NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = C.Lagrange Found 20 matches. 2003HI21 Ann.Phys.(New York) 306, 209 (2003) S.Hilaire, Ch.Lagrange, A.J.Koning Comparisons between various width fluctuation correction factors for compound nucleus reactions NUCLEAR REACTIONS 88Sr, 93Nb(n, n), (n, γ), E=0.001-6 MeV; calculated elastic and capture σ. 239Pu(n, n), (n, n'X), (n, F), E=0.001-10 MeV; calculated elastic, inelastic, and fission σ. Comparison of width fluctuation correction factors.
doi: 10.1016/S0003-4916(03)00076-9
1989CL08 Phys.Rev. C40, 2527 (1989) T.B.Clegg, G.Haouat, J.P.Delaroche, Ch.Lagrange, J.Chardine, M.T.McEllistrem, S.E.Hicks, G.R.Shen Dynamics of Collective Excitations in 190,192Os and 194Pt Observed by 8 MeV Neutron Scattering NUCLEAR REACTIONS 190,192Os, 194Pt(n, n), (n, n'), E=8 MeV; measured σ(θ); deduced model parameters. 190Os, 194Pt deduced deformation features.
doi: 10.1103/PhysRevC.40.2527
1986HA44 Phys.Rev. C34, 2075 (1986) L.F.Hansen, B.A.Pohl, C.Wong, R.C.Haight, Ch.Lagrange Measurements and Calculations of Neutron Scattering in the Actinide Region NUCLEAR REACTIONS 232Th, 238U, 239Pu(n, n), E=14.1 MeV; measured σ(E, θ=0°); deduced semi-microscopic, deformed optical model potentials.
doi: 10.1103/PhysRevC.34.2075
1986LA11 Phys.Rev. C33, 1616 (1986) Ch.Lagrange, D.G.Madland, M.Girod Semimicroscopic Calculations of Elastic, Inelastic, and Total Neutron Scattering by 239Pu in the Energy Range 10 keV ≤ E(n) ≤ 10 MeV NUCLEAR REACTIONS 239Pu(n, n), (n, n'), E=10 keV-10 MeV; calculated σ(θ), σ(E). Hartree-Fock method, semi-microscopic optical model.
doi: 10.1103/PhysRevC.33.1616
1985KU03 Phys.Rev. C31, 762 (1985) K.Kumar, Ch.Lagrange, M.Girod, B.Grammaticos Extended Coupled Channel Method for Baryon Scattering Based on the Dynamics of the Bohr Hamiltonian Deduced from a Microscopic Nucleon-Nucleon Hamiltonian NUCLEAR STRUCTURE 24Mg, 28Si, 150,152,148,154Sm; calculated Hartree-Fock-Bogoliubov potential parameters, form factors. NUCLEAR REACTIONS 24Mg, 28Si(α, α), (α, α'), E=120 MeV; analyzed σ(θ). 148,150,152,154Sm(n, n), E=1-14 MeV; calculated σ ratios; deduced optical model parameters. Extended coupled channel method, Bohr-Hamiltonian dynamics, microscopic approach.
doi: 10.1103/PhysRevC.31.762
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
1983LA02 J.Phys.(Paris) 44, 27 (1983) Interpretation Semi-Microscopique de la Diffusion Elastique et Inelastique de Nucleons par 208Pb NUCLEAR REACTIONS 208Pb(p, p), E=61.4 MeV; 208Pb(p, p'), E=61.25; 208Pb(p, n), E=45 MeV; 208Pb(n, n), (n, n'), E=8.5, 26 MeV; calculated σ(θ). Semi-microscopic model.
doi: 10.1051/jphys:0198300440102700
1983LA03 Nucl.Sci.Eng. 83, 396 (1983) Ch.Lagrange, O.Bersillon, D.G.Madland Coupled-Channel Optical-Model Calculations for Evaluating Neutron Cross Sections of Odd-Mass Actinides NUCLEAR REACTIONS 239Pu(n, n), (n, n'), E=0.01, 1, 4, 6 MeV; 241Pu(n, n), (n, n'), E=1, 4, 6 MeV; calculated total σ, σ(compound nucleus), σ(inelastic), σ(θ); deduced transmission coefficients. Coupled-channels model.
doi: 10.13182/NSE83-A17575
1983LA10 J.Phys.(London) G9, L97 (1983) Semi-Microscopic Calculations of Inelastic Neutron Scattering from Heavy Deformed Nuclei NUCLEAR REACTIONS 232Th(n, n), (n, n'), E=3.4 MeV; 238U(n, n), (n, n'), E=3.4, 8.56, 15.1 MeV; 154Sm(n, n), (n, n'), E=7 MeV; calculated σ(θ). Microscopic optical model, HFB nucleon densities, coupled-channels formalism.
doi: 10.1088/0305-4616/9/5/001
1982HA34 Nucl.Sci.Eng. 81, 491 (1982) G.Haouat, J.Lachkar, Ch.Lagrange, J.Jary, J.Sigaud, Y.Patin Neutron Scattering Cross Sections for 232Th, 233U, 235U, 238U, 239Pu, and 242Pu between 0.6 and 3.4 MeV NUCLEAR REACTIONS 232Th, 233,235,238U, 239,242Pu(n, n), (n, n'), E=0.6-3.4 MeV; measured σ(θ); deduced optical model parameters. 232Th, 235,238U, 239Pu levels deduced β2, β4.
doi: 10.13182/NSE82-A21439
1982LA10 Phys.Rev. C25, 2278 (1982) Phenomenological and Microscopic Optical Model Analyses of the Interaction of Low-Energy Nucleons with 93Nb NUCLEAR REACTIONS 93Nb(n, n), E=7, 8.05, 11 MeV; 93Nb(p, p), E=22.2 MeV; 93Nb(p, n), E=18.7, 49.4 MeV; analyzed σ(total), σ(θ); deduced neutron, proton optical potential differences, Coulomb absorption term role. Phenomenological, microscopic optical model analyses.
doi: 10.1103/PhysRevC.25.2278
1980LA15 Phys.Rev. C22, 896 (1980) (p, n) Reaction for 89 ≤ A ≤ 130 and an Anomalous Optical Model Potential for Sub-Coulomb Protons NUCLEAR REACTIONS 93Nb(p, p), E=22 MeV; 93Nb(p, n), E=18.7 MeV; 89Y, 103Rh(p, p), (p, n), E not given; analyzed σ(θ), s-, p-wave strength function data; deduced optical model parameters.
doi: 10.1103/PhysRevC.22.896
1980LA18 Nucl.Phys. A345, 193 (1980) Ch.Lagrange, J.Lachkar, G.Haouat, R.E.Shamu, M.T.McEllistrem Quadrupole Moments and Nucleon Excitation Strengths in Even-A Sm Isotopes NUCLEAR REACTIONS 148,152,154Sm(n, n), (n, n'), E=7 MeV; 148,152,154Sm(p, p), (p, p'), E=16 MeV; analyzed σ(θ); deduced optical model parameters. 148,152,154Sm levels deduced β2.
doi: 10.1016/0375-9474(80)90418-2
1980SH20 Phys.Rev. C22, 1857 (1980) R.E.Shamu, E.M.Bernstein, J.J.Ramirez, Ch.Lagrange Effects of Deformation on Neutron Total Cross Sections of Even-A Nd and Sm Isotopes NUCLEAR REACTIONS 142,144,146,148,150Nd(n, n), E=0.75-13.89 MeV; 148,150,152,154Sm(n, n), E=0.75-14.49 MeV; measured total σ(E); deduced deformation effects, isotopic dependence. 142,144,146,148,150Nd, 148,150,152,154Sm(n, n'), E=4, 7 MeV; analyzed data; 142,144,146,148,150Nd, 148,150,152,154Sm level deduced β2. Coupled-channels calculation.
doi: 10.1103/PhysRevC.22.1857
1979HA31 Phys.Rev. C20, 78 (1979) G.Haouat, J.Lachkar, C.Lagrange, M.T.McEllistrem, Y.Patin, R.E.Shamu, J.Sigaud Optical Potential and Nuclear Deformation for Even Nd Isotopes from Fast Neutron Scattering NUCLEAR REACTIONS 142,144,146,148,150Nd(n, n), (n, n'), E=7.0 MeV; measured σ(En, θ). 142,144,146,148,150Nd deduced optical model parameters, β2.
doi: 10.1103/PhysRevC.20.78
1977MC02 Phys.Rev. C15, 927 (1977) M.T.McEllistrem, R.E.Shamu, J.Lachkar, G.Haouat, C.Lagrange, Y.Patin, J.Sigaud, F.Cocu Deformation Effects in Neutron Scattering from the Sm Isotopes NUCLEAR REACTIONS 148,150,152,154Sm(n, n), (n, n'), E=7 MeV; measured σ(θ); deduced coupled-channels potential parameters. 148,150,152,154Sm deduced β2.
doi: 10.1103/PhysRevC.15.927
1976LA17 Acta Phys.Slovaca 26, 32 (1976) Determination of a Coherent Parameter Set for Coupled Channel Calculations of 238U Neutron Cross-Sections from 10 keV to 20 MeV NUCLEAR REACTIONS 238U(n, X), E=0.01-20 MeV; calculated σ(E); deduced coherent coupled channel parameter set.
1976SH06 Phys.Lett. 61B, 29 (1976) R.E.Shamu, C.H.Lagrange, E.M.Bernstein, J.J.Ramirez, T.Tamura, C.Y.Wong Quadrupole Deformation Parameters of 148,152,154Sm Determined from Neutron Total Cross Sections NUCLEAR REACTIONS 148,152,154Sm(n, X), E=0.75-14.5 MeV; measured relative σ. 148,152,154Sm deduced β.
doi: 10.1016/0370-2693(76)90553-0
1975LA18 Phys.Lett. 58B, 293 (1975) C.Lagrange, R.E.Shamu, T.Burrows, G.P.Glasgow, G.Hardie, F.D.McDaniel Effect of Nuclear Deformation on Neutron Elastic Scattering NUCLEAR REACTIONS 148,154Sm(n, n'), E=6.25 MeV; measured σ(En', θ). 148,154Sm(n, n), E=6.25 MeV; measured σ(θ). 148,154Sm deduced β.
doi: 10.1016/0370-2693(75)90656-5
1974LA25 J.Phys.(Paris), Suppl.Lett. 35, L-111 (1974) Effets Systematiques des Deformations Nucleaires sur la Section Efficace Totale Neutron-Noyau NUCLEAR REACTIONS 148,150,152,154Sm, 182W, 238U(n, X), E=2-20 MeV; calculated effects of nuclear deformations on total σ.
doi: 10.1051/jphyslet:01974003509011100
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