.Glashausser, A.Green, K.W.Jones, D.Mihailidis, D.Read, A.Sethi, B.H.Storm, Jr., R.de Swiniarski Spin Excitations in the 40Ca(p(pol), p(pol)') Reaction Revisited NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319 MeV; measured σ(E, θ), spin flip probabilities. Comparison with RPA, DWIA calculations.
doi: 10.1103/PhysRevC.61.037302
1996DE31 Nuovo Cim. 109A, 85 (1996) Study of Nuclear Deformation Parameters in the 12C(p, p')12C(*) Reaction between 200 and 800 MeV Through Dirac Coupled-Channel Calculations NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=200-800 MeV; analyzed σ(θ), analyzing power vs θ; deduced model parameters. 12C levels deduced deformation parameters. Dirac coupled-channels formalism.
doi: 10.1007/BF02734431
1996KA01 Phys.Rev. C53, 838 (1996) S.Karataglidis, P.J.Dortmans, K.Amos, R.de Swiniarski Multi-(h-bar)ω Shell Model Analyses of Elastic and Inelastic Proton Scattering from 14N and 16O NUCLEAR REACTIONS 14N, 16O(e, e), 16O(e, e'), E not given; calculated form factors. 12C(polarized p, p), (polarized p, p'), E=160 MeV; 14N(polarized p, p), (polarized p, p'), E=160 MeV; 16O(polarized p, p), (polarized p, p'), E=200 MeV; calculated σ(θ), analyzing power vs θ. Microscopic DWA, large space shell model wave functions.
doi: 10.1103/PhysRevC.53.838
1996KA65 Aust.J.Phys. 49, 645 (1996) S.Karataglidis, P.J.Dortmans, K.Amos, R.de Swiniarski Inelastic Proton Scattering Analyses and Ambiguities in Spin-Parity Assignments of States in 12C NUCLEAR REACTIONS 12C(polarized p, p'), E=200, 398 MeV; analyzed σ(θ, Ep'), A(y)(θ, Ep'). 12C deduced levels probable J, π. Fully microscopic distorted wave approximation.
doi: 10.1071/PH960645
1995DE32 Phys.Rev. C52, 1110 (1995) R.de Swiniarski, C.Glashausser, K.Jones, D.L.Pham Dirac Analysis of Deformation Parameters in the 12C(polarized p, p')12C Reaction NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=200-800 MeV: analyzed σ(θ), analyzing power vs θ. Relativistic Dirac coupled-channels calculations.
doi: 10.1103/PhysRevC.52.1110
1995DO31 Phys.Rev. C52, 3224 (1995) P.J.Dortmans, S.Karataglidis, K.Amos, R.de Swiniarski Fully Microscopic Model Analysis of the Elastic and Inelastic Scattering of Protons from 12C and for Energies in the Range 200 to 800 MeV NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=200-800 MeV; calculated σ(θ), analyzing power vs θ. DWA, medium modified effective two nucleon interactions.
doi: 10.1103/PhysRevC.52.3224
1995KA24 Phys.Rev. C52, 861 (1995) S.Karataglidis, P.J.Dortmans, K.Amos, R.de Swiniarski Fully Microscopic Model of 200 MeV Proton-12C Elastic and Inelastic Scattering NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=200 MeV; calculated σ(θ), analyzing power vs θ. 12C(e, e), (e, e'), E not given; calculated form factors. Fully microscopic model, realistic effective NN-interaction from Brueckner-Bethe-Goldstone equations.
doi: 10.1103/PhysRevC.52.861
1995PH02 Nuovo Cim. 108A, 401 (1995) Microscopic and Dirac Macroscopic Analyses of Elastic and Inelastic Scatterings of 135 MeV and 800 MeV Polarized Protons from 16O NUCLEAR REACTIONS 16O(polarized p, p), (polarized p, p'), E=135, 800 MeV; analyzed σ(θ), analyzing power vs θ data; deduced model parameters. Microscopic, Dirac macroscopic analyses.
doi: 10.1007/BF02787064
1994JO07 Phys.Rev. C50, 1982 (1994) K.W.Jones, C.Glashausser, R.de Swiniarski, F.T.Baker, T.A.Carey, J.R.Comfort, W.Cornelius, J.L.Escudie, M.Gazzaly, A.Green, M.Haji-Saeid, N.Hintz, G.Igo, J.B.McClelland, J.M.Moss, S.Nanda, C.A.Whitten Energy Dependence of the 12C(p, p')12C(*) Reaction from 200 to 800 MeV NUCLEAR REACTIONS 12C(polarized p, p'), E=200-800 MeV; measured σ(E, θ), analyzing power vs (E, θ). DWIA analysis.
doi: 10.1103/PhysRevC.50.1982
1994PH02 Nuovo Cim. 107A, 1405 (1994) Dirac Microscopic and Macroscopic Analyses of Elastic and Inelastic Scatterings of 800 MeV Polarized Protons from 12C and 16O NUCLEAR REACTIONS 12C, 16O(polarized p, p), (polarized p, p'), E=800 MeV; analyzed σ(θ), analyzing power vs θ. Microscopic macroscopic Dirac analysis.
doi: 10.1007/BF02775779
1993DE31 Nuovo Cim. 106A, 1119 (1993) R.De Swiniarski, F.T.Baker, A.Scott, C.Glashausser, K.W.Jones Elastic and Inelastic Scattering of 0.8 GeV Polarized Protons from 18O NUCLEAR REACTIONS 18O(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 18O level deduced L. Dirac equation based coupled-channels calculation.
doi: 10.1007/BF02773499
1992DE31 Z.Phys. A343, 179 (1992) R.de Swiniarski, D.L.Pham, J.Raynal Comparison of Higher Order Deformations in Several s-d Shell Nuclei Obtained through Schrodinger or Dirac Coupled-Channel Analysis of 800 MeV Polarized Protons Inelastic Scattering Experiments NUCLEAR REACTIONS 16O, 20Ne, 26,24Mg(polarized p, p'), E=800 MeV; analyzed σ(θ), analyzing power data. 16O, 20Ne, 24,26Mg deduced deformation parameters. Schrodinger, Dirac coupled-channel analyses comparison.
doi: 10.1007/BF01291822
1990DE26 Phys.Rev. C42, 1137 (1990) R.de Swiniarski, D.Beatty, E.Donoghue, R.W.Fergerson, M.Franey, M.Gazzaly, C.Glashausser, N.Hintz, K.W.Jones, J.B.McClelland, S.Nanda, M.Plum Comparison of Schrodinger and Dirac Coupled-Channels Analyses of the 28Si(p, p')28Si Reaction at 500 MeV NUCLEAR REACTIONS 28Si(polarized p, p), (polarized p, p'), E=500 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. Schrodinger, Dirac coupled-channels analyses.
doi: 10.1103/PhysRevC.42.1137
1990PH01 Z.Phys. A335, 37 (1990) Evidence for a Real Tensor Potential in the Inelastic Scattering of 800 MeV Polarized Protons from 20Ne Using the Dirac Phenomenology NUCLEAR REACTIONS 20Ne(polarized p, p), E=800 MeV; calculated σ(θ), analyzing power vs θ. Coupled-channels, Dirac phenomenology.
1990PH02 Nuovo Cim. 103A, 375 (1990) Dirac Optical-Model Analysis of Polarized Protons Elastic Scattering from 12C, 16,18O, 20Ne and 24,26Mg at 800 MeV NUCLEAR REACTIONS 12C, 16,18O, 20Ne, 24,26Mg(polarized p, p), E=800 MeV; analyzed σ(θ), analyzing power data; deduced model parameters. Dirac optical model.
doi: 10.1007/BF02790020
1988AM03 Nucl.Phys. A485, 653 (1988) K.Amos, R.de Swiniarski, L.Berge A Study of the Isoscalar Dipole Excitation (7.12 MeV) in 16O NUCLEAR REACTIONS 16O(polarized p, p), (polarized p, p'), E=135, 800 MeV; calculated σ(θ), analyzing power vs θ. 16O deduced level excitation mechanism.
doi: 10.1016/0375-9474(88)90559-3
1988BL08 Phys.Rev. C37, 1987 (1988) G.S.Blanpied, B.G.Ritchie, M.L.Barlett, G.W.Hoffmann, J.A.McGill, E.C.Milner, K.W.Jones, S.K.Nanda, R.de Swiniarski Elastic and Inelastic Scattering of 0.8 GeV Polarized Protons from 24Mg and 26Mg NUCLEAR REACTIONS 24,26Mg(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ. 24,26Mg deduced levels, L, deformation lengths, β(l).
doi: 10.1103/PhysRevC.37.1987
1988DE31 Nuovo Cim. 99A, 117 (1988) On the Spin-Orbit Deformation in Inelastic Scattering of Polarized Protons at Intermediate Energy NUCLEAR REACTIONS 16,18O(polarized p, p'), E=0.8 GeV; 12C(polarized p, p'), E=0.398, 0.697 MeV; calculated σ(θ), analyzing power vs θ. Coupled-channels method.
doi: 10.1007/BF02735217
1988DE35 Phys.Lett. 213B, 247 (1988) R.De Swiniarski, D.L.Pham, J.Raynal Dirac Coupled-Channels Analysis of Inelastic Scattering of 800 MeV Polarized Protons from 16O, 24Mg and 26Mg NUCLEAR REACTIONS 26,24Mg, 16O(polarized p, p), (polarized p, p'), E=800 MeV; calculated σ(θ), analyzing power vs θ. Coupled-channels, Dirac phenomenology.
doi: 10.1016/0370-2693(88)91755-8
1987PH01 Z.Phys. A326, 309 (1987) Analysis of the 12C + 12C Inelastic Scattering in the Energy Region 11-24 MeV/n NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=11-24 MeV/nucleon; calculated σ(θ); deduced optical model parameters. Coupled-channels theory.
1986JO01 Phys.Rev. C33, 17 (1986) K.W.Jones, C.Glashausser, R.de Swiniarski, S.Nanda, T.A.Carey, W.Cornelius, J.M.Moss, J.B.McClelland, J.R.Comfort, J.-L.Escudie, M.Gazzaly, N.Hintz, G.Igo, M.Haji-Saeid, C.A.Whitten, Jr. Energy Dependence of Deformation Parameters in the 12C(p(pol), p')12C Reaction NUCLEAR REACTIONS 12C(polarized p, p'), E=200-700 MeV; measured σ(θ), A(θ); deduced deformation lengths, optical model parameters. 12C deduced β2, β3, β4. Coupled channels analysis.
doi: 10.1103/PhysRevC.33.17
1984HA50 Phys.Rev. C30, 1795 (1984) G.Haouat, Ch.Lagrange, R.de Swiniarski, F.Dietrich, J.P.Delaroche, Y.Patin Nuclear Deformations of 24Mg, 28Si, and 32S from Fast Neutron Scattering NUCLEAR REACTIONS 24Mg, 28Si, 32S(n, n), (n, n'), E=9.76, 14.83 MeV; measured σ(En), σ(θ); deduced optical model parameters. 24Mg, 28Si, 32S deduced deformation parameters β2, β4, deformation lengths. Compound nucleus, coupled-channels model analyses.
doi: 10.1103/PhysRevC.30.1795
1984PH02 Nuovo Cim. 83A, 294 (1984) Optical-Model Analysis for 800 MeV Polarized-Proton Elastic Scattering from 12C, 16,18O, 20Ne and 24,26Mg NUCLEAR REACTIONS 12C, 16,18O, 20Ne, 24,26Mg(polarized p, p), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters.
doi: 10.1007/BF02902603
1983JO08 Phys.Lett. 128B, 281 (1983) K.W.Jones, C.Glashausser, S.Nanda, R.de Swiniarski, T.A.Carey, W.Cornelius, J.M.Moss, J.B.McClelland, S.J.Seestrom-Morris, J.R.Comfort, J.-L.Escudie, M.Gazzaly, N.Hintz, G.Igo, M.Haji-Saeid, C.A.Whitten Study of the 18.30 and 19.40 MeV States in 12C in Intermediate Energy Proton Scattering NUCLEAR REACTIONS 12C(p, p'), (polarized p, p'), E=398, 597, 698 MeV; measured σ(θ), analyzing power, spin-flip probabilities vs momentum transfer. 12C levels deduced J, π, T. DWIA analysis, shell model wave functions.
doi: 10.1016/0370-2693(83)90260-5
1983LA22 Nucl.Phys. A407, 233 (1983) G.La Rana, G.Nebbia, E.Tomasi, C.Ngo, X.S.Chen, S.Leray, P.Lhenoret, R.Lucas, C.Mazur, M.Ribrag, C.Cerruti, S.Chiodelli, A.Demeyer, D.Guinet, J.L.Charvet, M.Morjean, A.Peghaire, Y.Pranal, L.Sinopoli, J.Uzureau, R.De Swiniarski Linear Momentum Transfer Investigated in the 20Ne + 197Au and 209Bi Systems at 30 MeV/u NUCLEAR REACTIONS 197Au, 209Bi(20Ne, F), E=30 MeV/nucleon; measured fission (fragment)(fragment)-correlation, σ(fragment A), σ(fragment E); deduced fission σ, most probable projectile to nucleus linear momentum transfer. Monte Carlo simulation.
doi: 10.1016/0375-9474(83)90317-2
1983NE06 Z.Phys. A311, 247 (1983) G.Nebbia, E.Tomasi, C.Ngo, X.S.Chen, G.La Rana, S.Leray, P.Lhenoret, R.Lucas, C.Mazur, M.Ribrag, C.Cerruti, S.Chiodelli, A.Demeyer, D.Guinet, J.L.Charvet, M.Morjean, Y.Pranal, A.Peghaire, L.Sinopoli, J.Uzureau, R.de Swiniarski Investigation of Linear Momentum Transfer on the 20Ne + 197Au System at 30 MeV/A NUCLEAR REACTIONS 197Au(20Ne, F), E=30 MeV/nucleon; measured fission (fragment)(fragment)(θ), (fragment)(fragment)(φ); deduced projectile to fissioning nucleus momentum transfer. Tof telescope, solid state detectors.
doi: 10.1007/BF01415111
1982GL08 Phys.Lett. 116B, 215 (1982) C.Glashausser, R.De Swiniarski, K.Jones, S.Nanda, F.T.Baker, M.Grimm, V.Penumetcha, A.Scott, G.Adams, G.Igo, G.W.Hoffmann, J.Moss, W.Swenson, B.E.Wood Coupled-Channels Analysis of 800 MeV Polarized Proton Inelastic Scattering from 18O NUCLEAR REACTIONS 18O(polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 18O deduced β2, β4, β6. Coupled-channels analysis.
doi: 10.1016/0370-2693(82)90328-8
1980QU01 Z.Phys. A298, 37 (1980) P.Quentin, I.Brissaud, R.de Swiniarski The Determination of Hexadecapole Deformation Parameters in Actinide Nuclei and Their Variation Near the Nuclear Surface NUCLEAR STRUCTURE 238U; calculated nuclear density; deduced hexadecapole deformation β dependence on nuclear surface. Self-consistent calculation, Skyrme forces.
doi: 10.1007/BF01416026
1979BR27 Z.Phys. A293, 1 (1979) I.Brissaud, G.Berrier-Ronsin, J.Cameron, R.Frascaria, J.Kalifa, G.Bagieu, R.de Swiniarski Determination of the Multipole Deformation Parameters of 238U by 22 MeV Proton Inelastic Scattering NUCLEAR REACTIONS 238U(p, p'), E=22 MeV; measured σ(θ). 238U levels deduced β2, β4, β6. Coupled-channels analysis.
1979DE11 Can.J.Phys. 57, 540 (1979) R.de Swiniarski, Dinh-Lien Pham, G.Bagieu, H.V.Geramb Elastic and Inelastic Scattering of 40 MeV Polarized Protons from 90Zr and 92Zr NUCLEAR REACTIONS 90,92Zr(polarized p, p), (polarized p, p'), E=40 MeV; measured σ(θ), A(θ). Microscopic, macroscopic, DWBA analysis, coupled-channels calculations with vibrational model.
1979PH05 Z.Phys. A291, 327 (1979) Spin-Orbit Deformation in the Inelastic Scattering of Polarized Protons from 12C and 16O NUCLEAR REACTIONS 12C, 16O(polarized p, p), (polarized p, p'), E=20, 30, 40 MeV; calculated σ(θ), A(θ); deduced energy dependence of spin-orbit deformation. Coupled-channels collective model.
doi: 10.1007/BF01408382
1978BA75 Helv.Phys.Acta 51, 680 (1978) A.D.Bacher, H.E.Conzett, R.de Swiniarski, F.G.Resmini, T.A.Tombrello Analysis of 3He + 3He Elastic Scattering between 18 and 70 MeV with the Resonating Group Method of Brown and Tang NUCLEAR REACTIONS 4He(3He, 3He), E=18-70 MeV; measured σ(θ). Phase shift analysis, resonating-group calculations. Gas target.
1978DE28 Phys.Lett. 79B, 47 (1978) R.de Swiniarski, D.-L.Pham, G.Bagieu Inelastic Scattering of 40 MeV Polarized Protons Exciting the Low-Lying 2+ States in 90Zr and 92Zr NUCLEAR REACTIONS 90,92Zr(polarized p, p'), E=40 MeV; measured σ(θ), A(θ). 90,92Zr, 2+ levels deduced ratio of spin-orbit, central potential deformation parameters.
doi: 10.1016/0370-2693(78)90432-X
1978FU06 Phys.Rev. C18, 621 (1978) C.B.Fulmer, G.Mariolopoulos, G.Bagieu, A.J.Cole, R.de Swiniarski, D.H.Koang Scattering of 41-MeV α Particles and 46-MeV 3He from 27Al, 28Si, 29Si, and 30Si NUCLEAR REACTIONS 27Al, 28,29,30Si(3He, 3He), E=46 MeV; 27Al, 28,29,30Si(α, α), E=41 MeV; measured σ(θ). 27Al, 28,29,30Si deduced β2. Optical model, DWBA analysis.
doi: 10.1103/PhysRevC.18.621
1977DE03 Can.J.Phys. 55, 43 (1977) R.de Swiniarski, Dinh-Lien Pham, G.Bagieu Elastic and Inelastic Scattering of 30 MeV Polarized Protons from 90Zr, 92Zr, and 92Mo NUCLEAR REACTIONS 90,92Zr, 92Mo(polarized p, p), (polarized p, p'), E=30 MeV; measured σ(Ep', θ), A(θ). 90,92Zr, 92Mo levels deduced β.
doi: 10.1139/p77-006
1977PH02 Nuovo Cim. 41A, 543 (1977) Optical-Model Analysis for 30 MeV Polarized-Proton Elastic Scattering NUCLEAR REACTIONS 10,11B, 12C, 16O, 19F, 20,21Ne, 24Mg, 28Si, 32S(polarized p, p), E=30 MeV; analyzed σ(θ), A(θ); deduced optical model parameters.
doi: 10.1007/BF02730197
1976DE09 Phys.Lett. 61B, 37 (1976) R.De Swiniarski, G.Bagieu, M.Massaad, D.-L.Pham, M.Bedjidian, J.Y.Grossiord, M.Gusakow, J.R.Pizzi, C.B.Fulmer Macroscopic and Microscopic Model Analysis of Inelastic Scattering of 30 MeV Polarized Protons from 90,92Zr and 92Mo NUCLEAR REACTIONS 90,92Zr, 92Mo(polarized p, p'), E=30 MeV; measured σ(Ep', θ), A(θ) to levels in 90,92Zr, 92Mo.
doi: 10.1016/0370-2693(76)90555-4
1976DE12 Nucl.Phys. A261, 111 (1976) R.de Swiniarski, F.G.Resmini, D.L.Hendrie, A.D.Bacher Study of 16O, 20Ne, 22Ne, 28Si and 32S by Inelastic Scattering of Polarized Protons NUCLEAR REACTIONS 16O, 20,22Ne, 28Si, 32S(polarized p, p); measured σ(θ), A(θ); deduced form of spin-orbit potential. 20,22Ne, 28Si, 32S deduced deformation parameters. Optical model, coupled-channels analysis.
doi: 10.1016/0375-9474(76)90044-0
1976DE15 Helv.Phys.Acta 49, 227 (1976) R.de Swiniarski, F.G.Resmini, C.Glashausser, A.D.Bacher Study of 10B by Inelastic Scattering of 30.3 MeV Protons NUCLEAR REACTIONS 10B(p, p'), E=30.3 MeV; measured σ(Ep', θ). 10B deduced levels, L, J, π, β.
1976DE16 Helv.Phys.Acta 49, 241 (1976) R.de Swiniarski, J.Sherman, D.L.Hendrie, C.Glashausser, A.D.Bacher Study of Higher Excited States in 20Ne by Inelastic Scattering of 24.5 MeV Protons NUCLEAR REACTIONS 20Ne(p, p'), E=24.5 MeV; measured σ(Ep', θ). 20Ne deduced levels, J, π, β.
1976DE28 J.Phys.(Paris) 37, 1125 (1976) R.de Swiniarski, G.Bagieu, D.-L.Pham, M.Massaad, J.Y.Grossiord, A.Guichard Inelastic Scattering of 30 MeV Polarized Protons from 112Cd NUCLEAR REACTIONS 112Cd(polarized p, p), E=30 MeV; measured A(θ), σ(θ), deduced optical model parameters. 112Cd(polarized p, p'), E=30 MeV; measured σ(Ep', θ), A(θ). 112Cd deduced level configuration.
doi: 10.1051/jphys:0197600370100112500
1976DE29 Lett.Nuovo Cim. 16, 391 (1976) Studies of the Quadrupole and Hexadecapole Moments of 32S Through Inelastic Scattering of 17.5 MeV Protons and 30.3 MeV Polarized Protons NUCLEAR REACTIONS 32S(polarized p, p), E=17.5, 24.5, 30.3 MeV; analyzed σ; deduced optical model parameters. 32S deduced β2, β4.
doi: 10.1007/BF02750278
1975MA25 Phys.Lett. 57B, 139 (1975) R.S.Mackintosh, R.De Swiniarski A Folding Model Analysis of Inelastic Helion Scattering from 20Ne NUCLEAR REACTIONS 20Ne(3He, 3He'), E=68 MeV; calculated σ(E(3He'), θ). 20Ne deduced deformation β, quadrupole moment.
doi: 10.1016/0370-2693(75)90008-8
1974DE05 J.Phys.(Paris), Suppl.Lett. 35, L-25 (1974) R.de Swiniarski, G.Bagieu, A.J.Cole, P.Gaillard, A.Guichard, J.Y.Grossiord, M.Gusakow, J.R.Pizzi Confirmation of Hexadecapole Deformation in 20Ne from Scattering of 68 MeV 3He Particles NUCLEAR REACTIONS 20Ne(3He, 3He'), E=68 MeV; measured σ(E(3He), θ). 20Ne levels deduced hexadecapole deformation β4.
doi: 10.1051/jphyslet:0197400350302500
1974DE46 Can.J.Phys. 52, 2422 (1974) R.de Swiniarski, A.Genoux-Lubain, G.Bagieu, J.F.Cavaignac Multipole Deformations in 19F and in the Neon Isotopes and Electric Multipole Strength in 19F from Inelastic Scattering of 30 MeV Protons NUCLEAR REACTIONS 19F, 20,21,22Ne(p, p'), E=30 MeV; measured σ(Ep', θ). 19F, 20,21,22Ne levels deduced β, transition strengths.
1974GA16 J.Phys.(Paris) 35, 329 (1974) P.Gaillard, A.Guichard, J.Y.Grossiord, M.Gusakow, J.R.Pizzi, G.Bagieu, A.J.Cole, R.de Swiniarski Etude des Niveaux du 52Mn par Reaction (α, d) sur le 50Cr NUCLEAR REACTIONS 50Cr(α, d), E=31.2 MeV; measured σ(Ed, θ). 52Mn deduced levels, L.
doi: 10.1051/jphys:01974003504032900
1974GR02 Phys.Rev.Lett. 32, 173 (1974) J.Y.Grossiord, C.Coste, A.Guichard, M.Gusakow, A.K.Jain, J.R.Pizzi, G.Bagieu, R.de Swiniarski Study of Deuteron-Cluster Deformation Using the Reaction 6Li(d, tp)4He NUCLEAR REACTIONS 6Li(d, tp), E=27, 29.5 MeV; measured σ(Et, Ep, θ).
doi: 10.1103/PhysRevLett.32.173
1973DE06 Phys.Lett. 43B, 27 (1973) R.de Swiniarski, A.Genoux-Lubain, G.Bagieu, J.F.Cavaignac, D.H.Worledge, J.Raynal A Coupled-Channels Analysis of 30 MeV Proton Scattering from Low-Lying Positive-Parity States in 19F, 20Ne, 21Ne NUCLEAR REACTIONS 19F, 20,21Ne(p, p'), E=30 MeV; measured σ(θ). 19F, 20,21Ne deduced hexadecapole deformations β4.
doi: 10.1016/0370-2693(73)90535-2
1973DE27 Can.J.Phys. 51, 1293 (1973) R.de Swiniarski, H.E.Conzett, C.R.Lamontagne, B.Frois, R.J.Slobodrian Excitation of the Ground-State Rotational Band in 28Si by Inelastic Scattering of 25.25 MeV Polarized Protons NUCLEAR REACTIONS 28Si(polarized p, p'), E=25.25 MeV; measured σ(θ). Analyzing power. 28Si level deduced β2.
1973LA23 Phys.Lett. 45B, 465 (1973) C.R.Lamontagne, B.Frois, R.J.Slobodrian, H.E.Conzett, C.Leemann, R.De Swiniarski The Scattering of Polarized Protons from Si in the Giant Resonance Region of 29P NUCLEAR REACTIONS 28Si(p, p), E=17-29 MeV; measured σ(E;θ), A(θ).
doi: 10.1016/0370-2693(73)90645-X
1972BA83 Phys.Rev.Lett. 29, 1331 (1972) A.D.Bacher, F.G.Resmini, H.E.Conzett, R.de Swiniarski, H.Meiner, J.Ernst Observation of High-Lying Levels in 8Be from α-α Elastic Scattering NUCLEAR REACTIONS 4He(α, α), E=30-70 MeV; measured σ(E;θ); deduced phase shifts. 8Be deduced levels, J, π.
doi: 10.1103/PhysRevLett.29.1331
1972DE13 C.R.Acad.Sci., Ser.B 274, 506 (1972) Determination de la Deformation du 12C par Diffusion Inelastique de Protons Polarises NUCLEAR REACTIONS 12C(polarized p, p'), E=20, 20.3 MeV; analyzed σ(θ), P(θ). 12C deduced deformation parameter β2.
1972DE18 Phys.Rev.Lett. 28, 1139 (1972) R.de Swiniarski, A.D.Bacher, F.G.Resmini, G.R.Plattner, D.L.Hendrie Determination of Deformation Parameters of 20Ne and 22Ne by Inelastic Scattering of Polarized Protons NUCLEAR REACTIONS 20,22Ne(polarized p, p'), E=24.5 MeV; measured σ(θ), analyzing power(θ). 20,22Ne deduced deformation parameters β(L).
doi: 10.1103/PhysRevLett.28.1139
1970BA41 Nucl.Phys. A153, 409 (1970) A.D.Bacher, R.L.McGrath, J.Cerny, R.de Swiniarski, J.C.Hardy, R.J.Slobodrian The (3He, 6He) Reaction on 6Li and 7Li NUCLEAR REACTIONS 6,7Li(3He, 6He), E=53.2 MeV; measured σ(E(6He)) at θ=14.1°. 4Li deduced no T=2 states. Enriched target.
doi: 10.1016/0375-9474(70)90779-7
1970BL03 Phys.Rev. C1, 444 (1970) A.G.Blair, C.Glashausser, R.de Swiniarski, J.Goudergues, R.Lombard, B.Mayer, J.Thirion, P.Vaganov Excitation of Collective States in Light Nuclei by Inelastic Scattering of 20.3-MeV Polarized Protons NUCLEAR REACTIONS 12C, 16O, 24Mg, 26Mg, 27Al, 28Si, 40Ca(polarized p, p), (polarized p, p'), E=20.3 MeV; measured asymmetry, σ(θ). 24Mg, 28Si, 40Ca deduced deformation parameters β(L).
doi: 10.1103/PhysRevC.1.444
1969BA29 Phys.Letters 29B, 573 (1969) A.D.Bacher, F.G.Resmini, R.J.Slobodrian, R.De Swiniarski, H.Meiner, W.M.Tivol Observation of the 3He(p, n)3p Reaction at 25 MeV NUCLEAR REACTIONS 3He(p, n)3p, E=25 MeV; measured σ(En).
doi: 10.1016/0370-2693(69)90300-1
1969DE15 Phys.Rev.Letters 23, 317 (1969) R.de Swiniarski, C.Glashausser, D.L.Hendrie, J.Sherman, A.D.Bacher, E.A.McClatchie Evidence for Y4 Deformation in 20Ne and Other s-d Shell Nuclei NUCLEAR REACTIONS 20Ne(p, p'), E=24.5 MeV; 24Mg, 28Si, 32S(p, p'), E=17.5 MeV; measured σ(θ). 20Ne, 24Mg, 28Si, 32S deduced deformation parameters. Reanalysis of data.
doi: 10.1103/PhysRevLett.23.317
1969GL05 Phys.Rev. 184, 1217 (1969) C.Glashausser, R.de Swiniarski, J.Goudergues, R.M.Lombard, B.Mayer, J.Thirion Elastic and Inelastic Scattering of 20.3-MeV Polarized Protons from 90Zr, 92Zr, and 92Mo NUCLEAR REACTIONS 90,92Zr, 92Mo(polarized p, p), (p, p'), E = 20.3 MeV; measured σ(θ), Q, P(θ); deduced optical model parameters.
doi: 10.1103/PhysRev.184.1217
1968BL11 Izv.Akad.Nauk SSSR, Ser.Fiz. 32, 813 (1968);Bull.Acad.Sci.USSR, Phys.Ser. 32, 750 (1969) A.G.Blair, P.A.Vaganov, C.Glashausser, J.Goudergues, R.M.Lombard, B.Mayer, R.de Swiniarski, J.Thirion Asymmetry in the Distribution of Polarized 20 MeV Protons Elastically and Inelastically Scattered from 24Mg, 25Mg, 26Mg, 27Al and 28Si NUCLEAR REACTIONS 24Mg, 25Mg, 26Mg, 27Al, 28Si(p, p), (p, p'), E=20 MeV; measured σ(θ), P(θ); deduced optical model parameters.
1967GL06 Phys.Rev. 164, 1437 (1967) C.Glashausser, R.De Swiniarski, J.Thirion, A.D.Hill Inelastic-Scattering Studies with Polarized Protons NUCLEAR STRUCTURE 48Ti, 50Ti, 56Fe, 54Fe, 52Cr, 58Ni, 62Ni, 63Cu, 64Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.164.1437
1967KO04 Nucl.Phys. A94, 513 (1967) P.Kossanyi-Demay, R.De Swiniarski, C.Glashausser An Optical-Model Analysis of 18.6 MeV Proton Elastic Scattering NUCLEAR REACTIONS 48Ti, 50Ti, 52Cr, 54Fe, 56Fe, 58Ni, 62Ni, 63Cu, 64Ni(polarized p, p), E = 18.6 MeV; 52Cr, 60Ni, 62Ni(polarized p, p), E = 16.5 MeV; measured σ(θ), polarization (θ). Enriched targets.
doi: 10.1016/0375-9474(67)90428-9
1966GA05 Phys.Letters 21, 73 (1966) A.Garin, C.Glashausser, A.Papineau, R.De Swiniarski, J.Thirion Asymmetry in Elastic and Inelastic Scattering of Polarized Protons from 48Ti, 50Ti, 54Fe and 56Fe NUCLEAR STRUCTURE 48Ti, 50Ti, 56Fe, 54Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91347-3
1960BO26 J.Phys.Radium 21, 819 (1960) R.Bouchez, H.Beaumevielle, J.Fleury, P.Perrin, R.De Swiniarski, M.Chabre NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
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