NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Dinh-Lien Pham Found 27 matches. 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
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
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
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
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
1991PH01 Nuovo Cim. 104A, 1455 (1991) Comparison of Dirac and Schrodinger Coupled-Channel Analyses of Elastic and Inelastic Scatterings of 135 MeV Polarized Protons from 16O NUCLEAR REACTIONS 16O(polarized p, p), (polarized p, p'), E=135 MeV; calculated σ(θ), analyzing power vs θ. 16O levels deduced deformation parameters. Dirac, Schrodinger equations, coupled-channels analysis.
doi: 10.1007/BF02817427
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
1989BE14 Phys.Rev.Lett. 62, 2593 (1989) E.J.Beise, G.Dodson, M.Garcon, S.Hoibraten, C.Maher, D.L.Pham, R.P.Redwine, W.Sapp, K.E.Wilson, S.A.Wood, M.Deady Measurement of 16O(γ, n)15O at Medium Energies NUCLEAR REACTIONS 16O(γ, n), E=150, 200, 250 MeV; measured σ(θ). Recoil proton spectrometer.
doi: 10.1103/PhysRevLett.62.2593
1989GE04 Phys.Rev.Lett. 63, 734 (1989) D.F.Geesaman, R.Gilman, M.C.Green, R.J.Holt, J.P.Schiffer, B.Zeidman, G.Garino, M.Saber, R.E.Segel, E.J.Beise, G.W.Dodson, S.Hoibraten, D.L.Pham, R.P.Redwine, W.W.Sapp, C.F.Williamson, S.A.Wood, N.S.Chant, P.G.Roos, J.D.Silk, M.Deady, X.K.Maruyama Proton Propagation in Nuclei Studied in the A Dependence of the (e, e'p) Reaction in the Quasifree Region NUCLEAR REACTIONS 12C, 27Al, 58Ni, 181Ta(e, e'p), E=780 MeV; measured σ(θ(e'), θp) vs missing energy; deduced proton mean free path.
doi: 10.1103/PhysRevLett.63.734
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.
1986GI15 Phys.Rev.Lett. 57, 2637 (1986) S.Gilad, S.Hoibraten, W.J.Burger, G.W.Dodson, D.L.Pham, R.P.Redwine, E.Piasetzky, H.W.Baer, J.D.Bowman, F.H.Cverna, M.J.Leitch, U.Sennhauser, Th.S.Bauer, C.D.Q.Ingram, G.S.Kyle, D.Ashery, S.A.Wood, Z.Fraenkel Measurement of the Reaction 16O(π+, π0p) NUCLEAR REACTIONS 16O(π+, π0p), E=245 MeV; measured σ(θπ), πp-coin, σ(θp, E(π), θ(π)); deduced σ(π+, π+p)/σ(π+, π0p). Proton telescopes, pion spectrometer. Isobar-hole model calculations.
doi: 10.1103/PhysRevLett.57.2637
1986PH01 Nuovo Cim. 92A, 194 (1986) Optical-Model Analysis of the Elastic Scattering of 12C + 12C in the Energy Range (11-24) MeV/Nucleon NUCLEAR REACTIONS 12C(12C, 12C), E=11-24 MeV/nucleon; analyzed σ(θ); deduced model parameters.
doi: 10.1007/BF02727189
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
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
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
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
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
1976PH01 J.Phys.(Paris), Lett. 37, L-67 (1976) Investigation of the Quadrupole Deformation of 11B by Means of 30 MeV Polarized Proton Inelastic Scattering NUCLEAR REACTIONS 11B(polarized p, p'), E=30 MeV; analyzed σ(Ep', θ), A(θ). 11B deduced quadrupole deformation β2.
doi: 10.1051/jphyslet:0197600370406700
1972LI01 Nucl.Phys. A178, 375 (1972) Diffusion Deuton-Deuton avec des Deutons Polarises NUCLEAR REACTIONS 2H(d, d), 8-12 MeV; calculated σ(E;θ), P(E;θ). polarized beam, helicity formalism.
doi: 10.1016/0375-9474(72)90466-6
1972PH07 Nucl.Phys. A189, 665 (1972) Diffusion Deuton-Deuton dans le Cas de la Non Conservation du Spin de la Voie NUCLEAR REACTIONS 2H(d, d), calculated σ(θ), iT11(θ).
doi: 10.1016/0375-9474(72)90320-X
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