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Search: Author = S.Kuyucak

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2002KU20      Phys.Rev. C65, 064323 (2002)

S.Kuyucak, M.Honma

Mean Field Study of the Quadrupole-Octupole Degree of Freedom in the spdf Boson Model

doi: 10.1103/PhysRevC.65.064323
Citations: PlumX Metrics


2000BE07      Nucl.Phys. A669, 241 (2000)

E.Bezakova, A.E.Stuchbery, H.H.Bolotin, W.A.Seale, S.Kuyucak, P.Van Isacker

Electromagnetic Properties of Low-Excitation States in 191Ir and 193Ir and Supersymmetry Schemes

NUCLEAR REACTIONS 191,193Ir(58Ni, 58Ni'), E=155, 180 MeV; 191,193Ir(65Cu, 65Cu'), E=130 MeV; 191,193Ir(32S, 32S'), E=100 MeV; 191,193Ir(16O, 16O'), E=40 MeV; measured Eγ, Iγ(θ, H, T) in polarized Gd, Fe following Coulomb excitation, (recoil)γ-, (particle)γ-coin. 191,193Ir levels deduced g-factors, δ, T1/2. Thin-foil transient-field IMPAC technique, recoil-distance lifetime measurement.

NUCLEAR STRUCTURE 191,193Ir; calculated g-factors, B(M1), B(E2). Particle-triaxial-rotor model, supersymmetry models.

doi: 10.1016/S0375-9474(99)00565-5
Citations: PlumX Metrics


1999BA77      Phys.Rev. C60, 037302 (1999)

B.R.Barrett, S.Kuyucak, P.Navratil, P.Van Isacker

Is There a Proton-Neutron Interacting Boson Model Rule for M1 Properties ?

NUCLEAR STRUCTURE 168Er; calculated ground, vibrational bands level energies, transition matrix elements, g. Neutron-proton interacting boson model.

doi: 10.1103/PhysRevC.60.037302
Citations: PlumX Metrics


1999KU13      Phys.Rev. C59, 3146 (1999)

S.Kuyucak, M.Sugita

Tests and Applications of Self-Consistent Cranking in the Interacting Boson Model

doi: 10.1103/PhysRevC.59.3146
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1999KU29      Phys.Lett. 466B, 79 (1999)

S.Kuyucak

Shape-Phase Transitions in Mixed Parity Systems and the Onset of Octupole Deformation

doi: 10.1016/S0370-2693(99)01110-7
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1998HA10      Phys.Rev. C57, 1349 (1998)

K.Hagino, S.Kuyucak, N.Takigawa

Excitation of Nuclear Anharmonic Vibrations in Heavy-Ion Fusion Reactions

NUCLEAR REACTIONS 148Sm(16O, X), E(cm)=53-70 MeV; analyzed fusion σ, barrier distributions; deduced anharmonic phonon excitation effects.

doi: 10.1103/PhysRevC.57.1349
Citations: PlumX Metrics


1997BA81      J.Phys.(London) G23, 1159 (1997)

A.B.Balentekin, S.Kuyucak

Description of Nuclear Structure Effects in Sub-Barrier Fusion by the Interacting Boson Model

NUCLEAR REACTIONS, ICPND 148,154Sm, 186W(16O, X), E(cm)=50-80 MeV; analyzed fusion σ(E), barrier, angular momentum distributions; deduced barrier distribution, nuclear structure effects role. Interacting boson model calculations.

doi: 10.1088/0954-3899/23/10/002
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1997HA47      Phys.Rev.Lett. 79, 2943 (1997)

K.Hagino, N.Takigawa, S.Kuyucak

Role of Anharmonicities of Nuclear Vibrations in Fusion Reactions at Sub-Barrier Energies

NUCLEAR REACTIONS, ICPND 144Sm(16O, X), E(cm)=55-70 MeV; analyzed fusion σ; deduced fusion barrier, 144Sm anharmonic vibration role. sdf-interacting boson model.

doi: 10.1103/PhysRevLett.79.2943
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1997KU04      Phys.Lett. 393B, 261 (1997)

S.Kuyucak, K.-H.Kim, T.Otsuka

Shape Transitions in Proton-Neutron Systems

NUCLEAR STRUCTURE 192Os; calculated ground state band energies, E2 transitions, quadrupole moments. Proton-neutron systems.

doi: 10.1016/S0370-2693(96)01652-8
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1997TA24      J.Phys.(London) G23, 1367 (1997)

N.Takigawa, K.Hagino, S.Kuyucak

Probing Anharmonic Properties of Nuclear Surface Vibration by Heavy-Ion Fusion Reactions

NUCLEAR REACTIONS, ICPND 154Dy(16O, X), E(cm)=60-80 MeV; 144Sm(16O, X), E(cm)=55-70; calculated fusion σ, fusion barrier distribution; deduced surface vibrations effects. Interacting boson model. Comparisons with data.

doi: 10.1088/0954-3899/23/10/026
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1996BA57      Phys.Rev. C54, 1853 (1996)

A.B.Balantekin, A.J.DeWeerd, S.Kuyucak

Relations between Fusion Cross Sections and Average Angular Momenta

NUCLEAR REACTIONS 154Sm(16O, X), E=55-70 MeV; analyzed fusion; deduced fusion σ moments, angular momentum averages relation.

doi: 10.1103/PhysRevC.54.1853
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1996KU06      Phys.Rev. C53, 2194 (1996)

S.Kuyucak, M.Honma, T.Otsuka

Description of Superdeformed Nuclei in the Interacting Boson Model

NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196Pb, 148,150Gd, 152,154Dy; analyzed dynamic moment of inertia, B(λ) in some cases, superdeformed nuclei. Interacting boson model.

doi: 10.1103/PhysRevC.53.2194
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1996LI18      Nucl.Phys. A604, 305 (1996)

S.C.Li, S.Kuyucak

Description of Deformed Nuclei in the sdg Boson Model

NUCLEAR STRUCTURE 158,160,162Dy, 164,166,168Er, 168,170,172,174,176Yb, 170,172,174,176,178Hf, 228,230,232Th, 234,236,238U; calculated high-spin levels, ground-band energies, interband multipole transition matrix elements. Numerical diagonalization, analytical 1/N expansion techniques, sdg interacting boson model.

doi: 10.1016/0375-9474(96)00170-4
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1995AN15      Nucl.Phys. A593, 212 (1995)

S.S.Anderssen, A.E.Stuchbery, S.Kuyucak

Measured Magnetic Moments of 2+1 States in 190-198Pt and Interacting Boson Model Description of M1 Systematics in the Platinum Isotopes

NUCLEAR REACTIONS 190,192,194,196,198Pt(58Ni, 58Ni'), E=160 MeV; measured γ(θ, H, T) in thin polarized Gd, (particle)γ-coin, Coulomb excitation. 190,192,194,196,198Pt levels deduced g-factors. 190Pt levels deduced B(E2;0+1 → 2+1). Enriched target, thin-foil transient-field IMPAC technique.

NUCLEAR STRUCTURE 190,192,194,196,198Pt; calculated levels, B(E2), B(M1), δ, g. Proton-neutron interacting boson model (IBM-2), F-spin symmetry breaking.

doi: 10.1016/0375-9474(95)00350-A
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1995KU16      Phys.Lett. 348B, 315 (1995)

S.Kuyucak, A.E.Stuchbery

Consistent Description of Magnetic Dipole Properties in Transitional Nuclei

NUCLEAR STRUCTURE 188,190,192Os; analyzed γγ(θ) data. 186,188,190,192Os, 190,192,194,196,198Pt; calculated g-factors, M1 transition rates, proton to neutron deformation ratios. Interacting boson model.

doi: 10.1016/0370-2693(95)00152-B
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1995KU17      Phys.Lett. 349B, 253 (1995)

S.Kuyucak, S.C.Li

1/N Expansion Formalism for High-Spin States

NUCLEAR STRUCTURE 190,192,194Hg; calculated dynamic moments of inertia; deduced normal, superdeformed nuclei high-spin states analysis implications.

doi: 10.1016/0370-2693(95)00276-Q
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1995KU31      Phys.Lett. 354B, 189 (1995)

S.Kuyucak, S.C.Li

High-Spin States in Boson Models with Applications to Actinide Nuclei

NUCLEAR STRUCTURE 232Th, 234,236,238U; calculated high-spin levels, E2 transition matrix elements. Systematic study, 1/N expansion method, sd, sdg boson models.

doi: 10.1016/0370-2693(95)00685-E
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1994BA03      Phys.Rev. C49, 1079 (1994)

A.B.Balantekin, J.R.Bennett, S.Kuyucak

Systematic Study of Subbarrier Fusion in Rare-Earth Nuclei

NUCLEAR REACTIONS, ICPND 144,148,154Sm(16O, X), E(cm)=50-66 MeV; 186W(16O, X), E(cm) ≈ 62-78 MeV; 194Pt, 192Os(16O, X), E(cm)=65-80 MeV; calculated fusion σ(E); deduced barrier distribution shape changes, shape-phase transitions connection. Interacting boson model for structure effects.

doi: 10.1103/PhysRevC.49.1079
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1994BA16      Phys.Rev. C49, 1294 (1994)

A.B.Balantekin, J.R.Bennett, S.Kuyucak

Sub-Barrier Fusion in Generalized Boson Models

NUCLEAR REACTIONS, ICPND 154Sm(16O, X), E(cm)=50-70 MeV; calculated fusion σ(E), barrier distributions, average angular momentum vs E. Generalized boson models, sub-barrier fusion.

doi: 10.1103/PhysRevC.49.1294
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1994BA63      Phys.Lett. 335B, 295 (1994)

A.B.Balantekin, J.R.Bennett, S.Kuyucak

Effects of Nuclear Structure on Average Angular Momentum in Subbarrier Fusion

NUCLEAR REACTIONS, ICPND 154,152,150,148Sm(16O, X), E(cm)=50-70 MeV; 192Os, 194Pt(16O, X), E=64-80 MeV; 192Os, 194Pt(40Ca, X), E=158-182 MeV; calculated fusion σ(E); deduced structure effects on average angular momentum.

doi: 10.1016/0370-2693(94)90353-0
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1994KI01      Nucl.Phys. A567, 183 (1994)

T.Kibedi, G.D.Dracoulis, A.P.Byrne, P.M.Davidson, S.Kuyucak

Low-Spin Non-Yrast States and Collective Excitations in 174Os, 176Os, 178Os, 180Os, 182Os and 184Os

RADIOACTIVITY 174,176,178,180,182,184Ir(EC) [from 144Sm(32S, 2np), E=153 MeV; 149Sm(31P, 4n), E=148 MeV; 144Sm(37Cl, 3n), E=170 MeV; 164,166,168,170Er(19F, 5n), E=103, 108, 110 MeV]; measured Eγ, Iγ, γγ(t), γγ(θ), I(ce), (ce)γ(t). 174,176,178,180,182,184Os deduced levels, J, π, ICC, δ(E2/M1), E2 branching ratios, E0/E2 strengths between quasi-β, quasi-γ, ground-state band levels. Compton-suppressed hyperpure Ge detector array, superconducting solenoid electron spectrometer. Band-mixing model, shape coexistence, interacting boson model calculations.

doi: 10.1016/0375-9474(94)90733-1
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1994KU09      Nucl.Phys. A570, 187c (1994)

S.Kuyucak

Hexadecapole Degree of Freedom in the Interacting Boson Model

NUCLEAR STRUCTURE 188,190,192Os, 152,154Sm, 198,196,194,192Pt; compiled, reviewed model predictions, data on level spectra, B(λ), E2, E4 transition matrix elements; deduced need for g bosons. Interacting boson model, hexadecapole degree of freedom.

doi: 10.1016/0375-9474(94)90282-8
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1994LA02      Nucl.Phys. A568, 617 (1994)

G.J.Lampard, A.E.Stuchbery, H.H.Bolotin, S.Kuyucak

Magnetic Moment Measurements in 195Pt; A critical test of U(6/12) Supersymmetry

NUCLEAR REACTIONS 194,195Pt(58Ni, 58Ni'), E=250 MeV; measured γ(θ, H, T) in thin polarized Gd, (particle)γ-, γγ-coin, Coulomb excitation. 195Pt levels deduced J, π, g-factors, T1/2 limits, B(E2) ratios. Enriched targets, thin-foil transient-field IMPAC technique. DBLS.

NUCLEAR STRUCTURE 195Pt; calculated levels, g. Multi-j U(6/12) supersymmetry.

doi: 10.1016/0375-9474(94)90397-2
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1993BA38      Phys.Rev. C48, 1269 (1993)

A.B.Balantekin, J.R.Bennett, S.Kuyucak

Importance of Higher Order Coupling Effects in Sub-Barrier Fusion

NUCLEAR REACTIONS, ICPND 154Sm(16O, X), E(cm) ≈ 50-70 MeV; calculated fusion σ(E); deduced higher order coupling effects role. Green's function technique, interacting boson model.

doi: 10.1103/PhysRevC.48.1269
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1993KU05      Phys.Rev. C47, 1815 (1993)

S.Kuyucak, V.-S.Lac

Comment on ' Spectroscopy of Samarium Isotopes in the sdg Interacting Boson Model '

NUCLEAR STRUCTURE 152,154Sm; calculated levels, B(λ). Simple sd model compared to sdg interacting boson model.

doi: 10.1103/PhysRevC.47.1815
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1993KU11      Phys.Rev. C48, R13 (1993)

S.Kuyucak, A.E.Stuchbery

Critical Test of Multi-j Supersymmetries from Magnetic Moment Measurements

NUCLEAR STRUCTURE 195Pt; calculated stretched states g factor.

doi: 10.1103/PhysRevC.48.R13
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1993KU13      Phys.Rev. C48, 774 (1993)

S.Kuyucak, I.Morrison

Medium-Energy Hadron-Nucleus Scattering in the 1/N Expansion Formalism

NUCLEAR STRUCTURE A=160; calculated (p, p') σ(θ), E=800 MeV. Generalized algebraic-eikonal approach.

doi: 10.1103/PhysRevC.48.774
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1993LE01      Phys.Rev. C47, R437 (1993)

J.R.Leigh, N.Rowley, R.C.Lemmon, D.J.Hinde, J.O.Newton, J.X.Wei, J.C.Mein, C.R.Morton, S.Kuyucak, A.T.Kruppa

Reconciling Deformation Parameters from Fusion with Those from Coulomb Excitation

NUCLEAR REACTIONS 154Sm(16O, X), E(cm) ≈ 55-68 MeV; analyzed fusion data. 154Sm deduced deformation parameters consistency with Coulomb excitation fits.

doi: 10.1103/PhysRevC.47.R437
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1992BA54      Phys.Rev. C46, 2019 (1992)

A.B.Balantekin, J.R.Bennett, A.J.DeWeerd, S.Kuyucak

Subbarrier Fusion in the Interacting Boson Model

NUCLEAR REACTIONS, ICPND 154Sm(16O, X), E=50-70 MeV; calculated σ(E), average angular momentum vs E, barrier distributions. Interacting boson model, comparison with geometrical model.

doi: 10.1103/PhysRevC.46.2019
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1992LA05      Nucl.Phys. A539, 418 (1992)

V.-S.Lac, S.Kuyucak

Description of Transitional Nuclei in the sdg Boson Model

NUCLEAR STRUCTURE 192,194,196,198Pt, 192,190,188Os; calculated levels, E2 transitions reduced matrix elements, quadrupole moments. sdg boson model.

doi: 10.1016/0375-9474(92)90285-R
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1991KU02      Phys.Rev. C43, 1187 (1991)

S.Kuyucak, I.Morrison, T.Sebe

Hexadecapole Systematics in the Interacting Boson Model

NUCLEAR STRUCTURE 150Nd, 156Gd, 168Er; analyzed band structure; deduced hexadecapole degree of freedom role.

doi: 10.1103/PhysRevC.43.1187
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1991KU16      Phys.Lett. 263B, 146 (1991)

S.Kuyucak, V.-S.Lac, I.Morrison

Dynamic Shape Transitions in the Interacting Boson Model

NUCLEAR STRUCTURE 192Os; calculated intrinsic quadrupole moment. Interacting boson model, dynamical shape evolution.

doi: 10.1016/0370-2693(91)90577-D
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1991KU17      Phys.Lett. 263B, 347 (1991)

S.Kuyucak, V.-S.Lac, I.Morrison, B.R.Barrett

γ-Unstable Nuclei in the sdg Boson Model

NUCLEAR STRUCTURE 194,196,198Pt; calculated levels, E4 matrix elements. 126Xe; calculated levels. sdg boson model, O(6) limit.

doi: 10.1016/0370-2693(91)90471-2
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1988KU02      Phys.Lett. 202B, 169 (1988)

S.Kuyucak, I.Morrison

M1 Transitions in the (sdg) Boson Model

NUCLEAR STRUCTURE 154Gd; calculated reduced δ(E2/M1). Interacting (sdg) Boson model.

doi: 10.1016/0370-2693(88)90001-9
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1988KU21      Phys.Rev. C38, 2482 (1988)

S.Kuyucak, I.Morrison

β-Band Moment of Inertia Anomaly

NUCLEAR STRUCTURE 158,160,162,164Dy, 162,164,166,168,170Er, 166,168,170,172,174Yb, 170,172,174,176,178,180Hf; calculated ground, (β-), (γ)-band moment of inertia; deduced moment of inertia anomaly. Interacting boson model.

doi: 10.1103/PhysRevC.38.2482
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1988KU26      Phys.Lett. 215B, 10 (1988)

S.Kuyucak, I.Morrison, A.Faessler, A.Gelberg

g-Boson Effects in the Neutron-Proton IBM from 1/N Expansion

NUCLEAR STRUCTURE 168Er; calculated levels, transition matrix elements. Interacting boson model.

doi: 10.1016/0370-2693(88)91059-3
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1986BA64      J.Phys.(London) G12, L295 (1986)

M.E.Barclay, L.Cleemann, A.V.Ramayya, J.H.Hamilton, C.F.Maguire, W.C.Ma, R.Soundranayagam, K.Zhao, A.Balanda, J.D.Cole, R.B.Piercey, A.Faessler, S.Kuyucak

g-Factor Measurements in 68Ge and Evidence for Higher Multipole Forces

NUCLEAR STRUCTURE 68Ge; calculated levels, g, B(E2). Two-quasiparticle plus interacting boson model.

NUCLEAR REACTIONS 40Ca(32S, 4p), E=115 MeV; 12C(58Ni, 2p), E=160 MeV; measured recoil ion precession in external magnetic field. 68Ge levels deduced g, B(E2).

doi: 10.1088/0305-4616/12/12/006
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1986FA10      Nucl.Phys. A458, 381 (1986)

A.Faessler, S.Kuyucak, M.Wakai

IBA Description of Backbending in Odd-Mass Ce Isotopes

NUCLEAR STRUCTURE 129,131Ce; calculated levels, B(E2), g factors. Interacting boson-fermion model.

doi: 10.1016/0375-9474(86)90040-0
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1985FA03      Nucl.Phys. A438, 78 (1985)

A.Faessler, S.Kuyucak, A.Petrovici, L.Petersen

Rotor and IBA Description of Proton and Neutron Alignment in the Ba and Ce Isotopes

NUCLEAR STRUCTURE 126,128,130Ba, 130,132,134Ce; calculated levels, occupation probabilities, quasiparticle energies. Quasiparticle-core coupling, triaxial rotor, IBA models.

doi: 10.1016/0375-9474(85)90119-8
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1984KU08      Nucl.Phys. A420, 83 (1984)

S.Kuyucak, A.Faessler, M.Wakai

Two-and Three-Quasiparticle States in the Interacting Boson Model and a Unified Description of Even- and Odd-Mass Hg Isotopes

NUCLEAR STRUCTURE 189,190,191,192,193,194,195,196,197,198Hg; caluclated levels, B(E2), g. Interacting boson-fermion approximation, two-, three-quasiparticle states.

doi: 10.1016/0375-9474(84)90658-4
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1981IA01      Ann.Phys.(New York) 136, 19 (1981)

F.Iachello, S.Kuyucak

Interacting Boson-Fermion Model of Collective States 1. The Spin (6) Limit

NUCLEAR STRUCTURE 191,193Ir; calculated levels, B(λ), quadrupole moments, μ. Interacting boson, fermion model, spin (6) limit.

doi: 10.1016/0003-4916(81)90085-3
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