NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = X.R.Zhou Found 55 matches. 2024XU03 Phys.Rev. C 109, 024324 (2024) H.-T.Xue, Q.B.Chen, J.-W.Cui, C.-F.Chen, H.-J.Schulze, X.-R.Zhou Structure of low-lying states of 12C and 13ΛC in a beyond-mean-field approach
doi: 10.1103/PhysRevC.109.024324
2023DA18 Phys.Rev. C 108, 054306 (2023) First exploration of wobbling modes in an isotone chain: The N=59 case
doi: 10.1103/PhysRevC.108.054306
2023LI59 Phys.Rev. C 108, 064312 (2023) Y.-X.Liu, C.F.Chen, Q.B.Chen, H.-T.Xue, H.-J.Schulze, X.-R.Zhou Deformed charmed hypernuclei
doi: 10.1103/PhysRevC.108.064312
2023PA19 Chin.Phys.C 47, 064102 (2023) Y.-F.Pan, Y.-Y.Cheng, Y.Lu, H.Jiang, X.-R.Zhou, Y.-M.Zhao Robustness of pair structures for nuclear yrast states NUCLEAR STRUCTURE 28Si, 50Cr, 132Xe; calculated energy levels, J, π, quadrupole moments, yrast states using the nucleon-pair approximation (NPA) and shell-model effective interactions. Comparison with available data.
doi: 10.1088/1674-1137/acc1cc
2023XU03 Phys.Rev. C 107, 044317 (2023) H.-T.Xue, Y.-F.Chen, Q.B.Chen, Y.A.Luo, H.-J.Schulze, X.-R.Zhou Deformation and spin-orbit splitting of Λ hypernuclei in the Skyrme-Hartree-Fock approach NUCLEAR STRUCTURE 12,13C, 16O, 28Si, 32S, 40Ca, 51V, 89Y, 139La, 208Pb; calculated Λ separation energy for hypernuclei, two-dimensional density distributions of Λ orbits, potential energy surfaces, quadrupole deformations of core nucleus and Λ orbitals, Λ spin-orbit slitting. Deformed Skyrme-Hartree-Fock (DSHF) approach with SLy4 NN and SLL4 ΛN interactions. Discussed spin symmetry in the hyperon spectrum. Comparison to available experimental data.
doi: 10.1103/PhysRevC.107.044317
2022CH13 Eur.Phys.J. A 58, 21 (2022) Y.F.Chen, X.-R.Zhou, Q.B.Chen, Y.-Y.Cheng Lambda binding energies in the Skyrme-Hartree-Fock approach with various ΛN interactions NUCLEAR STRUCTURE 5,6He, 8He, 7,8,9Li, 7,8,9,10Be, 9,10,11,12B, 12,13,14C, 15,16N, 16O, 28Si, 32S, 40Ca, 51V, 89Y, 139La, 208Pb; calculated hypernuclei binding energies, deformation parameters, local mean fields in the framework of the Skyrme-Hartree-Fock (SHF) approach. Comparison with available data.
doi: 10.1140/epja/s10050-022-00672-3
2022CH36 Chin.Phys.C 46, 064109 (2022) C.F.Chen, Q.B.Chen, X.-R.Zhou, Y.Y.Chen, J-W.Cui, H.-J.Schulze Effects of Λ hyperons on the deformations of even-even nuclei NUCLEAR STRUCTURE 8Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca, 22,24,26,28Ne, 30,32,34,36Si, 42,44,46,48Ca; calculated potential energy surfaces as functions of quadrupole deformation, hyperon s.p. energy levels as function of quadrupole deformation, density distributions for the occupied s.p. orbits using the deformed Skyrme-Hartree-Fock approach.
doi: 10.1088/1674-1137/ac5b58
2022CU07 Chin.Phys.C 46, 074109 (2022) Beyond-mean-field study of 37ΛAr based on the Skyrme-Hartree-Fock model NUCLEAR STRUCTURE 36,37Ar; calculated hypernuclear states using the Skyrme-Hartree-Fock (SHF) model and a beyond-mean-field approach, including angular momentum projection (AMP) and the generator coordinate method (GCM).
doi: 10.1088/1674-1137/ac6357
2022GU03 Phys.Rev. C 105, 034322 (2022) J.Guo, C.F.Chen, X.-R.Zhou, Q.B.Chen, H.-J.Schulze ΛΛ pairing effects in spherical and deformed multi-Λ hyperisotopes NUCLEAR STRUCTURE 6He, 10,11,12Be, 12,13B, 40Ca, 132Sn, 208Pb, 24Mg, 56Fe, 104Zr; calculated ΛΛ separation energies (S(2Λ)) double-Λ hypernuclei. 40,46Ca, 132,160Sn, 208,272Pb, 24Mg, 56Fe, 104Zr; calculated pairing gaps, pairing energies of hypernuclei. 130Zr; calculated deformation dependence of single-particle level energies, pairing gap and occupation probabilities of hypernuclei. 278Pb; calculated Λ hyperon potentil; single-particle levels. Skyrme-Hartree-Fock approach with Skyrme force SLy5 for the NN interaction, the Nijmegen interaction NSC97f for the ΛN interaction, and the empirical prescription EmpC for the ΛΛ interaction. Comparison to available experimental data.
doi: 10.1103/PhysRevC.105.034322
2022GU11 Chin.Phys.C 46, 064106 (2022) J.Guo, D.H.Chen, X.-R.Zhou, Q.B.Chen, H.-J.Schulze Effects of a kaonic meson on the ground-state properties of nuclei NUCLEAR STRUCTURE 5,6,7,8,9,10,11,12,13,14,15,16,17,18Be, 11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28O, 15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34Ne; calculated energies of the highest-occupied nucleon s.p. levels, partial neutron and proton s.p. levels within an axially-deformed Skyrme-Hartree-Fock approach combined with a Skyrme-type kaon-nucleon interaction.
doi: 10.1088/1674-1137/ac5601
2022XU02 Phys.Rev. C 105, 014304 (2022) H.T.Xue, X.R.Zhou, S.Y.Zhang, B.C.He, Y.A.Luo, L.Li, F.Pan, J.P.Draayer Neutrinoless double-β decay in the nucleon-pair shell model RADIOACTIVITY 130Te, 134,136Xe(2β-); calculated nuclear matrix elements (NMEs) of g.s. to g.s. neutrinoless double-β decay (0νββ) in the nucleon pair shell-model framework, with surface-δ approximation (SDI) and the BCS approximation. Comparison with shell model (SM), quasiparticle random-phase approximation (QRPA), and IBM2 theoretical calculations. NUCLEAR STRUCTURE 130,134,136Xe, 130Te, 134,136Ba; calculated low-lying positive-parity levels p to 10+ using shell model in the surface-δ approximation (SD)-pair or the SDG-pair subspace. Comparison with experimental data taken from the ENSDF database at NNDC, BNL.
doi: 10.1103/PhysRevC.105.014304
2022XU11 Phys.Rev. C 106, 044306 (2022) H.-T.Xue, Q.B.Chen, X.-R.Zhou, Y.Y.Cheng, H.-J.Schulze Deformation and hyperon halo in hypernuclei NUCLEAR STRUCTURE 11,13,15,17,19,21,23C, 10Li, 11Be, 12B, 14N, 15O, 16F, 17Ne; calculated potential energy surface, deformation parameters for hypernucleus and Λ hyperon, Λ removal energy, density distributions of spherical and deformed Λ 1p states, rms radii. Deformed Skyrme-Hartree-Fock approach with combinations of the NN interactions SIII, SGII, SkI4 and the ΛN interactions LY1 and SLL4.
doi: 10.1103/PhysRevC.106.044306
2021BA37 Phys.Rev. C 104, 034312 (2021) Quadrupole phonon excitations and transition probabilities for low-lying states of neutron-rich Cd isotopes NUCLEAR STRUCTURE 122,124,126,128,130,132,134,136,138Cd; calculated positive-parity levels, J, B(E2), overlap between the low-lying yrast state with and the phonon state using nucleon-pair approximation (NPA) of the shell model using the phenomenological Hamiltonian and effective interaction jj46. Comparison with available experimental data.
doi: 10.1103/PhysRevC.104.034312
2021GU28 Phys.Rev. C 104, L061307 (2021) J.Guo, X.-R.Zhou, H.-J.Schulze Skyrme force for all known Ξ- hypernuclei NUCLEAR STRUCTURE 12Be, 13B, 15C; analyzed experimental results for Ξ- hypernuclei within a Skyrme-Hartree-Fock approach, with optimal Skyrme parameters determined for a consistent description of experimental data from KISO, IBUKI, KINKA, BNL-E885, BNL-E906, KEK-E224, and KEK-E176 facilities for these nuclei; calculated removal energies for the 1s and 1p states of 13B and 12Be Ξ- hypernuclei. Discussed role of deformation for 13B Ξ- hypernucleus.
doi: 10.1103/PhysRevC.104.L061307
2020FA03 Eur.Phys.J. A 56, 11 (2020) B.-C.Fang, W.-Y.Li, C.-F.Chen, J.-W.Cui, X.-R.Zhou, Y.-Y.Cheng Impurity effects of Λ hyperons on pΛorbitals
doi: 10.1140/epja/s10050-019-00006-w
2020JI05 Eur.Phys.J. A 56, 135 (2020) Y.Jin, X.R.Zhou, Y.-Y.Cheng, H.-J.Schulze Study of Ξ- hypernuclei in the Skyrme-Hartree-Fock approach
doi: 10.1140/epja/s10050-020-00143-7
2019CH32 Phys.Rev. C 100, 014318 (2019) Y.-Y.Cheng, J.-Ji.Shen, G.-J.Fu, X.-R.Zhou, Y.-M.Zhao, A.Arima Nucleon-pair wave functions in a single-J shell
doi: 10.1103/PhysRevC.100.014318
2019CH35 Phys.Rev. C 100, 024321 (2019) Y.-Y.Cheng, H.Wang, J.-J.Shen, X.-R.Zhou, Y.-M.Zhao, A.Arima Nucleon-pair picture of low-lying states in semi-magic and open-shell nuclei NUCLEAR STRUCTURE 43,44,45,46,47,48Ca, 130Pd, 131Ag, 132Cd; calculated level energies vs spin for negative-parity yrast states of odd-mass Ca and positive-parity yrast states for even mass Ca isotopes, overlaps between one-dimensional nucleon-pair wave functions and corresponding shell-model wave functions, nucleon-pair wave functions using the framework of nucleon-pair approximation (NPA) of the shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.024321
2019JI10 Prog.Theor.Exp.Phys. 2019, 123D03 (2019) Y.Jin, C.F.Chen, X.-R.Zhou, Y.-Y.Cheng, H.-J.Schulze Deformed K- nuclei in the Skyrme-Hartree-Fock approach NUCLEAR STRUCTURE 8Be, 16O, 20Ne, 40Ca, 208Pb; calculated hypernuclei central kaon potential, kaon removal energies using a two-dimensional Skyrme–Hartree–Fock model with a KN Skyrme force.
doi: 10.1093/ptep/ptz141
2018LI12 Phys.Rev. C 97, 034302 (2018) Structure of 9ΛBe and 10ΛΛBe using the beyond-mean-field Skyrme-Hartree-Fock approach NUCLEAR STRUCTURE 8Be, 9Be, 10Be; calculated potential energy surfaces for 8Be+Λ, angular momentum projected energy curves for 8be and hypernucleus 9Be, density distributions of nuclear matter for low-lying states of 8Be, 9Be hypernucleus, and 10Be double-hypernucleus, levels, J, π, B(E2) of 8Be, hypernucleus 9Be, and double-hypernucleus 10Be. Beyond-mean-field Skyrme-Hartree-Fock (SHF) model with SLy4+SLL4 interactions. Two-α structure reproduced for ground state of 8Be. Comparison with available experimental data, and with results of hypernuclear particle-rotor model.
doi: 10.1103/PhysRevC.97.034302
2018LU16 Eur.Phys.J. A 54, 193 (2018) Z.-J.Luo, K.Yu, X.-R.Zhou, J.-W.Cui, H.Sagawa Effects of deformation, pairing and tensor correlation on the evolution of bubble structure within the Skyrme-Hartree-Fock method NUCLEAR STRUCTURE 46Ar; calculated energy surface vs quadrupole deformation, proton density distributions, sp energy levels using axially symmetric DSHF (Deformed Skyrme-Hartree-Fock) approach (several Skyrme forces used). 43Cl; calculated partial-wave decomposition of the proton density.
doi: 10.1140/epja/i2018-12620-5
2017CU01 Phys.Rev. C 95, 024323 (2017) J.-W.Cui, X.-R.Zhou, L.-X.Guo, H.-J.Schulze Investigation of single- and double-Λ hypernuclei using a beyond-mean-field approach NUCLEAR STRUCTURE 13,14C, 21,22Ne; calculated levels, J, π of single- and double-hypernuclei with 12C and 20Ne as core nuclei, potential-energy surfaces as functions of deformation parameter β, core B(E2), rms charge radii. Beyond-mean-field approach with angular momentum projection (AMP) techniques and generator coordinate method (GCM) based on Skyrme-Hartree-Fock (SHF). Comparison with experimental data.
doi: 10.1103/PhysRevC.95.024323
2017CU04 Prog.Theor.Exp.Phys. 2017, 093D04 (2017) A beyond-mean-field model for Λ hypernuclei with Skyrme-type NΛ interaction NUCLEAR STRUCTURE 12C; calculated hypernuclei properties using beyond-mean-field approach based on the Skyrme-Hartree-Fock model.
doi: 10.1093/ptep/ptx120
2017WU06 Phys.Rev. C 95, 034309 (2017) X.Y.Wu, H.Mei, J.M.Yao, X.-R.Zhou Beyond-mean-field study of the hyperon impurity effect in hypernuclei with shape coexistence NUCLEAR STRUCTURE 36,37Ar; calculated total energy, potential energy curves (PECs), correlation between the hyperon Λ separation energy and density overlap, quadrupole deformation parameters (β2, βΛ), rms radii of hypernuclei, neutrons, protons, and the hyperon, proton skin, density distribution contours for normal-deformed and superdeformed (SD) bands in 36Ar and 37Ar hypernucleus. 36Ar, 37Ar; calculated total energies for the mean-field states (MF), particle number projected states (N and Z), and particle number and angular momentum projected states, levels, J, π, collective wave functions of normal and superdeformed band in 36Ar and hypernucleus 37Ar using PC-F1 and PCY-S2 interactions. Relativistic mean field and beyond based on a relativistic point-coupling energy functional. Comparison with available experimental data.
doi: 10.1103/PhysRevC.95.034309
2016ZH29 Phys.Rev. C 94, 024331 (2016) Exotic structure of medium-heavy hypernuclei in the Skyrme Hartree-Fock model NUCLEAR STRUCTURE 36,37,38,39,40Ar, 40,41Ca; calculated energy surfaces as a function of deformation parameter β2, quadrupole deformation parameters, root mean square radii, binding energies, Λ separation energies for the ground states and superdeformed (SD) states, and two-dimensional density distributions for 37,38,39,40Ar, 41Ca hypernuclei and their core nuclei 36,37,38,39Ar, 40Ca. 37,38,39,40Ar, 41Ca; calculated Λ separation energies and spatial overlap between Λ and nucleons at the ground state and SD minima for hypernuclei. Skyrme Hartree-Fock (SHF)+BCS model with a microscopic ΛN interaction. Comparison with antisymmetrized molecular dynamics (AMD), and relativistic mean field (RMF) calculations.
doi: 10.1103/PhysRevC.94.024331
2015CU01 Phys.Rev. C 91, 054306 (2015) J.-W.Cui, X.-R.Zhou, H.-J.Schulze Shape and energy spectra of Λ hypernuclei from a Skyrme-Hartree-Fock model and a beyond-mean-field calculation NUCLEAR STRUCTURE 12,13C, 20,21Ne, 24,25,26,27Mg, 26,27,28,29Si; calculated levels, J, π, B(E2), potential energy surface (PES) contours in (β, γ) plane, root-mean-square (rms) radii and deformation β of core nuclei 12C, 20Ne, 24,26Mg, 26,28Si, and hypernuclei 13C, 21Ne, 25,27Mg, 27,29Si. Triaxial shape-constrained Skyrme-Hartree-Fock mean-field model with a density-dependent pairing interaction and NSC89NΛ interaction. Comparison with available experimental data.
doi: 10.1103/PhysRevC.91.054306
2015WU07 Phys.Rev. C 92, 054321 (2015) Global performance of multireference density functional theory for low-lying states in sd-shell nuclei NUCLEAR STRUCTURE 16,18,20,22,24,26,28,30,32Ne, 20,22,24,26,28,30,32,34,36,38,40Mg, 24,26,28,30,32,34,36,38,40,42,44,46,48Si, 26,28,30,32,34,36,38,40,42,44,46,48S, 30,32,34,36,38,40,42,44,46,48,50,52Ar; calculated dynamical correlation energies, binding energies, S(2n), charge density distributions, root-mean-square charge radii, proton depletion factors, energies of first 2+ and 4+ states, B(E2) for first 2+ states, spectroscopic quadrupole moments, neutron-proton decoupling factor, longitudinal C2 form factor for first 2+ in 24Mg, 28Si, 32S. Multireference density functional theory (MR-DFT) based on relativistic point-coupling energy density functional (EDF) using PC-PK1 and PC-F1 forces, and PN1DAMP+GCM. Comparison with other theoretical calculations, and with available experimental data.
doi: 10.1103/PhysRevC.92.054321
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
2013LI05 Phys.Rev. C 87, 014333 (2013) A.Li, E.Hiyama, X.-R.Zhou, H.Sagawa Tensor correlation, pairing interaction, and deformation in Ne isotopes and Ne hypernuclei NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30Ne; calculated β2 as function of neutron number for normal, and double-Λ hypernuclei. 26,30Ne; calculated energy surfaces as function of β2. Tensor and pairing effects on the quadruple deformation. Skyrme-Hartree-Fock model with BCS approximation, and two different hyperon-nucleon interactions for double-Λ hypernuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.014333
2013ZH30 Int.J.Mod.Phys. E22, 1350038 (2013) Kaonic Nuclei in the Skyrme-Hartree-Fock Approach NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; calculated hypernuclei, kaon chemical potential, kaon and nucleon densities. Skyrme-Hartree-Fock nuclear structure approach.
doi: 10.1142/S0218301313500389
2013ZH40 Nucl.Phys. A914, 332c (2013) Kaonic nuclei in the Skyrme-Hartree-Fock approach NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; calculated K- hypernuclei chemical potential, 16O K- hypernucleus calculated neutron, proton, kaon density distribution, radius using combination of standard SHF (Skyrme HF) model with chiral model for kaon-nucleon interaction.
doi: 10.1016/j.nuclphysa.2012.12.121
2012CU01 Chin.Phys.Lett. 29, 022101 (2012) J.-W.Cui, X.-R.Zhou, F.-Q.Chen, Y.Sun, C.-L.Wu Analyses of β-Bands of 230, 232Th and 232, 234U by the Projected Shell Model NUCLEAR STRUCTURE 230,232Th, 232,234U; calculated ground and β-bands, deformation parameters, energy schemes. Projected shell model, comparison with experimental data.
doi: 10.1088/0256-307X/29/2/022101
2011CH16 Chin.Phys.Lett. 28, 042101 (2011) 174Hf and 174Yb by the Projected Shell Model with Improved 4-quasiparticle basis NUCLEAR STRUCTURE 174Hf, 174Yb; calculated rotational bands, energies, J, π. Projected shell model, comparison with experimental data.
doi: 10.1088/0256-307X/28/4/042101
2010LI06 Phys.Rev. C 81, 025806 (2010) A.Li, X.R.Zhou, G.F.Burgio, H.-J.Schulze Protoneutron stars in the Brueckner-Hartree-Fock approach and finite-temperature kaon condensation
doi: 10.1103/PhysRevC.81.025806
2009CH71 Chin.Phys.C 33, Supplement 1, 24 (2009) Level statistics for the even-even Yb isotopes NUCLEAR STRUCTURE 160,162,164,166,168,172Yb; calculated level statistics; deduced discrepancies with the nearest-neighbor spacing distribution.
doi: 10.1088/1674-1137/33/S1/008
2009WE07 Chin.Phys.C 33, Supplement 1, 116 (2009) Properties of Zr hypernuclei in deformed Skyrme Hartree-Fock approach NUCLEAR STRUCTURE 80,100,122,138,139,142,188Zr; calculated two-neutron separation energy, neutron radii, hyperon separation energy. Deformed self-consistent Skyrme-Hartee-Fock approach.
doi: 10.1088/1674-1137/33/S1/037
2009ZH45 Chin.Phys.C 33, Supplement 1, 82 (2009) Properties of deformed Λ hypernuclei NUCLEAR STRUCTURE 8,9,10Be, 8,9,10,11B; calculated binding energy surfaces for core hypernuclei. Extended deformation in a self-consistent deformed SHF (DSHF) model.
doi: 10.1088/1674-1137/33/S1/027
2008SA39 Phys.Rev. C 78, 041304 (2008) H.Sagawa, X.R.Zhou, T.Suzuki, N.Yoshida Possible shape coexistence and magnetic dipole transitions in 17C and 21Ne NUCLEAR STRUCTURE 17C, 21Ne; calculated excitation energies, B(M1), g-factors, magnetic dipole moments, electric quadrupole moments, deformations. Shell model and Skyrme Hartree-Fock calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.041304
2008ZH25 Phys.Rev. C 78, 054306 (2008) X.-R.Zhou, A.Polls, H.-J.Schulze, I.Vidana Λ hyperons and the neutron drip line NUCLEAR STRUCTURE 6,7,8,9,10,11,12,13,14,15,16,17,18,19,20Be, 22,23,24,25,26,27,28O; calculated neutron single-particle levels, binding energies, quadrupole deformations. Hypernuclei. Skyrme Hartree-Fock calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.054306
2008ZH30 Int.J.Mod.Phys. E17, Supplement 1, 192 (2008) X.-R.Zhou, H.-J.Schulze, H.Sagawa Properties of nuclei and hypernuclei with the deformed Skyrme Hartree-Fock Model NUCLEAR STRUCTURE 7,9Be, 8,9,10B, 11,12C, 27Si, 50V; calculated deformations, radii. Deformed HF calculations.
doi: 10.1142/S0218301308011859
2007SA40 Phys.Rev. C 76, 024301 (2007) H.Sagawa, S.Yoshida, X.-R.Zhou, K.Yako, H.Sakai Charge exchange spin-dipole excitations in 90Zr and 208Pb and the neutron matter equation of state NUCLEAR REACTIONS 90Zr(n, p), 90Zr, 208Pb(p, n), E*<70 MeV; calculated spin dipole strength distributions using Skyrme Hartree Fock plus random phase approximation.
doi: 10.1103/PhysRevC.76.024301
2007ZH35 Phys.Rev. C 76, 034312 (2007) X.-R.Zhou, H.-J.Schulze, H.Sagawa, C.-X.Wu, E.-G.Zhao Hypernuclei in the deformed Skyrme-Hartree-Fock approach NUCLEAR STRUCTURE 7,8,9,10Be, 8,9,10,11B, 11,12,13C, 27,28Si, 50,51V, 88,89Y, 207,208Pb; calculated binding energies and deformation parameters using a deformed Hartree-Fock approach for Λ hypernuclei.
doi: 10.1103/PhysRevC.76.034312
2006HA31 J.Phys.(London) G32, 1105 (2006) I.Hamamoto, H.Sagawa, X.-R.Zhou Weakly bound neutrons and quadrupole response function in the many-body pair correlation of neutron drip line nuclei NUCLEAR STRUCTURE 84Ni; calculated quasiparticle energies, quadrupole response function. Simplified HFB equation, surface-type and volume-type pairing.
doi: 10.1088/0954-3899/32/8/003
2006ZH44 Int.J.Mod.Phys. E15, 1779 (2006) X.-R.Zhou, H.Sagawa, X.-Z.Zhang Evolution of deformations in sd and pf shell nuclei NUCLEAR STRUCTURE 18O, 20,22Ne, 24Mg, 28,30Si, 32,34S, 36Ar, 42Ca, 46Ti, 50Cr, 54Fe, 58Ni; calculated energy surfaces, deformation, quadrupole moments.
doi: 10.1142/S0218301306005368
2005SA59 Phys.Rev. C 72, 054311 (2005) Evolution of deformations in medium-mass nuclei NUCLEAR STRUCTURE 16O, 18,20Ne, 22,24Mg, 26,28Si, 30,32S, 34,36Ar, 38,40Ca, 42,44Ti, 46,48Cr, 50,52Fe, 54,56Ni; calculated deformation parameters, quadrupole moments. Deformed Skyrme-Hartree-Fock model with pairing correlations.
doi: 10.1103/PhysRevC.72.054311
2005SA63 Eur.Phys.J. A 25, Supplement 1, 535 (2005) H.Sagawa, X.R.Zhou, X.Z.Zhang, T.Suzuki Deformations and electromagnetic moments of light exotic nuclei NUCLEAR STRUCTURE 12,14,16,18,20,22C, 18,20,22,24,26,28,30,32Ne; calculated deformation energy, transitions B(E2). 9,11,13,15,17,19C; calculated quadrupole moments, μ. Deformed Skyrme-Hartree-Fock and shell model calculations.
doi: 10.1140/epjad/i2005-06-065-5
2005ZH23 Phys.Rev.Lett. 95, 051101 (2005) X.-R.Zhou, H.-J.Schulze, F.Pan, J.P.Draayer Strong Hyperon-Nucleon Pairing in Neutron Stars
doi: 10.1103/PhysRevLett.95.051101
2004SA58 Phys.Rev. C 70, 054316 (2004) H.Sagawa, X.R.Zhou, X.Z.Zhang, T.Suzuki Deformations and electromagnetic moments in carbon and neon isotopes NUCLEAR STRUCTURE 9,10,11,12,13,14,15,16,17,18,19,20,21,22C, 18,19,20,21,22,23,24,25,26,28Ne; calculated level energies, deformation, quadrupole moments, μ, B(E2). Deformed Skyrme Hartree-Fock model, isospin-dependent core polarization charges.
doi: 10.1103/PhysRevC.70.054316
2004SU13 Phys.Lett. B 589, 83 (2004) Y.Sun, X.-R.Zhou, G.-L.Long, E.-G.Zhao, P.M.Walker Nuclear structure of 178Hf related to the spin-16, 31-year isomer NUCLEAR STRUCTURE 178Hf; calculated levels, J, π, rotational bands, deformation; deduced high-spin isomer features. Projected shell model, comparison with data.
doi: 10.1016/j.physletb.2004.03.066
2004ZH06 Phys.Rev. C 69, 018801 (2004) X.R.Zhou, G.F.Burgio, U.Lombardo, H.-J.Schulze, W.Zuo Three-body forces and neutron star structure
doi: 10.1103/PhysRevC.69.018801
2004ZH36 Phys.Rev. C 70, 048802 (2004) X.-R.Zhou, H.-J.Schulze, E.-G.Zhao, F.Pan, J.P.Draayer Pairing gaps in neutron stars
doi: 10.1103/PhysRevC.70.048802
2003JU02 Phys.Rev. C 67, 034302 (2003) A.Jungclaus, B.Binder, A.Dietrich, T.Hartlein, H.Bauer, Ch.Gund, D.Pansegrau, D.Schwalm, D.Bazzacco, E.Farnea, S.Lunardi, C.Rossi-Alvarez, C.Ur, G.de Angelis, A.Gadea, D.R.Napoli, X.R.Zhou, Y.Sun Excited bands and signature dependent electromagnetic decay properties in neutron-rich 159, 161, 163Dy NUCLEAR REACTIONS 158,160Gd(7Li, xnyp), E=56 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 159,161,163Dy deduced high-spin levels, J, π, configurations, B(E1)/B(E2). GASP, ISIS arrays, projected shell model calculations.
doi: 10.1103/PhysRevC.67.034302
2003ZH22 Nucl.Phys. A723, 375 (2003) X.R.Zhou, E.G.Zhao, B.G.Dong, X.Z.Zhang, G.L.Long Collective properties of low-lying octupole excitations in 20882Pb126, 6020Ca40 and 288O20 NUCLEAR STRUCTURE 28O, 60Ca, 208Pb; calculated isoscalar and isovector octupole strength distributions, transition densities, giant resonance features. Self-consistent Hartree-Fock approach, RPA, particle-vibration coupling.
doi: 10.1016/S0375-9474(03)01366-6
2002ZH03 Chin.Phys.Lett. 19, 184 (2002) Spectral Statistics in the Cranking Model
doi: 10.1088/0256-307X/19/2/313
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