NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Raynal Found 23 matches. 2005RA14 Phys.Rev. C 71, 057602 (2005) Spin-orbit transition interactions
doi: 10.1103/PhysRevC.71.057602
2003QU02 Phys.Rev. C 67, 067601 (2003) J.M.Quesada, R.Capote, A.Molina, M.Lozano, J.Raynal Analytical expressions for the dispersive contributions to the nucleon-nucleus optical potential
doi: 10.1103/PhysRevC.67.067601
1998DO16 Phys.Rev. C58, 2249 (1998) P.J.Dortmans, K.Amos, S.Karataglidis, J.Raynal Microscopic Model Analyses of the Elastic Scattering of 65 MeV Protons from Targets of Diverse Mass NUCLEAR REACTIONS 6,7,9,11Li, 11B, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 40Ar, 40,42,44,48Ca, 46,48,50Ti, 52Cr, 54,56Fe, 59Co, 89Y, 90Zr, 98,100Mo, 118Sn, 144,152,154Sm, 160Gd, 164Dy, 166,168Er, 174,176Yb, 178,180Hf, 182,184W, 192Os, 208Pb, 209Bi, 232Th, 238U(polarized p, p), E=65 MeV; calculated σ(θ), Ay(θ). Comparison with data. Nonlocal coordinate space optical potentials.
doi: 10.1103/PhysRevC.58.2249
1995LE38 Ann.Phys.(New York) 239, 243 (1995) A.Le Yaouanc, L.Oliver, J.-C.Raynal High-Order Expansion of the Energy Eigenvalues of a Relativistic Coulomb Equation
doi: 10.1006/aphy.1995.1034
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
1992FR09 Phys.Rev. D45, 259 (1992) J.-M.Frere, J.Galand, A.Le Yaouanc, L.Oliver, O.Pene, J.-C.Raynal Neutron Electric Dipole Moment in Left-Right-Symmetric Models NUCLEAR STRUCTURE 1n; calculated QCD corrections to dominant left-right exchange contribution to electric dipole moment.
doi: 10.1103/PhysRevD.45.259
1991AB02 Phys.Lett. 256B, 508 (1991) A.Abada, J.Galand, A.Le Yaouanc, L.Oliver, O.Pene, J.-C.Raynal Cancellation of the Neutron Electric Dipole Moment in Quark Model Calculations of Baluni's CP Violating Strong Interaction NUCLEAR STRUCTURE 1n; calculated electric dipole moment cancellation; deduced potential dependence. Quark models.
doi: 10.1016/0370-2693(91)91799-2
1991KI05 Z.Phys. A339, 489 (1991) J.Kiener, G.Gsottschneider, H.J.Gils, H.Rebel, V.Corcalciuc, S.K.Basu, G.Baur, J.Raynal Investigation of Sequential Break-Up Mode 6Li → 6Li(*) (3+1) → α + d of 156 MeV 6Li Projectiles on 208Pb in the Very Forward Angular Hemisphere NUCLEAR REACTIONS 208Pb(6Li, 6Li), (6Li, 6Li'), E=156 MeV; measured σ(θ), dα-coin following projectile breakup; deduced breakup mechanism.
doi: 10.1007/BF01288432
1990RA21 Aust.J.Phys. 43, 9 (1990) Which Potentials have to be Surface Peaked to Reproduce Large Angle Proton Scattering at High Energy ( Question ) NUCLEAR REACTIONS 40Ca(polarized p, p), E=497, 800 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ; deduced model parameters. Dirac, Schrodinger formalism.
1990SH26 Phys.Rev. C42, 1592 (1990) S.Shim, B.C.Clark, E.D.Cooper, S.Hama, R.L.Mercer, L.Ray, J.Raynal, H.S.Sherif Comparison of Relativistic and Nonrelativistic Approaches to the Collective Model Treatment of p + 40Ca Inelastic Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=497.5 MeV; calculated σ(θ), analyzing power, spin rotation function vs θ. Dirac, Schrodinger coupled-channels formalisms.
doi: 10.1103/PhysRevC.42.1592
1989AM05 Aust.J.Phys. 42, 591 (1989) Deformation and Spin 1 Effects NUCLEAR REACTIONS 13C(polarized p, p), E=547 MeV; calculated σ(θ), analyzing power vs θ. Nonrelativistic optical model potential.
doi: 10.1071/PH890591
1989RA03 Phys.Lett. 218B, 403 (1989) J.Raynal, H.S.Sherif, A.M.Kobos, E.D.Cooper, J.I.Johansson Dirac Coupled Channel Calculations and Nucleon Scattering at Large Momentum Transfer NUCLEAR REACTIONS 40Ca(polarized p, p), E=800 MeV; calculated σ(θ), analyzing power vs θ. Dirac coupled-channels method.
doi: 10.1016/0370-2693(89)91435-4
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
1987RA18 Phys.Lett. 196B, 7 (1987) Ambiguity on the Imaginary Potentials in the Dirac Formalism for the Elastic and the Inelastic Scattering of Nucleons NUCLEAR REACTIONS, MECPD 40Ca(p, p), (p, p'), E=497 MeV; calculated σ(θ), analyzing power, polarization; deduced model parameters. Dirac formalism.
doi: 10.1016/0370-2693(87)91666-2
1985BA74 Nucl.Phys. A437, 93 (1985) A.Baeza, B.Bilwes, R.Bilwes, J.Diaz, J.L.Ferrero, J.Raynal Inelastic Scattering of 32S on 28Si NUCLEAR REACTIONS 28Si(32S, 32S), (32S, 32S'), E=77, 90, 97.09 MeV; measured σ(θ); deduced reaction mechanism, total σ. 28Si levels deduced excitation σ.
doi: 10.1016/0375-9474(85)90228-3
1984BA61 Phys.Lett. 149B, 73 (1984) A.Baeza, J.Diaz, J.L.Ferrero, B.Bilwes, R.Bilwes, J.Raynal Mutual Excitation of 32S + 28Si at 90 and 97.09 MeV NUCLEAR REACTIONS 28Si(32S, 32S), (32S, 32S'), E=90, 97.01 MeV; measured σ(θ), (Q)-value spectra; deduced simultaneous, sequential excitation amplitude interference, surface shape roles. Coupled-channels analysis.
doi: 10.1016/0370-2693(84)91554-5
1981RA08 Phys.Rev. C23, 2571 (1981) Recurrence Relations for Distorted-Wave Born Approximation Coulomb Excitation Integrals and Their use in Coupled Channel Calculations NUCLEAR REACTIONS 74Ge, 28Si(16O, 16O'), E=56 MeV; 238U(p, p'), E=22 MeV; calculated σ(θ). DWBA, recurrence relations for Coulomb integrals.
doi: 10.1103/PhysRevC.23.2571
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
1973KU11 Phys.Lett. 45B, 184 (1973) A.B.Kurepin, R.M.Lombard, J.Raynal Method for Identification of the Nuclear Collective Modes NUCLEAR REACTIONS 148,152Sm(polarized p, p'), E=24.5 MeV; measured nothing, calculated A(θ).
doi: 10.1016/0370-2693(73)90177-9
1973LO12 Phys.Rev.Lett. 31, 1015 (1973) Polarized-Proton Inelastic Scattering on 32S and Possible Evidence for A Hexadecapole Phonon State NUCLEAR REACTIONS 32S(p, p'), E=24.5 MeV; measured σ(Ep', θ), A(θ).
doi: 10.1103/PhysRevLett.31.1015
1972BA52 Nucl.Phys. A189, 353 (1972) G.Bassani, N.Saunier, B.M.Traore, J.Raynal, A.Foti, G.Pappalardo Optical-Model Analysis of 6Li Elastic Scattering NUCLEAR REACTIONS 11B, 12C, 13C(6Li, 6Li), E=28 MeV; measured σ(θ); deduced optical potentials. Self-supporting enriched 11B, 13C targets. Natural 12C target.
doi: 10.1016/0375-9474(72)90300-4
1972LO07 C.R.Acad.Sci., Ser.B 274, 761 (1972) R.Lombard, H.Kamitsubo, J.Raynal, J.Gosset Etude des Etats Collectifs de 32S et de 34S par Diffusion Inelastique de Protons Polarises NUCLEAR REACTIONS 32,34S(polarized p, p'), E=24.5 MeV; analyzed σ(θ), analyzing power(θ); deduced optical model parameters. 32,34S levels deduced deformation parameters β(L).
1961RA12 J.Phys.Radium 22, 560 (1961) NUCLEAR STRUCTURE 1H; measured not abstracted; deduced nuclear properties.
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