NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = N.Vinh-Mau Found 45 matches. 2015BL01 Phys.Rev. C 91, 014612 (2015) G.Blanchon, M.Dupuis, H.F.Arellano, N.Vinh Mau Microscopic positive-energy potential based on the Gogny interaction NUCLEAR REACTIONS 40Ca(p, p), E=9.86, 10.37, 13.49, 14.51, 15.97, 18.57, 19.57, 21, 23.5, 25, 26.3, 27.5, 30.3, 40 MeV; 40Ca(n, n), E=2.06, 3.29, 5.3, 5.88, 6.5, 7.91, 9.91, 13.9, 16.9, 19, 21.7, 25.5, 30.3, 40 MeV; 40Ca(polarized p, p), E=14.51, 15.97, 18.57, 40 MeV; 40Ca(polarized n, n), E=9.91, 11, 13.9, 16.9 MeV; analyzed differential σ(E, θ), integral σ(E), and analyzing power Ay(θ, E). Calculation based on Greens function formalism in the random-phase approximation with the finite-range Gogny effective interaction, and including effects of intermediate single-particle resonances.
doi: 10.1103/PhysRevC.91.014612
2010BL08 Phys.Rev. C 82, 034313 (2010) G.Blanchon, N.Vinh Mau, A.Bonaccorso, M.Dupuis, N.Pillet Particle-particle random-phase approximation applied to beryllium isotopes NUCLEAR STRUCTURE 8,10,12,14Be; calculated levels, J, π, pp-RPA amplitudes, E1 strength distribution, S(2n), rms radii. Comparison to experimental data. Particle-particle random-phase approximation (pp-RPA) method using Woods-Saxon potential for the neutron-core interaction and D1S Gogny force for the neutron-neutron interaction.
doi: 10.1103/PhysRevC.82.034313
2010BL12 J.Phys.:Conf.Ser. 205, 012003 (2010) G.Blanchon, A.Bonaccorso, D.M.Brink, N.Vinh Mau 10-11Li and 13-14Be studied by projectile fragmentation and pp-RPA NUCLEAR STRUCTURE 10Li, 13Be; calculated halo nuclei scattering lengths, resonance parameters, 2n separation energies. 12,14Be; calculated halo nuclei radii, 2n separation energies. Time-dependent projectile fragmentation model with core-vibration model of two-neutron halo nuclei. Compared with data. NUCLEAR REACTIONS 12C(11Li, n9Li), (14Be, n12Be), E=250 MeV/nucleon; calculated σ(E), n-9Li and n-12Be relative energy spectrum using time-dependent projectile fragmentation model with core-vibration model of two-neutron halo nuclei. Compared with data.
doi: 10.1088/1742-6596/205/1/012003
2007BL02 Nucl.Phys. A784, 49 (2007) G.Blanchon, A.Bonaccorso, D.M.Brink, A.Garcia-Camacho, N.Vinh Mau Unbound exotic nuclei studied by projectile fragmentation NUCLEAR REACTIONS 12C(11Be, n10Be), E=67 MeV/nucleon; calculated relative energy spectrum. NUCLEAR STRUCTURE 13,14Be; calculated resonance features in unbound neutron states.
doi: 10.1016/j.nuclphysa.2006.11.033
2007BL19 Nucl.Phys. A791, 303 (2007) G.Blanchon, A.Bonaccorso, D.M.Brink, N.Vinh Mau 10Li spectrum from 11Li fragmentation NUCLEAR REACTIONS 12C(11Li, n)9Li, E=264 MeV/nucleon; calculated σ as function of neutron-9Li relative energy using a projectile fragmentation model.
doi: 10.1016/j.nuclphysa.2007.04.014
2005VI07 Phys.Rev. C 71, 054317 (2005) Discretization of the continuum in 6He: A schematic model to test the validity of the concept NUCLEAR STRUCTURE 6He; calculated pairing energies, level energies; deduced effect of discretization of the continuum.
doi: 10.1103/PhysRevC.71.054317
2004BL11 Nucl.Phys. A739, 259 (2004) G.Blanchon, A.Bonaccorso, N.Vinh Mau Unbound exotic nuclei studied by transfer to the continuum reactions NUCLEAR REACTIONS 9Li(d, p), (9Be, 8Be), (13C, 12C), E=2 MeV/nucleon; calculated transition probabilities for neutron transfer to unbound states, final state interaction features.
doi: 10.1016/j.nuclphysa.2004.04.106
2003VI10 Nucl.Phys. A722, 104c (2003) Two-body correlations in halo nuclei and effective interactions NUCLEAR STRUCTURE 9,11Li, 10,12Be, 12,14C; calculated wave functions, two-neutron separation energies. 14N; calculated levels, J, π. RPA approach, Gogny interaction, comparisons with data.
doi: 10.1016/S0375-9474(03)01344-7
2002PA15 Phys.Rev. C65, 044004 (2002) Two-Body Correlations in N = 8 and 10 Nuclei and Effective Neutron-Neutron Interactions in Tamm-Dancoff and Two-Particle Random Phase Approximation Models NUCLEAR STRUCTURE 6He, 9,11Li, 10,12,14Be, 12,14C; calculated two-neutron separation energies. Particle-particle RPA, Gogny effective interaction.
doi: 10.1103/PhysRevC.65.044004
2001AU01 Phys.Rev. C63, 017301 (2001) About Coulomb Energy Shifts in Halo Nuclei NUCLEAR STRUCTURE 17O, 17F, 11Be, 11N; calculated single-particle energies, Coulomb energy shifts.
doi: 10.1103/PhysRevC.63.017301
2000PA14 Nucl.Phys. A669, 135 (2000) Quasielastic Scattering of 11Li and 12Be on 12C NUCLEAR REACTIONS 12C(11Li, 11Li'), (12Be, 12Be'), E ≈ 60 MeV/nucleon; 28Si(11Li, 11Li'), E=29 MeV/nucleon; calculated quasielastic σ(θ). 11Li deduced two-neutron wavefunction component. Folding model potential plus fitted polarization potential. Comparisons with data.
doi: 10.1016/S0375-9474(99)00432-7
1999LA20 Phys.Rev. C60, 027303 (1999) M.Labiche, F.M.Marques, O.Sorlin, N.Vinh Mau Structure of 13Be and 14Be NUCLEAR STRUCTURE 14Be calculated two-neutron separation energies, radii; deduced halo features. 13Be deduced ground-state energy, J, π. Comparisons with data.
doi: 10.1103/PhysRevC.60.027303
1997BO08 Nucl.Phys. A615, 245 (1997) Low Energy Dipole Modes in 14C, 12Be and 11Li. Coulomb Dissociation of 11Li NUCLEAR STRUCTURE 14C, 12Be, 11Li; calculated levels, low energydipoles modes, B(λ). Two-neutron pairing model. NUCLEAR REACTIONS 208Pb, 63Cu, 27Al, 12C(11Li, X), E=0.03-0.8 Gev/nucleon; calculated two-neutron Coulomb dissociation σ. Two-neutron pairing model.
doi: 10.1016/S0375-9474(97)00013-4
1997GR18 Phys.Rev. C56, 2885 (1997) Low Lying States in 11N and 15F NUCLEAR STRUCTURE 11N, 15F; calculated low-lying resonances energy, Γ. Comparisons with experiment.
doi: 10.1103/PhysRevC.56.2885
1996VI09 Nucl.Phys. A607, 163 (1996) Structure of the 11Li Nucleus NUCLEAR STRUCTURE 14C, 12Be; calculated levels. 11Li; calculated levels, two-neutron separation energy, radius. Three-body model, zero-range density-dependent pairing interaction.
doi: 10.1016/S0375-9474(96)00246-1
1995VI06 Nucl.Phys. A592, 33 (1995) Particle-Vibration Coupling in One Neutron Halo Nuclei NUCLEAR STRUCTURE 11Be, 13,15C; calculated spectra. Particle-vibration coupling.
doi: 10.1016/0375-9474(95)00298-F
1993VI01 Phys.Rev. C47, 899 (1993) N.Vinh Mau, J.L.Ferrero, J.C.Pacheco, B.Bilwes Comment on ' Dynamical Polarization Potential Due to the Excitation of Collective States ' NUCLEAR REACTIONS 40Ca(16O, 16O), E=104-650 MeV; analyzed dynamical polarization potential features; deduced inelastic channels role.
doi: 10.1103/PhysRevC.47.899
1993VI05 Nucl.Phys. A560, 879 (1993) N.Vinh Mau, J.C.Pacheco, J.L.Ferrero, R.Bilwes Sub- and Near-Barrier Fusion Potentials and Cross Sections NUCLEAR REACTIONS, ICPND 208Pb(16O, 16O), E=78-312.6 MeV; calculated σ(θ), fusion σ(E). 40Ca(32S, X), E=80-110 MeV; calculated fusion σ(E). Closure approximation model.
doi: 10.1016/0375-9474(93)90176-X
1992VI07 Nucl.Phys. A548, 381 (1992) The Width of the Giant Dipole Resonance at Finite Temperature NUCLEAR STRUCTURE 208Pb; calculated giant dipole resonance width vs temperature. Schematic model.
doi: 10.1016/0375-9474(92)90690-L
1991BI02 Nucl.Phys. A526, 292 (1991) B.Bilwes, R.Bilwes, N.Vinh Mau, J.L.Ferrero, J.C.Pacheco Dispersion Relation for Microscopic Heavy-Ion Potentials and Description of Elastic Scattering above the Coulomb Barrier for 32S on 40Ca NUCLEAR REACTIONS 40Ca(32S, 32S), E=90-151.5 MeV; calculated σ(θ). Closure approximation model.
doi: 10.1016/0375-9474(91)90288-H
1991VI03 Nucl.Phys. A531, 435 (1991) N.Vinh Mau, J.L.Ferrero, J.C.Pacheco, B.Bilwes Low-Energy 16O + 208Pb Elastic Scattering an Attempt to Analyze the Microscopic Effective Potential NUCLEAR REACTIONS 208Pb(16O, 16O), E=96-312.6 MeV; calculated σ(θ). Closure approximation, semi-phenomenological potentials models comparison.
doi: 10.1016/0375-9474(91)90620-L
1990CH25 Phys.Lett. 242B, 313 (1990) Ph.Chomaz, D.Vautherin, N.Vinh Mau A Comment on RPA Calculations of Photoabsorption by Hot Nuclei NUCLEAR STRUCTURE 40Ca; calculated isoscalar quadrupole mode energies, response functions. RPA, hot nuclei photoabsorption.
doi: 10.1016/0370-2693(90)91767-6
1990FE05 Nucl.Phys. A514, 367 (1990) J.L.Ferrero, J.C.Pacheco, A.Baeza, J.M.Barrigon, B.Bilwes, R.Bilwes, N.Vinh Mau Elastic Scattering of 35Cl and 37Cl on 24Mg NUCLEAR REACTIONS 24Mg(35Cl, 35Cl), (37Cl, 37Cl), E(cm)=40.7, 48.8 MeV; measured σ(E, θ); deduced isotopic effects on absorption. Woods-Saxon, folding model, closure approximation analyses.
doi: 10.1016/0375-9474(90)90076-X
1990LA17 Nucl.Phys. A518, 441 (1990) l-Dependent Local Potentials Equivalent to a Non-Local Potential NUCLEAR REACTIONS 4He(n, n), (p, p), E not given; calculated equivalent local potential parameter features. Peierls-Vinh Mau local approximation.
doi: 10.1016/0375-9474(90)90139-D
1987VI04 Nucl.Phys. A470, 406 (1987) A Consistent Derivation of the Real and Imaginary Parts of the Heavy Ion Potential below and above the Coulomb Barrier NUCLEAR REACTIONS 40Ca(16O, 16O), E=55.6-214 MeV; 208Pb(16O, 16O), E=129.5-312.6 MeV; calculated potential parameters; deduced anomaly characteristics. Optical model, closure approximation.
doi: 10.1016/0375-9474(87)90010-8
1986TR09 Nucl.Phys. A458, 460 (1986) T.Troudet, D.Vautherin, N.Vinh Mau Effect of Correlations on the Relation between Excitation Energy and Temperature NUCLEAR STRUCTURE 58Ni, 40Ca; calculated level density vs temperature. RPA.
doi: 10.1016/0375-9474(86)90045-X
1986VI07 Nucl.Phys. A457, 413 (1986) Closure Approximation to the Absorptive Potential in Heavy Ion Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=84, 360 MeV; 28Si(16O, 16O), E=50, 55 MeV; 40Ca(16O, 16O), E=74, 104, 214 MeV; 208Pb(16O, 16O), E=129.5, 192, 312.6 MeV; calculated imaginary potential vs internucleus distance, energy. Feshbach theory, closure approximation.
doi: 10.1016/0375-9474(86)90387-8
1985VI06 Nucl.Phys. A445, 245 (1985) Effect of Residual Interactions on Nuclear Level Densities NUCLEAR STRUCTURE 40Ca, 56Ni; calculated level densities. RPA.
doi: 10.1016/0375-9474(85)90070-3
1984VA15 Nucl.Phys. A422, 140 (1984) Temperature Dependence of Collective States in the Random-Phase Approximation NUCLEAR STRUCTURE 40Ca; calculated dipole, isoscalar octupole strength vs temperature. Collective states, RPA.
doi: 10.1016/0375-9474(84)90434-2
1982LA24 Nucl.Phys. A391, 118 (1982) The Imaginary Part of the Local Potential Equivalent to the Non-Local α-Nucleus Optical Potential NUCLEAR REACTIONS 40Ca(α, α), E=50, 100 MeV; calculated local equivalent potential imaginary part. Feshbach formalism.
doi: 10.1016/0375-9474(82)90222-6
1981BO21 Phys.Lett. 102B, 109 (1981) A.Bouyssy, N.Vinh Mau, D.M.Brink A Critical Analysis of the Eikonal Approximation in the Derivation of the Alpha-Nucleus Potential NUCLEAR REACTIONS 40Ca(α, α), E=75 MeV; calculated absorptive alpha-nucleus potential term. Exact Greens function, eikonal approximation.
doi: 10.1016/0370-2693(81)91041-8
1981DU07 Nucl.Phys. A355, 141 (1981) F.Duggan, M.Lassaut, F.Michel, N.Vinh Mau Antisymmetrization and Density-Dependent Effects within the Folding Model Approach to α-Nucleus Scattering NUCLEAR REACTIONS 40Ca(α, α), E=104 MeV; calculated σ(θ). Folding model, α-nucleus potential from Hartree-Fock approximation, antisymmetrization, density dependent forces.
doi: 10.1016/0375-9474(81)90135-4
1980LA20 Nucl.Phys. A349, 372 (1980) Low-Energy Nucleon-Alpha Scattering: Microscopic potentials and phase shifts NUCLEAR REACTIONS 4He(n, n), E<25 MeV; calculated phase shifts. Antisymmetrized folding model, effective interactions, local equivalent potentials.
doi: 10.1016/0375-9474(80)90295-X
1977VI04 Phys.Lett. 71B, 5 (1977) A Microscopic Calculation of the Alpha-Nucleus Potential NUCLEAR REACTIONS 40Ca(α, α), E=50-150 MeV; calculated potentials. Microscopic calculation.
doi: 10.1016/0370-2693(77)90725-0
1976VI03 Nucl.Phys. A257, 189 (1976) Optical Potential for Low-Energy Neutrons: Imaginary Potential for Neutron-40Ca Elastic Scattering NUCLEAR REACTIONS 40Ca(n, n), E=low; calculated potential.
doi: 10.1016/0375-9474(76)90627-8
1974BO22 Nucl.Phys. A224, 331 (1974) Two-Particle RPA for Oxygen and Calcium NUCLEAR STRUCTURE 18F, 14,18O, 14N, 42Sc, 38,42Ca, 38K; calculated levels. NUCLEAR REACTIONS 16O, 40Ca(t, p), calculated σ. 18O, 42Ca levels deduced S.
doi: 10.1016/0375-9474(74)90691-5
1974BO31 Nucl.Phys. A229, 1 (1974) Particle-Hole and Particle-Particle RPA Ground State Correlations and the Green Function Formalism NUCLEAR STRUCTURE 16O, 40Ca; calculated correlation energies.
doi: 10.1016/0375-9474(74)90671-X
1973BO14 Phys.Lett. 44B, 139 (1973) Neutron Emission in Muon Capture by 40Ca NUCLEAR REACTIONS 40Ca(μ-, n); calculated σ(En), asymmetry(En).
doi: 10.1016/0370-2693(73)90504-2
1972BO11 Nucl.Phys. A185, 32 (1972) Spectrum and Asymmetry of Neutrons Emitted after Polarized Muon Capture by 16O and 40Ca NUCLEAR REACTIONS 16O, 40Ca(μ-, nν), E approx 0; calculated σ(En, θ(n)). polarized beam; pure shell model, p-H configuration mixing nuclear wave functions.
doi: 10.1016/0375-9474(72)90549-0
1971BO21 Phys.Lett. 35B, 269 (1971) Pairing Vibrations in 18O and 18F NUCLEAR STRUCTURE 18F, 18O; calculated levels. Pairing vibration model.
doi: 10.1016/0370-2693(71)90254-1
1971DE12 Phys.Lett. 35B, 28 (1971) Parity Non Conserving Effects in 181Ta and 175Lu RADIOACTIVITY 175Yb, 181Hf; calculated γ-circular polarization. 175Lu, 181Ta transitions calculated γ-circular polarization.
doi: 10.1016/0370-2693(71)90430-8
1969VI01 Phys.Letters 29B, 408 (1969) The Circular Polarization of γ Rays from 181Ta and the Parity Violating One Pion Exchange Potential RADIOACTIVITY 181Ta; calculated γ circular polarization; deduced parity violation in nuclear forces.
doi: 10.1016/0370-2693(69)90232-9
1962GI02 Phys.Letters, 1, 25 (1962) NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(62)90267-6
1962VI01 Nuclear Phys. 29, 89 (1962) The T = 1 Excited States of C12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90168-2
1962VI02 Phys.Letters, 1, 36 (1962) The 0+ States in Oxygen NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
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