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NSR database version of April 27, 2024.

Search: Author = J.Cui

Found 23 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 ¹³_ΛC in a beyond-mean-field approach

doi: 10.1103/PhysRevC.109.024324
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2023WA23      Chin.Phys.C 47, 084101 (2023)

Y.-Z.Wang, F.-Z.Xing, J.-P.Cui, Y.-H.Gao, J.-Z.Gu

Roles of tensor force and pairing correlation in two-proton radioactivity of halo nuclei

RADIOACTIVITY ¹⁸Mg, ²⁰Si(2p); calculated T_1/2 using different Skyrme interactions, Q-values; deduced small effect of tensor force. The framework of spherical Skyrme-Hartree-Fock-Bogoliubov theory.

doi: 10.1088/1674-1137/acd680
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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
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2022CU01      Nucl.Phys. A1017, 122341 (2022)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Improved effective liquid drop model for α-decay half-lives

RADIOACTIVITY ^{255,256,258,259,261,263}Rf, ^{256,257,258,259}Db, ²⁷⁰Db, ^259,260,261Sg, ²⁶³Sg, ^267,269,271Sg, ²⁶³Sg, ^267,269,271Sg, ^260,261Bh, ^265,266,267Bh, ^270,272,274Bh, ^264,265,266Hs, ^268,269,270Hs, ^273,275Hs, ²⁷⁰Mt, ^274,275,276Mt, ²⁷⁸Mt, ²⁶⁷Ds, ^269,270,271Ds, ²⁷³Ds, ^277,279,281Ds, ²⁷²Rg, ^{278,279,280,281,282}Rg, ²⁷⁷Cn, ^281,283Cn, ^284,285Cn, ²⁷⁸Nh, ^{282,283,284,285,286}Nh, ^{285,286,287,288,289}Fl, ²⁸⁷Mc, ^289,290Mc, ^{290,291,292,293}Lv, ^293,294Ts, ²⁹⁴Og(α); calculated T_1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122341
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2022CU02      Nucl.Phys. A1017, 122341 (2022)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Improved effective liquid drop model for α-decay half-lives

RADIOACTIVITY ^{255,256,258,259,261,263}Rf, ^{256,257,258,259,270}Db, ^{259,260,261,263,267,269,271}Sg, ^{260,261,265,266,267,270,272,274}Bh, ^{264,265,266,268,269,270,273,275}Hs, ^{270,274,275,276,278}Mt, ^{267,269,270,271,273,277,279,281}Ds, ^{272,278,279,280,281,282}Rg, ^{277,281,283,284,285}Cn, ^{278,282,284,285,286}Nh, ^{285,286,287,288,289}Fl, ^{287,288,289,290}Mc, ^{290,291,292,293}Lv, ^293,294Ts, ^{278,282,286,290,294,298,302,306}Og, ^{281,285,289,293,297,301,305,309}119, ^{286,290,294,298,302,306,310,289,293,297,301,305,309}120(α); calculated T_1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122341
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2022CU07      Chin.Phys.C 46, 074109 (2022)

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

Beyond-mean-field study of ³⁷_ΛAr 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
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2022XI08      Nucl.Phys. A1028, 122528 (2022)

F.Xing, H.Qi, J.Cui, Y.Gao, Y.Wang, J.Gu, G.Yong

An improved Gamow-like formula for α-decay half-lives

RADIOACTIVITY ^{214,215,216,217,218}U, ^{219,220,221,222,223,224}Np, ^{221,222,223,224,225,226,227}Pu, ^{224,225,226,227,228}Am, ^231,232Cm, ^{233,234,235,236,237,238,239,240,241,242}Bk, ^234,235,236Cf, ^237,238,239Es, ^{239,240,241,242,243,244}Fm, ^241,242,243Md, ^{246,247,248,249,250}No, ^249,250,251Lr, ^{251,252,253,254}Rf, ^253,254,255Db, ^256,257,258Sg, ^{258,259,260,261,262,263}Bh, ^261,262Hs, ^263,264,265Mt, ^{261,262,263,264,265,266}Ds, ^{266,267,268,269,270,271,272,273}Rg, ^{270,271,272,273,274,275,276}Cn, ^{272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290}Nh, ^{278,279,280,281,282,283,284,285,286,287,288,289,290,291}Fl, ^{281,282,283,284,285,286,287,288,289,290,291,292}Mc, ^{283,284,285,286,287,288,289}Lv, ^{285,286,287,288,289,290,291,292}Ts, ^{288,289,290,291,292,293}Og, ²⁹⁵Og, ^{290,291,292,293,294,295,296}119, ^{291,292,293,294,295,296,297,298,299,300}120, ^{287,288,289,290,291}Og, ^283,284Lv, ^279,280,281Fl, ^275,276Cn, ^271,272,273Ds, ²⁹⁴120, ^268,269Hs, ^264,265Sg, ²⁸¹Fl(α); calculated T_1/2; deduced an improved Gamow-like (IMGL) formula parameters. Comparison with available data.

doi: 10.1016/j.nuclphysa.2022.122528
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2021XI06      Chin.Phys.C 45, 124105 (2021)

F.Xing, J.Cui, Y.Wang, J.Gu

Two-proton radioactivity of ground and excited states within a unified fission model

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); ⁵Be, ^6,7B, ⁸C, ¹⁰N, ¹¹O, ^13,14F, ¹⁵Ne, ¹⁷Na, ²²Si, ²⁴P, ²⁶S, ^28,29Cl, ^29,30Ar, ^31,32K, ^33,34Ca, ⁴⁵Sc, ^35,37Sc, ^37,38,39Ti, ^39,40V, ^41,42Cr, ^43,44Mn, ⁴⁷Co, ⁴⁹Ni, ⁵²Cu, ⁵⁵Zn, ^56,57,58Ga, ^58,59Ge, ^60,61,62As, ^63,64Se, ^65,66Br, ⁶⁸Kr, ⁸¹Mo, ⁸⁵Ru, ¹⁰⁸Xe(2p); analyzed available data; calculated T_1/2. Comparison with the AME2020 table, available data.

doi: 10.1088/1674-1137/ac2425
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2020CU01      Phys.Rev. C 101, 014301 (2020), Erratum Phys.Rev. C 104, 029902 (2021)

J.P.Cui, Y.H.Gao, Y.Z.Wang, J.Z.Gu

Two-proton radioactivity within a generalized liquid drop model

RADIOACTIVITY ⁶Be, ¹²O, ¹⁶Ne, ¹⁹Mg, ⁴⁵Fe, ⁴⁸Ni, ⁵⁴Zn, ⁶⁷Kr(2p); calculated half-lives for 2p decay mode using generalized liquid drop model (GLDM) and compared with experimental half-lives, and other theoretical calculations. ²²Si, ²⁶S, ³⁴Ca, ^38,39Ti, ⁴²Cr, ⁴⁹Ni, ⁵⁵Zn, ^58,59,60Ge, ⁶⁴Se(2p); predicted half-lives using GLDM for 2p radioactivity.

doi: 10.1103/PhysRevC.101.014301
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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 p_Λorbitals

doi: 10.1140/epja/s10050-019-00006-w
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2019CU01      Nucl.Phys. A987, 99 (2019)

J.P.Cui, Y.Xiao, Y.H.Gao, Y.Z.Wang

α-decay half-lives of neutron-deficient nuclei

RADIOACTIVITY Z=80-118(α); calculated α-decay T_1/2 of neutron-deficient nuclei using Effective Liquid Drop Model (ELDM), generalized Liquid Drop Model (GLDM) within fission-like and cluster-like modes and using Royer and Denisov formulae; T_1/2 compared to data; deduced that GLDM gives higher values than calculations using other approaches; calculated, predicted T_1/2 n-deficient nuclei not measured using GLDM with WS4 Q_α values.

doi: 10.1016/j.nuclphysa.2019.04.008
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2018CU01      Phys.Rev. C 97, 014316 (2018)

J.P.Cui, Y.L.Zhang, S.Zhang, Y.Z.Wang

α-decay half-lives of superheavy nuclei

RADIOACTIVITY ^{255,256,258,259,261,263}Rf, ^{256,257,258,259,270}Db, ^{259,260,261,263,267,269,271}Sg, ^{260,261,265,266,267,270,272,274}Bh, ^{264,265,266,268,269,270,273,275}Hs, ^{270,274,275,276,278}Mt, ^{267,269,270,271,273,277,279,281}Ds, ^{272,278,279,280,281,282}Rg, ^{277,281,283,284,285}Cn, ^{278,282,283,284,285,286}Nh, ^{285,286,287,288,289}Fl, ^{287,288,289,290}Mc, ^{290,291,292,293}Lv, ^293,294Ts, ²⁹⁴Og(α); calculated α-decay half-lives of superheavy nuclei, and compared with experimental values; deduced hindrance factors. ^{289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304}Og, ^{290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305}119, ^{291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306}120(α); calculated Q(α) and corresponding half-lives using theoretical WS4, FRDM, KTUY and GHFB mass tables. Effective liquid drop model (ELDM).

doi: 10.1103/PhysRevC.97.014316
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2018LI12      Phys.Rev. C 97, 034302 (2018)

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

Structure of ⁹_ΛBe and ¹⁰_ΛΛBe 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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2017WA04      Phys.Rev. C 95, 014302 (2017)

Y.Z.Wang, J.P.Cui, Y.L.Zhang, S.Zhang, J.Z.Gu

Competition between α decay and proton radioactivity of neutron-deficient nuclei

RADIOACTIVITY ¹⁰⁹I, ¹¹²Cs, ¹⁵⁷Ta, ^{160,161,161m,162,163}Re, ^{164m,165,165m,166,166m,167,167m}Ir, ^{169,170,170m,171m,173}Au, ^{177,177m,178,179}Tl, ^185,185mBi(p), (α); calculated half-lives, and compared with available experimental values, penetration probabilities. ¹⁰⁵Sb, ¹⁰⁸I, ¹¹³Cs, ¹¹⁷La, ¹²¹Pr, ^130,131,132Eu, ^135,136Tb, ^140,141,141mHo, ^{144,145,146,147,147m}Tm, ^{150,150m,151,151m}Lu, ^155,156,156mTa, ¹⁵⁹Re, ¹⁶⁴Ir, ^171,172,172mAu, ¹⁷⁶Tl(α); calculated α-decay half-lives, and compared with experimental proton-decay half-lives. ¹¹⁶La, ^157mTa, ^159mRe, ^168,169,169mIr, ^184,186,187Bi(p); calculated proton-decay half-lives, and compared with experimental α-decay half-lives. ^155,156Ta, ^159,160,161Re, ^164,165Ir, ^169,170,171Au, ¹⁷⁶Tl, ¹⁸⁵Bi; predicted dominant proton decay mode. ¹⁵⁷Ta, ^162,163Re, ^{165,166,167,168,169}Ir, ^172,173Au, ^177,178,179Tl, ^184,186,187Bi; predicted dominant α decay mode. Effective liquid drop model (ELDM). Comparison with predictions of microscopic model (MM) and with available experimental values.

doi: 10.1103/PhysRevC.95.014302
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2017ZH03      Phys.Rev. C 95, 014311 (2017)

S.Zhang, Y.Zhang, J.Cui, Y.Wang

Improved semi-empirical relationship for α-decay half-lives

RADIOACTIVITY ^106,108Te, ¹¹²Xe, ¹¹⁴Ba, ^146,148Sm, ^148,150,152Gd, ^150,152,154Dy, ^152,154Er, ^154,156,158Yb, ^156,158,160Hf, ^{158,160,162,166}W, ^{162,166,170,174}Os, ^{168,170,174,176,178,180,182,184,188,190}Pt, ^{174,176,180,182,184,188}Hg, ^{186,188,190,210}Pb, ^{190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^{194,196,198,200,202,206,208,210,212,218,220,222}Rn, ^{204,206,208,210,212,214,220,222,224,226}Ra, ^{210,216,218,222,224,226,228,230,232}Th, ^{224,226,228,230,232,234,236,238}U, ^{230,232,234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{240,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^252,256No, ^256,258Rf, ^260,262Sg, ^264,266,270Hs, ²⁷⁰Ds, ^286,288Fl, ^290,292Lv, ²⁹⁴Og(α); ^105,107Te, ¹⁰⁹Xe, ¹⁴⁷Sm, ¹⁵¹Gd, ^151,153Dy, ^153,155Er, ^155,157Yb, ¹⁵⁷Hf, ^159,165W, ^{161,167,169,173}Os, ^{167,169,171,173,175,177,181,182}Pt, ^{173,175,177,179,183,185}Hg, ¹⁹¹Pb, ^{187,189,191,195,197,199,201,205,207,209,211,213}Po, ^{195,197,199,201,203,207,209,211,213,215,219,221}Rn, ^{203,205,209,211,213,215,217,219,221}Ra, ^{211,213,215,217,219,221,223,225,227}Th, ^{217,219,223,225,235}U, ^239,241Pu, ^{241,243,245,247}Cm, ^249,251Cf, ^{251,253,255,257}Fm, ²⁶³Rf, ^{259,261,269,271}Sg, ^265,267,273Hs, ^{267,269,271,273,277,281}Ds, ^281,285Cn, ^287,289Fl, ^291,293Lv(α); ¹¹¹I, ¹⁴⁷Eu, ^149,151Tb, ¹⁵³Tm, ^169,177Ir, ^{173,181,183,185}Au, ^177,179Tl, ^{187,189,193,195,211,213}Bi, ^{197,199,201,203,205,207,209,211,213,215,217,219}At, ^{201,203,205,207,209,211,213,215,217,219,221,223}Fr, ^{209,211,213,215,217,219,221,223,225,227}Ac, ^{213,215,217,219,225,227,231}Pa, ^{235,237,239,241,243}Np, ^239,241,243Am, ^243,245,249Bk, ^243,244Es, ^255,257Lr, ^257,259,263Db, ^261,267Bh, ²⁷⁵Mt, ²⁷⁹Rg, ^283,285Nh, ^287,289Mc, ²⁹³Ts(α); ^110,112I, ¹¹⁴Cs, ¹⁴⁸Eu, ^152,154Ho, ^154,156Tm, ¹⁵⁸Lu, ¹⁶²Ta, ^160,162Re, ¹⁶⁶Ir, ^{170,172,174,182}Au, ¹⁸²Tl, ^212,214Bi, ^{196,198,200,202,204,208,210,212,214,216,218}At, ^{200,202,204,206,208,210,212,214,216,218,220}Fr, ^{206,208,210,212,214,216,218,222,224}Ac, ^{212,216,226,230}Pa, ²⁵⁴Es, ²⁵⁶Md, ^256,258Db, ^{260,264,266,270,272,274}Bh, ^{268,274,276,278}Mt, ^{272,274,278,280}Rg, ^{278,282,284,286}Nh, ^288,290Mc, ²⁹⁴Ts(α); calculated α-decay half-lives, and preformation probabilities using improved semi-empirical formulation by introducing a precise radius formula and an analytic expression for preformation probability. Comparison with experimental half-lives. ^{278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308}Og, ^{280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309}119, ^{283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310}120, ^{286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311}121(α); predicted α-decay half-lives for the superheavy nuclides using ImSahu, SemFIS2, and UNIV2 formulas.

doi: 10.1103/PhysRevC.95.014311
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2016CU01      Int.J.Mod.Phys. E25, 1650056(2016)

J.P.Cui, Y.L.Zhang, S.Zhang, Y.Z.Wang

Systematic study on α-decay half-lives of Bi isotopes

RADIOACTIVITY ^{184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214}Bi(α); calculated T_1/2. The generalized liquid drop model (GLDM) and several sets of Royer's analytic formulas, comparison with experimental data.

doi: 10.1142/S0218301316500567
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2016KU02      Int.J.Mod.Phys. E25, 1650012 (2016)

Y.Kun, X.Zhou, J.Cui

Shape evolution and energy spectra of Pt isotopes

NUCLEAR STRUCTURE ^{178,180,182,184,186,188,190,192,194}Pt; calculated Potential energy curves of as a function of the axial quadrupole deformation parameter, angular momentum projected deformation energy curves, J, π, level energies, B(E2). Nonrelativistic Skyrme-Hartree-Fock (SHF) approach plus a density-dependent pairing in the BCS approximation.

doi: 10.1142/S0218301316500129
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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, 232}Th and ^{232, 234}U 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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Note: The following list of authors and aliases matches the search parameter J.Cui: , J.P.CUI, J.W.CUI