NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = C.Mahaux Found 53 matches. 2000CA46 Ann.Phys.(New York) 281, 223 (2000) Relationship between Feshbach's and Green's Function Theories of the Nucleon-Nucleus Mean Field
doi: 10.1006/aphy.2000.6011
1997CA31 Ann.Phys.(New York) 254, 130 (1997) Final State Interactions and Target Correlations in Inclusive (e, e') Reactions
doi: 10.1006/aphy.1996.5640
1994MA07 Nucl.Phys. A568, 1 (1994) Critical Study of the Dispersive n-90Zr Mean Field by Means of a New Variational Method NUCLEAR REACTIONS 90Zr(n, n), E=8-24 MeV; calculated σ(θ). Mean field, optical model approaches.
doi: 10.1016/0375-9474(94)90002-7
1993MA36 Nucl.Phys. A560, 5 (1993) Temporal Nonlocality of Nuclear and Atomic Mean Fields NUCLEAR REACTIONS 208Pb(n, n), E=-10 to 60 MeV; calculated optical potential components behavior, system self energy; deduced temporary nonlocality features. Complex mean field.
doi: 10.1016/0375-9474(93)90079-D
1992MA43 Nucl.Phys. A546, 65c (1992) Embedding of Correlations in the Nuclear Mean Field NUCLEAR REACTIONS 208Pb(e, e'p), E not given; calculated spectral function. Complex mean field.
doi: 10.1016/0375-9474(92)90502-B
1991JE02 Phys.Rev. C43, 2211 (1991) J.-P.Jeukenne, C.Mahaux, R.Sartor Dependence of the Fermi Energy Upon Neutron Excess NUCLEAR STRUCTURE A=40-208; calculated symmetry potential strength near Fermi energy. Dispersion relation related analysis input.
doi: 10.1103/PhysRevC.43.2211
1991MA15 Nucl.Phys. A528, 253 (1991) Dispersion Relation Approach to the Mean Field and Spectral Functions of Nucleons in 40Ca NUCLEAR REACTIONS 40Ca(n, n), (p, p), E=30-50 MeV; calculated potential radius parameters vs E. 40Ca(polarized p, p), E=19.6-48 MeV; 40Ca(polarized n, n), E=5-40 MeV; calculated σ(θ), analyzing power vs θ. Dispersion relation approach to mean field.
doi: 10.1016/0375-9474(91)90090-S
1990MA60 Nucl.Phys. A516, 285 (1990) Dispersive Versus Constant-Geometry Models of the Neutron-208Pb Mean Field NUCLEAR REACTIONS 208Pb(n, n), E ≈ 0-16 MeV; calculated σ(E). Mean field approach.
doi: 10.1016/0375-9474(90)90310-I
1989MA20 Nucl.Phys. A493, 157 (1989) From Scattering to Very Deeply Bound Neutrons in 208Pb: Extended and improved moment approaches NUCLEAR REACTIONS 208Pb(n, n), E=10-40 MeV; calculated σ(θ). Complex mean field.
doi: 10.1016/0375-9474(89)90395-3
1989MA48 Nucl.Phys. A503, 525 (1989) Variational Moment Approach to the Single-Particle Properties of Protons in 208Pb NUCLEAR STRUCTURE 208Pb; calculated proton single particle state properties, transfer reaction spectroscopic strengths. Variational moment approach.
doi: 10.1016/0375-9474(89)90248-0
1988JE03 Phys.Rev. C38, 2573 (1988) J.-P.Jeukenne, C.H.Johnson, C.Mahaux Surface Contributions to the Complex Neutron-208Pb Mean Field between -20 and +20 MeV NUCLEAR REACTIONS 208Pb(n, n), E=7-14 MeV; analyzed data; model parameters. Local optical model.
doi: 10.1103/PhysRevC.38.2573
1988JO07 Phys.Rev. C38, 2589 (1988) Neutron-40Ca Mean Field between -80 and +80 MeV from a Dispersive Optical-Model Analysis NUCLEAR REACTIONS 40Ca(n, n), E=5.3-40 MeV; analyzed data; deduced model parameters. Dispersive optical model analysis.
doi: 10.1103/PhysRevC.38.2589
1988MA21 Nucl.Phys. A481, 381 (1988) Single-Particle Potential and Quasiparticle Properties of Protons in 208Pb NUCLEAR REACTIONS 208Pb(p, p), E=-20-40 MeV; calculated potential features, proton quasiparticle strength. Mean field approach.
doi: 10.1016/0375-9474(88)90335-1
1988MA22 Nucl.Phys. A481, 407 (1988) Isovector, Isoscalar and Coulomb Contributions to the Mean Field in 208Pb NUCLEAR REACTIONS 208Pb(p, p), (n, n), E=-20-40 MeV; calculated potential features, differences; deduced isovector, isoscalar and Coulomb contributions. Mean field methods.
doi: 10.1016/0375-9474(88)90336-3
1988MA40 Nucl.Phys. A484, 205 (1988) The p-40Ca and n-40Ca Mean Fields from the Iterative Moment Approach NUCLEAR REACTIONS 40Ca(p, p), (n, n), E=-25-75 MeV; calculated mean field parameters. Iterative moment technique.
doi: 10.1016/0375-9474(88)90071-1
1987JA11 Nucl.Phys. A473, 509 (1987) Mean Square Deviation from a Slater Determinant and Scaling Effects in Models of the Correlated Ground State of Nuclear Matter and of 208Pb NUCLEAR STRUCTURE 208Pb; calculated charge density distribution. Mean square deviation approach.
doi: 10.1016/0375-9474(87)90138-2
1987JO04 Phys.Rev. C36, 2252 (1987) C.H.Johnson, D.J.Horen, C.Mahaux Unified Description of the Neutron-208Pb Mean Field between - 20 and + 165 MeV from the Dispersion Relation Constraint NUCLEAR REACTIONS 208Pb(n, n), (polarized n, n), E=1-25 MeV; measured σ(θ), analyzing power vs θ, σ(E). 208Pb deduced single particle densities, spectroscopic factors, rms radii, occupation numbers. Unified model, dispersion relation constraint.
doi: 10.1103/PhysRevC.36.2252
1987MA28 Nucl.Phys. A468, 193 (1987) Extrapolation from Positive to Negative Energy of the Woods-Saxon Parametrization of the n-208Pb Mean Field NUCLEAR STRUCTURE 209Pb; calculated neutron single particle energies. Mean field techniques. NUCLEAR REACTIONS 208Pb(n, X), E=20-40 MeV; calculated optical model parameters, radial moment, moment ratios. Mean field techniques.
doi: 10.1016/0375-9474(87)90515-X
1987MA53 Phys.Rev. C36, 1777 (1987) Fermi-Surface Anomaly for Neutrons in Yttrium NUCLEAR REACTIONS 89Y(n, n), E not given; calculated n-nucleus interaction potential features. Dispersion relation approach.
doi: 10.1103/PhysRevC.36.1777
1987MA60 Nucl.Phys. A475, 247 (1987) Properties of the Quasiparticle Excitations in 207Pb and 209Pb from an Extrapolation of the Optical-Model Potential NUCLEAR STRUCTURE 209,207Pb; calculated quasiparticle excitation characteristics. 208Pb; calculated neutron density distribution.
doi: 10.1016/0375-9474(87)90165-5
1986JA05 Nucl.Phys. A452, 445 (1986) Effect of Correlations on the Momentum Distribution of Protons in 208Pb NUCLEAR STRUCTURE 208Pb; calculated proton momentum distributions; deduced correlations role.
doi: 10.1016/0375-9474(86)90208-3
1986JA12 Phys.Rev. C34, 468 (1986) M.Jaminon, J.-P.Jeukenne, C.Mahaux Dependence upon Mass Number and Neutron Excess of the Real Part of the Proton Optical Potential for Mass Number 44 ≤ A ≤ 72 COMPILATION A=40-80; calculated proton optical potentials; deduced mass number, neutron excess dependences.
doi: 10.1103/PhysRevC.34.468
1986JA17 Phys.Rev. C34, 2084 (1986) Real Part of the Neutron and Proton Optical Potentials at 11 MeV for Mass Numbers 40 ≤ A ≤ 76 COMPILATION A=40-76; compiled, analyzed 11 MeV (p, p), (n, n) data; deduced potential parameters. Optical model.
doi: 10.1103/PhysRevC.34.2084
1986JA18 Phys.Rev. C34, 2097 (1986) Radial Shape of the Optical Potential for 35 and 11 MeV Protons on Targets with Mass Number 10 < A < 80 COMPILATION A=10-80; compiled, analyzed 11, 35 MeV proton scattering data; deduced potential radial shapes. Optical model.
doi: 10.1103/PhysRevC.34.2097
1986MA04 Nucl.Phys. A449, 354 (1986) Causality and the Threshold Anomaly of the Nucleus-Nucleus Potential NUCLEAR REACTIONS 40Ca(16O, 16O), E=38-214 MeV; 208Pb(16O, 16O), E=60-240 MeV; calculated potential volume integrals; deduced threshold anomaly causality principle relationship.
doi: 10.1016/0375-9474(86)90009-6
1986MA11 Nucl.Phys. A451, 441 (1986) Energy Dependence of the Global Properties of the Empirical Nucleon-Nucleus Potential for 40Ca, 132Sn and 208Pb NUCLEAR REACTIONS 40Ca, 208Pb(p, p), (n, n), E not given; calculated nucleon-nucleus potential global properties energy dependence. NUCLEAR STRUCTURE 40Ca, 132Sn, 208Pb; calculated proton rms radii.
doi: 10.1016/0375-9474(86)90069-2
1986MA35 Nucl.Phys. A456, 134 (1986) Radial and Energy Dependence of the Dispersive Contributions to the α + 16O and α + 40Ca Potentials near the Threshold Anomaly NUCLEAR REACTIONS 16O(α, α), E=20-80 MeV; 40Ca(α, α), E=58-72 MeV; calculated nucleus-nucleus potential characteristics; deduced dispersion contributions radial, energy dependences.
doi: 10.1016/0375-9474(86)90370-2
1986MA53 Nucl.Phys. A458, 25 (1986) Empirical and Theoretical Investigation of the Average Potential of Nucleons in 40Ca and 208Pb NUCLEAR REACTIONS 40Ca, 208Pb(p, p), (n, n), E not given; calculated complex mean field radial moments; deduced average potential. Optical model, dispersion relation approach.
doi: 10.1016/0375-9474(86)90281-2
1986MA60 Phys.Rev.Lett. 57, 3015 (1986) Calculation of the Shell-Model Potential from the Optical-Model Potential NUCLEAR REACTIONS 208Pb(n, n), E=20-40 MeV; calculated shell model potential parameters energy dependence. Dispersion relation approach, optical model base.
doi: 10.1103/PhysRevLett.57.3015
1986MA61 Phys.Rev. C34, 2119 (1986) Empirical Evidence of an Energy Dependence of the Radial Shape of the Real Part of the Optical Potential NUCLEAR REACTIONS 40Ca(p, p), 208Pb(p, p), (p, n), E ≈ 10-40 MeV; analyzed potential parameter fits to data; deduced potential shape radial dependence.
doi: 10.1103/PhysRevC.34.2119
1986MA69 Nucl.Phys. A460, 466 (1986); Erratum Nucl.Phys. A472, 769 (1987) Dispersion Relation Approach to the Extrapolation towards Negative Energy of the Optical Potential in 40Ca and 208Pb NUCLEAR REACTIONS 40Ca(p, p), E=9-20 MeV; 40Ca(n, n), E=9-14 MeV; 208Pb(n, n), E=4-40 MeV; 208Pb(p, p), E=15-30 MeV; calculated optical model real part radial moments. Dispersion relation approach.
doi: 10.1016/0375-9474(86)90425-2
1985JA10 Nucl.Phys. A440, 228 (1985) Dependence of the Density Distribution of 208Pb on the Occupation Probabilities of Shell-Model Orbits NUCLEAR STRUCTURE 208Pb; calculated proton density distribution. Independent particle model, Hartree-Fock approach.
doi: 10.1016/0375-9474(85)90339-2
1985JA11 Phys.Lett. 158B, 103 (1985) Inability of any Hartree-Fock Approximation to Reproduce Simultaneously the Density and Momentum Distributions of Nuclei NUCLEAR STRUCTURE 208Pb; calculated charge density distribution, proton orbit occupation probabilities; deduced Hartree-Fock approximation limitations.
doi: 10.1016/0370-2693(85)91372-3
1985NA01 Phys.Rev.Lett. 54, 1136 (1985) M.A.Nagarajan, C.C.Mahaux, G.R.Satchler Dispersion Relation and the Low-Energy Behavior of the Heavy-Ion Optical Potential NUCLEAR REACTIONS 208Pb(16O, 16O), E=80-220 MeV; calculated potential parameter energy dependence.
doi: 10.1103/PhysRevLett.54.1136
1984BO20 Phys.Lett. 140B, 163 (1984) P.F.Bortignon, R.A.Broglia, C.H.Dasso, C.Mahaux Level Dependence of the Self-Energy Correction to the Hartree-Fock Single-Particle Energies in 208Pb NUCLEAR STRUCTURE 208Pb; calculated single particle energies; deduced self-energy correction level dependence. Hartree-Fock approach, Skyrme interaction.
doi: 10.1016/0370-2693(84)90912-2
1984CA25 Z.Phys. A318, 31 (1984) On the Difference between the Effective Charges Used for Bound States of 29Si and for Low-Energy Neutron Radiative Capture by 28Si NUCLEAR REACTIONS 28Si(n, γ), E=560 keV; calculated p-wave radial function; deduced external capture dominance, neutron E1 effective charge dependence of capture process.
doi: 10.1007/BF02117211
1984MA61 Nucl.Phys. A431, 486 (1984) Effective Masses, Occupation Probabilities and Quasiparticle Strengths in 208Pb NUCLEAR STRUCTURE 209Pb, 209Bi; calculated neutron, proton mean field characterizing parameters. 208Pb; calculated shell orbit occupation probabilities. Dispersion relations, effective mass.
doi: 10.1016/0375-9474(84)90120-9
1983JE02 Nucl.Phys. A394, 445 (1983) Shell and Space-Truncation Effects in Calculations of the Effective Mass NUCLEAR STRUCTURE 208Pb; calculated effective mass, optical potential imaginary term. Schematic models.
doi: 10.1016/0375-9474(83)90117-3
1983JO07 Phys.Rev. C27, 1913 (1983) C.H.Johnson, N.M.Larson, C.Mahaux, R.R.Winters Calculation of the Energy-Averaged Scattering Function from High Resolution Low-Energy Neutron Scattering Data NUCLEAR REACTIONS 32S(n, n), E ≈ 0.2-0.9 MeV; calculated σ(compound nucleus), σ(shape elastic) vs E. Optical model scattering function, energy averaging, p-wave neutrons.
doi: 10.1103/PhysRevC.27.1913
1983MA28 Phys.Lett. 126B, 1 (1983) Energy Dependence of the Coulomb Correction and the Symmetry Potential in 208Pb NUCLEAR STRUCTURE 208Pb; analyzed single nucleon potential data; deduced symmetry potential enhancement near Fermi surface.
doi: 10.1016/0370-2693(83)90002-3
1983MA52 Phys.Scr. T5, 74 (1983) Dynamical Content of the Shell Model NUCLEAR STRUCTURE 208Pb; calculated single particle neutron energies. Hartree-Fock approximation, dynamical corrections.
doi: 10.1088/0031-8949/1983/T5/011
1983MA66 Nucl.Phys. A410, 271 (1983) Contribution of Core Polarization to Single-Particle Energies in 208Pb NUCLEAR STRUCTURE 208Pb; calculated neutron, proton single particle energies; deduced core polarization role. Dispersion relation approach.
doi: 10.1016/0375-9474(83)90202-6
1983SO09 Nucl.Phys. A411, 27 (1983) Differences between Dynamical Theories of Giant Resonances NUCLEAR STRUCTURE 208Pb; calculated giant resonance effective particle-hole gap; deduced dynamical correction model dependence.
doi: 10.1016/0375-9474(83)90506-7
1982MA09 Nucl.Phys. A378, 205 (1982) Polarization and Correlation Contributions to the Shell-Model Potential in 40Ca and 208Pb NUCLEAR REACTIONS 40Ca, 208Pb(n, n), E=5-25 MeV; calculated potential; deduced polarization, correlation contributions, effective mass width. Dispersion relation.
doi: 10.1016/0375-9474(82)90589-9
1977JE04 Phys.Rev. C16, 80 (1977) J.-P.Jeukenne, A.Lejeune, C.Mahaux Optical-Model Potential in Finite Nuclei from Reid's Hard Core Interaction NUCLEAR REACTIONS 12C, 16O, 27Al, 40Ca, 58Ni, 120Sn, 208Pb(p, p); calculated optical-model potentials.
doi: 10.1103/PhysRevC.16.80
1976JE01 Phys.Lett. 62B, 256 (1976) J.-P.Jeukenne, A.Lejeune, C.Mahaux Coulomb Correlation Due to the True Nonlocality of the Optical-Model Potential NUCLEAR REACTIONS 208Pb(n, n'), (p, p'); calculated Coulomb correction.
doi: 10.1016/0370-2693(76)90068-X
1974BA04 Phys.Rev. C9, 723 (1974) Statistical Analysis of Intermediate Structure NUCLEAR REACTIONS 40Ca(p, p'), 56Fe, 206Pb(n, n), 244Cm(n, X), 187Re, 115In(n, γ), 90Zr, Sn(γ, X), 70Ge(p, p), 239Pu(n, F); calculated significance level of intermediate structure, using new statistical tests.
doi: 10.1103/PhysRevC.9.723
1974JE03 Phys.Rev. C10, 1391 (1974) J.-P.Jeukenne, A.Lejeune, C.Mahaux Optical-Model Potential in Nuclear Matter from Reid's Hard Core Interaction NUCLEAR REACTIONS 40Ca, 58Ni(p, p); calculated scattering potential.
doi: 10.1103/PhysRevC.10.1391
1973BO32 Phys.Lett. 45B, 81 (1973) Relation between the Background Cross Section and the Correlation between Partial Widths NUCLEAR REACTIONS 29Si, 208Pb(γ, n), 169Tm(n, γ); measured nothing, calculated background σ.
doi: 10.1016/0370-2693(73)90069-5
1973BO47 Nucl.Phys. A215, 605 (1973) Radiative Capture of Low-Energy Neutrons in the Shell-Model Approach to Nuclear Reactions NUCLEAR REACTIONS 56Fe, 58Ni(n, γ); calculated Iγ. 57Fe, 59Ni resonances calculated level-width.
doi: 10.1016/0375-9474(73)90493-4
1972BB09 Phys.Lett. 42B, 392 (1972) A Statistical Test for Intermediate Structure NUCLEAR REACTIONS 115In(n, γ), 206Pb(n, n); analyzed intermediate structure.
doi: 10.1016/0370-2693(72)90089-5
1971MA56 Nucl.Phys. A177, 103 (1971) Resonance Wave Functions and Resonance Parameters from the Coupled-Channel Method NUCLEAR REACTIONS 40Ca(γ, X), E < 26 MeV; calculated phase shifts. 40Ca calculated giant resonance partial widths. Coupled-channel approximation.
doi: 10.1016/0375-9474(71)90165-5
1969MA35 Nucl.Phys. A138, 481 (1969) Isospin Mixing in the Giant Dipole Resonance of Self-Conjugate Nuclei NUCLEAR REACTIONS 12C, 16O, 40Ca(γ, n), (γ, p), E < 28 MeV; calculated σ(E); deduced isospin mixing effects.
doi: 10.1016/0375-9474(69)90234-6
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