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NSR database version of April 24, 2024.

Search: Author = Z.C.Gao

Found 44 matches.

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2024GA07      Phys.Rev. C 109, 024307 (2024)

T.J.Gao, J.-B.Lu, Y.Ma, Y.Zhang, S.Q.Zhang, H.D.Wang, J.-Q.Liu, P.-Y.Yang, Zh.Ren, Ch.-Q.Li, Q.B.Chen, Z.C.Gao, J.Li, K.Y.Ma, G.Dong

Evidence for possible multiple chiral doublet bands with identical configuration in the odd-odd nucleus 126Cs

doi: 10.1103/PhysRevC.109.024307
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2023LI33      Chin.Phys.C 47, 074102 (2023)

Z.-J.Lian, X.Lu, X.-W.Li, Z.-C.Gao, Y.-S.Chen

Weighted variation after projection method for low-lying nonyrast states

NUCLEAR STRUCTURE 48Cr, 27Al; calculated level energies; deduced a simple algorithm to further improve the previous variation after projection (VAP) wave functions for low-lying nonyrast states. Comparison with available data.

doi: 10.1088/1674-1137/acccda
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2023LU03      Phys.Rev. C 107, 054313 (2023)

X.Lu, Z.-J.Lian, Z.-C.Gao

Mixing of one-particle-one-hole projected states with the variation after projection wave functions

NUCLEAR STRUCTURE 26Mg, 48,49Cr, 56Ni; calculated state energies including high-spin ones. Mixing of one-particle-one-hole projected states with the variation after projection (VAP) wave functions. Comparison to shell-model calculations.

doi: 10.1103/PhysRevC.107.054313
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2022GA02      Phys.Lett. B 824, 136795 (2022)

Z.-C.Gao

Variation after projection calculations for high-spin states

NUCLEAR STRUCTURE 24Mg, 48Cr; analyzed available data; calculated level energies, B(E2), high-spin states. The variation after projection (VAP) method.

doi: 10.1016/j.physletb.2021.136795
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2022LI56      Phys.Rev. C 106, 044308 (2022)

Z.-J.Lian, X.Lu, Z.-C.Gao

Energy-variance extrapolation for high-spin states with fully optimized variation after projection wave functions

NUCLEAR STRUCTURE 48,49Cr, 58Ni; calculated state energies including high-spin states. Energy-variance extrapolation method with fully optimized VAP (variation after projection) wave functions. Comparison to shell-model calculations.

doi: 10.1103/PhysRevC.106.044308
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2022LV06      Phys.Rev. C 105, 054308 (2022)

C.-J.Lv, Y.Sun, Y.Fujita, H.Fujita, L.-J.Wang, Z.-C.Gao

Effect of nuclear deformation on the observation of a low-energy super-Gamow-Teller state

NUCLEAR REACTIONS 42Ca(3He, t), E=140 MeV/nucleon; calculated Gamow-Teller strength distribution. Reproduced experimentally observed so-called low-energy super-GT (LeSGT) state population. Projected shell model (PSM) calculations.

NUCLEAR STRUCTURE 82Nb; calculated Gamow-Teller strength in charge exchange reactions populating excited states in 82Nb from ground state of 82Zr. Results point on absence of low-energy super-GT (LeSGT) state in 82Nb.

doi: 10.1103/PhysRevC.105.054308
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2022SO20      Astrophys.J. 941, 56 (2022)

N.Song, S.Zhang, Z.H.Li, G.X.Li, Z.C.Gao, H.K.Wang

Influence of Neutrino-Nuclear Reactions on the Abundance of 74Se

NUCLEAR REACTIONS 74Ge(ν, e-), E<60 MeV; calculated σ using experimental and theoretical B(GT).

doi: 10.3847/1538-4357/aca328
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2021YA18      Phys.Rev. C 104, 014306 (2021)

T.Ya, Y.-J.Chen, Y.-S.Chen, Z.-C.Gao, L.Liu

Axial shape asymmetry and high-spin states in nuclei with Z=100 suggested by the projected total energy surface approach

NUCLEAR STRUCTURE 246,248,250,252,254,256Fm; calculated levels, J, π, yrast bands, moment of inertia of yrast bands as function of rotational frequency, β2 and γ deformation parameters, local triaxial minima, energy surfaces, axial asymmetry shapes; deduced backbending phenomenon at about spin 18+ due to the alignment excitation of two quasi-neutrons of the high-j shell. Projected total-energy surface (PTES), total Routhian surface (TRS), and variation after projection (VAP) calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.104.014306
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2019WA07      Phys.Lett. B 790, 498 (2019)

X.B.Wang, G.X.Dong, Z.C.Gao, Y.S.Chen, C.W.Shen

Tetrahedral symmetry in the ground state of 16O

NUCLEAR STRUCTURE 16O; calculated mean-field energies, octupole and quadrupole moments, potential energy surfaces, ground state band using Skyrme functional HF.

doi: 10.1016/j.physletb.2019.02.001
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2018WA21      Phys.Rev. C 98, 021301 (2018)

J.-Q.Wang, Z.-C.Gao, Y.-J.Ma, Y.S.Chen

New algorithm in the variation after projection calculations for non-yrast nuclear states

NUCLEAR STRUCTURE 20,22,24,26,28Ne, 24,26,28,30Mg, 28,30,32Si, 32,34S, 36Ar; calculated energies of ten lowest 0+ levels. 24,25,26Mg, 26Al; calculated energies of levels up to 14+. Variation after projection (VAP) approach, and shell model with USDB interaction; deduced differences between the two calculations.

doi: 10.1103/PhysRevC.98.021301
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2017YA17      Phys.Rev. C 95, 064307 (2017)

T.Ya, Y.He, Z.-C.Gao, J.-Q.Wang, Y.S.Chen

Implementation of the variation-after-projection approach in calculations with a time-odd Hartree-Fock mean field

NUCLEAR STRUCTURE 24,25,26Mg, 26Al; calculated variation-after-projection (VAP) energies, B(E2), J-scheme shell model dimension; deduced energy differences between the shell model energies and the present VAP energies. 20,22,24,26,28Ne, 24,26,28,30Mg, 28,30,32Si, 32,34S, 36Ar; calculated VAP energies, and compared with previous VAP calculations and shell-model energies for the ground states of even-even nuclei. Time-odd Hartree-Fock (HF) mean field with Slater determinants.

doi: 10.1103/PhysRevC.95.064307
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2017YA18      Phys.Rev. C 95, 064316 (2017)

T.Ya, Y.-S.Chen, Z.-C.Gao, L.Liu, Y.-J.Chen

Beyond-mean-field effects on nuclear triaxiality

NUCLEAR STRUCTURE 170,172,174,176,178W; calculated level energies, transition quadrupole moments, and projected total energy surfaces (PTES) in (ϵ2, γ) plane for positive-parity yrast bands up to 20+, level energies of γ bands. Investigated beyond-mean-field effects on nuclear triaxiality by projected total energy surface, based on the triaxial projected shell model and hybridized macroscopic-microscopic method. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.064316
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2016CH13      Phys.Rev. C 93, 044310 (2016)

Q.M.Chen, X.G.Wu, Y.S.Chen, C.B.Li, Z.C.Gao, G.S.Li, F.Q.Chen, C.Y.He, Y.Zheng, S.P.Hu, J.Zhong, Y.H.Wu, H.W.Li, P.W.Luo

Lifetime measurements in 180Pt

NUCLEAR REACTIONS 156Gd(28Si, 4n), E=144 MeV; measured Eγ, Iγ, γγ-coin, level half-lives by recoil-distance Doppler shift method using a plunger and differential decay curve analysis at HI-13 tandem accelerator of CIAE-Beijing. 180Pt; deduced levels, J, π, B(E2), transition quadrupole moments for levels in the yrast band. Systematics of B(E2), E(4+)/E(2+) ratios, yrast and γ bands in 176,178,180,182,184,186Pt. Comparison with triaxial projected shell model (TPSM) calculations.

doi: 10.1103/PhysRevC.93.044310
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2016SU10      Phys.Lett. B 756, 323 (2016)

J.Su, W.P.Liu, N.T.Zhang, Y.P.Shen, Y.H.Lam, N.A.Smirnova, M.MacCormick, J.S.Wang, L.Jing, Z.H.Li, Y.B.Wang, B.Guo, S.Q.Yan, Y.J.Li, S.Zeng, G.Lian, X.C.Du, L.Gan, X.X.Bai, Z.C.Gao, Y.H.Zhang, X.H.Zhou, X.D.Tang, J.J.He, Y.Y.Yang, S.L.Jin, P.Ma, J.B.Ma, M.R.Huang, Z.Bai, Y.J.Zhou, W.H.Ma, J.Hu, S.W.Xu, S.B.Ma, S.Z.Chen, L.Y.Zhang, B.Ding, Z.H.Li, G.Audi

Revalidation of the isobaric multiplet mass equation at A = 53, T = 3/2

RADIOACTIVITY 53Ni(EC), (ECp) [from Be(58Ni, X)53Ni, E=68.3 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced T1/2, level scheme, J, π, isobaric analog state, mass excess, explanation of unexpected deviation from the isobaric multiplet mass equation (IMME) at A=53, T=3/2.

doi: 10.1016/j.physletb.2016.03.024
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2015CH04      Phys.Rev. C 91, 014317 (2015)

Y.-J.Chen, Z.-C.Gao, Y.-S.Chen, Y.Tu

Octupole bands and simplex inversion in the neutron-rich nucleus 145Ba

NUCLEAR STRUCTURE 145Ba; calculated levels, J, π, rotational bands, single-proton and single-neutron levels as a function of quadrupole and octupole deformation, configuration mixing, simplex inversion; evidence for reflection asymmetric shape in the ground state and low-lying states. Reflection asymmetric shell model. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.014317
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2015CH59      Int.J.Mod.Phys. E24, 1550081 (2015)

Y.-J.Chen, Y.-S.Chen, Z.-C.Gao, Y.Tu

The octupole deformation of 143Ba

NUCLEAR STRUCTURE 143Ba; calculated energy levels, J. π, rotational bands, B(E1)/B(E2) values. The reflection asymmetric shell model (RASM), comparison with available data.

doi: 10.1142/S0218301315500810
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2015GA42      Phys.Rev. C 92, 064310 (2015)

Z.-C.Gao, M.Horoi, Y.S.Chen

Variation after projection with a triaxially deformed nuclear mean field

NUCLEAR STRUCTURE 20,22,24,26,28Ne, 24,26,28,30Mg, 28,30,32Si, 32,34S, 36Ar; calculated converged energies and associated shape parameters for even-even sd-shell nuclei with the USDB Hamiltonian. Variation after projection (VAP) calculations on spin, isospin, and mass number of a triaxially deformed Hartree-Fock-Bogoliubov vacuum state.

doi: 10.1103/PhysRevC.92.064310
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2014CU01      Phys.Rev. C 90, 014321 (2014)

J.-W.Cui, X.-R.Zhou, F.-Q.Chen, Y.Sun, C.-L.Wu, Z.-C.Gao

Description of collective and quasiparticle excitations in deformed actinide nuclei: The first application of the multishell shell model for heavy nuclei

NUCLEAR STRUCTURE 230,232Th, 232,234,236U, 240Pu; calculated levels, J, π, ground-, β-, γ-, and K=0 to K=7 bands, 2-quasiparticle configurations, B(E2), staggering parameter. Heavy shell model (HSM), an extension of projected shell model (PSM). Comparison with experimental data.

doi: 10.1103/PhysRevC.90.014321
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2014LI45      Phys.Rev. C 90, 047302 (2014)

C.B.Li, F.Q.Chen, X.G.Wu, C.Y.He, Y.Zheng, G.S.Li, Q.M.Chen, Z.C.Gao, Q.L.Xia, W.P.Zhou, S.P.Hu, H.W.Li, J.L.Wang, J.J.Liu, Y.H.Wu, P.W.Luo

Lifetime measurement of the first 2+ state in 178Pt

NUCLEAR REACTIONS 154Gd(28Si, 4n), E=146 MeV; measured Eγ, γγ-coin, γγγ(t), half-life of the first 2+ state by fast-timing technique using Ge-LaBr3-LaBr3 detectors. 178Pt; deduced levels, B(E2). Potential energy surface (PES) calculations. Systematics of B(E2) for first 2+ states in 176,178,180,182,184Pt isotopes and comparison with calculations using generator coordinate method.

doi: 10.1103/PhysRevC.90.047302
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2012ZH30      Phys.Rev. C 86, 014320 (2012)

Y.Zheng, L.H.Zhu, X.G.Wu, Z.C.Gao, C.Y.He, G.S.Li, L.L.Wang, Y.S.Chen, Y.Sun, X.Hao, Y.Liu, X.Q.Li, B.Pan, Y.J.Ma, Z.Y.Li, H.B.Ding

Abnormal signature inversion and multiple alignments in doubly odd 126I

NUCLEAR REACTIONS 124Sn(7Li, 5n)126I, E=48 MeV; measured Eγ, Iγ, γγ-coin, DCO ratios. 126I; deduced levels, J, π, multipolarity, rotational bands, alignments, configurations, signature inversion, Routhians. Comparison with triaxial projected shell-model (TPSM) and cranked-shell-model (CSM) calculations. Evidence for 4-quasiparticle chiral structures.

doi: 10.1103/PhysRevC.86.014320
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2011GA22      Phys.Rev. C 83, 057303 (2011)

Z.-C.Gao, M.Horoi, Y.S.Chen, Y.J.Chen, Tuya

Can one identify the intrinsic structure of the yrast states in 48Cr after the backbending?

NUCLEAR STRUCTURE 48Cr; calculated levels, J, π, B(E2), configurations for yrast states using projected configuration interaction (PCI) method. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.057303
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2011LI25      Phys.Rev. C 83, 064310 (2011)

S.H.Liu, J.H.Hamilton, A.V.Ramayya, Y.S.Chen, Z.C.Gao, S.J.Zhu, L.Gu, E.Y.Yeoh, N.T.Brewer, J.K.Hwang, Y.X.Luo, J.O.Rasmussen, W.C.Ma, J.C.Batchelder, A.V.Daniel, G.M.Ter-Akopian, Yu.Ts.Oganessian, A.Gelberg

Signature inversion in odd-odd 114Rh: First identification of high-spin states in very neutron-rich 114Rh and application of the triaxial projected shell model

RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin, fission yields ratios using the Gammasphere array. 114Rh; deduced levels, J, π, rotational bands, signature inversion, configurations. Comparison with Triaxial Projected Shell Model calculations. Systematics of negative-parity yrast bands of odd-odd Rh nuclei with A=104-114.

doi: 10.1103/PhysRevC.83.064310
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2011WA22      Chin.Phys.C 35, 753 (2011)

H.-K.Wang, Z.-C.Gao, Y.-S.Chen, J.-Y.Guo, Y.-J.Chen, Y.Tu

The structure of the spherical tensor forces in the USD and GXPF1A shell model Hamiltonians

doi: 10.1088/1674-1137/35/8/010
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2010CH35      Nucl.Phys. A834, 378c (2010)

Y.S.Chen, Z.-C.Gao

Tetrahedral instability in superheavy nuclei

NUCLEAR STRUCTURE 228,230Th, 248,250Cf; calculated octupole bands, levels, J, π. 268Sg; calculated rotational bands, levels, J, π; deduced deformation parameters. Reflection asymmetric shell model. Comparison with data.

doi: 10.1016/j.nuclphysa.2010.01.044
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2010YA23      Nucl.Phys. A848, 260 (2010)

T.Ya, Y.S.Chen, S.Y.Yu, C.W.Shen, Z.C.Gao, Y.J.Chen, L.Liu

Triaxial superdeformed bands in odd-odd 160∼168Lu isotopes

NUCLEAR STRUCTURE 160,162,164,166,168Lu; calculated triaxial superdeformed band deformation, configurations, related properties with total routhian surface model. Comparison with odd-even systematics and data.

doi: 10.1016/j.nuclphysa.2010.09.004
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2009CH70      Chin.Phys.C 33, Supplement 1, 1 (2009)

Y.-S.Chen, Z.C.Gao

Triaxial rotation in atomic nuclei

NUCLEAR STRUCTURE 118,124Cs, 157Ho; calculated signature inversion, projection of the total angular momentum on the intrinsic principal axis; deduced signature inversion impact on rotation of triaxial nucleus. Comparison with experimental data.

doi: 10.1088/1674-1137/33/S1/001
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2009GA03      Phys.Rev. C 79, 014311 (2009)

Z.-C.Gao, M.Horoi

Angular momentum projected configuration interaction with realistic Hamiltonians

NUCLEAR STRUCTURE 28Si; calculated ground-state energies. 20Ne, 24Mg, 28Si, 36Ar; calculated deformation HF energies. 24Mg, 28Si, 48Cr, 56Ni; calculated quadrupole moments, B(E2). 24Mg, 28Si, 48Cr; calculated levels, J, π. 52Fe, 56Ni; calculated yrast band energies using full configuration interaction method.in sd-pf shell space.

doi: 10.1103/PhysRevC.79.014311
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2009GA29      Phys.Rev. C 80, 034325 (2009)

Z.-C.Gao, M.Horoi, Y.S.Chen

Improved basis selection for the projected configuration interaction method applied to medium-heavy nuclei

NUCLEAR STRUCTURE 56Ni, 68,70,76Se, 76Ge; calculated level energies using Projection Configuration Interaction (PCI) and full configuration interaction (CI) approaches. 76Ge, 76Se; calculated low-lying 0+ states.

doi: 10.1103/PhysRevC.80.034325
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2008CH15      Phys.Rev. C 77, 061305 (2008)

Y.-S.Chen, Y.Sun, Z.-C.Gao

Nonaxial-octupole effect in superheavy nuclei

NUCLEAR STRUCTURE 220,222,224,226,228,230Ra, 224,226,228,230,232Th, 230,232,234,236,238U, 236,238,240,242Pu, 246,248Cm, 248,250,252Cf, 250Fm, 252No; calculated band head energies, comparison with experimental data. 246Cm, 248Cf, 250Fm, 252No; calculated levels, J, π, B(E3). Reflection Asymmetric Shell Model.

doi: 10.1103/PhysRevC.77.061305
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2008CH35      Int.J.Mod.Phys. E17, Supplement 1, 146 (2008)

Y.S.Chen, Z.C.Gao

Triaxial reflection asymmetric shell model

NUCLEAR STRUCTURE 248,250,252Cf, 226,228Ra; calculated negative parity bands, level energies, J, π; deduced octupole spectra. Reflection Asymmetric Shell Model calculations.

doi: 10.1142/S0218301308011823
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2006GA11      Phys.Lett. B 634, 195 (2006)

Z.-C.Gao, Y.S.Chen, Y.Sun

Signature inversion -- manifestation of drift of the rotational axis in triaxial nuclei

NUCLEAR STRUCTURE 118,120,122,124,126,128,130Cs; calculated rotational band energies vs spin. 124Cs; calculated B(M1)/B(E2) vs spin. Reflection asymmetric shell model, comparison with data.

doi: 10.1016/j.physletb.2006.01.033
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2006GA36      Phys.Rev. C 74, 054303 (2006)

Z.-C.Gao, Y.Sun, Y.-S.Chen

Shell model method for Gamow-Teller transitions in heavy, deformed nuclei

NUCLEAR STRUCTURE 156Ho, 164Dy; calculated rotational bands level energies, B(E2), B(GT). Projected shell model framework.

RADIOACTIVITY 164Ho(EC), (β-); calculated log ft, Gamow-Teller transition rates. Projected shell model framework.

doi: 10.1103/PhysRevC.74.054303
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2005CH34      Eur.Phys.J. A 24, 185 (2005)

Y.J.Chen, Y.S.Chen, C.W.Shen, Z.C.Gao, S.J.Zhu, Y.Tu

Theoretical simulation for identical bands

NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196,198Pb, 198Po, 166,168,170,172,174,176Yb, 166,168,170,172,174,176,178Hf; calculated normal-deformed and superdeformed rotational band energies, spins; deduced identical bands frequency, related features. Reflection asymmetric shell model.

doi: 10.1140/epja/i2005-10007-5
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2005CH37      Chin.Phys.Lett. 22, 1362 (2005)

Y.-J.Chen, Y.-S.Chen, S.-J.Zhu, Z.-C.Gao, Y.Tu

Reflection-Asymmetric Shell Model Description of the Neutron-Rich 142, 145Ba Nuclei

NUCLEAR STRUCTURE 142,145Ba; calculated octupole-deformed rotational bands levels, J, π, configurations. Reflection-asymmetric shell model, comparison with data.

doi: 10.1088/0256-307X/22/6/018
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2005YU04      Chin.Phys.Lett. 22, 1628 (2005)

D.-Q.Yuan, Y.-N.Zheng, D.-M.Zhou, Y.Zuo, E.-P.Du, X.Duan, C.-H.Wang, Q.Luo, X.-G.Wu, G.-S.Li, S.-X.Wen, G.-J.Xu, Z.-C.Gao, Y.-S.Chen, S.-Y.Zhu

Measurements of g-Factor of Rotational Levels in 83Y

NUCLEAR REACTIONS 58Ni(28Si, 3p), E=98 MeV; measured Eγ, Iγ(θ, H, t), γγ-coin. 83Y deduced g-factors for rotational band levels. Transient field technique, comparison with cranking model predictions.

doi: 10.1088/0256-307X/22/7/019
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2004CH20      Chin.Phys.Lett. 21, 802 (2004)

Y.-J.Chen, Y.-S.Chen, Z.-C.Gao

Theoretical Simulation for Identical Bands

NUCLEAR STRUCTURE A=142-198; calculated normal-deformed and superdeformed rotational band energies; deduced frequency of occurrence of identical bands.

doi: 10.1088/0256-307X/21/5/011
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2004GA23      Chin.Phys.Lett. 21, 806 (2004)

Z.-C.Gao, Y.-S.Chen, J.Meng

Rotational Band Structures of Non-Axial Octupole Deformed Shapes

NUCLEAR STRUCTURE 148Sm; analyzed rotational band level energies; deduced possible non-axial deformations.

doi: 10.1088/0256-307X/21/5/012
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2002GA18      Chin.Phys.Lett. 19, 650 (2002)

Z.-C.Gao, Y.-S.Chen, J.Meng

Band Structures of the Axial and Triaxial Deformed Nuclei in the Reflection Asymmetric Shell Model

doi: 10.1088/0256-307X/19/5/313
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2001CH02      Phys.Rev. C63, 014314 (2001)

Y.S.Chen, Z.C.Gao

Reflection Asymmetric Shell Model for Octupole-Deformed Nuclei

NUCLEAR STRUCTURE 222,224,226,228,230Ra; calculated rotational bands energy vs spin. Reflection-asymmetric shell model, octupole-deformed nuclei. Comparison with data.

doi: 10.1103/PhysRevC.63.014314
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2001GA32      Chin.Phys.Lett. 18, 352 (2001)

Z.-C.Gao, Y.-S.Chen

Reflection Asymmetric Shell Model for the Description of Octupole Rotational Bands

NUCLEAR STRUCTURE 224Ra; calculated yrast rotational band energy vs spin; deduced octupole deformation features. Reflection asymmetric shell model, comparison with data.

doi: 10.1088/0256-307X/18/3/314
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2001GA48      Chin.Phys.Lett. 18, 1186 (2001)

Z.-C.Gao, Y.-S.Chen, J.Meng

Garvey-Kelson Mass Relations and n-p Interaction

doi: 10.1088/0256-307X/18/9/310
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2001GA66      Chin.Phys.Lett. 18, 1564 (2001)

Z.-C.Gao, Y.-S.Chen, J.Meng

Reflection Asymmetric Shell Model on the Projected Woods-Saxon + BCS Basis

NUCLEAR STRUCTURE 228Th; calculated octupole rotational band energies. Reflection asymmetric shell model, comparison with data.

doi: 10.1088/0256-307X/18/12/307
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2001ZH44      Hyperfine Interactions 136/137, 205 (2001)

S.Y.Zhu, Q.Luo, Y.G.Wang, Z.G.Fan, Y.J.Xu, R.Wang, J.Z.Zhu, G.S.Li, X.A.Liu, X.G.Wu, S.X.Wen, G.J.Xu, Z.C.Gao, X.Z.Zhang, Y.S.Chen, K.Matsuta, M.Fukuda, M.Mihara, T.Minamisono

g-Factor Measurements of Rotational States in 84, 86Zr

NUCLEAR REACTIONS 58Ni(28Si, 2p), E=98 MeV; 58Ni(32S, 4p), E=110 MeV; measured Eγ, Iγ(θ, H, t). 84,86Zr deduced g factors for rotational band states. Transient-field technique.

doi: 10.1023/A:1020532332334
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2000ZH28      Chin.Phys.Lett. 17, 560 (2000)

S.-Y.Zhu, Q.Luo, G.-S.Li, Z.-G.Fan, Y.-J.Xu, Z.-C.Gao, S.-X.Wen, X.-G.Wu, X.-A.Liu, G.-J.Xu, J.-Z.Zhu, Y.-S.Chen, K.Matsuta, M.Fukuda, M.Mihara, T.Minamisono

Rotational State g-Factors in 84Zr

NUCLEAR REACTIONS 58Ni(28Si, 2p), E=98 MeV; measured Eγ, Iγ(θ, H, t) in polarized Fe. 84Zr deduced rotational band levels g-factors, configurations. Transient field technique.


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