NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = Z.C.Gao Found 44 matches. 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
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
2023LU03 Phys.Rev. C 107, 054313 (2023) 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
2022GA02 Phys.Lett. B 824, 136795 (2022) 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
2022LI56 Phys.Rev. C 106, 044308 (2022) 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
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
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
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
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
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
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
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
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
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
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
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
2015GA42 Phys.Rev. C 92, 064310 (2015) 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
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
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
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
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
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
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
2010CH35 Nucl.Phys. A834, 378c (2010) 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
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
2009CH70 Chin.Phys.C 33, Supplement 1, 1 (2009) 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
2009GA03 Phys.Rev. C 79, 014311 (2009) 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
2009GA29 Phys.Rev. C 80, 034325 (2009) 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
2008CH15 Phys.Rev. C 77, 061305 (2008) 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
2008CH35 Int.J.Mod.Phys. E17, Supplement 1, 146 (2008) 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
2006GA11 Phys.Lett. B 634, 195 (2006) 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
2006GA36 Phys.Rev. C 74, 054303 (2006) 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
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
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
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
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
2004GA23 Chin.Phys.Lett. 21, 806 (2004) 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
2002GA18 Chin.Phys.Lett. 19, 650 (2002) Band Structures of the Axial and Triaxial Deformed Nuclei in the Reflection Asymmetric Shell Model
doi: 10.1088/0256-307X/19/5/313
2001CH02 Phys.Rev. C63, 014314 (2001) 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
2001GA32 Chin.Phys.Lett. 18, 352 (2001) 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
2001GA48 Chin.Phys.Lett. 18, 1186 (2001) Garvey-Kelson Mass Relations and n-p Interaction
doi: 10.1088/0256-307X/18/9/310
2001GA66 Chin.Phys.Lett. 18, 1564 (2001) 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
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
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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