NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Meyer Found 87 matches. 2024DA05 Phys.Rev. C 109, 034316 (2024) Ph.Da Costa, K.Bennaceur, J.Meyer, W.Ryssens, M.Bender Impact of choices for center-of-mass correction energy on the surface energy of Skyrme energy density functionals
doi: 10.1103/PhysRevC.109.034316
2022PR11 Phys.Rev. C 106, 054321 (2022) P.Proust, Y.Lallouet, D.Davesne, J.Meyer Surface energy coefficient of an N2LO Skyrme energy functional: A semiclassical extended Thomas-Fermi approach
doi: 10.1103/PhysRevC.106.054321
2019RY02 Phys.Rev. C 99, 044315 (2019) W.Ryssens, M.Bender, K.Bennaceur, P.-H.Heenen, J.Meyer Impact of the surface energy coefficient on the deformation properties of atomic nuclei as predicted by Skyrme energy density functionals NUCLEAR STRUCTURE 74Kr, 180,186,188,190,192,194,196,198,200Hg, 186Pb, 226Ra, 240Pu; calculated deformation energy surfaces as function of β20 parameter. 110Zr, 282Cn, 294Og; calculated deformation energy surface contours in (β, γ) plane. 180Hg, 226Ra, 240Pu; calculated heights of first, second and third barrier heights, and energies of fission isomers. Z=90-120, N=140-186; calculated binding energies and other gross properties. 188Hg; calculated Nilsson diagrams for single-particle neutron and proton states. 186,188,190,192,194,196,198,200Hg, 188,190,192,194,196,198,200,202Pb; calculated excitation energies and multipole deformations βp, l0 of the proton distribution of the superdeformed minima, S(2n), and charge quadrupole deformations β2, p for 190,192,194Hg, 192,194,196Pb. 194Hg; calculated dynamical moment of inertia of the superdeformed band as a function of cranking frequency. Z=50, N=46-74; calculated S(2n) for even-even nuclei. Z=44-74, N=82; calculated S(2p) for even-even nuclei. 144Ba; calculated deformation energy surface as a function of octupole deformation parameter β30. 218,220,222,224,226,228,230,232Th; calculated deformation energy surfaces as function of β20 and β30 parameters. 110Zr; calculated deformation energy surface as a function of non-axial octupole deformation parameter β32. Energy density functional (EDF) methods with SLy5sX parametrizations of the Skyrme EDF. Comparison with available experimental data.
doi: 10.1103/PhysRevC.99.044315
2018BE22 Acta Phys.Pol. B49, 331 (2018) P.Becker, D.Davesne, J.Meyer, J.Navarro, A.Pastore Skyrme N2LO Pseudo-potential for Calculations of Properties of Atomic Nuclei NUCLEAR STRUCTURE 132Sn; calculated isoscalar densities vs radius using N2LO extension of usual Skyrme pseudo-potential, neutron effective mass vs density and effective masses of neutrons and protons vs asymmetry parameter using Symmetric Nuclear Matter (SNM) and Pure Neutron Matter (PNM). 40,42,44,46,48,50,52,54Ca, 58,60,62,64,66,68Ni, 110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 136,138,140,142,144,146,148,150,152,154,156,158.160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,!96,198,200,202,204,206,208,210,212,214Pb; calculated average pairing gaps vs neutron number. Compared with data.
doi: 10.5506/aphyspolb.49.331
2018DA05 Phys.Rev. C 97, 044304 (2018) D.Davesne, J.Navarro, J.Meyer, K.Bennaceur, A.Pastore Two-body contributions to the effective mass in nuclear effective interactions
doi: 10.1103/PhysRevC.97.044304
2017BE28 Phys.Rev. C 96, 044330 (2017) P.Becker, D.Davesne, J.Meyer, J.Navarro, A.Pastore Solution of Hartree-Fock-Bogoliubov equations and fitting procedure using the N2LO Skyrme pseudopotential in spherical symmetry NUCLEAR STRUCTURE 208Pb; calculated isoscalar densities, radial dependence of coefficients using the SN2LO1 and SLy5 interactions, for centrifugal and spin-orbit fields. 208Pb, 120Sn, 40Ca; calculated energies (total, kinetic, field, spin-orbit, Coulomb, and neutron pairing) using the WHISKY and LENTEUR codes with self-consistent HF calculations and the SLy5 interaction. 40Ca, 208Pb; calculated neutron single-particle energies around the Fermi energy for SLy5 and SN2LO1 parametrizations. 34,36,38,40,42,44,46,48,50,52,54,56Ca, 48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78Ni, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sn, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 48Ca, 50Ti, 52Cr, 54Fe, 56Ni, 58Zn, 60Ge, 78Ni, 80Zn, 82Ge, 84Se, 86Kr, 88Sr, 90Zr, 92Mo, 94Ru, 96Pd, 98Cd, 100Sn, 130Cd, 132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb, 206Hg, 208Pb, 210Po, 212Rn, 214Ra, 216Th, 218U; calculated binding energies and proton radii for isotopic and isotonic chains using extended Skyrme interaction SN2LO1, and compared with experimental values, as well as with calculations using the SLy5 parametrization.
doi: 10.1103/PhysRevC.96.044330
2016JO08 Phys.Rev. C 94, 024335 (2016) R.Jodon, M.Bender, K.Bennaceur, J.Meyer Constraining the surface properties of effective Skyrme interactions NUCLEAR STRUCTURE 240Pu; calculated surface energy coefficients, deformation energy curves as a function of the dimensionless mass quadrupole moment, correlation between the excitation energy of the fission isomer and the height of the inner and outer fission barriers, nuclear-matter properties. Calculations involved 76 parametrizations of the Skyrme energy density functionals (EDF) using Hartree-Fock (HF) with quantal shell effects, extended Thomas-Fermi (ETF) or modified Thomas-Fermi (MTF) approximations; discussed differences between different methods.
doi: 10.1103/PhysRevC.94.024335
2015DA06 Phys.Rev. C 91, 064303 (2015) D.Davesne, J.Navarro, P.Becker, R.Jodon, J.Meyer, A.Pastore Extended Skyrme pseudopotential deduced from infinite nuclear matter properties
doi: 10.1103/PhysRevC.91.064303
2015DA15 Phys.Scr. 90, 114002 (2015) D.Davesne, J.Meyer, A.Pastore, J.Navarro Partial wave decomposition of the N3LO equation of state
doi: 10.1088/0031-8949/90/11/114002
2013HE26 Phys.Rev. C 88, 064323 (2013) V.Hellemans, A.Pastore, T.Duguet, K.Bennaceur, D.Davesne, J.Meyer, M.Bender, P.-H.Heenen Spurious finite-size instabilities in nuclear energy density functionals NUCLEAR STRUCTURE 16O, 40,48Ca, 78Ni, 176Sn, 208Pb; calculated binding energies; investigated instabilities in energy density functional (EDF) calculations to finite-wavelength instabilities of homogeneous symmetric computed at the RPA level. Nine parameterizations based on traditional form of the Skyrme EDF.Systematic calculations with both HOSPHE and LENTEUR formalisms.
doi: 10.1103/PhysRevC.88.064323
2013PA17 Phys.Scr. T154, 014014 (2013) A.Pastore, D.Davesne, K.Bennaceur, J.Meyer, V.Hellemans Fitting Skyrme functionals using linear response theory NUCLEAR STRUCTURE Z=20, 28, 50, 82; analyzed available data and fitted binding energies, charge radii. Linear response theory in symmetric nuclear matter.
doi: 10.1088/0031-8949/2013/T154/014014
2013SA63 Phys.Rev. C 88, 064326 (2013) J.Sadoudi, T.Duguet, J.Meyer, M.Bender Skyrme functional from a three-body pseudopotential of second order in gradients: Formalism for central terms
doi: 10.1103/PhysRevC.88.064326
2012PA11 Phys.Rev. C 85, 054317 (2012) A.Pastore, D.Davesne, Y.Lallouet, M.Martini, K.Bennaceur, J.Meyer Nuclear response for the Skyrme effective interaction with zero-range tensor terms. II. Sum rules and instabilities
doi: 10.1103/PhysRevC.85.054317
2012PA13 Int.J.Mod.Phys. E21, 1250040 (2012) A.Pastore, K.Bennaceur, D.Davesne, J.Meyer Linear response in infinite nuclear matter as a tool to reveal finite size instabilities
doi: 10.1142/S0218301312500401
2012PA32 Phys.Rev. C 86, 044308 (2012) A.Pastore, M.Martini, V.Buridon, D.Davesne, K.Bennaceur, J.Meyer Nuclear response for the Skyrme effective interaction with zero-range tensor terms. III. Neutron matter and neutrino propagation
doi: 10.1103/PhysRevC.86.044308
2009BE45 Phys.Rev. C 80, 064302 (2009) M.Bender, K.Bennaceur, T.Duguet, P.-H.Heenen, T.Lesinski, J.Meyer Tensor part of the Skyrme energy density functional. II. Deformation properties of magic and semi-magic nuclei NUCLEAR STRUCTURE 40,48Ca, 56,68,78Ni, 80,90,96,100,110Zr, 100,120,132Sn, 186,208Pb; calculated proton and neutron Nilsson diagrams, single-particle energy spectra, deformation energy curves, isoscalar tensor energies using nuclear energy density functionals (EDF) and T22, T26, T44, T62, SLy5, SLy5+T, SLy4, SLy4T, SLy4T(min), SLy4T(self) and TZA parametrizations. Investigated impact of tensor terms in the Skyrme energy density functional on deformation properties of magic and semi-magic nuclei.
doi: 10.1103/PhysRevC.80.064302
2009DA15 Phys.Rev. C 80, 024314 (2009); Erratum Phys.Rev. C 84, 059904 (2011) D.Davesne, M.Martini, K.Bennaceur, J.Meyer Nuclear response for the Skyrme effective interaction with zero-range tensor terms
doi: 10.1103/PhysRevC.80.024314
2009DU13 Int.J.Mod.Phys. E18, 2007 (2009) T.Duguet, T.Lesinski, K.Hebeler, K.Bennaceur, A.Schwenk, J.Meyer Non-empirical energy density functional for nuclei: The pairing part
doi: 10.1142/S0218301309014172
2009LE24 Eur.Phys.J. A 40, 121 (2009) T.Lesinski, T.Duguet, K.Bennaceur, J.Meyer Non-empirical pairing energy density functional; First order in the nuclear plus Coulomb two-body interaction NUCLEAR STRUCTURE Ca, Ni, Sn, Pb; calculated pair gap energies for semi-magic isotonic and isotopic chains using the energy density functional method.
doi: 10.1140/epja/i2009-10780-y
2008BA09 Phys.Rev. C 77, 024311 (2008) J.Bartel, K.Bencheikh, J.Meyer Extended Thomas-Fermi density functionals in the presence of a tensor interaction in spherical symmetry NUCLEAR STRUCTURE 90Zr, 208Pb; calculated neutron spin-orbit densities, neutron spin-orbit potentials. T42 Skyrme parameterization.
doi: 10.1103/PhysRevC.77.024311
2007LE22 Phys.Rev. C 76, 014312 (2007) T.Lesinski, M.Bender, K.Bennaceur, T.Duguet, J.Meyer Tensor part of the Skyrme energy density functional: Spherical nuclei NUCLEAR STRUCTURE Ca, Ni, Sn, Pb; calculated single particle energies using the Skyrme interaction with Tensor terms.
doi: 10.1103/PhysRevC.76.014312
2006LE36 Phys.Rev. C 74, 044315 (2006) T.Lesinski, K.Bennaceur, T.Duguet, J.Meyer Isovector splitting of nucleon effective masses, ab initio benchmarks and extended stability criteria for Skyrme energy functionals NUCLEAR STRUCTURE 78Ni, 132,156Sn, 208Pb; calculated single-particle energy levels. Sn, Pb; calculated binding energies, pair gap energies vs neutron number. 40Ca, 56Ni; calculated nucleon density distributions.
doi: 10.1103/PhysRevC.74.044315
2004CO05 Nucl.Phys. A731, 34 (2004) B.Cochet, K.Bennaceur, P.Bonche, T.Duguet, J.Meyer Compressibility, effective mass and density dependence in Skyrme forces
doi: 10.1016/j.nuclphysa.2003.11.015
2004CO06 Int.J.Mod.Phys. E13, 187 (2004) B.Cochet, K.Bennaceur, J.Meyer, P.Bonche, T.Duguet Skyrme forces with extended density dependence
doi: 10.1142/S021830130400193X
2004CO13 Phys.Rev. C 70, 024307 (2004) G.Colo, N.Van Giai, J.Meyer, K.Bennaceur, P.Bonche Microscopic determination of the nuclear incompressibility within the nonrelativistic framework NUCLEAR STRUCTURE 16O, 40,48Ca, 56,78Ni, 100,132Sn, 208Pb; analyzed binding energies, radii; deduced parameters. 208Pb; calculated giant monopole resonance energy; deduced nuclear incompressibility.
doi: 10.1103/PhysRevC.70.024307
2003BE78 C.R.Physique 4, 555 (2003) K.Bennaceur, P.Bonche, J.Meyer Mean field theories and exotic nuclei
doi: 10.1016/S1631-0705(03)00060-4
2003ME35 Ann.Phys.(Paris) 28, 1 (2003) Interactions effectives, theories de champ moyen, masses et rayons nucleaires
2002DU01 Phys.Rev. C65, 014310 (2002) T.Duguet, P.Bonche, P.-H.Heenen, J.Meyer Pairing Correlations. I. Description of Odd Nuclei in Mean-Field Theories NUCLEAR STRUCTURE 150,151,152,153,154,155,156,157,158,159,160Ce; calculated single-particle levels, deformation parameters, pairing effects. 119,121,123,125,127,129,131,133,135,137,139,141,143,145,147,149,151,153,155,157,159,161,163,165Ce; calculated odd-even energy differences, polarization effect, pairing effects. Mean-field approach.
doi: 10.1103/PhysRevC.65.014310
2002DU02 Phys.Rev. C65, 014311 (2002) T.Duguet, P.Bonche, P.-H.Heenen, J.Meyer Pairing Correlations. II. Microscopic Analysis of Odd-Even Mass Staggering in Nuclei NUCLEAR STRUCTURE Ce, Sn; calculated odd-even mass differences, role of pairing correlations.
doi: 10.1103/PhysRevC.65.014311
2000BO53 Phys.Rev. C62, 064903 (2000) V.Borchers, J.Meyer, S.Gieseke, G.Martens, C.C.Noack Poincare-Covariant Parton Cascade Model for Ultrarelativistic Heavy-Ion Reactions NUCLEAR REACTIONS 1H(p-bar, X), E(cm)=200-1800 GeV; S(S, X), Pb(Pb, X), 197Au(197Au, X), E=high; calculated parton pseudorapidity and transverse momentum distributions. Poincare-covariant parton cascade model.
doi: 10.1103/PhysRevC.62.064903
2000BU06 Eur.Phys.J. A 7, 347 (2000) N.Buforn, A.Astier, J.Meyer, M.Meyer, S.Perries, N.Redon, O.Stezowski, M.G.Porquet, I.Deloncle, A.Bauchet, J.Duprat, B.J.P.Gall, C.Gautherin, E.Gueorguieva, F.Hoellinger, T.Kutsarova, R.Lucas, A.Minkova, N.Schulz, H.Sergolle, Ts.Venkova, A.N.Wilson Evidence for Deformation in 113-116Cd Isotopes NUCLEAR REACTIONS 176Yb(28Si, F), E=145 MeV; measured Eγ, Iγ(θ), γγ-coin. 113,114,115,116Cd deduced high-spin levels J, π, alignments, deformation. Comparison with theoretical calculations. Eurogam2 array.
doi: 10.1007/s100500050401
2000BU23 Phys.Scr. T88, 45 (2000) N.Buforn, A.Astier, J.Meyer, M.Meyer, S.Perries, N.Redon, M.G.Porquet, I.Deloncle, A.Bauchet, F.Azaiez, S.Bouneau, C.Bourgeois, J.Duprat, B.J.P.Gall, C.Gautherin, E.Gueorguieva, F.Hoellinger, T.Kutsarova, R.Lucas, A.Minkova, N.Schulz, H.Sergolle, T.Venkova, A.N.Wilson High-Spin Structure of the 113-116Cd Isotopes Produced by Heavy-Ion Induced Fission Reaction NUCLEAR REACTIONS 176Yb(28Si, F)113Cd/114Cd/115Cd/116Cd/, E=165 MeV; measured Eγ, Iγ, γγ-coin. 113,114,115,116Cd deduced high-spin levels, J, π. Level systematics in neighboring isotopes discussed. Eurogam II array.
doi: 10.1238/Physica.Topical.088a00045
2000DO02 Nucl.Phys. A665, 419 (2000) Nuclear Surface and Curvature Properties for SLy Skyrme Forces and Nuclei in the Inner Neutron-Star Crust
doi: 10.1016/S0375-9474(99)00397-8
2000DR06 Nucl.Phys. A663-664, 843c (2000) L.O.C.Drury, D.C.Ellisson, J.-P.Meyer Interpreting the Cosmic Ray Composition
doi: 10.1016/S0375-9474(99)00728-9
2000ME03 Phys.Rev. C61, 035202 (2000) J.Meyer, G.Papp, H.-J.Pirner, T.Kunihiro Renormalization Group Flow Equation at Finite Density
doi: 10.1103/PhysRevC.61.035202
2000SC01 Phys.Lett. 473B, 25 (2000) K.Schwenzer, J.Meyer, H.J.Pirner Unifying Nucleon and Quark Dynamics at Finite Baryon Number Density
doi: 10.1016/S0370-2693(99)01462-8
1999BO57 Nucl.Phys. A661, 587c (1999) V.Borchers, S.Gieseke, G.Martens, J.Meyer, C.C.Noack A Poincare-Covariant Parton Cascade Model for Ultrarelativistic Heavy-Ion Reactions NUCLEAR REACTIONS 1H(p-bar, X), E(cm)=200 GeV; 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated parton momentum, rapidity distributions. Poincare-covariant parton cascade model.
doi: 10.1016/S0375-9474(99)85094-5
1999DA30 Nucl.Phys. (Supplement) A654, 655c (1999) H.Dancer, S.Perries, P.Bonche, H.Flocard, P.-H.Heenen, J.Meyer, M.Meyer Generator Coordinate Method and Superdeformation in A = 190 Nuclei NUCLEAR STRUCTURE 190,192,194,196Hg, 192,194,196,198Pb; calculated E0, E2 transition rates for decay out of superdeformed bands; deduced E2 transition dominance.
doi: 10.1016/S0375-9474(00)88520-6
1999PI05 Nucl.Phys. A652, 142 (1999) J.Piperova, D.Samsoen, P.Quentin, K.Bencheikh, J.Bartel, J.Meyer Bulk Properties of Rotating Nuclei and the Validity of Liquid Drop Model at Finite Angular Momenta NUCLEAR STRUCTURE Z=20-98; calculated Routhians; deduced liquid-drop model parameters vs spin. 90Zr, 150Sm, 208Pb, 240Pu; calculated proton distribution radii, Coulomb energies. 236U; calculated fissility parameter vs spin.
doi: 10.1016/S0375-9474(99)00159-1
1998CH17 Nucl.Phys. A635, 231 (1998); Erratum Nucl.Phys. A643, 441 (1998) E.Chabanat, P.Bonche, P.Haensel, J.Meyer, R.Schaeffer A Skyrme Parametrization from Subnuclear to Neutron Star Densities Part II. Nuclei Far from Stabilities NUCLEAR STRUCTURE Ni, Sn, Pb; calculated binding energies, two-neutron separation energies. Pb; calculated isotopic shifts. 208Pb; calculated single-particle levels. Several Skyrme parametrizations compared.
doi: 10.1016/S0375-9474(98)00180-8
1998DA20 Phys.Rev. C58, 2068 (1998) H.Dancer, P.Bonche, H.Flocard, P.-H.Heenen, J.Meyer, M.Meyer Monopole Strength and Decay Out of Superdeformed Bands in the A = 190 Mass Region from Theories Beyond the Mean Field NUCLEAR STRUCTURE 190,192,194,196,198Hg, 192,194,196,198,200Pb; calculated E0, E2 transition rates from superdeformed bands; deduced E2 transitions dominance. Generator coordinate method, comparison with two-level model.
doi: 10.1103/PhysRevC.58.2068
1997CH49 Nucl.Phys. A627, 710 (1997) E.Chabanat, P.Bonche, P.Haensel, J.Meyer, R.Schaeffer A Skyrme Parametrization from Subnuclear to Neutron Star Densities NUCLEAR STRUCTURE 16O, 40,48Ca, 56,78Ni, 100,132Sn, 208Pb; calculated binding energies, radii; deduced parameters. Skyrme parametrization.
doi: 10.1016/S0375-9474(97)00596-4
1997PE04 Phys.Rev. C55, 1797 (1997) S.Perries, D.Samsoen, J.Meyer, M.Meyer, P.Quentin Collective Gyromagnetic Ratios and the Structure of Odd Superdeformed A = 190 Nuclei NUCLEAR STRUCTURE 152Sm, 158Gd, 162Dy, 166Er, 174Yb, 178Hf, 182,184W, 188,190,192Os, 194Pt; calculated ground state collective gyromagnetic factors. 190,192,194,196,198,200Pb, 188,190,192,194,196,198Hg; calculated gyromagnetic ratios at superdeformed minima, (g(K)-g(R)/Q0)K. 193Hg, 193Pb, 193,195Tl; calculated superdeformed minima magnetic properties. Microsocopic approach.
doi: 10.1103/PhysRevC.55.1797
1996BA49 Acta Phys.Pol. B27, 133 (1996) J.Bartel, K.Bencheikh, E.Chabanat, J.Meyer, I.Mikhailov, J.Piperova, P.Quentin, D.Samsoen Extended Thomas-Fermi Description of Rotating Nuclei
1996MI28 Nucl.Instrum.Methods Phys.Res. B108, 62 (1996) R.W.Michelmann, H.Baumann, A.Markwitz, J.D.Meyer, K.Bethge Investigation of Ultra Thin SiN(x)O(y) Layers Produced by Low-Energy Ion Implantation with NRA and Channeling-RBS NUCLEAR REACTIONS 18O(p, α), E=152 keV; measured α spectra; 15N(p, αγ), E=429 keV; measured γ spectra; deduced implanted ions depth profile in Si.
doi: 10.1016/0168-583X(95)01047-5
1996PR17 Nucl.Instrum.Methods Phys.Res. B117, 18 (1996) U.Prigge, J.D.Meyer, R.W.Michelmann, K.Bethge Investigation of the Reaction 15N(α, n)18F for Materials Analysis NUCLEAR REACTIONS 15N(α, n), E=8-14 MeV; measured σ. Materials analysis application discussed.
doi: 10.1016/0168-583X(96)00233-9
1996SO21 Nucl.Instrum.Methods Phys.Res. B 113, 399 (1996) M.Soltani-Farshi, J.D.Meyer, P.Misaelides, K.Bethge Cross section of the 32S(α, p)35Cl nuclear reaction for sulphur determination NUCLEAR REACTIONS 32S(α, p), E=5.9-12 MeV; measured products, 35Cl, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry O0870.
doi: 10.1016/0168-583X(95)01415-2
1996VO23 Nucl.Instrum.Methods Phys.Res. B117, 21 (1996) M.Vollmer, J.D.Meyer, R.W.Michelmann, K.Bethge Boron Detection using the Nuclear Reaction 11B(p, α)2α NUCLEAR REACTIONS 11B(p, α), E=150-800 keV; measured σ(θ). Boron impurity detection application.
doi: 10.1016/0168-583X(96)00235-2
1995BB02 Int.J.Mod.Phys. E4, 385 (1995) A U(qp)(u2) Rotor Model for Rotational Bands of Superdeformed Nuclei NUCLEAR STRUCTURE 130La, 132Ce, 134,136Nd, 146,148,150Gd, 152Dy, 190,192,194Hg, 192,194,196,198Pb, 194Tl; analyzed superdeformed band associated transitions Eγ, Iγ. Nonrigid rotor model based on two-parameter U(qp)(u2) quantum algebra.
doi: 10.1142/S0218301395000122
1995CH57 Phys.Scr. T56, 231 (1995) E.Chabanat, P.Bonche, P.Haensel, J.Meyer, R.Schaeffer New Skyrme Effective Forces for Supernovae and Neutron Rich Nuclei NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140Sn; calculated two neutron separation energies. Z=32-78; calculated two proton separation energies. Hartree-Fock plus BCS formalism, new Skyrme-like effective interactions.
doi: 10.1088/0031-8949/1995/T56/034
1995ME07 Nucl.Phys. A588, 597 (1995) J.Meyer, P.Bonche, M.S.Weiss, J.Dobaczewski, H.Flocard, P.-H.Heenen Quadrupole and Octupole Correlations in Normal, Superdeformed and Hyperdeformed States of 194Pb NUCLEAR STRUCTURE 192,194,196,198,200Pb; calculated superdeformed band population evolution, spectra, energy curves vs quadrupole moment, quadrupole, octupole correlations in normal, hyperdeformed bands as well. Generator coordinate method.
doi: 10.1016/0375-9474(95)00055-6
1994BA07 J.Phys.(London) G20, L13 (1994) A U(qp)(u2) Model for Rotational Bands of Nuclei NUCLEAR STRUCTURE 192,194Hg, 192,194,196,198Pb; calculated γ transition energies, rotating superdeformed nuclei. Two-parameter quantum algebra based rotational model.
doi: 10.1088/0954-3899/20/1/003
1994BO24 Nucl.Phys. A574, 185c (1994) P.Bonche, E.Chabanat, B.Q.Chen, J.Dobaczewski, H.Flocard, B.Gall, P.H.Heenen, J.Meyer, N.Tajima, M.S.Weiss Microscopic Approach to Collective Motion NUCLEAR STRUCTURE 192Hg, 194Pb; calculated superdeformed bands, energies, quadrupole moments, dynamical, rigid body moments of inertia, Eγ. 194,196,198,200,202,204,206,208,210,212,214,216,218,220Pb; calculated proton, neutron rms radii. Microscopic approach, collective motion.
doi: 10.1016/0375-9474(94)90045-0
1994CH24 Phys.Lett. 325B, 13 (1994) E.Chabanat, J.Meyer, K.Bencheikh, P.Quentin, J.Bartel Equilibrium Deformations of Rotating Nuclei in a Self-Consistent Semiclassical Approach NUCLEAR STRUCTURE 90Zr, 56Ni, 208Pb; calculated deformation to sphericity energies ratio. 90Zr; calculated extended Thomas-Fermi moment of inertia vs rotational energy frequency. Other nuclei also studied. Self-consistent semi-classical approach.
doi: 10.1016/0370-2693(94)90064-7
1993BE31 Nucl.Phys. A557, 459c (1993) K.Bencheikh, P.Quentin, J.Bartel, J.Meyer A Semiclassical Description of Rapidly Rotating Nuclei NUCLEAR STRUCTURE 16O, 56Ni, 90Zr, 140Ce, 240Pu, 202,208,214Pb, 116,132Sn; calculated moments of inertia. Extended Thomas-Fermi model, other Sn, Pb isotopes included.
doi: 10.1016/0375-9474(93)90562-C
1993SK01 Nucl.Phys. A551, 109 (1993) J.Skalski, P.-H.Heenen, P.Bonche, H.Flocard, J.Meyer Octupole Correlations in Superdeformed Mercury and Lead Nuclei: A generator-coordinate method analysis NUCLEAR STRUCTURE 194Pb, 194,192Hg; calculated axial, nonaxial octupole level energies built on superdeformed states, B(λ); deduced weak coupling. Generator coordinate method, self-consistent Hartree-Fock BCS basis.
doi: 10.1016/0375-9474(93)90306-I
1992KR07 Nucl.Phys. A542, 43 (1992) S.J.Krieger, P.Bonche, M.S.Weiss, J.Meyer, H.Flocard, P.-H.Heenen Super-Deformation and Shape Isomerism: Mapping the isthmus NUCLEAR STRUCTURE Z=108-152; calculated excitation energy, rigid moment of inertia. 190,192,194,196,198,200,202,204,206,210,212,214,216,218,220,222,224,226,228,230Pb calculated rigid moment of inertia, quadrupole moment, superdeformed isomers; deduced shape isomerism isthmus superdeformation region. Microscopic Hartree-Fock-BCS formalism.
doi: 10.1016/0375-9474(92)90395-Z
1992MA47 Nucl.Instrum.Methods Phys.Res. B71, 65 (1992) Modifications of the Gallium Arsenide Crystal Surface during Annealing NUCLEAR REACTIONS, ICPND 12C, 16O(d, p), E=1.4 MeV; measured yield; deduced GaAs crystal surface modifications during annealing.
doi: 10.1016/0168-583X(92)95341-N
1991ME07 Nucl.Phys. A533, 307 (1991) J.Meyer, P.Bonche, J.Dobaczewski, H.Flocard, P.H.Heenen Pairing Vibrations and Stability of Superdeformed States NUCLEAR STRUCTURE 194Hg; calculated levels, quadrupole moments; deduced pairing vibrations role in superdeformed state stability.
doi: 10.1016/0375-9474(91)90492-O
1990AY02 Nucl.Phys. A515, 365 (1990) J.Aysto, P.P.Jauho, Z.Janas, A.Jokinen, J.M.Parmonen, H.Penttila, P.Taskinen, R.Beraud, R.Duffait, A.Emsallem, J.Meyer, M.Meyer, N.Redon, M.E.Leino, K.Eskola, P.Dendooven Collective Structure of the Neutron-Rich Nuclei, 110Ru and 112Ru RADIOACTIVITY 110,112Tc(β-) [from 228U(p, F), E=20 MeV]; measured β-decay T1/2, Qβ-, Iγ, I(ce), β-γ-.γγ-coin. 110,112Ru deduced levels, J, π, level systematics, mass quadrupole moments, equilibrium shapes. Ge, Si-Li, plastic detectors. Hartree-Fock potential energy calculations. NUCLEAR STRUCTURE 108,110,112Ru; calculated levels, mass quadrupole moments, equilibrium shapes. Hartree-Fock calculations.
doi: 10.1016/0375-9474(90)90590-I
1990BO14 Nucl.Phys. A510, 466 (1990) P.Bonche, J.Dobaczewski, H.Flocard, P.-H.Heenen, J.Meyer Analysis of the Generator Coordinate Method in a Study of Shape Isomerism in 194Hg NUCLEAR STRUCTURE 194Hg; calculated deformation energy, large amplitude quadrupole dynamics. Collective BCS basis states, generator coordinate method.
doi: 10.1016/0375-9474(90)90062-Q
1990BO40 Nucl.Phys. A519, 509 (1990) P.Bonche, J.Dobaczewski, H.Flocard, P.H.Heenen, S.J.Krieger, J.Meyer, M.S.Weiss Quadrupole Collective Correlations and the Depopulation of the Superdeformed Bands in Mercury NUCLEAR STRUCTURE 190,192,194,196,198Hg; calculated deformation energy, wave functions, proton quadrupole moments, superdeformed band decay Iγ. Self-consistent generator coordinate method, Hartree-Fock plus BCS wave functions.
doi: 10.1016/0375-9474(90)90443-P
1990GL02 Ann.Phys.(New York) 197, 205 (1990) P.Gleissl, M.Brack, J.Meyer, P.Quentin A Density Variational Approach to Nuclear Giant Resonances at Zero and Finite Temperature NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 140Ce, 208Pb; calculated giant resonances, sum rule quantities. Density variational approach, zero, finite temperatures.
doi: 10.1016/0003-4916(90)90211-6
1990MI11 Nucl.Instrum.Methods Phys.Res. B51, 1 (1990) R.W.Michelmann, J.Krauskopf, J.D.Meyer, K.Bethge Excitation Functions for the Reactions 10B(d, n)11C and 12C(d, n)13N for Charged Particle Activation Analysis NUCLEAR REACTIONS, ICPND 10B, 12C(d, n), E=0.5-6 MeV; measured absolute σ(E). Particle activation analysis.
doi: 10.1016/0168-583X(90)90530-8
1990QU01 Phys.Rev. C41, 341 (1990); Erratum Phys.Rev. C43, 361 (1991) P.Quentin, N.Redon, J.Meyer, M.Meyer Approximate Energy Correction for Particle Number Symmetry Breaking in Constrained Hartree-Fock plus BCS Calculations NUCLEAR STRUCTURE 40Ca; calculated nucleon gap energies, deformation potential energy vs mass quadrupole moment. 106Cd; calculated deformation potential energy vs mass quadrupole moment. 92,94,96,98,100,102Zr; calculated proton quadrupole deformation parameter vs nucleon number. 196Pt, 240Pu; calculated axial deformation potential energy vs instrinsic quadrupole moment. Constrained Hartree-Fock plus BCS.
doi: 10.1103/PhysRevC.41.341
1989BO24 Nucl.Phys. A500, 308 (1989) P.Bonche, S.J.Krieger, P.Quentin, M.S.Weiss, J.Meyer, M.Meyer, N.Redon, H.Flocard, P.-H.Heenen Superdeformation and Shape Isomerism at Zero Spin NUCLEAR STRUCTURE 186,196,194,192,190,188,186,202,210Os, 200,198,196,194,192,190,188,186Pt, 194,202,210,218Hg; calculated Hartree-Fock energies, energy surfaces. 192,194,196,198,200,202,204,206,208,210,212,214,216,218Hg; calculated secondary minima deformations. 194,196,198Pt; calculated axial deformation energies. 66,68Ni, 190,192Pt, 206,208,210Os, 194,196,214Hg; deduced possible superdeformation effects. Microscopic Hartree-Fock plus BCS.
doi: 10.1016/0375-9474(89)90426-0
1989LI06 Nucl.Instrum.Methods Phys.Res. B36, 7 (1989) V.Liebler, K.Bethge, J.Krauskopf, J.D.Meyer, P.Misaelides, G.Wolf Determination of Excitation Functions for Carbon Detection by Charged Particle Activation Analysis NUCLEAR REACTIONS, ICPND 12C(3He, α), (3He, d), E=0.4-14 MeV; measured absolute σ(E). Charged particle activation analysis.
doi: 10.1016/0168-583X(89)90053-0
1988RE08 Phys.Rev. C38, 550 (1988) N.Redon, J.Meyer, M.Meyer, P.Quentin, P.Bonche, H.Flocard, P.-H.Heenen Proton-Rich Exotic Heavy Nuclei: Self-consistent calculations NUCLEAR STRUCTURE 92,96,98,100,102,104,106,108,110Cd; 142,140,138,136,134,132Sm; calculated potential energy surfaces; deduced deformation features.
doi: 10.1103/PhysRevC.38.550
1987GL08 J.Phys.(Paris), Colloq.C-2, 3 (1987) P.Gleissl, M.Brack, J.Meyer, Ph.Quentin Nuclear Giant Resonances in Coordinate Space - A Semiclassical Density Functional Approach NUCLEAR STRUCTURE 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb; calculated isoscalar, isovector energies. A=20-235; calculated giant resonance energies vs mass. 40Ca, 90Zr, 208Pb; calculated sum rules, monopole energies. 208Pb; calculated giant resonance energies vs temperature. Semi-classical model.
1987LE26 Nucl.Phys. B294, 1013 (1987) F.Lehar, A.de Lesquen, J.P.Meyer, L.van Rossum, P.Chaumette, J.Deregel, J.Fabre, J.M.Fontaine, F.Perrot, J.Ball, C.D.Lac, A.Michalowicz, Y.Onel, D.Adams, J.Bystricky, V.Ghazikhanian, C.A.Whitten, A.Penzo Measurement of the Spin Correlation Parameter A(oonn(pp)) in a Large Angular Region between 0.88 and 2.7 GeV NUCLEAR REACTIONS 1H(polarized p, p), E=0.88-2.7 GeV; measured spin correlation parameters. Polarized target.
doi: 10.1016/0550-3213(87)90619-5
1987PE17 Nucl.Phys. B294, 1001 (1987) F.Perrot, J.M.Fontaine, F.Lehar, A.de Lesquen, J.P.Meyer, L.van Rossum, P.Chaumette, J.Deregel, J.Fabre, J.Ball, C.D.Lac, A.Michalowicz, Y.Onel, B.Aas, D.Adams, J.Bystricky, V.Ghazikhanian, G.Igo, F.Sperisen, C.A.Whitten, A.Penzo Measurement of the pp Analyzing Power A(oono) in a Large Angular Region between 0.88 and 2.7 GeV NUCLEAR REACTIONS 1H(polarized p, p), E=0.88-2.7 GeV; measured analyzing powers vs θ. Polarized target.
doi: 10.1016/0550-3213(87)90618-3
1986ME03 Phys.Lett. 172B, 122 (1986) J.Meyer, J.Bartel, M.Brack, P.Quentin, S.Aicher A Simple Gaussian Approximation for the One-Body Density Matrix NUCLEAR STRUCTURE 40Ca, 208Pb; calculated defect function, proton distribution, total binding energies. 16O, 48Ca, 90Zr; calculated total binding energies. Gaussian density matrix approach.
doi: 10.1016/0370-2693(86)90820-8
1986RE15 Phys.Lett. 181B, 223 (1986) N.Redon, J.Meyer, M.Meyer, P.Quentin, M.S.Weiss, P.Bonche, H.Flocard, P.-H.Heenen A Self-Consistent Study of Triaxial Deformations in Heavy Nuclei NUCLEAR STRUCTURE 138Sm, 186Pt, 192Os; calculated constant pairing matrix elements, potential energy surfaces. Lattice Hartree-Fock + BCS calculations.
doi: 10.1016/0370-2693(86)90036-5
1983ME19 Phys.Lett. 133B, 279 (1983) A Sum Rule Description of Giant Resonances at Finite Temperature NUCLEAR STRUCTURE 208Pb; calculated isovector dipole, isoscalar monopole resonance energy vs temperature. Sum rule method.
doi: 10.1016/0370-2693(83)90146-6
1982ME08 Nucl.Phys. A385, 269 (1982) J.Meyer, P.Quentin, B.K.Jennings The Isovector Dipole Mode: A simple sum rule approach NUCLEAR REACTIONS 16O, 40Ca, 208Pb(γ, X), E not given; calculated σ(photoabsorption). Sum rules, different models.
doi: 10.1016/0375-9474(82)90172-5
1978ME14 Lett.Nuovo Cim. 22, 355 (1978) J.Meyer, R.S.Nahabetian, E.Elbaz Optical-Model Analysis of Vector Polarized 6Li Elastic Scattering on 12C, 16O, 28Si and 58Ni Nuclei NUCLEAR REACTIONS 12C, 16O, 28Si, 58Ni(polarized 6Li, 6Li), E=22.8 MeV; measured σ(θ), A(θ).
doi: 10.1007/BF02820582
1978ME20 J.Phys.(Paris), Lett. 39, L-158 (1978) J.Meyer, R.S.Nahabetian, E.Elbaz Exact-Finite-Range DWBA Analysis of 12C(6Li, α)14N Reaction at E(6Li) = 20 MeV NUCLEAR REACTIONS 12C(polarized 6Li, α), E=20 MeV; calculated iT11. 14N levels deduced reaction mechanism. Exact finite range DWBA.
doi: 10.1051/jphyslet:019780039011015800
1973EL04 Phys.Rev. C7, 1445 (1973) E.Elbaz, C.Fayard, G-H.Lamot, J.Meyer, R.S.Nahabetian, J.Pigeon, P.Boschan Survey of Some Nuclear Properties Given by a Nonlocal Separable Nucleon-Nucleon Interaction NUCLEAR STRUCTURE 3H, 4He, 12C, 16O, 28Si, 32S, 40Ca calculated binding energy; 20Ne, 24Mg, 28Si, 32S, 36Ar calculated Hartree-Fock energies, energy gap, mean J2. 20Ne, 24Mg, 28Si calculated measured B(E2).
doi: 10.1103/PhysRevC.7.1445
1973ME05 Yad.Fiz. 17, 1197 (1973); Sov.J.Nucl.Phys. 17, 623 (1974) Variation of Nuclear Quadrupole Moments Due to Rotation, Calculated with Residual ph and pp Interactions NUCLEAR STRUCTURE 150Nd, 152,154Sm, 154,156,158,160Gd, 156,158,160,162,164Dy, 158,160,162,164,166,168,170Er, 168,170,172,174,176Yb, 172,174,176,178,180Hf; calculated variation of nuclear quadrupole moments due to rotation.
1973ME08 Nucl.Phys. A203, 17 (1973) Change of Nuclear Radii Due to Rotation; Calculation of Mossbauer and Muonic Isomer Shifts NUCLEAR STRUCTURE 150Nd, 152,154Sm, 154,156,158,160Gd, 156,158,160,162,164Dy, 158,160,162,164,166,168,170Er, 164,166,168,170,172,174,176,178Yb, 172,174,176,178,180Hf, 180,182,184,186W, 188,190,192Os; calculated Mossbauer, muonic isomer shifts of 2+-70+ transitions.
doi: 10.1016/0375-9474(73)90421-1
1972EL16 LYCEN-7213 (1972) E.El Baz, J.Meyer, R.Nahabetian, J.Pigeon DWBA Analysis of Sub-Coulomb Multi-Transfer Reactions
1972ME10 Phys.Lett. 39B, 330 (1972) Theoretical Investigation of the Muonic and Mossbauer Isomer Shifts in 153Eu
doi: 10.1016/0370-2693(72)90130-X
1972ME18 Nucl.Phys. A193, 60 (1972) Calculation of Moments of Inertia and Gyromagnetic Ratios Including Residual p-h and p-p Interaction
doi: 10.1016/0375-9474(72)90235-7
1972ME21 Radiochim.Acta 17, 76 (1972) Charge des Atomes de Recul 208Pb et 208Tl Formes par Desintegration a de 212Po et 212Bi RADIOACTIVITY 212Po, 212Bi; measured 208Pb, 208Tl recoil charges.
1972ME24 Phys.Scr. 6, 283 (1972) 2+ Isomer Shifts of Rare-Earth Nuclei NUCLEAR STRUCTURE 154,156,158,160Gd, 158,160,162,164Dy, 164,166,168Er, 168,170,172,174Yb; calculated isomer shift.
doi: 10.1088/0031-8949/6/5-6/014
1970BU08 Nucl.Phys. A149, 488 (1970) J.-P.Burq, G.Hadinger, J.Kouloumdjian, J.Meyer Asymetries Produites par les Deutons de 28 MeV Polarises Vectoriellement dans les Diffusions Elastiques 12C(d, d)12C, 28Si(d, d)28Si et 40Ca(d, d)40Ca NUCLEAR REACTIONS 12C, 28Si, 40Ca(vector-polarized d, d), Ed=28 MeV; measured σ(θ), P(θ); deduced optical-model parameters.
doi: 10.1016/0375-9474(70)91042-0
1967YT03 Physica 34, 559 (1967) C.Ythier, J.C.Meyer, J.Konijn, R.Van Lieshout Sur la Desintegration de 81Se NUCLEAR STRUCTURE 81Se; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-8914(67)90227-3
Back to query form Note: The following list of authors and aliases matches the search parameter J.Meyer: , J.C.MEYER, J.D.MEYER, J.P.MEYER |