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NSR database version of April 27, 2024.

Search: Author = J.W.Cui

Found 10 matches.

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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
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2022CU07      Chin.Phys.C 46, 074109 (2022)

J.-W.Cui, R.Wang, X.-R.Zhou

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
Citations: PlumX Metrics


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
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2018LI12      Phys.Rev. C 97, 034302 (2018)

W.-Y.Li, J.-W.Cui, X.-R.Zhou

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
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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
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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
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2017CU04      Prog.Theor.Exp.Phys. 2017, 093D04 (2017)

J.-W.Cui, X.-R.Zhou

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
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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
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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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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
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