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NSR database version of April 11, 2024.

Search: Author = M.Waroquier

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2003DE10      Phys.Rev.Lett. 90, 152501 (2003)

Y.Dewulf, W.H.Dickhoff, D.Van Neck, E.R.Stoddard, M.Waroquier

Saturation of Nuclear Matter and Short-Range Correlations

doi: 10.1103/PhysRevLett.90.152501
Citations: PlumX Metrics

2003DI12      Phys.Rev. C 68, 064307 (2003)

A.E.L.Dieperink, Y.Dewulf, D.Van Neck, M.Waroquier, V.Rodin

Nuclear symmetry energy and the neutron skin in neutron-rich nuclei

doi: 10.1103/PhysRevC.68.064307
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2003KO05      Phys.Rev. C 67, 015207 (2003)

A.Yu.Korchin, D.Van Neck, M.Waroquier

Electromagnetic interaction in chiral quantum hadrodynamics and decay of vector and axial-vector mesons

doi: 10.1103/PhysRevC.67.015207
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2002DE25      Phys.Rev. C65, 054316 (2002)

Y.Dewulf, D.Van Neck, M.Waroquier

Effects of Self-Consistency in a Green's Function Description of Saturation in Nuclear Matter

doi: 10.1103/PhysRevC.65.054316
Citations: PlumX Metrics

2002SC15      Acta Phys.Pol. B33, 847 (2002)

O.Scholten, S.Kondratyuk, L.Van Daele, D.Van Neck, M.Waroquier, A.Yu.Korchin

Compton Scattering on the Proton and Light Nuclei in the Δ-Resonance Region

NUCLEAR REACTIONS 1H, 4He, 12C(γ, γ), E ≈ 150-500 MeV; calculated Compton scattering σ(θ); deduced medium modification, Δ resonance effects. Comparison with data.

2002VA01      Phys.Rev. C65, 014613 (2002)

L.Van Daele, A.Yu.Korchin, D.Van Neck, O.Scholten, M.Waroquier

Coherent Compton Scattering on Light Nuclei in the Δ-Resonance Region

NUCLEAR REACTIONS 1H, 4He, 12C(γ, γ), E=150-500 MeV; calculated Compton scattering σ(θ); deduced role of Δ resonance, medium effects. Impulse approximation, comparisons with data.

doi: 10.1103/PhysRevC.65.014613
Citations: PlumX Metrics

2001DE33      Phys.Lett. 510B, 89 (2001)

Y.Dewulf, D.Van Neck, M.Waroquier

Short-Range Correlations in Nuclear Matter using Green's Functions within a Discrete Pole Approximation

doi: 10.1016/S0370-2693(01)00560-3
Citations: PlumX Metrics

1999KO12      Phys.Rev. C59, 1890 (1999); Comment Phys.Rev. C63, 019801 (2001)

A.Yu.Korchin, D.Van Neck, O.Scholten, M.Waroquier

Radiative Proton-Deuteron Capture in a Gauge Invariant Relativistic Model

NUCLEAR REACTIONS 2H(polarized p, γ), E=100-500 MeV; calculated σ(θ), Ay(θ), tensor analyzing powers. 3He(e, e'p), (e, e'd), E=390, 560 MeV; calculated σ(E, θ). Gauge invariant relativistic model. Comparison with data.

doi: 10.1103/PhysRevC.59.1890
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1998KO60      Phys.Lett. 441B, 17 (1998)

A.Yu.Korchin, D.Van Neck, M.Waroquier, O.Scholten, A.E.L.Dieperink

Production of e+e- Pairs in Proton-Deuteron Capture to 3He

NUCLEAR REACTIONS 2H(p, γ), (p, ee+), E=190, 350 MeV; calculated response functions, σ(θ); deduced time-like form factors influence. 3He(γ, p), E < 400 MeV; calculated σ(E, θ).

doi: 10.1016/S0370-2693(98)01197-6
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1998VA07      Phys.Rev. C57, 2308 (1998)

D.Van Neck, M.Waroquier, A.E.L.Dieperink, S.C.Pieper, V.R.Pandharipande

Center-of-Mass Effects on the Quasihole Spectroscopic Factors in the 16O(e, e'p) Reaction

NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated spectroscopic factors; deduced center-of-mass effect. Variational Monte Carlo calculation.

doi: 10.1103/PhysRevC.57.2308
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1998VA26      Phys.Rev. C58, 3359 (1998)

D.Van Neck, M.Waroquier

Single-Particle Properties in Self-Bound Systems

doi: 10.1103/PhysRevC.58.3359
Citations: PlumX Metrics

1997DE17      Phys.Lett. 396B, 7 (1997)

Y.Dewulf, D.Van Neck, L.Van Daele, M.Waroquier

Long-Range COrrelations in Finite Nuclei: Comparison of two self-consistent treatments

NUCLEAR STRUCTURE 16O; calculated s-, p-state Hartree-Fock, relativistic Hartree-Fock energies, occupation probability, spectroscopic factor, binding energy per nucleon; deduced long-range correlations related features. Green's function approach, self-consistent treatment.

doi: 10.1016/S0370-2693(97)00135-4
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1997RY01      Nucl.Phys. A624, 581 (1997)

J.Ryckebusch, V.Van der Sluys, K.Heyde, H.Holvoet, W.Van Nespen, M.Waroquier, M.Vanderhaeghen

Electroinduced Two-Nucleon Knockout and Correlations in Nuclei

NUCLEAR REACTIONS 12C(e, e'2p), (e, e'np), E=700 MeV; 16O(e, e'2p), (e, e'np), E=1.2 GeV; calculated σ(θ), pn(θ), pp(θ); 12C(e, e'pX), (γ, pX), E ≈ 200 MeV; analyzed σ(θ) vs missing energy; deduced reaction mechanisms relative importance.

doi: 10.1016/S0375-9474(97)00385-0
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1997VA07      Phys.Rev. C55, 1982 (1997)

V.Van der Sluys, K.Heyde, J.Ryckebusch, M.Waroquier

Systematic Study of Coulomb Distortion Effects in Exclusive (e, e'p) Reactions

NUCLEAR REACTIONS 16O(e, e'p), E=455.8 MeV; 40Ca(e, e'p), E=460 MeV; 90Zr(e, e'p), E=346.5, 350.7 MeV; 208Pb(e, e'p), E=412.3 MeV; analyzed reduced σ vs missing momentum. 15N, 39K, 89Y, 207Tl levels deduced spectroscopic factors. CDWBA approach, systematic study of Coulomb distortion.

doi: 10.1103/PhysRevC.55.1982
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1997VA15      Phys.Rev. C56, 1398 (1997)

D.Van Neck, L.Van Daele, Y.Dewulf, M.Waroquier

Nuclear Overlap Functions Determined by the Asymptotic Behavior of the One-Body Density Matrix

NUCLEAR STRUCTURE 16O; calculated orbital occupation numbers, spectroscopic factors, overlap functions with low-lying quasihole states, neutron density, momentum distributions; deduced central, noncentral correlations role. Correlated basis function theory, asymptotic behaviour.

doi: 10.1103/PhysRevC.56.1398
Citations: PlumX Metrics

1997VA27      Acta Phys.Hung.N.S. 6, 29 (1997)

D.Van Neck, M.Waroquier, K.Heyde

Nucleon-Nucleon Correlations and the Coulomb Displacement Energy

NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated Coulomb displacement energies; deduced pair correlations role. Nolen-Shiffer anomaly.

1996RY05      Phys.Rev. C54, 3313 (1996)

J.Ryckebusch, L.Machenil, M.Vanderhaeghen, V.Van der Sluys, M.Waroquier

Reply to ' Comment on ' Multinucleon Mechanisms in (γ, N) and (γ, NN) Reactions' '

NUCLEAR REACTIONS 12C(γ, X), E ≈ 200-400 MeV; calculated proton-neutron knockout contribution to total photon absorption σ(E); deduced shell model effects role in Δ33 propagator.

doi: 10.1103/PhysRevC.54.3313
Citations: PlumX Metrics

1996VA04      Phys.Rev. C53, 2231 (1996)

D.Van Neck, A.E.L.Dieperink, M.Waroquier

Natural Orbitals, Overlap Functions, and Mean-Field Orbitals in an Exactly Solvable A-Body System

NUCLEAR STRUCTURE A=3; A=10; A=100; calculated one-body density, natural orbitals characteristics. Nontrivial many-body system.

doi: 10.1103/PhysRevC.53.2231
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1996VA11      Z.Phys. A355, 107 (1996)

D.Van Neck, A.E.L.Dieperink, M.Waroquier

Single-Particle Properties in an Exactly Solvable A-Body System

NUCLEAR STRUCTURE A=10; calculated bound, continuum single particle overlap functions contribution to density, momentum distributions.

doi: 10.1007/s002180050085
Citations: PlumX Metrics

1996VA14      Phys.Rev. C54, 1322 (1996)

V.Van der Sluys, J.Ryckebusch, M.Waroquier

Exclusive (e, e'p) Reaction at High Missing Momenta

NUCLEAR REACTIONS 16O(e, e'p), E=500 MeV; 208Pb(e, e'p), E=487 MeV; calculated reduced σ; deduced ground state correlations role at high missing momenta. Nonrelativistic many-body framework, one-, two-body nuclear currents, electron distortion, final state interactions.

doi: 10.1103/PhysRevC.54.1322
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1995RY02      Phys.Lett. 350B, 1 (1995)

J.Ryckebusch, M.Vanderhaeghen, K.Heyde, M.Waroquier

Short-Range Correlations in (e, e'p) and (e, e'pp) Reactions on Complex Nuclei

NUCLEAR REACTIONS 12C(e, e'p), E=0.478, 2 GeV; analyzed σ(θ(e'), E(e'), θp, Ep); deduced short-range correlations role. Nonrelativistic model, mean field potential.

doi: 10.1016/0370-2693(95)00323-D
Citations: PlumX Metrics

1995VA12      Phys.Rev. C51, 2664 (1995)

V.Van der Sluys, J.Ryckebusch, M.Waroquier

Two-Body Currents in Inclusive Electron Scattering

NUCLEAR REACTIONS 12C, 40Ca(e, e'), E not given; calculated longitudinal, transverse response functions, ratio; deduced two-body currents role. Hartree-Fock plus RPA model.

doi: 10.1103/PhysRevC.51.2664
Citations: PlumX Metrics

1995VA23      Nucl.Phys. A595, 219 (1995)

M.Vanderhaeghen, K.Heyde, J.Ryckebusch, M.Waroquier

Pion Photoproduction Through the Δ Resonance Region: Relativistic versus non-relativistic unitary models

NUCLEAR REACTIONS 1n(γ, π-), E=194-400 MeV; 1H(γ, π+), E=250-400 MeV; 1H(γ, π0), E=220-380 MeV; calculated σ(θ), asymmetry, polarization in some cases. Fully relativistic, gauge invariant, unitary pion photoproduction model.

doi: 10.1016/0375-9474(95)00386-1
Citations: PlumX Metrics

1994RY02      Nucl.Phys. A568, 828 (1994)

J.Ryckebusch, M.Vanderhaeghen, L.Machenil, M.Waroquier

Effects of the Final-State Interaction in (γ, pn) and (γ, pp) Processes

NUCLEAR REACTIONS 12C(γ, np), (γ, 2p), E=80-240 keV; calculated σ(E), ratio. 16O(γ, np), E=200 MeV; calculated σ(θp, θn) vs proton momentum. Shell model, final state interactions, pionic currents, intermediate Δ creation.

doi: 10.1016/0375-9474(94)90362-X
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1994RY03      Phys.Rev. C49, 2704 (1994)

J.Ryckebusch, L.Machenil, M.Vanderhaeghen, V.Van der Sluys, M.Waroquier

Multinucleon Mechanisms in (γ, N) and (γ, NN) Reactions

NUCLEAR REACTIONS 16O(γ, n), E=150-250 MeV; calculated σ(θ). 12C(γ, n), E=75, 100 MeV; calculated σ(θn, En); 12C(γ, p), E=123, 151 MeV; calculated σ(θp, Ep). 40Ca(γ, p), E=60 MeV; calculated σ(θp, Ep) vs missing energy. 16O(γ, np), (γ, 2p), E=281 MeV; calculated σ(θp, Ep); deduced multinucleon mechanisms similarity in (γ, p), (e, e'p) processes. Microscopic model.

doi: 10.1103/PhysRevC.49.2704
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1994RY04      Phys.Lett. 333B, 310 (1994)

J.Ryckebusch, V.Van der Sluys, M.Waroquier, L.J.H.M.Kester, W.H.A.Hesselink, E.Jans, A.Zondervan

Two-Nucleon Knockout Contributions to the 12C(e, e'p) Reaction in the Dip and Δ(1232) Regions

NUCLEAR REACTIONS 12C(e, e'p), E=475 MeV; calculated missing energy spectrum; deduced (e, e'np), (e, e'2p) contributions. Unfactorized two-nucleon emission model.

doi: 10.1016/0370-2693(94)90147-3
Citations: PlumX Metrics

1994VA10      Phys.Rev. C49, 2695 (1994)

V.Van der Sluys, J.Ryckebusch, M.Waroquier

Effects of Meson-Exchange Currents on the (e(pol), e'p) Structure Functions

NUCLEAR REACTIONS 40Ca, 16O(polarized e, e'p), (e, e'p), E not given; calculated structure function. Electron distortion effects, meson exchange currents.

doi: 10.1103/PhysRevC.49.2695
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1994VA33      Nucl.Phys. A580, 551 (1994)

M.Vanderhaeghen, L.Machenil, J.Ryckebusch, M.Waroquier

On Meson-Exchange and Δ-Isobar Currents in the Two-Nucleon Photoabsorption Mechanism

NUCLEAR REACTIONS 16O(γ, np), E=60-300 MeV; calculated σ(E), σ(θp, θn) for different conditions; deduced ρ-meson degree of freedom role. Factorized, unfactorized model.

doi: 10.1016/0375-9474(94)90781-1
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1993MA35      Phys.Lett. 316B, 17 (1993)

L.Machenil, M.Vanderhaeghen, J.Ryckebusch, M.Waroquier

Absorption Mechanisms in Photon Induced Two-Body Knockout

NUCLEAR REACTIONS, ICPND 16O(γ, np), (γ, 2p), E=60-300 MeV; calculated σ(E), σ(θp, θn) vs proton momentum; deduced heavy meson exchange, intermediate Δ creation roles.

doi: 10.1016/0370-2693(93)90650-7
Citations: PlumX Metrics

1993VA01      Nucl.Phys. A551, 210 (1993)

V.Van der Sluys, D.Van Neck, M.Waroquier, J.Ryckebusch

Fragmentation of Single-Particle Strength in Spherical Open-Shell Nuclei: Application to the spectral functions in 142Nd

NUCLEAR STRUCTURE 142Nd, 141Pr, 143Pm; calculated levels, single particle strength fragmentation. Equation-of motion method.

doi: 10.1016/0375-9474(93)90479-H
Citations: PlumX Metrics

1993VA08      Nucl.Phys. A563, 1 (1993)

D.Van Neck, M.Waroquier, V.Van der Sluys, K.Heyde

Proton Hole States in 208Pb, Studied by Means of a Self-Consistent Solution of the Second-Order Dyson Equation for Single-Particle Propagators

NUCLEAR STRUCTURE 208Pb; calculated levels, width, summed single particle spectroscopic strength distributions. Green's function formalism.

NUCLEAR REACTIONS 208Pb(e, e'p), E not given; calculated spectral functions. Green's function formalism.

doi: 10.1016/0375-9474(93)90009-M
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1992RY02      Phys.Rev. C46, R829 (1992)

J.Ryckebusch, K.Heyde, L.Machenil, D.Ryckbosch, M.Vanderhaeghen, M.Waroquier

Meson Exchange Currents and High-Resolution (γ, p) Reactions

NUCLEAR REACTIONS 12C(γ, p), E=48-78 MeV; calculated σ(θ). Mean field approach, meson exchange currents.

doi: 10.1103/PhysRevC.46.R829
Citations: PlumX Metrics

1992RY04      Phys.Lett. 291B, 213 (1992)

J.Ryckebusch, L.Machenil, M.Vanderhaeghen, M.Waroquier

Do Proton-Neutron Pairs Behave Like Quasideuterons in the Photoaborption Process ( Question )

NUCLEAR REACTIONS 16O(γ, np), E=50-300 MeV; calculated σ(E); deduced factorization limitation. Pion exchange, Δ included.

doi: 10.1016/0370-2693(92)91033-6
Citations: PlumX Metrics

1992VA04      Phys.Lett. 274B, 143 (1992)

D.Van Neck, M.Waroquier, V.Van der Sluys, J.Ryckebusch

Occupation Numbers in a Shell-Model Approach

NUCLEAR STRUCTURE 16O, 40,48Ca; calculated single particle state occupation probabilities. Shell model approach.

doi: 10.1016/0370-2693(92)90513-4
Citations: PlumX Metrics

1991VA07      Nucl.Phys. A530, 347 (1991)

D.Van Neck, M.Waroquier, J.Ryckebusch

Self-Consistent Solution of the Second-Order Dyson Equation for Single-Particle Propagators, with Application to the Spectral Functions of 48Ca

NUCLEAR STRUCTURE 48Ca; analyzed spectral functions. Green function approach, self-consistent solution of Dyson equation.

doi: 10.1016/0375-9474(91)90807-I
Citations: PlumX Metrics

1990SC12      Nucl.Phys. A510, 70 (1990)

J.M.Schippers, J.M.Schreuder, S.Y.van der Werf, K.Allaart, N.Blasi, M.Waroquier

Study of 116Sn via Neutron Pickup and Proton Stripping Reactions

NUCLEAR REACTIONS 117Sn(d, t), E=50 MeV; 117Sn(3He, α), E=50 MeV; 115In(3He, d), E=50 MeV; 115In(α, t), E=65 MeV; measured σ(θ). 116Sn deduced levels, J, π, spectroscopic factors. Comparison with model calculations.

doi: 10.1016/0375-9474(90)90288-W
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1990VA13      Phys.Lett. 249B, 157 (1990)

D.Van Neck, M.Waroquier, J.Ryckebusch

Proton Spectral Functions for the Hole States in 89Y using a Self-Consistent Microscopic Formalism

NUCLEAR STRUCTURE 89Y; calculated proton hole spectral functions, low-lying level spectroscopic factors, occupation probabilities. Self-consistent microscopic formalism.

doi: 10.1016/0370-2693(90)91235-4
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1989HE02      Phys.Lett. 218B, 287 (1989)

K.Heyde, C.de Coster, J.Ryckebusch, M.Waroquier

Equivalence of the Spherical and Deformed Shell-Model Approach to Intruder States

NUCLEAR STRUCTURE 186,188,190,192,194,196,198,200,202,204,206Pb, 107,109,111,113,115,117,119,121In; calculated levels, deformation.

doi: 10.1016/0370-2693(89)91582-7
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1989RE06      Phys.Lett. 228B, 31 (1989)

K.Reiner, P.Grabmayr, G.Mauser, G.Mertens, G.J.Wagner, J.Friedrich, N.Voegler, K.T.Knopfle, J.Ryckebusch, K.Heyde, D.Van Neck, M.Waroquier

(e, e'p) Study of the Continuum of 58Ni above the Giant Resonance Region

NUCLEAR REACTIONS 58Ni(e, e'p), E=183 MeV; measured σ(θ(e'), θ(p)) vs excitation energy. 58Ni deduced continuum multipole strength distribution.

doi: 10.1016/0370-2693(89)90520-0
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1989RY01      Phys.Lett. 216B, 252 (1989)

J.Ryckebusch, K.Heyde, D.Van Neck, M.Waroquier

Quasi-Elastic 16O(e, e'p) Cross Sections in a Self-Consistent Microscopic Model

NUCLEAR REACTIONS 16O(e, e'p), E=500 MeV; calculated nucleon momentum distribution. Self-consistent microscopic model.

doi: 10.1016/0370-2693(89)91109-X
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1989RY03      Phys.Lett. 222B, 183 (1989)

J.Ryckebusch, K.Heyde, D.Van Neck, M.Waroquier

On the Separation between the Longitudinal and Transverse Strength in Quasi-Elastic (e, e'p) Reactions

NUCLEAR REACTIONS 40Ca, 12C(e, e'p), E not given; calculated transverse to longitudinal strength ratio. Continuum RPA.

doi: 10.1016/0370-2693(89)91248-3
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1989RY06      Nucl.Phys. A503, 694 (1989)

J.Ryckebusch, K.Heyde, D.Van Neck, M.Waroquier

Aspects of the Final-State Interaction and Long-Range Correlations in Quasi-Elastic (e, e'p) and (e, e'n) Reactions

NUCLEAR REACTIONS 16O(e, e'p), (e, e'n), E=481 MeV; calculated response functions. 12C(e, e'p), E=500 MeV; calculated effective momentum distributions. Self-consitent Hartree-Fock, continuum RPA models.

doi: 10.1016/0375-9474(89)90436-3
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1989RY07      Nucl.Phys. A505, 755 (1989)

J.Ryckebusch, K.Heyde, D.Van Neck, M.Waroquier, K.Reiner, P.Grabmayr, G.J.Wagner

Coincidence 58Ni(e, e'p(i)) Cross Sections at Moderate Energy and Momentum Transfer

NUCLEAR REACTIONS 58Ni(e, e'p), E=183 MeV; analyzed σ(θ(e'), θ(p), E(e')), other data; deduced reaction mechanism. Self-consistent Hartree-Fock, continuum RPA.

doi: 10.1016/0375-9474(89)90040-7
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1988HE13      Nucl.Phys. A484, 275 (1988)

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

Intruder States in Odd-Mass and Odd-Odd Nuclei

NUCLEAR STRUCTURE 190,192,194,196,198,200,202,204,206,208Pb, 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated pairing energies; 111,113,115,117,119,121In, 113,115,117,119,121,123,125,127Sb; calculated intruder state energies. N=49, 50, 51, 81, 82, 83; calculated 1particle-2 hole state energies. Shell model.

doi: 10.1016/0375-9474(88)90073-5
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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
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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
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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.

1987RY03      Phys.Lett. 194B, 453 (1987)

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

A Mean-Field Description of (γ, p(i)) Cross Sections at Medium Energies

NUCLEAR REACTIONS 40Ca(γ, p), E=40-400 MeV; 16O(γ, n), (γ, p), E=40-400 MeV; calculated σ(θ) vs E. Direct knockout model.

doi: 10.1016/0370-2693(87)90215-2
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1987VA30      Phys.Rev. C36, 1796 (1987)

S.Y.van der Werf, J.M.Schippers, N.Blasi, G.T.Emery, M.N.Harakeh, C.W.de Jager, M.Waroquier

Core Polarization and Quenching in Stretched Spin States: Case study of the 9- E(x) = 3.522 MeV State in 116Sn

NUCLEAR REACTIONS, MECPD 116Sn(polarized p, p), E=133.8 MeV; measured σ(θ), analyzing power vs θ. 116Sn(e, e'), E not given; measured form factors. 115In(α, t), E=65 MeV; measured σ(θ). 116Sn level deduced quenching characteristics.

doi: 10.1103/PhysRevC.36.1796
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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
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1986VA02      Phys.Lett. 166B, 372 (1986)

S.Y.Van Der Werf, N.Blasi, M.N.Harakeh, G.Wenes, A.D.Bacher, G.T.Emery, C.W.Glover, W.P.Jones, H.J.Karwowski, H.Nann, C.Olmer, P.Den Heijer, C.W.De Jager, H.De Vries, J.Ryckebusch, M.Waroquier

High-Spin 1p-1h Configurations in 116Sn and Their Fragmentation as seen in the Reactions 116Sn(p(pol), p'), 116Sn(e, e'), 115In(He, d) and 115In(α, t)

NUCLEAR REACTIONS 116Sn(polarized p, p'), E=133.8 MeV; measured σ(θ), σ(Ep'), A(θ). 116Sn(e, e'), E=350 MeV; measured σ(E(e)), form factors. 115In(α, t), E=65 MeV; 115In(3He, d), E=50 MeV; measured σ(Et), σ(Ed). 116Sn deduced levels, J, π, L, stretched configuration fragmentation, transition amplitudes. DWBA analysis, shell model comparison.

doi: 10.1016/0370-2693(86)91582-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2672.

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
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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
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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
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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
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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
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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
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1984MH01      Nucl.Phys. A412, 113 (1984)

A.Mheemeed, K.Schreckenbach, G.Barreau, H.R.Faust, H.G.Borner, R.Brissot, P.Hungerford, H.H.Schmidt, H.J.Scheerer, T.Von Egidy, K.Heyde, J.L.Wood, P.Van Isacker, M.Waroquier, G.Wenes, M.L.Stelts

The Level Structure of 114Cd from (n, γ) and (d, p) Studies

NUCLEAR REACTIONS 113Cd(n, γ), E=thermal, 2 keV, 24 keV; 113Cd(n, e-), E=thermal; 113Cd(d, p), E=10 MeV; measured Eγ, Iγ, I(ce), E(p), σ(E(p)). 114Cd deduced levels, J, π, ICC, γ-branching, E0 branches. Curved crystal spectrometers, Ge(Li) pair spectrometers, magnetic conversion electron spectrometer, magnetic spectrograph, enriched targets. Comparison with proton 2p-2h coupling, interacting boson model configuration mixing calculations.

doi: 10.1016/0375-9474(84)90388-9
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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
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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
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1983HE06      Nucl.Phys. A398, 235 (1983)

K.Heyde, P.Van Isacker, M.Waroquier, G.Wenes, Y.Gigase, J.Stachel

g-Boson Excitations in the Interacting Boson Model

NUCLEAR STRUCTURE 104Ru; calculated levels, B(E2), branching ratios. Interacting boson model, g bosons.

doi: 10.1016/0375-9474(83)90485-2
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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
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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
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1983PU02      Nucl.Phys. A401, 269 (1983)

N.G.Puttaswamy, W.Oelert, A.Djaloeis, C.Mayer-Boricke, P.Turek, P.W.M.Glaudemans, B.C.Metsch, K.Heyde, M.Waroquier, P.Van Isacker, G.Wenes, V.Lopac, V.Paar

Structure of the Energy Levels of 53, 55, 57Mn from the (d, 3He) Reaction on Iron Isotopes at 80 MeV

NUCLEAR REACTIONS 54,56,58Fe(d, 3He), E=80 MeV; measured σ(E(3He)), σ(θ). 53,55,57Mn deduced levels, L, S. DWBA analysis, shell model, quasiparticle-core coupling, cluster vibration model calculations.

doi: 10.1016/0375-9474(83)90530-4
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1983WA16      Nucl.Phys. A404, 269 (1983)

M.Waroquier, K.Heyde, G.Wenes

An Effective Skyrme-Type Interaction for Nuclear Structure Calculations (I). Ground-State Properties

NUCLEAR STRUCTURE 16O, 206,208Pb, 90Zr, 132Sn, 38,40,42,44,46,48,50Ca; calculated binding energy per nucleon, proton, neutron point rms radii, charge radii. 58Ni; calculated charge density, radial moments.

doi: 10.1016/0375-9474(83)90550-X
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1983WA17      Nucl.Phys. A404, 298 (1983)

M.Waroquier, G.Wenes, K.Heyde

An Effective Skyrme-Type Interaction for Nuclear Structure Calculation (II). Excited-State Properties

NUCLEAR STRUCTURE 130Sn; calculated levels, B(λ), T1/2. 16O, 208Pb; calculated levles, B(λ), GDR fragmentation. 18O, 42,50Ca, 58Ni, 134Te; calculated levels. 40,48Ca, 90Zr, 132Sn, 146Gd; calculated GDR fragmentation. Effective Skyrme type interaction.

doi: 10.1016/0375-9474(83)90551-1
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1983WA23      Phys.Rev. C28, 1791 (1983)

M.Waroquier, J.Bloch, G.Wenes, K.Heyde

Influence of 2p-2h Ground State Correlations on Charge Distributions of Doubly-Closed Shell Nuclei

NUCLEAR STRUCTURE 16O, 40,48Ca; calculated rms charge radii, charge distributions. TDA, Skyrme type interaction, ground state correlation.

doi: 10.1103/PhysRevC.28.1791
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1982HE05      Phys.Rev. C25, 3160 (1982)

K.Heyde, P.Van Isacker, M.Waroquier, G.Wenes, M.Sambataro

Description of the Low-Lying Levels in 112,114Cd

NUCLEAR STRUCTURE 112,114Cd; calculated levels, B(λ), T1/2, γ-branching. Interacting boson approximation, two-particle, two-hole excitations.

doi: 10.1103/PhysRevC.25.3160
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1982SC09      Phys.Lett. 110B, 364 (1982)

K.Schreckenbach, A.Mheemeed, G.Barreau, T.von Egidy, H.R.Faust, H.G.Borner, R.Brissot, M.L.Stelts, K.Heyde, P.van Isacker, M.Waroquier, G.Wenes

The Importance of Intruder States in 114Cd

NUCLEAR REACTIONS 113Cd(n, γ), (n, e-), E=thermal; 113Cd(n, γ), E=2, 24 keV; measured Eγ, Iγ, I(ce). 114Cd deduced levels, γ-branching ratio, J, π, T1/2, B(E0), B(E2). Two-particle, two-hole core coupling calculations.

doi: 10.1016/0370-2693(82)91273-4
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1982VA14      Nucl.Phys. A380, 383 (1982)

P.Van Isacker, K.Heyde, M.Waroquier, G.Wenes

An Extension of the Interacting Boson Model and Its Application to the Even-Even Gd Isotopes

NUCLEAR STRUCTURE 154,156,158,160Gd; calculated levels, B(λ). Extended interacting boson model.

doi: 10.1016/0375-9474(82)90566-8
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1982WE12      Phys.Rev. C26, 1692 (1982)

G.Wenes, K.Heyde, M.Waroquier, P.Van Isacker

Projected Quasiparticles Calculations in the Heavy N = 82 Isotones

NUCLEAR STRUCTURE 145Eu, 147Tb, 149Ho, 151Tm; calculated levels. 144Sm, 146Gd, 148Dy, 150Er; calculated levels, B(E2) ratios, T1/2. Quasiparticle model, number projection.

doi: 10.1103/PhysRevC.26.1692
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1981HU03      Nucl.Phys. A352, 247 (1981)

M.Huyse, K.Cornelis, G.Lhersonneau, J.Verplancke, W.B.Walters, K.Heyde, P.Van Isacker, M.Waroquier, G.Wenes, H.Vincx

The Decay of Mass-Separated 99g,99mAg

RADIOACTIVITY 99,99mAg [from 92Mo(14N, 2p5n), 90Zr(14N, 5n), E=110 MeV]; measured Eγ, Iγ, γγ-coin, β+ endpoint energies, ICC; deduced log ft. 99Ag, 99Pd deduced levels, J, π. Mass separation, Ge(Li), Ge detectors, plastic scintillators, mini-orange spectrometer.

NUCLEAR REACTIONS 92Mo(14N, 5n2p), 90Zr(14N, 5n), E=110 MeV. 99Ag, 99Pd deduced levels.

NUCLEAR STRUCTURE 99,101,103,105,107,109,111Ag; calculated energy splittings. 99Pd calculated level scheme, decoupled bands. Core-particle coupling model.

doi: 10.1016/0375-9474(81)90379-1
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1981VA12      Phys.Lett. 104B, 5 (1981)

P.Van Isacker, K.Heyde, M.Waroquier, G.Wenes

The Hexadecapole Degree of Freedom in Rotational Nuclei

NUCLEAR STRUCTURE 156Gd; calculated levels, B(E2). Interacting boson model, hexadecapole degree of freedom.

doi: 10.1016/0370-2693(81)90842-X
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1981WE02      Phys.Lett. 98B, 398 (1981)

G.Wenes, P.Van Isacker, M.Waroquier, K.Heyde, J.Van Maldeghem

Collective Bands in Doubly Even Sn Nuclei

NUCLEAR STRUCTURE 112,114,118,116Sn; calculated levels, rotational bands, B(E2). Two-particle, two-hole excitation coupling to quadrupole vibrations.

doi: 10.1016/0370-2693(81)90439-1
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1981WE06      Phys.Rev. C23, 2291 (1981)

G.Wenes, P.Van Isacker, M.Waroquier, K.Heyde, J.Van Maldeghem

Collective Bands in Doubly-Even Sn Nuclei: Energy spectra and electromagnetic decay properties

NUCLEAR STRUCTURE 112,114,116,118Sn; calculated levels, band structure, B(E2), B(E0). Two-particle, two-hole excitation coupled to spherical quadrupole vibrations.

doi: 10.1103/PhysRevC.23.2291
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1980AB10      Nucl.Phys. A349, 301 (1980)

M.C.Abreu, V.Berg, J.Oms, K.Heyde, M.Waroquier, P.Van Isacker, G.Wenes, and the ISOCELE Collaboration

Transition Probabilities between the First Excited State and the Ground State in the N=81 Nuclei 139Ce, 141Nd, 143Sm and 145Gd

RADIOACTIVITY 143Eu [from Gd(p, xn2p); mass separation]; measured I(ce), ceγ(t). 143Sm level deduced T1/2, γ-multipolarity, δ, B(M1), B(E2). Natural target, magnetic spectrometer, scintillation detector. Intermediate coupling calculations, N=81 systematics.

doi: 10.1016/0375-9474(80)90289-4
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1980HE10      Phys.Rev. C22, 1267 (1980)

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

Unified Description of Odd-Mass In Nuclei. III. Application to 119,121In

NUCLEAR STRUCTURE 119,121In; calculated levels, S, δ, T1/2, static moments, B(λ). Unified description.

doi: 10.1103/PhysRevC.22.1267
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1979BR07      Nucl.Phys. A318, 335 (1979)

J.Bron, W.H.A.Hesselink, A.van Poelgeest, J.J.A.Zalmstra, M.J.Uitzinger, H.Verheul, K.Heyde, M.Waroquier, H.Vincx, P.van Isacker

Collective Bands in Even Mass Sn Isotopes

NUCLEAR REACTIONS 110,112,114,116Cd(α, 2n), E=17-33 MeV; measured Eγ, Iγ, γγt-coin, σ(Eγ, θ), E(ce), I(ce), linear polarizations. 112,114,116,118Sn deduced levels, J, π, γ-branching, δ. Enriched targets, Ge(Li), Si(Li) detectors. Structure calculation, total potential energy surfaces, J, π=0+ bandheads calculation.

doi: 10.1016/0375-9474(79)90653-5
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1979HE03      Nucl.Phys. A318, 381 (1979)

K.Heyde, M.Waroquier, P.van Isacker, H.Vincx

Possible Evidence for Deformed 7/2- States in N = 29 Nuclei

NUCLEAR STRUCTURE 53Cr, 55Fe; calculated total potential energy surfaces for Nilsson orbital 7/2-, (303), level schemes, μ, quadrupole moment, δ, T1/2.

doi: 10.1016/0375-9474(79)90655-9
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1979LI12      Nucl.Phys. A324, 141 (1979)

J.R.Lien, G.Lovhoiden, K.Aareskjold, S.El Kazzaz, C.Ellegaard, K.Heyde, M.Waroquier, P.Van Isacker, H.Vincx, J.R.Rekstad, P.Kleinheinz

Studies of Single-Neutron Holes in the Transitional Nuclei N = 83-89: The 142Ce(d, t)141Ce and 142Ce(3He, α)141Ce Pick-up Rections

NUCLEAR REACTIONS 142Ce(d, t), E=17 MeV; 142Ce(3He, α), E=24 MeV; measured σ(Et, θ), σ(Eα, θ). 141Ce deduced levels, L, π, S. Enriched target. Unified model calculations.

doi: 10.1016/0375-9474(79)90084-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1808.

1979VA02      Phys.Rev. C19, 498 (1979)

P.Van Isacker, K.Heyde, M.Waroquier, H.Vincx

Collective and Noncollective Excitations in Odd-Even N = 83 Nuclei

NUCLEAR STRUCTURE 143Nd, 145Sm, 147Gd, 149Dy; calculated levels, J, π, B(E3). Collective vibrational core plus two quasi-proton excitations.

doi: 10.1103/PhysRevC.19.498
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1979WA07      Phys.Lett. 83B, 9 (1979)

M.Waroquier, K.Heyde, P.Van Isacker, H.Vincx

The Extended Skyrme Force Versus Realistic Interactions: Application on 42Ca

NUCLEAR STRUCTURE 42Ca; calculated energy levels. Self-consistent calculation with extended Skyrme force.

doi: 10.1016/0370-2693(79)90876-1
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1979WA08      Phys.Rev. C19, 1983 (1979)

M.Waroquier, J.Sau, K.Heyde, P.Van Isacker, H.Vincx

Extended-Skyrme-Force Calculation: Theoretical Description and Application to Ca and Sn Isotopes

NUCLEAR STRUCTURE 40,42,44,46,48Ca, 104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated ground state properties, rms radii, charge density distribution. Extended Skyrme force with momentum-dependent three-body term, spin-stability conditions.

doi: 10.1103/PhysRevC.19.1983
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1978HE08      Phys.Rev. C17, 1219 (1978)

K.Heyde, M.Waroquier, R.A.Meyer

Unified Description of Odd-Mass Indium Nuclei I. General Theory and Comparison to 113In and 115In Levels Populated in the Decay of 113Sn and 115Cd-m, g

RADIOACTIVITY 113Sn, 115m,115Cd; measured Eγ, Iγ; deduced log ft. 113,115In deduced levels. Unified model analysis, Compton suppression.

doi: 10.1103/PhysRevC.17.1219
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1978HE15      Nucl.Phys. A303, 313 (1978)

K.Heyde, M.Waroquier, P.Van Isacker, H.Vincx, S.Gales, V.Paar

Study of Isobaric Analogue Resonances in f-p Shell Nuclei: A Unified-Model Description

NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr, 54Fe, 58Ni(3He, dp); analyzed data. 49Ca, 51Ti, 53Cr, 55Fe, 59Ni deduced levels, S.

doi: 10.1016/0375-9474(78)90361-5
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1977FO03      Phys.Rev. C15, 1732 (1977)

D.B.Fossan, M.Gai, A.K.Gaigalas, D.M.Gordon, R.E.Shroy, K.Heyde, M.Waroquier, H.Vincx, P.Van Isacker

Deformed 9/2+ Proton-Hole States in Odd-A I Nuclei

NUCLEAR REACTIONS 114,116,118,120,122,124Sn(6Li, 3nγ), E=25-35 MeV; measured γγ-coin, γ(E, θ, t). 117,119,121,123,125,127I deduced levels, J, π, λ.

doi: 10.1103/PhysRevC.15.1732
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1977HE14      Phys.Rev. C16, 489 (1977)

K.Heyde, M.Waroquier, P.Van Isacker, H.Vine

Magnetic Moment of the Jπ = 6+ Isomeric Level in 134Te

NUCLEAR STRUCTURE 134Te; calculated levels, J, π, g.

doi: 10.1103/PhysRevC.16.489
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1977HE25      Nucl.Phys. A292, 237 (1977)

K.Heyde, M.Waroquier, P.Van Isacker, H.Vincx

Description of Positive Parity Bands in Odd-Mass In Isotopes

NUCLEAR STRUCTURE 107,109,111,113,115,117,119In; calculated parity band structure.

doi: 10.1016/0375-9474(77)90371-2
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1977VA17      Nucl.Phys. A292, 125 (1977)

P.Van Isacker, M.Waroquier, H.Vincx, K.Heyde

The Jπ = 9/2+ Bands in Odd-Mass Sb and I Isotopes: Evidence for Deformed States (Question)

NUCLEAR STRUCTURE 113,115,117,119Sb, 117,119,121,123,125,127I; calculated rotational band structure, B(λ).

doi: 10.1016/0375-9474(77)90362-1
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1976HE16      Phys.Lett. 64B, 135 (1976)

K.Heyde, M.Waroquier, H.Vincx, P.Van Isacker

Coexistence of Spherical and Deformed States Near Closed Shells

NUCLEAR STRUCTURE Tl, Sb, In; calculated coexistence of spherical, deformed states.

doi: 10.1016/0370-2693(76)90313-0
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1975HE05      Nucl.Phys. A241, 219 (1975)

K.Heyde, M.Waroquier, H.Vincx

Coupling between Collective and Generalized Neutron Particle-Hole Excitations: Application to 142Nd

NUCLEAR REACTIONS 142Nd(p, p'); calculated σ(Ep', θ). 142Nd levels deduced S.

doi: 10.1016/0375-9474(75)90313-9
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1975HE14      Phys.Lett. 57B, 429 (1975)

K.Heyde, M.Waroquier, H.Vincx

On the Systematics of the 1i13/2 Single-Particle Level in the N = 83 Isotones

NUCLEAR STRUCTURE 137Xe, 139Ba, 141Ce, 143Nd, 145Sm, 147Gd; analyzed systematics of N=83 isotones.

doi: 10.1016/0370-2693(75)90260-9
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1975UY01      Nucl.Phys. A241, 135 (1975)

J.Uyttenhove, K.Heyde, H.Vincx, M.Waroquier

Possible Evidence for Microsecond Shape Isomerism in Tl Isotopes

RADIOACTIVITY 201mTl [from (γ, n)], 202mTl, 204mTl [from (γ, n)]; measured T1/2, Eγ. Natural target, Ge(Li) detector.

doi: 10.1016/0375-9474(75)90368-1
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1974HE23      Nucl.Phys. A234, 216 (1974)

K.Heyde, M.Waroquier, H.Vincx, P.J.Brussaard

Generalized Neutron Particle-Hole States in an Extended Unified Model

NUCLEAR STRUCTURE 136Xe, 138Ba, 140Ce, 142Nd, 144Sm; calculated levels, S.

NUCLEAR REACTIONS 137Ba(d, p), 136Xe, 140Ce, 142Nd, 144Sm(p, p'); calculated σ. 136Xe, 138Ba, 140Ce, 142Nd, 144Sm deduced resonances, J, π.

doi: 10.1016/0375-9474(74)90387-X
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1974WA11      Z.Phys. 268, 11 (1974)

M.Waroquier, K.Heyde

Nuclear Structure of the Heavy N = 82 Isotones: 144Sm and 146Gd

NUCLEAR STRUCTURE 144Sm, 146Gd; calculated levels, B(E2). 134Te, 136Xe, 138Ba, 140Ce, 142Nd levels calculated B(E2).

doi: 10.1007/BF01670056
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1974WA18      Phys.Rev. C10, 1548 (1974)

M.Waroquier, K.Heyde

Comments on the Effective M2 and E3 Transition Probabilities for the 1h11/2 Single-Quasiproton States

NUCLEAR STRUCTURE 141Pr; calculated B(M2), B(E3).

doi: 10.1103/PhysRevC.10.1548
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1973HE03      Phys.Lett. 43B, 1 (1973)

K.Heyde, M.Waroquier, G.Vanden Berghe, P.J.Brussaard

Generalized Neutron Particle-Hole States in an Extended Unified-Model Description

NUCLEAR STRUCTURE 140Ce; calculated levels, population through IAR. Extended unified model.

doi: 10.1016/0370-2693(73)90527-3
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1973VA10      Z.Phys. 259, 37 (1973)

G.Vanden Berghe, K.Heyde, M.Waroquier

Core Polarization Corrections to Magnetic Dipole Moments and Transitions

NUCLEAR STRUCTURE 87Rb, 87Sr, 89Y, 91Zr, 113In, 115Sn, 123Sb, 139,141Ce; calculated μ, B(M1).

doi: 10.1007/BF01394477
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1972VA11      Phys.Lett. 38B, 467 (1972)

G.Vanden Berghe, K.Heyde, M.Waroquier

Isobaric Analog Resonance Properties in a Unified Model Calculation

NUCLEAR REACTIONS 140Ce(p, p'), E not given; analyzed IAR data. 141Pr calculated isobaric analog resonance level-width. 141Ce deduced wave functions.

doi: 10.1016/0370-2693(72)90518-7
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1972VA28      Nucl.Phys. A196, 303 (1972)

G.Vanden Berghe, M.Waroquier

On the Coexistence of Quadrupole and Octupole Vibrations in 145Sm

NUCLEAR STRUCTURE 145Sm; calculated levels, γ-branching, S. Particle-core coupling model.

doi: 10.1016/0375-9474(72)90966-9
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