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NSR database version of April 27, 2024.

Search: Author = J.Z.Gu

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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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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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2021DO01      Phys.Lett. B 813, 136063 (2021)

J.M.Dong, Q.Zhao, L.J.Wang, W.Zuo, J.Z.Gu

α-Cluster formation in heavy α-emitters within a multistep model

RADIOACTIVITY ^{202,204,206,208,210,212,214,216,218}Po, ^{204,206,208,210,212,214,216,218,220}Rn, ^{206,208,210,212,214,216,218,220,222}Ra(α); calculated formation probability values, contour plots within a multistep model.

doi: 10.1016/j.physletb.2021.136063
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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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2019DO01      Phys.Rev. C 99, 014319 (2019)

J.M.Dong, J.Z.Gu, Y.H.Zhang, W.Zuo, L.J.Wang, Yu.A.Litvinov, Y.Sun

Beyond Wigner's isobaric multiplet mass equation: Effect of charge-symmetry-breaking interaction and Coulomb polarization

NUCLEAR STRUCTURE A=13, 15, 17, 19, 21, 23, 25, 27, 29, 31, 33, 35, 37, 39, 41, 43, 45, 47, 49, 51, 53, 55, 57, 59, 61; calculated coefficient of the added cubic term to the isobaric multiplet mass equation (IMME) for T=3/2 isobaric quartets, and density differences between neutron and proton for A=37 and 43 isobaric doublets. A=12, 16, 20, 24, 28, 32, 36; calculated coefficients of the added cubic and quartic terms to the isobaric multiplet mass equation (IMME) for T=2 isobaric quintets. Deduced general deviation from the original IMME, and the magnitude of the deviation exhibiting an oscillation-like behavior with mass number, modulated by the shell effect. Comparison with available experimental values.

doi: 10.1103/PhysRevC.99.014319
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2019WA10      Chin.Phys.Lett. 36, 32101 (2019)

Y.-Z.Wang, Y.Li, C.Qi, J.-Z.Gu

Pairing Effects on Bubble Nuclei

NUCLEAR STRUCTURE ⁴⁶Ar, ²⁰⁶Hg; calculated proton density distributions, occupation probabilities of the proton s states; deduced the difference between the bubble structure with the surface pairing and those with the volume and mixed pairings.

doi: 10.1088/0256-307x/36/3/032101
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2019WA30      Chin.Phys.C 43, 114101 (2019)

Y.-Z.Wang, X.-D.Su, C.Qi, J.-Z.Gu

Tensor force effect on the exotic structure of neutron-rich Ca isotopes*

NUCLEAR STRUCTURE ^{56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74}Ca; calculated two neutron separation energy, radii, neutron density distributions using spherical Skyrme-Hartree-Fock-Bogoliubov (SHFB) approach.

doi: 10.1088/1674-1137/43/11/114101
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2018DO02      Phys.Rev. C 97, 021301 (2018)

J.M.Dong, Y.H.Zhang, W.Zuo, J.Z.Gu, L.J.Wang, Y.Sun

Generalized isobaric multiplet mass equation and its application to the Nolen-Schiffer anomaly

ATOMIC MASSES ²⁰O, ⁵³Ni, ²⁰⁸Pb; calculated first-order symmetry energy coefficient for charge symmetry breaking (CSB) and second-order charge-independent breaking (CIB) components using SLy4, SLy5 and KBD interactions. Derived a generalized isobaric mass multiplet equation (GIMME), and applied to the study of Nolen-Schiffer anomaly (NSA) in the Coulomb displacement energy of mirror nuclei. A=10-60; calculated contributions of the CSB and CIB effects to coefficients of T_z and T_z2 using SLy4 interaction. ¹⁵O, ¹⁵N; ¹⁷F, ¹⁷O; ³⁹Ca, ³⁹K; ⁴¹Sc, ⁴¹Ca; calculated Δ_NSA for T=1/2 mirror pairs due to CSB effects using SLy4, SLy5 and KBD interactions. A=18-42; calculated Coulomb displacement energy (CDE) of the T=1 mirror pairs using SLy4 interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.97.021301
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2018DO04      Phys.Rev. C 97, 034318 (2018)

J.M.Dong, L.J.Wang, W.Zuo, J.Z.Gu

Constraints on Coulomb energy, neutron skin thickness in ²⁰⁸Pb, and symmetry energy

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated neutron skin thickness, density-dependent symmetry energy coefficient of nuclear matter by constraining the Coulomb energy with the mirror nuclei. A=17-65; calculated Coulomb displacement energies (CDEs) for T=1/2 mirror pairs, and compared with experimental data. ⁴⁸Ca, ⁶⁸Ni, ¹³²Sn, ²⁰⁸Pb, ²⁹⁸Fl; calculated symmetry energy using self-consistent Skyrme-Hartree-Fock approach with SLy4 interaction. Discussed charge-symmetry-breaking (CSB) effect.

doi: 10.1103/PhysRevC.97.034318
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2018DO09      Phys.Atomic Nuclei 81, 283 (2018)

J.M.Dong, W.Zuo, J.Z.Gu

The Fourth-Order Symmetry Energy of Finite Nuclei

NUCLEAR STRUCTURE ²⁰⁸Pb; compiled published calculations of Fourth-Order Symmetry Energy using a large set of Skyrme interactions.

doi: 10.1134/S1063778818030109
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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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2016DO08      Chin.Phys.Lett. 33, 102101 (2016)

J.-M.Dong, W.Zuo, J.-Z.Gu

First-Order Symmetry Energy Induced by Neutron-Proton Mass Difference

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated symmetry energy. Skyrme energy density functionals.

doi: 10.1088/0256-307X/33/10/102101
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2015WA05      Phys.Rev. C 91, 017302 (2015)

Y.Z.Wang, Z.Y.Hou, Q.L.Zhang, R.L.Tian, J.Z.Gu

Effect of a tensor force on the proton bubble structure of ²⁰⁶Hg

NUCLEAR STRUCTURE ²⁰⁶Hg; calculated proton density distribution by Skyrme-Hartree-Fock approach with the SLy5, SLy5+T, and SLy5+T_w interactions. Unlikely scenario for proton bubble structure in ²⁰⁶Hg because of the pairing correlation. Discussed antibubble effect from the pairing interaction based on Skyrme-Hartree-Fock-Bogoliubov approach.

doi: 10.1103/PhysRevC.91.017302
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2015WA35      Phys.Rev. C 92, 064301 (2015)

Y.Z.Wang, S.J.Wang, Z.Y.Hou, J.Z.Gu

Systematic study of α-decay energies and half-lives of superheavy nuclei

RADIOACTIVITY ^{270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302}Ds, ^{272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304}Cn, ^{274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306}Fl, ^{276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308}Lv, ^{278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310}Og, ^{284,286,288,290,292,294,296,298,300,302,304,306,308,310,312}120(α); calculated α-decay energies Q(α) and α-decay half-lives of the superheavy nuclei (SHN) using 20 models and 18 empirical formulas. Comparison with the calculated values, and available experimental data.

doi: 10.1103/PhysRevC.92.064301
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2014WA15      Phys.Rev. C 89, 047301 (2014)

Y.Z.Wang, J.Z.Gu, Z.Y.Hou

Preformation factor for α particles in isotopes near N = Z

RADIOACTIVITY ^{105,106,107,108,109,110}Te, ^{108,109,110,111,112}I, ^{109,110,111,112,113}Xe, ^112,114Cs(α); calculated α-particle preformation factors using the generalized liquid drop model, and experimental data for Q values and half-lives. Discussion of odd-even effect on preformation factor.

doi: 10.1103/PhysRevC.89.047301
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2014WA37      Chin.Phys.Lett. 31, 102102 (2014)

Y.-Z.Wang, J.-Z.Gu, G.-L.Yu, Z.-Y.Hou

Tensor Force Effect on Shape Coexistence of N = 28 Neutron-Rich Isotones

NUCLEAR STRUCTURE ⁴⁰Mg, ⁴⁶Ar, ⁴²Si, ⁴⁴S; calculated potential energy surfaces, shell correction energies; deduced impact of tensor force. Skyrme-Hartree-Fock-Bogoliubov approach.

doi: 10.1088/0256-307X/31/10/102102
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2013WA05      Eur.Phys.J. A 49, 15 (2013)

Y.Z.Wang, J.Z.Gu, Z.Y.Li, G.L.Yu, Z.Y.Hou

The effect of the tensor force on the bubble structure in Ar isotopes

NUCLEAR STRUCTURE ^{32,34,36,38,40,42,44,46,48,50,52,54,56}Ar; calculated single-particle levels, J, π, occupational probabilities, proton density distributions using Skyrme-Hartree-Fock approach with different tensor forces; deduced bubble possibility.

doi: 10.1140/epja/i2013-13015-x
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2013WA08      J.Phys.(London) G40, 045105 (2013)

Y.Z.Wang, G.L.Yu, Z.Y.Li, J.Z.Gu

Systematic study of tensor force effect on pseudospin orbital splittings in Sn isotopes

NUCLEAR STRUCTURE Z=50; calculated proton pseudospin orbital splittings. SHFB approach, tensor force.

doi: 10.1088/0954-3899/40/4/045105
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2012CH05      J.Phys.(London) G39, 035104 (2012)

L.-W.Chen, J.-Z.Gu

Correlations between the nuclear breathing mode energy and properties of asymmetric nuclear matter

NUCLEAR STRUCTURE ²⁰⁸Pb, ^100,132Sn; calculated nuclear isoscalar giant monopole resonance (ISGMR) energies, response functions; deduced correlations between ISGMR and symmetry energies. Microscopic HF calculations.

doi: 10.1088/0954-3899/39/3/035104
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2011DO12      Phys.Rev. C 84, 014303 (2011)

J.M.Dong, W.Zuo, J.Z.Gu, Y.Z.Wang, L.G.Cao, X.Z.Zhang

Effects of tensor interaction on pseudospin energy splitting and shell correction

NUCLEAR STRUCTURE ^{106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn; calculated proton and neutron pseudospin orbit splittings. ¹³²Sn, ²⁹⁸Fl; calculated neutron and proton shell correction energies, single particle spectra. Skyrme-Hartree-Fock approach with the SLy5+TF and T31+TF parameter sets combined with the BCS method.

doi: 10.1103/PhysRevC.84.014303
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2011WA10      Phys.Rev. C 83, 054305 (2011)

Y.Z.Wang, J.Z.Gu, J.M.Dong, X.Z.Zhang

Systematic study of tensor effects in shell evolution

NUCLEAR STRUCTURE Z=8, 20, 28, N=8-50 (even N); N=8, 20, 28, Z=6-32 (even Z); calculated evolution of magic gaps with and without tensor forces, proton spin-orbit potentials and radial wave function square, energy differences between the 1d_5/2 and 1d_3/2 single proton states in Ca isotopes. Hartree-Fock-Bogliubov approach with several Skyrme interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.054305
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2011WA28      Chin.Phys.Lett. 28, 102101 (2011)

Y.-Z.Wang, J.-Z.Gu, X.-Z.Zhang, J.-M.Dong

Tensor Effect on Bubble Nuclei

NUCLEAR STRUCTURE ³⁴Si, ⁴⁶Ar; calculated proton density distributions, single-particle spectra and proton spin-orbit potential. Hartree-Fock-Bogoliubov (HFB) approach.

doi: 10.1088/0256-307X/28/10/102101
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2011WA29      Phys.Rev. C 84, 044333 (2011)

Y.Z.Wang, J.Z.Gu, X.Z.Zhang, J.M.Dong

Tensor effects on the proton sd states in neutron-rich Ca isotopes and bubble structure of exotic nuclei

NUCLEAR STRUCTURE ^{40,42,44,46,48,50,52,54,56,58,60,62,64,66,68}Ca; calculated energy differences of the proton single-particle states with and without tensor force. ^48,64Ca; calculated proton spin-orbit potentials and squared radial wave functions, proton single-particle energies. ⁴⁶Ar, ²⁰⁶Hg; calculated proton single-particle spectrum, proton density distributions. Hartree-Fock-Bogoliubov (HFB) approach with Skyrme interactions SLy5+T, SLy5+Tw and several sets of the TIJ parameterizations. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.044333
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2010GU10      Nucl.Phys. A834, 87c (2010)

J.-Z.Gu, B.-B.Peng, W.-H.Zou, S.-F.Shen

Decay out of A Superdeformed Band: Chaoticity Dependence and A Microscopic Understanding

NUCLEAR STRUCTURE ^{188,190,192,194,196}Hg; calculated super-deformed bands, E2 transition strengths, angular momentum, deformation using projected shell model with HFB based on Gogny force.

doi: 10.1016/j.nuclphysa.2010.01.026
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2010SH17      Nucl.Phys. A834, 90c (2010)

S.-F.Shen, F.Pan, J.-Z.Gu, L.-H.Zhu, X.-G.Wu, J.P.Draayer, T.-D.Wen

Low-spin states and level structure of odd-even rubidium isotope: ⁸³Rb

RADIOACTIVITY ⁸³Sr(β⁺); measured Eγ, Iγ, γγ-coin. ⁸³Rb; deduced levels, J, π, yrast states. Comparison with projected shell model.

doi: 10.1016/j.nuclphysa.2010.01.027
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2010WA31      Eur.Phys.J. A 44, 287 (2010)

Y.Z.Wang, J.Z.Gu, J.M.Dong, B.B.Peng

Properties of α-decay to ground and excited states of heavy nuclei

RADIOACTIVITY ^222,224,226Ra, ^{226,228,230,232}Th, ^{228,230,232,234,236,238}U, ^{234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{244,246,248,250,252}Cf, ^248,250,252Fm, ²⁵²No(α); calculated branching ratios, T_1/2 using generalized liquid drop model and Royer's formula. Comparison with data and other models.

doi: 10.1140/epja/i2010-10948-4
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2010WA35      Int.J.Mod.Phys. E19, 1961 (2010)

Y.Z.Wang, J.Z.Gu, J.M.Dong, B.B.Peng

Properties of alpha decay to rotational bands of heavy nuclei

RADIOACTIVITY ^254,256,258No, ^256,258,260Rf(α); calculated branching ratios, T_1/2 of α-decays of the ground and rotational bands. Generalized Liquid Drop Model (GLDM).

doi: 10.1142/S0218301310016442
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2010ZO01      Chin.Phys.Lett. 27, 012101 (2010)

W.-H.Zou, J.-Z.Gu

Yrast Properties of Dysprosium Isotopes in the Double Mid-Shell Region

NUCLEAR STRUCTURE ^{164,166,168,170,172,174}Dy; calculated level energies, moment of inertia, yrast bands using projected shell model; deduced ¹⁷⁰Dy back-bending. Comparison with experimental data.

doi: 10.1088/0256-307X/27/1/012101
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2010ZO02      Chin.Phys.C 34, 56 (2010)

W.-H.Zou, Y.Tian, S.-F.Shen, J.-Z.Gu, B.-B.Peng, D.-D.Zhang, Z.-Y.Ma

Nuclear structure around ⁸⁰Zr

NUCLEAR STRUCTURE ^80,82,84Zr; calculated potential energy surfaces, ground state bands. Projected shell model (PSM) and relativistic Hartee-Bogoliubov (RHB) theory.

doi: 10.1088/1674-1137/34/1/010
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2010ZO03      Phys.Rev. C 82, 024309 (2010)

W.-h.Zou, Y.Tian, J.-z.Gu, S.-f.Shen, J.-m.Yao, B.-b.Peng, Z.-y.Ma

Microscopic description of nuclear structure around ⁸⁰Zr

NUCLEAR STRUCTURE ^80,82,84Zr; calculated ground-state total binding energies and angular momentum projected potential energy surfaces (AMPPES) using projected shell model with a quadrupole constrained relativistic Hartree-Bogoliubov (RHB) theory and NL3 effective interaction and Gogny D1S interaction for the pairing force. Shape coexistence and shape transitions, and decay out of superdeformed rotational bands.

doi: 10.1103/PhysRevC.82.024309
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2009SH28      Int.J.Mod.Phys. E18, 1603 (2009)

S.-F.Shen, X-J.Wang, T.-T.Wang, T.-D.Wen, J.-Z.Gu, Z.-D.Liu, Z.-S.Zhang, F.-R.Xu, S.-J.Zheng, J.-Y.Liu

Decay of ¹⁸⁸Re and TRS calculations for its daughter nuclide ¹⁸⁸Os

RADIOACTIVITY ¹⁸⁸Re(β^-); measured Eγ, Iγ, γγ-coin.; deduced quadrupole deformation and triaxiality parameters. Comparison with Hartree-Fock-Bogoliubov, total Routhian surface calculations.

doi: 10.1142/S0218301309013762
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2007SA46      Phys.Rev. C 76, 034327 (2007); Erratum Phys.Rev. C 77, 049902 (2008)

H.Sagawa, S.Yoshida, G.-M.Zeng, J.-Z.Gu, X.-Z.Zhang

Isospin dependence of incompressibility in relativistic and nonrelativistic mean field calculations

NUCLEAR STRUCTURE ^{112,114,116,118,120,122,124}Sn, ²⁰⁸Pb; calculated isoscalar giant monopole resonance strength distributions using Skyrme-HF and relativistic mean field models.

doi: 10.1103/PhysRevC.76.034327
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2001GU18      Nucl.Phys. A690, 382 (2001)

J.Z.Gu, H.A.Weidenmuller

Coulomb Excitation of Double Giant Dipole Resonances

NUCLEAR REACTIONS ²⁰⁸Pb(²⁰⁸Pb, ²⁰⁸Pb'), E=200-10000 MeV/nucleon; calculated σ(E), energy-integrated σ, enhancement factors for Coulomb excitation of double GDR. Brink-Axel mechanism.

doi: 10.1016/S0375-9474(01)00356-6
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1999GU18      Phys.Rev. C60, 035211 (1999)

J.-Z.Gu, H.-S.Zong, Y.-X.Liu, E.-G.Zhao

Statistical Properties of the Charmonium Spectrum and a New Mechanism of J/ψ Suppression

doi: 10.1103/PhysRevC.60.035211
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1999GU23      Nucl.Phys. A660, 197 (1999)

J.-Z.Gu, H.A.Weidenmuller

Decay Out of a Superdeformed Band

doi: 10.1016/S0375-9474(99)00362-0
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1999ZO01      Phys.Rev. C59, 2782 (1999)

H.-S.Zong, J.-Z.Gu, X.-F.Zhang, Y.-X.Liu, E.-G.Zhao

Relativistic Description of J/ψ Dissociation in Hot Matter

doi: 10.1103/PhysRevC.59.2782
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1999ZO03      Phys.Rev. C60, 055208 (1999)

H.-S.Zong, X.-F.Lu, J.-Z.Gu, C.-H.Chang, E.-G.Zhao

Vacuum Condensates in the Global Color Symmetry Model

doi: 10.1103/PhysRevC.60.055208
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1998GU08      Chin.Phys.Lett. 15, 318 (1998)

J.-Z.Gu, E.-G.Zhao, Y.-Z.Zhuo, X.-S.Wu, H.-S.Zong

Classical Dynamics of a Nucleon in Heavy Nuclei

doi: 10.1088/0256-307X/15/5/003
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1998GU12      Eur.Phys.J. A 2, 115 (1998)

J.-Z.Gu, E.-G.Zhao, Y.-Z.Zhuo, X.-Z.Wu, H.-S.Zong

Classically Dynamical Behaviour of a Nucleon in Heavy Nuclei

doi: 10.1007/s100500050099
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1998GU24      Eur.Phys.J. A 3, 217 (1998)

J.-Z.Gu, Y.-Z.Zhuo, E.-G.Zhao, X.-Z.Wu, H.-S.Zong

Dynamical Origin of the Quantum Chaotic Motion of a Single Particle in the Two-Center Shell Model

doi: 10.1007/s100500050171
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1997GU21      Nucl.Phys. A625, 621 (1997)

J.-Z.Gu, X.-Z.Wu, Y.-Z.Zhuo, E.-G.Zhao

Quantum Chaotic Motion of a Single Particle in Heavy Nuclei

NUCLEAR STRUCTURE ²³⁸U; calculated levels, nearest-neighbor level spacing distributions; deduced chaotic motion deformation dependence.

doi: 10.1016/S0375-9474(97)00503-4
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1996GU02      Z.Phys. A354, 15 (1996)

J.-Z.Gu, X.-Z.Wu, Y.-Z.Zhuo

The Statistical Properties of Single-Particle Levels in Rotating Heavy Nuclei

NUCLEAR STRUCTURE ²³⁸U; calculated single particle levels, curvature, spacing distributions vs cranked frequency. Rotating two-center shell model.

doi: 10.1007/s002180050008
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1996GU22      Nucl.Phys. A611, 315 (1996)

J.-Z.Gu, X.-Z.Wu, Y.-Z.Zhuo

The Single-Particle Spectrum and Its Spacing and Curvature Distributions in Rotating Heavy Nuclei

NUCLEAR STRUCTURE ²³⁸U; calculated proton single particle levels in rotating system; deduced level spacing, curvature distributions, model parameters dependence.

doi: 10.1016/S0375-9474(96)00402-2
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1995GU24      Chin.J.Nucl.Phys. 17, No 4, 305 (1995)

J.-Z.Gu, X.-Z.Wu, Y.-Z.Zhuo, Y.-S.Ling

A Method to Deal with the Heavy Ion Induced Fission Based on Diffusion Model

NUCLEAR STRUCTURE ²⁴⁰Pu; calculated fission rate. Heavy ion induced fission, diffusion model.

1994GU13      Z.Phys. A349, 53 (1994)

J.Z.Gu, Y.-S.Ling

Investigation of the Induced Nuclear Fission with Coordinate-Dependent Mass, Friction and Temperature

NUCLEAR STRUCTURE ²⁴⁰Pu; calculated fission rates. Lie algebra method, with, without coordinate-dependent mass, friction, temperature.

doi: 10.1007/BF01296333
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1994GU21      Chin.J.Nucl.Phys. 16, No 3, 251 (1994)

J.-Z.Gu, Y.-S.Ling

A Method to Solve the Fokker-Planck Equation with Coordinate-Dependent Mass, Friction and Temperature

NUCLEAR STRUCTURE ²⁴⁰Pu; calculated fission rate at saddle point. Fokker-Planck equation, coordinate-dependent mass, friction, temperature.