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NSR database version of May 3, 2024.

Search: Author = G.Vanden Berghe

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1988VA19      Phys.Rev. C38, 414 (1988)

J.Vanthournout, H.De Meyer, G.Vanden Berghe

Symmetry-Preserving Higher-Order Terms in the O(6) Limit of the Interacting Boson Model

NUCLEAR STRUCTURE ¹⁹⁶Pt; calculated levels, B(λ). Interacting boson model, O(6) limit.

doi: 10.1103/PhysRevC.38.414
Citations: PlumX Metrics

1985VA10      Phys.Rev. C32, 1049 (1985)

G.Vanden Berghe, H.E.De Meyer, P.Van Isacker

Symmetry-Conserving Higher-Order Interaction Terms in the Interacting Boson Model

NUCLEAR STRUCTURE ^154,156,158Gd, ^162,164,166Er; calculated levels; deduced dynamical supersymmetry conserving higher order terms. Interacting boson model.

doi: 10.1103/PhysRevC.32.1049
Citations: PlumX Metrics

1980PA21      Nucl.Phys. A350, 139 (1980)

V.Paar, G.Vanden Berghe, C.Garrett, J.R.Leigh, G.D.Dracoulis

Expermental and Theoretical Investigation of a Quasi-f_7/2 Multiplet Pattern in ¹⁴⁷Sm

NUCLEAR REACTIONS ¹⁴⁷Sm(α, α'), E=8, 10, 13 MeV; measured σ(Eα). ¹⁴⁷Sm levels deduced B(E2), configuration. Enriched target.

doi: 10.1016/0375-9474(80)90392-9
Citations: PlumX Metrics

1980VA01      Z.Phys. A294, 183 (1980)

G.Vanden Berghe, V.Paar

The ¹⁴²Ce(d, p)¹⁴³Ce Reaction and a Quasi-f₇/₂ Pattern in ¹⁴³Ce in the Cluster-Vibration Model

NUCLEAR STRUCTURE ¹⁴³Ce; calculated levels, S. Cluster-vibration model.

doi: 10.1007/BF01435054
Citations: PlumX Metrics

1977BR08      Nucl.Phys. A279, 365 (1977)

J.Bron, W.H.A.Hesselink, H.Bedet, H.Verheul, G.Vanden Berghe

High-Spin States in ¹¹⁵Sb

NUCLEAR REACTIONS ¹¹³In(α, 2nγ), E=20-30 MeV; measured Eγ, Iγ, αγ-delay, γγ-Δt coin, σ(Eγ, θ), I(ce). ¹¹⁵Sb deduced levels, J, π, T_1/2, B(λ), ICC. Enriched targets; Ge(Li), Si(Li) detectors.

doi: 10.1016/0375-9474(77)90573-5
Citations: PlumX Metrics

1977VA09      Z.Phys. A281, 355 (1977)

G.Vanden Berghe

Interplay of Valence-Shell Clusters and the Vibrational Field in ²⁰⁵Pb And ²⁰⁶Pb

NUCLEAR STRUCTURE ^205,206Pb; calculated levels, S, B(E2).

1976VA14      Nucl.Phys. A265, 479 (1976)

G.Vanden Berghe

Semimicroscopic Description for the Negative Parity States of ⁶⁷Zn

NUCLEAR STRUCTURE ⁶⁷Zn; calculated negative parity states, quadrupole moment, μ, B(λ), δ, T_1/2.

doi: 10.1016/0375-9474(76)90556-X
Citations: PlumX Metrics

1976VA27      Z.Phys. A279, 223 (1976)

G.Vanden Berghe

A Semi-Microscopic Calculation for the (2p-1f) Nuclei ⁵⁹Ni, ⁵⁶Fe and ⁵⁷Fe

NUCLEAR STRUCTURE ⁵⁹Ni, ^57,56Fe; calculated levels, B(λ), δ, S. Semi-microscopic calculation.

1975VA05      Z.Phys. A272, 245 (1975)

G.Vanden Berghe

A Theoretical Interpretation of the Nuclear Structure of the Doubly-Even N = 84 Nuclei

NUCLEAR STRUCTURE ¹⁴⁰Ba, ¹⁴²Ce, ¹⁴⁴Nd, ¹⁴⁶Sm, ¹⁴⁸Gd; calculated levels. ¹⁴⁴Nd levels calculated S.

1975VA08      Z.Phys. A274, 51 (1975)

G.Vanden Berghe

Interplay of Valence-Shell Clusters and the Vibrational Field in ⁵⁸Ni

NUCLEAR STRUCTURE ⁵⁸Ni; calculated levels, B(λ), quadrupole moment, δ, γ-branching, T_1/2.

1974DE35      Nucl.Phys. A231, 141 (1974)

E.Degrieck, G.Vanden Berghe

Structure and Electromagnetic Properties of the Doubly Even Te Isotopes

NUCLEAR STRUCTURE ^{122,124,126,128,130,132,134}Te; calculated levels, S.

doi: 10.1016/0375-9474(74)90298-X
Citations: PlumX Metrics

1974VA05      Z.Phys. 266, 139 (1974)

G.Vanden Berghe

On the Coexistence of Three-Particle Clustering and Collective Core Vibrations in ¹²⁹I

NUCLEAR STRUCTURE ¹²⁹I; calculated levels, S, μ, quadrupole moment.

1973DE54      Z.Phys. 265, 393 (1973)

E.Degrieck, G.Vanden Berghe

On the Nature of the Isomeric 6⁺ State in the Heavy Doubly-Even Te Isotopes

NUCLEAR STRUCTURE ^{128,130,132,134}Te; calculated levels, J, π, T_1/2, B(E2).

doi: 10.1007/BF01391613
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1973VA15      Z.Phys. 262, 25 (1973)

G.Vanden Berghe, E.Degrieck

The Two-Particle-One-Hole States in the Odd-A Antimony Isotopes

NUCLEAR REACTIONS ^{118,120,122,124,126,128}Te(d, ³He); calculated S. ^{117,119,121,123,125,127}Sb calculated levels, J, π. ¹²¹Sb calculated transitions, B(E2), level-width.

doi: 10.1007/BF01394805
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1972WA27      Phys.Lett. 41B, 267 (1972)

M.Waroquier, G.Van Den Berghe

The Jπ = 11/2^-(1) Isomeric State in the Odd-Proton N = 82 Nuclei

NUCLEAR STRUCTURE ^137mCs, ^139mLa, ^141mPr, ^143mPm, ¹⁴⁵Eu; calculated T_1/2, B(M2), B(E3), γ-branching. Quasiparticle Tamm-Dancoff approximation.

doi: 10.1016/0370-2693(72)90575-8
Citations: PlumX Metrics

1971HE11      Phys.Lett. 35B, 211 (1971)

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

On the Nature of the Isomeric State in the Doubly-Even N = 82 Nuclei

NUCLEAR STRUCTURE ¹³⁴Te, ¹³⁶Xe, ¹³⁸Ba, ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm isomers calculated T_1/2. Quasiparticle model.

doi: 10.1016/0370-2693(71)90176-6
Citations: PlumX Metrics

1971VA07      Nucl.Phys. A163, 478 (1971)

G.Vanden Berghe, K.Heyde

Structure and Electromagnetic Properties of the Odd-A Antimony Isotopes in a Unified-Model Calculation

NUCLEAR STRUCTURE ^{115,117,119,121,123,125}Sb; calculated levels, B(E2). Unified model.

doi: 10.1016/0375-9474(71)90504-5
Citations: PlumX Metrics

1971VA11      Nucl.Phys. A165, 662 (1971)

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

Unified Model Calculations for the N = 83 Nuclei

NUCLEAR STRUCTURE ¹³⁷Xe, ¹³⁹Ba, ¹⁴¹Ce, ¹⁴³Nd; calculated levels, μ, quadrupole moment, B(λ), S for (d, p). Unified model.

doi: 10.1016/0375-9474(71)90477-5
Citations: PlumX Metrics

1970VA06      Nucl.Phys. A144, 558 (1970)

G.Vanden Berghe, K.Heyde

Penetration Effects on Internal Conversion for l-Forbidden M1 Transitions in a Unified Model

NUCLEAR STRUCTURE ^119,121,125Sb, ^129,131I, ¹⁴³Pr, ^147,149Pm; calculated penetration factors for L-forbidden M1 transitions. Unified model.

doi: 10.1016/0375-9474(70)90345-3
Citations: PlumX Metrics

1970VA17      Phys.Lett. 32B, 173 (1970)

G.Vanden Berghe, K.Heyde

Level Schemes and Properties of the Odd-Mass Sb Isotopes

NUCLEAR STRUCTURE ^117,119,121Sb; calculated levels, B(E2), μ, quadrupole moment, S for (³He, d).

doi: 10.1016/0370-2693(70)90464-8
Citations: PlumX Metrics

1969HE03      Nucl.Phys. A126, 381(1969)

K.Heyde, G.Vanden Berghe

Unified-Model Calculations for ¹³⁹Ce

NUCLEAR STRUCTURE ¹³⁹Ce calculated levels. Unified model.

doi: 10.1016/0375-9474(69)90473-4
Citations: PlumX Metrics