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NSR database version of May 30, 2024.

Search: Author = J.Meyer

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the XUNDL database. For more information, click here.

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
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2000DO02      Nucl.Phys. A665, 419 (2000)

F.Douchin, P.Haensel, J.Meyer

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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0870.

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
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1995BB02      Int.J.Mod.Phys. E4, 385 (1995)

R.Barbier, J.Meyer, M.Kibler

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
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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
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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
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1994BA07      J.Phys.(London) G20, L13 (1994)

R.Barbier, J.Meyer, M.Kibler

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
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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
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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
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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
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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
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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
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1992MA47      Nucl.Instrum.Methods Phys.Res. B71, 65 (1992)

A.Mader, J.D.Meyer, K.Bethge

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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0507.

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2016.

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
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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
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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
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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
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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
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1983ME19      Phys.Lett. 133B, 279 (1983)

J.Meyer, P.Quentin, M.Brack

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
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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
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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
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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
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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
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1973ME05      Yad.Fiz. 17, 1197 (1973); Sov.J.Nucl.Phys. 17, 623 (1974)

J.Meyer, J.Speth

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)

J.Meyer, J.Speth

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
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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)

J.Meyer, J.Speth

Theoretical Investigation of the Muonic and Mossbauer Isomer Shifts in 153Eu

doi: 10.1016/0370-2693(72)90130-X
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1972ME18      Nucl.Phys. A193, 60 (1972)

J.Meyer, J.Speth, J.H.Vogeler

Calculation of Moments of Inertia and Gyromagnetic Ratios Including Residual p-h and p-p Interaction

doi: 10.1016/0375-9474(72)90235-7
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1972ME21      Radiochim.Acta 17, 76 (1972)

J.Meyer, J.M.Paulus, J.C.Abbe

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)

J.Meyer, J.Speth

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
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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
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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
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Note: The following list of authors and aliases matches the search parameter J.Meyer: , J.C.MEYER, J.D.MEYER, J.P.MEYER