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NSR database version of April 26, 2024.

Search: Author = J.Moreau

Found 23 matches.

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1988RY03      Nucl.Phys. A476, 237 (1988)

J.Ryckebusch, M.Waroquier, K.Heyde, J.Moreau, D.Ryckbosch

An RPA Model for the Description of One-Nucleon Emission Processes and Application to 16O(γ, n) Reactions

NUCLEAR REACTIONS 16O(γ, p), E=80, 100 MeV; 16O(γ, n), E=80 MeV; calculated σ(θ). Coordinate space RPA.

doi: 10.1016/0375-9474(88)90483-6
Citations: PlumX Metrics


1987HE09      Nucl.Phys. A466, 189 (1987)

K.Heyde, J.Jolie, J.Moreau, J.Ryckebusch, M.Waroquier, P.van Duppen, M.Huyse, J.L.Wood

A Shell-Model Description of 0+ Intruder States in Even-Even Nuclei

NUCLEAR STRUCTURE 106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated 0+ intruder state energies. 190,192,194,196,198,200,202,204,206,208Pb; calculated intruder state energies, monopole, quadupole binding energy corrections. 90,92,94,96,98,100Zr; calculated 2p-2h intruder state energies, pairing energy contributions. 96,98,100,102,104Mo; calculated monopole energy correction term. 146,148,150,152,154,156,158,160Gd; calculated intruder state energies. Shell model.

doi: 10.1016/0375-9474(87)90439-8
Citations: PlumX Metrics


1987KU07      Helv.Phys.Acta 60, 456 (1987)

D.Kusnezov, A.Bruder, V.Ionescu, J.Kern, M.Rast, K.Heyde, P.Van Isacker, J.Moreau, M.Waroquier, R.A.Meyer

Mixing of the Ground Band and Two-Particle Four-Hole Intruder Band in 110Cd

NUCLEAR STRUCTURE 110Cd; calculated positive parity levels, J, π. Interacting boson model, configuration mixing calculations.


1986HE13      Phys.Lett. 176B, 255 (1986)

K.Heyde, J.Jolie, J.Moreau, J.Ryckebusch, M.Waroquier, J.L.Wood

A New Prescription for Determining Particle-Hole Interactions near Closed Shells

NUCLEAR STRUCTURE 20O, 21F, 22Ne, 40,41,42Ti, 60Ni, 61Cu, 62Zn, 100Zr, 101Nb, 102Mo, 132Sn, 133Sb, 134Te, 207Tl, 208Pb, 209Bi, 210Po; calculated particle-hole matrix elements; deduced energy shift from Blomqvist prescription. Data input.

doi: 10.1016/0370-2693(86)90159-0
Citations: PlumX Metrics


1985BO31      Phys.Rev.Lett. 55, 1661 (1985)

D.Bohle, A.Richter, K.Heyde, P.Van Isacker, J.Moreau, A.Sevrin

Study of the Mixed-Symmetry J(π) = 2+ States in 156Gd with Inelastic Electron Scattering

NUCLEAR REACTIONS 156Gd(e, e'), E=36, 42, 45 MeV; measured σ(E(e')); deduced effective neutron, boson charges. 156Gd deduced levels, J, π, B(E2) strength distribution. Interacting boson model.

doi: 10.1103/PhysRevLett.55.1661
Citations: PlumX Metrics


1985JO01      Nucl.Phys. A438, 15 (1985)

J.Jolie, P.Van Isacker, K.Heyde, J.Moreau, G.Van Landeghem, M.Waroquier, O.Scholten

Multilevel Description of the Rh Isotopes in the Interacting Boson-Fermion Model

NUCLEAR STRUCTURE 101,103,105,107,109Rh; calculated levels, B(λ), C2S. Interacting boson-fermion model.

doi: 10.1016/0375-9474(85)90116-2
Citations: PlumX Metrics


1985SC07      Nucl.Phys. A438, 41 (1985)

O.Scholten, K.Heyde, P.Van Isacker, J.Jolie, J.Moreau, M.Waroquier, J.Sau

Mixed-Symmetry States in the Neutron-Proton Interacting Boson Model

NUCLEAR STRUCTURE 98,100,102,104,106,108,110,112,114,116,118,120,122,124,126Pd, 186,188,190,192,196,198Pt; calculated levels, F-spin vector reduced matrix elements. 148,150,152,154,156Sm; calculated levels, B(λ), F-spin vector reduced matrix elements. 156,158Gd, 168Er; calculated levels. Interacting boson model, different dynamical symmetries.

doi: 10.1016/0375-9474(85)90118-6
Citations: PlumX Metrics


1984HE05      Phys.Rev. C29, 1420 (1984)

K.Heyde, P.Van Isacker, M.Waroquier, J.Moreau

Triaxial Shapes in the Interacting Boson Model

NUCLEAR STRUCTURE 104Ru; calculated levels, B(E2); deduced cubic terms role. Interacting boson model, U(5), O(6), SU(3) limits.

doi: 10.1103/PhysRevC.29.1420
Citations: PlumX Metrics


1984HE06      Phys.Rev. C29, 1428 (1984)

K.Heyde, J.Jolie, P.Van Isacker, J.Moreau, M.Waroquier

High-Spin States and the Boson Cutoff in Rotational Nuclei: Application to even-even Dy nuclei

NUCLEAR STRUCTURE 154,156,158,160,162,164Dy; calculated levels, potential energy surfaces, quadrupole deformation, B(E2), backbending effects. Interacting boson model.

doi: 10.1103/PhysRevC.29.1428
Citations: PlumX Metrics


1984HE07      Phys.Rev. C29, 1859 (1984)

K.Heyde, J.Moreau, M.Waroquier

Evidence for very Large Deformation in Neutron Deficient Nuclei with Z ≈ 40

NUCLEAR STRUCTURE 76,78,80,82,84,86,88,90,92,94,96,98,100Zr; calculated potential energy vs quadrupole deformation. 79Sr; calculated levels, static quadrupole moment, μ, δ(E2/M1), B(λ). 78,80,82,84,86Sr; calculated levels, quadrupole moments, isotopic, isomer shifts. Interacting boson model.

doi: 10.1103/PhysRevC.29.1859
Citations: PlumX Metrics


1984ME09      Phys.Lett. 140B, 159 (1984)

R.A.Meyer, K.Heyde, P.Van Isacker, M.Waroquier, J.Moreau, J.L.Wood

Interaction between Neutron Particle-Hole and Octupole Core-Coupled States in N = 83 Nuclei

NUCLEAR STRUCTURE 147Gd, 145Sm; calculated levels; deduced neutron particle-hole, octupole core coupled state interaction, intruder state role.

RADIOACTIVITY 145Eu(EC), (β+) [from mass separation]; measured Eγ, Iγ. 145Sm deduced levels, J, π, γ-multipolarity data.

doi: 10.1016/0370-2693(84)90911-0
Citations: PlumX Metrics


1984VA24      Phys.Lett. 144B, 1 (1984)

P.Van Isacker, K.Heyde, J.Jolie, M.Waroquier, J.Moreau, O.Scholten

M1 Transition Strengths in the Neutron-Proton Interacting Boson Model

NUCLEAR STRUCTURE 148,150,152,154Sm; calculated B(M1). Interacting boson model, different limits.

doi: 10.1016/0370-2693(84)90163-1
Citations: PlumX Metrics


1984VA37      Phys.Lett. 149B, 26 (1984)

P.Van Isacker, J.Jolie, K.Heyde, M.Waroquier, J.Moreau, O.Scholten

The U(5) → O(6) Transition in the U(6/12) Supersymmetry Scheme and Its Application to the Odd-A Rh Isotopes

NUCLEAR STRUCTURE 101,103,105,107,109Rh; calculated levels, one-nucleon transfer spectroscopic ratios; deduced supersymmetry selection rule validity. 103Rh; calculated B(E2); deduced supersymmetry selection rule validity. Interacting boson model, U(6/12) group.

doi: 10.1016/0370-2693(84)91544-2
Citations: PlumX Metrics


1983HE20      Phys.Lett. 132B, 15 (1983)

K.Heyde, P.Van Isacker, J.Jolie, J.Moreau, M.Waroquier

High Spin States and the Boson Cut-Off in Rotational Nuclei

NUCLEAR STRUCTURE 158Dy; calculated effective boson number vs angular momentum, B(E2) vs spin. 156Dy; calculated yrast state spin alignment, B(E2) vs spin. 160,162Dy; calculated yrast state B(E2) vs spin.

doi: 10.1016/0370-2693(83)90213-7
Citations: PlumX Metrics


1983MO15      Phys.Rev. C28, 1640 (1983)

J.Moreau, K.Heyde, M.Waroquier

Nuclear Temperature Effects in the Scission-Point Model of Nuclear Fission

NUCLEAR STRUCTURE 235U, 252Cf; calculated fission fragment yields vs mass distribution; deduced nuclear temperature effects. Scission point model, energy conservation consistency.

doi: 10.1103/PhysRevC.28.1640
Citations: PlumX Metrics


1964GR33      Helv.Phys.Acta 37, 608 (1964)

L.Grenacs, F.Gygax, R.Hess, J.Moreau

Recherche de l'Effet de Recul Nucleaire sur la Correlation Directionnelle β-γ Perturbee dans la Desintegration de l'Ho-166

NUCLEAR STRUCTURE 166Ho; measured not abstracted; deduced nuclear properties.


1954MO38      J.Phys.Radium 15, 380 (1954)

J.Moreau

Etude de la Radioactivite de 109Pd

doi: 10.1051/jphysrad:01954001505038001
Citations: PlumX Metrics


1954MO43      Arkiv Fysik 7, 391 (1954)

J.Moreau

Etude de la Radioactivite de Sb125


1954MO83      Compt.rend. 239, 800 (1954)

J.Moreau

Etude de la Radioactivite de 124Sb


1954MO88      Compt.Rend. 239, 1130 (1954)

J.Moreau

Etude de la Radioactivite de 122Sb


1954TH36      Arkiv Fysik 8, 219 (1954)

S.Thulin, J.Moreau, H.Atterling

The Decay of As71


1954TH39      Arkiv Fysik 8, 229 (1954)

S.Thulin, J.Moreau, H.Atterling

The Decay of Kr79


1952MO29      Compt.Rend. 235, 38 (1952)

J.Moreau, J.Perez y Jorba

Etude des Spectres β- de 90Y, 91Y, 142Pr, 86Rb


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