NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = M.Waroquier Found 106 matches. Showing 1 to 100. [Next]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
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
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
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
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
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
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
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
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
1998VA26 Phys.Rev. C58, 3359 (1998) Single-Particle Properties in Self-Bound Systems
doi: 10.1103/PhysRevC.58.3359
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1983WA16 Nucl.Phys. A404, 269 (1983) 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
1983WA17 Nucl.Phys. A404, 298 (1983) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1975HE05 Nucl.Phys. A241, 219 (1975) 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
1975HE14 Phys.Lett. 57B, 429 (1975) 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
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
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
1974WA11 Z.Phys. 268, 11 (1974) 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
1974WA18 Phys.Rev. C10, 1548 (1974) 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
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
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
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
1972VA28 Nucl.Phys. A196, 303 (1972) 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
Back to query form [Next] |