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NSR database version of May 10, 2024.

Search: Author = J.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 T1/2 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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2022CH32      Phys.Rev. A 105, 063108 (2022)

Y.-Q.Chu, Z.-F.Wan, F.Ritterbusch, W.-K.Hu, J.-Q.Gu, S.-M.Hu, Z.-H.Jia, W.Jiang, Z.-T.Lu, L.-T.Sun, A.-M.Tong, J.S.Wang, G.-M.Yang

Optically enhanced discharge excitation and trapping of 39Ar

ATOMIC PHYSICS 39Ar; measured frequencies; deduced loading rate in an atom trap by enhancing the generation of metastable atoms in a discharge source. Comparison with calculations.

doi: 10.1103/PhysRevA.105.063108
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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 255,256,258,259,261,263Rf, 256,257,258,259Db, 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, 278,279,280,281,282Rg, 277Cn, 281,283Cn, 284,285Cn, 278Nh, 282,283,284,285,286Nh, 285,286,287,288,289Fl, 287Mc, 289,290Mc, 290,291,292,293Lv, 293,294Ts, 294Og(α); calculated T1/2. 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 255,256,258,259,261,263Rf, 256,257,258,259,270Db, 259,260,261,263,267,269,271Sg, 260,261,265,266,267,270,272,274Bh, 264,265,266,268,269,270,273,275Hs, 270,274,275,276,278Mt, 267,269,270,271,273,277,279,281Ds, 272,278,279,280,281,282Rg, 277,281,283,284,285Cn, 278,282,284,285,286Nh, 285,286,287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 278,282,286,290,294,298,302,306Og, 281,285,289,293,297,301,305,309119, 286,290,294,298,302,306,310,289,293,297,301,305,309120(α); calculated T1/2. Comparison with available data.

doi: 10.1016/j.nuclphysa.2021.122341
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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 214,215,216,217,218U, 219,220,221,222,223,224Np, 221,222,223,224,225,226,227Pu, 224,225,226,227,228Am, 231,232Cm, 233,234,235,236,237,238,239,240,241,242Bk, 234,235,236Cf, 237,238,239Es, 239,240,241,242,243,244Fm, 241,242,243Md, 246,247,248,249,250No, 249,250,251Lr, 251,252,253,254Rf, 253,254,255Db, 256,257,258Sg, 258,259,260,261,262,263Bh, 261,262Hs, 263,264,265Mt, 261,262,263,264,265,266Ds, 266,267,268,269,270,271,272,273Rg, 270,271,272,273,274,275,276Cn, 272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290Nh, 278,279,280,281,282,283,284,285,286,287,288,289,290,291Fl, 281,282,283,284,285,286,287,288,289,290,291,292Mc, 283,284,285,286,287,288,289Lv, 285,286,287,288,289,290,291,292Ts, 288,289,290,291,292,293Og, 295Og, 290,291,292,293,294,295,296119, 291,292,293,294,295,296,297,298,299,300120, 287,288,289,290,291Og, 283,284Lv, 279,280,281Fl, 275,276Cn, 271,272,273Ds, 294120, 268,269Hs, 264,265Sg, 281Fl(α); calculated T1/2; deduced an improved Gamow-like (IMGL) formula parameters. Comparison with available data.

doi: 10.1016/j.nuclphysa.2022.122528
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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 202,204,206,208,210,212,214,216,218Po, 204,206,208,210,212,214,216,218,220Rn, 206,208,210,212,214,216,218,220,222Ra(α); calculated formation probability values, contour plots within a multistep model.

doi: 10.1016/j.physletb.2021.136063
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2021WA29      Chin.Phys.C 45, 044111 (2021)

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

An improved semi-empirical relationship for cluster radioactivity

RADIOACTIVITY 212,214Po, 236,238Pu, 222,224,226Ra, 228,230Th, 230,232,234,236U, 242Cm, 213Po, 215At, 221Fr, 221,223Ra, 225Ac, 231Pa, 233,235U(α), 226Th(14C), (18O), 232Th, 230,236U(24Ne), 232Th, 236U(26Ne), 232,233,235U(28Mg), 237Np(30Mg), 240Pu, 241Am(34Si); calculated preformation factors P of the cluster radioactivity and α-decay, T1/2. Comparison with available data.

doi: 10.1088/1674-1137/abe112
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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 T1/2. 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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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 56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74Ca; 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 Tz and Tz2 using SLy4 interaction. 15O, 15N; 17F, 17O; 39Ca, 39K; 41Sc, 41Ca; calculated ΔNSA 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,162,163Re, 164m,165,165m,166,166m,167,167mIr, 169,170,170m,171m,173Au, 177,177m,178,179Tl, 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, 144,145,146,147,147mTm, 150,150m,151,151mLu, 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, 165,166,167,168,169Ir, 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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2015DO02      Phys.Rev. C 91, 034315 (2015)

J.Dong, W.Zuo, J.Gu

Constraints on neutron skin thickness in 208Pb and density-dependent symmetry energy

NUCLEAR STRUCTURE 208Pb; calculated neutron skin thickness and density dependence of symmetry energy based on a high linear correlation between skin thickness and the symmetry energy coefficient of nuclear matter at saturation density. Discussed measurement issues of skin thickness using novel Pb radius experiment (PREX).

doi: 10.1103/PhysRevC.91.034315
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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+Tw 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 270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302Ds, 272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304Cn, 274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306Fl, 276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308Lv, 278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310Og, 284,286,288,290,292,294,296,298,300,302,304,306,308,310,312120(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 105,106,107,108,109,110Te, 108,109,110,111,112I, 109,110,111,112,113Xe, 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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2013DO01      Phys.Rev. C 87, 014303 (2013)

J.Dong, W.Zuo, J.Gu

Origin of symmetry energy in finite nuclei and density dependence of nuclear matter symmetry energy from measured α-decay energies

NUCLEAR STRUCTURE 208Pb; symmetry energy distribution, isospin asymmetry distribution function, polarizations of neutron and proton densities using the Skyrme-energy density functional and Hartree-Fock approach; deduced neutron skin thickness from experimental α-energies, and compared with other methods.

doi: 10.1103/PhysRevC.87.014303
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2013GU31      Phys.Rev. C 88, 044325 (2013)

X.Guan, K.D.Launey, J.Gu, F.Pan, J.P.Draayer

Level statistical properties of the spherical mean-field plus standard pairing model

NUCLEAR STRUCTURE 48,49,50,51,52,53Ca; calculated level spacing distribution, spectral rigidity, statistical energy spectra. 42,43,44,45,46,47,48,49,50,51,52Ca; calculated pairing gap and compared with experimental data. Spherical mean-field plus standard pairing model calculations, with pairing strength deduced from experimental data. Comparison with Gaussian orthogonal ensemble (GOE) predictions, and Poisson distribution.

doi: 10.1103/PhysRevC.88.044325
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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 32,34,36,38,40,42,44,46,48,50,52,54,56Ar; 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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2012DO02      Phys.Rev. C 85, 034308 (2012)

J.Dong, W.Zuo, J.Gu, U.Lombardo

Density dependence of the nuclear symmetry energy constrained by mean-field calculations

NUCLEAR STRUCTURE 208Pb; calculated neutron skin thickness relation to saturation density, slope parameter, curvature parameter, properties of neutron stars, based on mean-field interactions. Comparison with previous studies.

doi: 10.1103/PhysRevC.85.034308
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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 106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn; 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 1d5/2 and 1d3/2 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 40,42,44,46,48,50,52,54,56,58,60,62,64,66,68Ca; 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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2010DO10      Phys.Rev. C 81, 064309 (2010)

J.Dong, W.Zuo, J.Gu, Y.Wang, B.Peng

α-decay half-lives and Qα values of superheavy nuclei

RADIOACTIVITY 271Sg, 270,272,274Bh, 275Hs, 274,275,276,278Mt, 279Ds, 278,279,280,282Rg, 281,283,284,285,287Cn, 281,282,283,284,286,288Nh, 285,286,287,288,289,291Fl, 286,287,288,289,290,292Mc, 289,290,291,292,293,295Lv, 293,294,295Ts, 294,295Og(α); calculated Q(α) and half-lives using Unified Fission Model (UFM). Comparison with experimental data.

doi: 10.1103/PhysRevC.81.064309
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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 188,190,192,194,196Hg; 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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2010GU22      Nucl.Phys. A844, 245c (2010)

J.-A.Gu

Dark energy crisis

doi: 10.1016/j.nuclphysa.2010.05.043
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2010SH12      Phys.Rev. C 82, 014306 (2010), Erratum Phys.Rev. C 91, 029902 (2015)

S.Shen, G.Han, S.Wen, F.Pan, J.Zhu, J.Gu, J.P.Draayer, X.Wu, L.Zhu, C.He, G.Li, B.Yu, T.Wen, Y.Yan

High-spin states and level structure in 84Rb

NUCLEAR REACTIONS 70Zn(18O, 3np), E=75 MeV; measured Eγ, Iγ, γγ-coin, DCO. 84Rb; deduced levels, J, π, multipolarities, bands, configurations, kinematic moments of inertia. Total Routhian surface calculations. Comparison with projected shell-model calculations, and with structures of 80,82Rb.

doi: 10.1103/PhysRevC.82.014306
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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, 226,228,230,232Th, 228,230,232,234,236,238U, 234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 244,246,248,250,252Cf, 248,250,252Fm, 252No(α); calculated branching ratios, T1/2 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, T1/2 of α-decays of the ground and rotational bands. Generalized Liquid Drop Model (GLDM).

doi: 10.1142/S0218301310016442
Citations: PlumX Metrics


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 164,166,168,170,172,174Dy; 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
Citations: PlumX Metrics


2008GU19      Int.J.Mod.Phys. E17, Supplement 1, 292 (2008)

J.Gu

Random matrix theory and its application to the decay out of a superdeformed band

doi: 10.1142/S0218301308011938
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2008SH15      Int.J.Mod.Phys. E17, 1061 (2008)

S.Shen, Y.Li, J.Gu, F.Xu, T.Wen, Y.Liu, Y.Yang

New levels and transitions in 72Ge observed in the 72As(β+ +EC)72Ge decay

RADIOACTIVITY 72As(β+), (EC) [from 72Ge(p, n), E=16 MeV]; measured Eγ, Iγ, log ft. 72Ge; deduced levels, J, π.

doi: 10.1142/S0218301308010118
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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 112,114,116,118,120,122,124Sn, 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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2007SH35      Eur.Phys.J. A 32, 149 (2007)

S.Shen, K.Fang, J.Gu, Q.Liu, F.Xu

Decay of 1.643 h 95Ru and its daughter's level structure

RADIOACTIVITY 95Ru(β+), (EC) [from 92Mo(α, n), E=17 MeV]; measured Eγ, Iγ, γγ-coinc. 95Tc deduced levels, J, π. Compared results to model calculations.

doi: 10.1140/epja/i2007-10382-9
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Data from this article have been entered in the XUNDL database. For more information, click here.


2006GU13      Phys.Rev. C 73, 055803 (2006)

J.Gu, H.Guo, X.Li, Y.Liu, F.Xu

Antikaon condensation and deconfinement phase transition in neutron stars

doi: 10.1103/PhysRevC.73.055803
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2006GU27      Eur.Phys.J. A 30, 455 (2006)

J.F.Gu, H.Guo, X.G.Li, Y.X.Liu, F.R.Xu

Phase transition to color-flavor-locked matter and condensation of Goldstone bosons in neutron star matter

doi: 10.1140/epja/i2006-10142-5
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2005LI02      Chinese Physics 14, 95 (2005)

Y.Li, S.-F.Shen, S-H.Shi, J.-H.Gu, J.-Y.Liu, H.Xu

New levels and transitions in 72Ge following the decay of 72Ga

RADIOACTIVITY 72Ga(β-) [from 71Ga(n, γ)]; measured β-delayed Eγ, Iγ, γγ-coin; deduced log ft. 72Ge deduced levels, J, π, β-feeding intensities.

doi: 10.1088/1009-1963/14/1/018
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2005LI09      Chinese Physics 14, 487 (2005)

Y.Li, S.-F.Shen, J.-H.Gu, S.-H.Shi, J.-Y.Liu

A study on the decay of 72As

RADIOACTIVITY 72As(EC) [from 72Ge(p, n)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 72Ge deduced levels, J, π.

doi: 10.1088/1009-1963/14/3/027
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2005SH03      J.Phys.Soc.Jpn. 74, 299 (2005)

S.Shen, Y.Li, S.Shi, J.Gu, J.Liu

New Low-Spin Levels in 72Ge and Discussion of Its Yrast Band Structure

RADIOACTIVITY 72Ga(β-) [from 71Ga(n, γ)]; measured β-delayed Eγ, Iγ, γγ-coin; deduced log ft. 72Ge deduced levels, J, π, β-feeding intensities.

doi: 10.1143/JPSJ.74.299
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2005SH59      High Energy Phys. and Nucl.Phys. (China) 29, 139 (2005)

S.-F.Shen, Y.Li, J.-H.Gu

New Low-Spin Levels in 76Se and Discussion of Its Yrast Band Structure


2004LI62      Int.J.Mod.Phys. E13, 933 (2004)

Y.Li, S.Shen, W.Huang, S.Shi, J.Gu, J.Liu, H.Xu

Low-spin states of 76Se excited in 76Br(β+ + EC)76Se decay

RADIOACTIVITY 76Br(EC), (β+) [from 75As(α, 3n) and 76Se(p, n)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 76Se deduced levels, J, π, configurations.

doi: 10.1142/S0218301304002600
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2004SH17      J.Phys.Soc.Jpn. 73, 1180 (2004)

S.Shen, Y.Li, W.Huang, S.Shi, J.Gu, J.Liu, H.Xu

Decay of 76Br and Its Daughter's Level Structure

RADIOACTIVITY 76Br(β+), (EC) [from 75As(α, 3n) and 76Se(p, n)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 76Se deduced levels, J, π, branching ratios. Comparison with projected shell model calculations.

doi: 10.1143/JPSJ.73.1180
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2004SH18      Prog.Theor.Phys.(Kyoto) 111, 721 (2004)

S.Shen, J.Gu, W.Shen, Z.Xing, Z.Zhu

On the Mechanism of Signature Inversion in the Doubly Odd Nuclei 80, 82Rb

NUCLEAR STRUCTURE 80,82Rb; calculated levels, J, π, configurations, rotational bands; deduced signature inversion mechanism. Angular momentum projected shell model.

doi: 10.1143/PTP.111.721
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2003SH03      Phys.Lett. B 554, 115 (2003)

S.Shen, J.Gu, S.Shi, J.Liu, J.Zhou, W.Shen

Signature inversion caused by shape change in 84Rb

NUCLEAR STRUCTURE 84Rb; calculated rotational bands levels, J, π, configurations; deduced change in deformation. Angular momentum projected shell model, comparisons with data.

doi: 10.1016/S0370-2693(03)00002-9
Citations: PlumX Metrics


2003ZH06      Eur.Phys.J. A 16, 299 (2003)

L.Zhang, K.Morita, Q.Y.Hu, A.Yoshida, J.H.Zhao, Z.K.Li, J.W.Zheng, Y.H.Pu, H.Kudo, H.Wei, C.F.Wang, H.M.Fan, J.N.Gu, Y.Yano

A new measurement of 208Tl levels

RADIOACTIVITY 208Hg(β-) [from Pb(18O, X)]; measured Eγ, Iγ, γγ-coin. 208Tl deduced levels, β-feeding intensities. Comparison with shell model predictions.

doi: 10.1140/epja/i2002-10129-2
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Data from this article have been entered in the XUNDL database. For more information, click here.


2002GU03      Nucl.Phys. A697, 611 (2002)

P.Guazzoni, L.Zetta, J.N.Gu, A.Vitturi, Y.Eisermann, G.Graw, R.Hertenberger, M.Jaskola

Structure of the 89Zr via the High-Resolution 91Zr(p, t)89Zr Reaction and Shell-Model Calculations

NUCLEAR REACTIONS 91Zr(p, t), E=25 MeV; measured σ(E, θ). 89Zr deduced levels, L, π. DWBA analysis, shell-model calculations. Q3D spectrometer.

doi: 10.1016/S0375-9474(01)01271-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0932. Data from this article have been entered in the XUNDL database. For more information, click here.


2002GU27      Phys.Rev. C 66, 054312 (2002)

J.Gu, L.Gao, B.Hu

Finite size effect on the strength function in a random matrix analysis

doi: 10.1103/PhysRevC.66.054312
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2002LI41      Appl.Radiat.Isot. 57, 399 (2002)

Y.Li, S.Shen, S.Shi, J.Gu, X.Yu, J.Liu, J.Zeng

A Decay Study of 70As

RADIOACTIVITY 70As(EC), (β+) [from 70Ge(p, n)]; measured Eγ, Iγ, γγ-coin. 70Ge deduced levels, J, π.

doi: 10.1016/S0969-8043(02)00126-4
Citations: PlumX Metrics


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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2001SH07      Acta Phys.Pol. B32, 183 (2001)

S.Shen, Z.Wang, S.Shi, J.Gu, J.Liu, Z.Zhu

Study of One-Quasiproton Bands of 129La using the Projected Shell Model

NUCLEAR STRUCTURE 129La; calculated levels, J, π, rotational bands. Projected shell model, comparison with data.


2001SH15      J.Radioanal.Nucl.Chem. 247, 241 (2001)

S.Shen, K.Fang, J.Liu, J.Gu, S.Shi, Y.Li

Decay of 1.643-hr 95Ru to 95Tc

RADIOACTIVITY 95Ru(EC) [from 92Mo(α, n)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 95Tc deduced levels, J, π.

doi: 10.1023/A:1006780930371
Citations: PlumX Metrics


2000GU20      Acta Phys.Pol. B31, 417 (2000)

P.Guazzoni, L.Zetta, M.Jaskola, J.N.Gu, A.Vitturi, Y.Eisermann, G.Graw, R.Hertenberger, G.Staudt

High Resolution Measurement of the 91Zr(p, t)89Zr Reaction

NUCLEAR REACTIONS 91Zr(p, t), E=25 MeV; measured σ(E, θ). 89Zr deduced levels, J, π, configurations. High-resolution measurement. Shell model calculations.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0932.


2000SH48      J.Radioanal.Nucl.Chem. 246, 423 (2000)

S.Shen, J.Liu, J.Gu, X.Yu, Y.Li, D.Yin, S.Shi

188Os Low Excited Levels

RADIOACTIVITY 188Re(β-); measured Eγ, Iγ(t), γγ-coin; deduced β-branching ratios. 188Os deduced levels, J, π.

doi: 10.1023/A:1006728104225
Citations: PlumX Metrics


2000SH49      Eur.Phys.J. A 9, 463 (2000)

S.Shen, X.Yu, S.Shi, J.Gu, J.Liu, Y.Li, Z.Zhu

Decay of 83Sr and Level Structure of 83Rb

RADIOACTIVITY 83Sr(β+), (EC) [from 85Rb(p, 3n)]; measured Eγ, Iγ, γγ-coin. 83Rb deduced levels, J, π, branching ratios, log ft. Comparison with shell model calculations.

doi: 10.1007/s100500070004
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2000SH51      High Energy Phys. and Nucl.Phys. (China) 24, 306 (2000)

S.-F.Shen, Y.Li, S.-H.Shi, J.-H.Gu, J.-Y.Liu, K.-M.Fang, J.-Z.Zhou

Study of 101 Mo Decay


2000YU03      Int.J.Mod.Phys. E9, 471 (2000)

X.Yu, S.Shi, J.Gu, J.Liu, W.Li, S.Shen, Y.Li

Low-Spin States of 83Rb Excited in the 83Sr(β+ + EC)83Rb Decay

RADIOACTIVITY 83Sr(β+), (EC) [from 85Rb(p, 3n)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 83Rb deduced levels, J, π. Radiochemical separation.

doi: 10.1142/S0218301300000350
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1999FA20      High Energy Phys. and Nucl.Phys. (China) 23, 820 (1999)

K.Fang, J.Liu, S.Shi, J.Gu, J.Zeng, X.Yu, S.Shen, Y.Li

Decay of 95Ru


1999GU14      J.Phys.(London) G25, B1 (1999)

J.N.Gu, C.H.Zhang, A.Vitturi

Shell Model Treatment of the Structure of Light Neutron-Rich Nuclei

NUCLEAR STRUCTURE 11Li, 11Be, 12,13,14B; calculated levels, J, π, μ, Q. Shell model. Comparison with data.

doi: 10.1088/0954-3899/25/6/701
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1999LI56      High Energy Phys. and Nucl.Phys. (China) 23, 320 (1999)

Y.Li, J.Gu, X.Yu, J.Liu, Y.Cao, J.Zeng, W.Li, S.Shi

Study of the Low Excited States of 72Ge


1999WU01      Phys.Rev. C59, 215 (1999)

X.Wu, J.Gu, A.Iwamoto

Statistical Properties of Quasiparticle Spectra in Deformed Nuclei

NUCLEAR STRUCTURE Cf; calculated quasiparticle level spacing distributions vs deformation; deduced statistical properties, pairing effect.

doi: 10.1103/PhysRevC.59.215
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1999ZH32      Phys.Rev. C60, 054316 (1999)

C.-H.Zhang, S.-J.Wang, J.-N.Gu

Shell Model Studies of Nuclei with A = 92-98

NUCLEAR STRUCTURE 92,93,94,95Mo, 95Tc, 94,95,96Ru, 96,97,98Pd, 92,94Zr; calculated levels, J, π, configurations. Partition truncation method, comparisons with data.

doi: 10.1103/PhysRevC.60.054316
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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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1998GU07      Eur.Phys.J. A 1, 365 (1998)

P.Guazzoni, M.Jaskola, L.Zetta, J.N.Gu, A.Vitturi, G.Graw, R.Hertenberger, P.Schiemenz, B.Valnion, U.Atzrott, G.Staudt

Study of the 90Zr(p(pol), α)87Y Reaction at 22 MeV

NUCLEAR REACTIONS 90Zr(polarized p, α), E=22 MeV; measured σ(θ), A(y)(θ) vs excitation energy. 87Y deduced levels, J, π. Distorted wave analysis, shell-model calculations.

doi: 10.1007/s100500050071
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0919.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1998JA20      Acta Phys.Pol. B29, 385 (1998)

M.Jaskola, P.Guazzoni, L.Zetta, J.N.Gu, A.Vitturi, G.Graw, R.Hertenberger, B.Valnion, F.Nuoffer, G.Staudt

A Study of the 90Zr(p, t) 88Zr Reaction

NUCLEAR REACTIONS 90Zr(p, t), (p, p), E=25 MeV; measured reaction products, Ep, Ip; deduced σ(θ), level energies, J, π. DWBA theory using double folding triton potential, comparison with shell model calculations.


1998YU07      High Energy Phys. and Nucl.Phys. (China) 22, 1082 (1998)

X.Yu, S.Shi, J.Gu, J.Liu, W.Li, J.Zeng, J.Tian, Y.Li, J.Zhou

Low-lying level structure of 83Rb


1998ZH23      Phys.Rev. C58, 851 (1998)

C.-H.Zhang, S.-J.Wang, J.-N.Gu

Independent Nucleon-Pair Motion and Homologous Structure in Nuclei with A ∼ 150

NUCLEAR STRUCTURE 148,149,150,151,152Dy, 148Gd, 150,151,152Er, 149Tb, 151Ho, 153Tm; calculated levels, J, π; deduced independent nucleon pair motion, related features. Shell model, weak coupling scheme. Comparison with data.

doi: 10.1103/PhysRevC.58.851
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1997GU01      Z.Phys. A356, 381 (1997)

P.Guazzoni, M.Jaskola, L.Zetta, J.Gu, A.Vitturi, G.Graw, R.Hertenberger, D.Hofer, P.Schiemenz, B.Valnion, U.Atzrott, G.Staudt, G.Cata-Danil

Spectroscopy of 88Y Homologous Levels

NUCLEAR REACTIONS 91Zr(polarized p, α), E=22 MeV; measured σ(θ), spectra, analyzing power vs θ; deduced model parameters. 88Y deduced levels, J, π, configuration. Shell model.

doi: 10.1007/s002180050193
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0398.


1997GU06      Phys.Rev. C55, 2395 (1997)

J.N.Gu, A.Vitturi, C.H.Zhang, P.Guazzoni, L.Zetta, G.Graw, M.Jaskola, G.Staudt

Homologous States and the Structure of Nuclei in the Lead Region

NUCLEAR STRUCTURE 206Pb, 205Tl; calculated levels. 206Pb deduced homologoue state to 205Tl parent states. Shell model.

doi: 10.1103/PhysRevC.55.2395
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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
Citations: PlumX Metrics


1997GU29      Acta Phys.Hung.N.S. 6, 111 (1997)

J.N.Gu, C.H.Zhang, A.Vitturi

The Structure of 11Be

NUCLEAR STRUCTURE 11Be; calculated levels, J, π; deduced ground state parity inversion. Phenomenological shell model.


1997WU09      Phys.Rev.Lett. 79, 4542 (1997)

X.Wu, J.Gu, Y.Zhuo, Z.Li, Y.Chen, W.Greiner

Possible Understanding of Hyperdeformed 144-146Ba Nuclei Appearing in the Spontaneous Fission of 252Cf

NUCLEAR STRUCTURE 252Cf; calculated level spacings vs deformation during fission process; deduced statistical properties, hyperdeformed daughter nucleus formation.

RADIOACTIVITY 252Cf(SF); calculated level spacings vs deformation during fission process; deduced statistical properties, hyperdeformed daughter nucleus formation.

doi: 10.1103/PhysRevLett.79.4542
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1996XU03      Phys.Rev. C54, 1481 (1996)

S.Xu, Y.Xie, Q.Pan, Y.Luo, C.Zhang, J.Zhang, Y.Wang, X.Zhang, J.Gu, Y.Ge, X.Yin, C.Wang, Z.Xing, X.Chen

Low Lying States in 153Ho and 157Tm from Electron Capture and β+ Decay of 153Er and 157Yb

RADIOACTIVITY 153Er, 157Yb(β+), (EC); analyzed data; deduced log ft, I(EC+β+). 153Ho, 157Tm deduced levels, J, π.

NUCLEAR STRUCTURE 153Ho, 157Tm; calculated levels, band structure. Shell model.

doi: 10.1103/PhysRevC.54.1481
Citations: PlumX Metrics


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.


1995YU01      Z.Phys. A352, 235 (1995)

S.Yuan, W.Yang, W.Mou, X.Zhang, Z.Li, X.Yu, J.Gu, Y.Guo, Z.Gan, H.Liu, J.Guo

A New Isotope of Protactinium: 239Pa

NUCLEAR REACTIONS U(18O, X), E=50 MeV/nucleon; measured Eγ, Iγ, γγ(X-ray)-coin, γγ(X-ray)(t); deduced evidence for 239Pa.

RADIOACTIVITY 239Pa(β-) [from U(18O, X), E=50 MeV/nucleon]; measured Eγ, Iγ, γγ(X-ray)-coin, γγ(X-ray)(t); deduced T1/2. 239U deduced transitions.

doi: 10.1007/BF01289491
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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.


1992GU18      Chin.J.Nucl.Phys. 14, No 4, 337 (1992)

J.Gu, Y.Ling

Applications of Lie Algebra in the Local Potential Method

NUCLEAR STRUCTURE 240Pu; calculated fission rate. Lie algebra based propagator, solution of Fokker-Planck equation.


1992SH12      Z.Phys. A342, 369 (1992)

S.Shi, W.D.Huang, Y.Li, D.Z.Yin, J.H.Gu, J.Q.Tian

Identification of a New Neutron Rich Isotope 202Pt

NUCLEAR REACTIONS 204Hg(n, n2p), E=fast; measured Eγ, Iγ, decay curve; deduced evidence for 202Pt.

RADIOACTIVITY 202Pt(β-) [from 204Hg(n, n2p), E=fast]; measured Eγ, Iγ, decay curve; deduced T1/2.

doi: 10.1007/BF01291520
Citations: PlumX Metrics


1986WA34      Chin.J.Nucl.Phys. 8, 57 (1986)

Wang Gongqing, Zhu Jiabi, Tao Zhenlan, Zheng Wanhui, Gu Jiahui

Electron Capture Decay and Isomer Transition of 91mNb

RADIOACTIVITY 91mNb(EC), (IT) [from 89Y(α, 2n), E=32 MeV]; measured Eγ, Iγ, T1/2; deduced log ft. 91Zr deduced transition γ multipolarity, I(ce) ratio, ICC. Ge(Li) detector, chemical separation.


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Note: The following list of authors and aliases matches the search parameter J.Gu: , J.A.GU, J.F.GU, J.H.GU, J.N.GU, J.Q.GU, J.Z.GU