NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.Zhao Found 112 matches. Showing 1 to 100. [Next]2018WA16 Phys.Rev. C 98, 014615 (2018) B.Wang, W.-J.Zhao, E.-G.Zhao, S.-G.Zhou Theoretical study of the capture of stable 39K and neutron-rich radioactive 46K by 181Ta NUCLEAR REACTIONS 181Ta(39K, X), E=180-210 MeV; 181Ta(46K, X), E=190-215 MeV; calculated capture σ(E) using empirical coupled-channel (ECC) model and the universal fusion function (UFF) prescription; deduced barrier parameters, and fusion functions. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.014615
2017WA02 At.Data Nucl.Data Tables 114, 281 (2017) B.Wang, K.Wen, W.-J.Zhao, E.-G.Zhao, S.-G.Zhou Systematics of capture and fusion dynamics in heavy-ion collisions NUCLEAR REACTIONS 89Y(12C, X), 59Co(14N, X), E(cm)<100 MeV; calculated capture excitation functions by using an empirical coupled-channel (ECC) model for 182<ZpZt<1640. Comparison with available data.
doi: 10.1016/j.adt.2016.06.003
2017ZH05 Phys.Rev. C 95, 014320 (2017) J.Zhao, B.-N.Lu, E.-G.Zhao, S.-G.Zhou Tetrahedral shapes of neutron-rich Zr isotopes from a multidimensionally constrained relativistic Hartree-Bogoliubov model NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114Zr; calculated potential energy curves as function of β20, binding energy and β32 deformation, ground state binding energies, quadrupole deformation β20, axial octupole deformation β30, nonaxial octupole deformation β32, and hexadecapole deformation β40, binding energies for various energy minima for oblate, pear-like, tetrahedral and prolate shapes, neutron and proton single-particle levels near the Fermi surface and pairing energies for 110Zr, potential energy surfaces for A=106-114 Zr isotopes in (β30, β32) plane. Multidimensionally constrained relativistic Hartree-Bogoliubov (MDC-RHB) model with relativistic functionals DD-PC1 and PC-PK1. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.014320
2016WA04 Phys.Rev. C 93, 014615 (2016) B.Wang, W.-J.Zhao, A.Diaz-Torres, E.-G.Zhao, S.-G.Zhou Systematic study of suppression of complete fusion in reactions involving weakly bound nuclei at energies above the Coulomb barrier NUCLEAR REACTIONS 89Y, 124Sn, 144Sm, 169Tm, 181Ta, 187Re, 208Pb, 209Bi(9Be, X), E(cm)=10-55 MeV; 90,96Zr, 154Sm, 159Tb, 197Au, 198Pt, 208Pb, 209Bi(6Li, X), E=10-55 MeV; 159Tb, 165Ho, 197Au, 198Pt, 209Bi(7Li, X), E=10-60 MeV; 159Tb, 209Bi(10B, X), (11B, X), E(cm)=30-80 MeV; calculated complete fusion σ(E). Empirical coupled-channel model with and without breakup effects. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.014615
2015ZH03 Phys.Rev. C 91, 014321 (2015) J.Zhao, B.-N.Lu, D.Vretenar, E.-G.Zhao, S.-G.Zhou Multidimensionally constrained relativistic mean-field study of triple-humped barriers in actinides NUCLEAR STRUCTURE 226,228,230,232Th, 232,234,236,238U; calculated energy curves as function of deformation parameter β20, two dimensional potential energy surfaces (PES) in (β20, β30) plane, odd-even differences of binding energies, excitation energies of the second saddle point, third (hyperdeformed) minimum, and third saddle point, depth of third potential well. Covariant density functional theory (CDFT) with relativistic mean field (MDCRMF) model and nonlinear point-coupling functional PC-PK1 and density-dependent functional DD-ME2, with pairing correlations in BCS approximation.
doi: 10.1103/PhysRevC.91.014321
2014DA13 Phys.Rev. C 90, 044609 (2014) G.-F.Dai, L.Guo, E.-G.Zhao, S.-G.Zhou Dissipation dynamics and spin-orbit force in time-dependent Hartree-Fock theory NUCLEAR REACTIONS 16O(16O, X), E(cm)=40-220 MeV; calculated relative scattering kinetic energy, energy dissipation, separation density profiles, fusion σ. Time-dependent Hartree-Fock (TDHF) theory. Comparison with experimental data and other calculations.
doi: 10.1103/PhysRevC.90.044609
2014LU01 Phys.Rev. C 89, 014323 (2014) B.-N.Lu, J.Zhao, E.-G.Zhao, S.-G.Zhou Multidimensionally-constrained relativistic mean-field models and potential-energy surfaces of actinide nuclei NUCLEAR STRUCTURE 240Pu; calculated potential energy curves as function of deformation and truncations, three-dimensional potential energy surface contours as function of deformation around the ground state, the inner barrier, and fission isomer. 230,232Th, 232,234,236,238,240U, 238,240,242,244,246Pu, 242,244,246,248,250Cm, 250,252Cf; calculated potential energy curves around the ground states and the first and second fission barriers, heights of the first second fission barriers. Multidimensionally-constrained relativistic mean-field (MDC-RMF) models, with the solution of Dirac equation in an axially deformed harmonic oscillator (ADHO) basis. Importance of nonaxial and spatial reflection asymmetric shapes in the study of potential energy surfaces and fission barriers of actinides and Superheavy nuclei. Comparison with available experimental data.
doi: 10.1103/PhysRevC.89.014323
2014LU17 Phys.Scr. 89, 054028 (2014) B.-N.Lu, J.Zhao, E.-G.Zhao, S.-G.Zhou Multidimensionally constrained relativistic mean field model and applications in actinide and transfermium nuclei NUCLEAR STRUCTURE 240Pu; calculated potential energy vs deformation for various selfconsistent symmetries using covariant density functional.
doi: 10.1088/0031-8949/89/5/054028
2014WA07 Phys.Rev. C 89, 037601 (2014) Synthesis of superheavy nuclei with Z=118 in hot fusion reactions NUCLEAR REACTIONS 249,250,251,252Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E(cm)=190-260 MeV; 248Cm(50Ti, 2n), (50Ti, 3n), (50Ti, 4n), (50Ti, 5n), 244Pu(54Cr, 2n), (54Cr, 3n), (54Cr, 4n), (54Cr, 5n), E(cm)=200-280 MeV; calculated evaporation residue σ(E) for formation of Z=118 isotopes. Dinuclear system model with dynamical potential energy surface (DNS-DyPES model). Relevance to production of superheavy elements at JINR-Flerov Laboratory facility.
doi: 10.1103/PhysRevC.89.037601
2014WA36 Phys.Rev. C 90, 034612 (2014) B.Wang, W.-J.Zhao, P.R.S.Gomes, E.-G.Zhao, S.-G.Zhou Systematic study of breakup effects on complete fusion at energies above the Coulomb barrier NUCLEAR REACTIONS 90Zr(6Li, X), E not given; 165Ho, 208Pb(7Li, X), E not given; 144,152Sm, 159Tb, 197Au, 198Pt, 209Bi(6Li, X), (7Li, X), E not given; 89Y, 144Sm, 124Sn, 186W, 208Pb, 209Bi(9Be, X), E not given; 159Tb, 209Bi(10B, X), E not given; 159Tb, 209Bi(11B, X), E not given; 89Y, 152Sm, 159Tb, 181Ta, 208Pb(12C, X), E not given; 159Tb, 181Ta, 207Pb(13C, X), E not given; 103Rh, 148,150Nd, 159Tb, 169Tm(16O, X), E not given; calculated dimensionless complete fusion (CF) functions. Discussed systematics of suppression factors. Comparison with universal fusion functions, and available experimental values. Proposed an analytical formula between the CF suppression factor and the breakup threshold energy.
doi: 10.1103/PhysRevC.90.034612
2013LU11 Phys.Rev. C 88, 024323 (2013) Pseudospin symmetry in single-particle resonances in spherical square wells
doi: 10.1103/PhysRevC.88.024323
2013ZH15 Phys.Rev. C 87, 054308 (2013) Z.-H.Zhang, J.Meng, E.-G.Zhao, S.-G.Zhou Rotational properties of the superheavy nucleus 256Rf and its neighboring even-even nuclei in a particle-number-conserving cranked shell model NUCLEAR STRUCTURE 256Rf, 250Fm, 252,254No; calculated levels, kinematic and dynamic moments of inertia for g.s. rotational band, proton and neutron single-particle levels near the Fermi surface. Cranked shell model (CSM) with pairing correlations treated by a particle-number conserving method. Comparison with experimental data. Discussed effect of high order ϵ6 deformation parameter.
doi: 10.1103/PhysRevC.87.054308
2013ZH16 Phys.Rev. C 87, 054314 (2013) Z.-H.Zhang, P.-W.Zhao, J.Meng, J.-Y.Zeng, E.-G.Zhao, S.-G.Zhou Nuclear superfluidity for antimagnetic rotation in 105Cd and 106Cd NUCLEAR STRUCTURE 105,106Cd; calculated Nilsson levels for protons and neutrons, kinematic moments of inertia, B(E2), angular momentum vectors of neutrons with and without pairing, anti-magnetic rotational bands, shears angle. Cranked shell model with the pairing correlations and particle-number-conserving method. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.054314
2013ZH27 Eur.Phys.J. A 49, 77 (2013) S.-S.Zhang, E.-G.Zhao, S.-G.Zhou Theoretical study of the two-proton halo candidate 17Ne including contributions from resonant continuum and pairing correlations NUCLEAR STRUCTURE 17Ne; calculated two-proton halo candidate density distribution compared to that of 15O core, single-proton resonance orbits, energy, width, occupation probabilities using ACCC (analytical continuation in the coupling constant) within relativistic mean field with resonant BCS.
doi: 10.1140/epja/i2013-13077-8
2012LI11 Phys.Rev. C 85, 024312 (2012) L.Li, J.Meng, P.Ring, E.-G.Zhao, S.-G.Zhou Deformed relativistic Hartree-Bogoliubov theory in continuum NUCLEAR STRUCTURE 20,22,24,26,28,30,32,34,36,38,40,42Mg; calculated binding energy, quadrupole deformation β2, rms radius, neutron Fermi energy, S(2n), neutron density profiles. 42Mg; calculated binding energy, neutron pairing tensor, single neutron levels and density distribution contours of ground state, neutron halo contributions. Deformed relativistic Hartree Bogoliubov (RHB) theory, Woods-Saxon (WS) basis. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.024312
2012LI22 Chin.Phys.Lett. 29, 042101 (2012) L.-L.Li, J.Meng, P.Ring, E.-G.Zhao, S.-G.Zhou Odd Systems in Deformed Relativistic Hartree Bogoliubov Theory in Continuum
doi: 10.1088/0256-307X/29/4/042101
2012LU02 Phys.Rev. C 85, 011301 (2012) Potential energy surfaces of actinide nuclei from a multidimensional constrained covariant density functional theory: Barrier heights and saddle point shapes NUCLEAR STRUCTURE 240Pu, 248Cm; calculated potential energy surfaces. 230,232Th, 232,234,236,238U, 238,240,242,244Pu, 242,244,246,248Cm; calculated inner and outer fission barrier heights. Importance of triaxial and octupole shapes in fission path. Multidimensional constrained covariant density functional theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.011301
2012LU17 Phys.Rev.Lett. 109, 072501 (2012) Pseudospin Symmetry in Single Particle Resonant States
doi: 10.1103/PhysRevLett.109.072501
2012WA12 Phys.Rev. C 85, 041601 (2012) N.Wang, E.-G.Zhao, W.Scheid, S.-G.Zhou Theoretical study of the synthesis of superheavy nuclei with Z=119 and 120 in heavy-ion reactions with trans-uranium targets NUCLEAR REACTIONS 238U, 237Np, 242Pu, 243Am, 248Cm, 249Bk, 249Cf(48Ca, xn)283Cn/282Nh/286Fl/288Mc/292Lv/293Ts/294Og, E(cm)=194.7-211.3 MeV; 249Bk, 249,251Cf(50Ti, xn)295119/296120/298120, E(cm)=220-280 MeV; calculated maximal values of evaporation-residue cross sections. Dinuclear system model with a dynamical potential energy surface (DNS-DyPES). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.041601
2012ZH01 Phys.Rev. C 85, 014324 (2012) Z.-H.Zhang, X.-T.He, J.-Y.Zeng, E.-G.Zhao, S.-G.Zhou Systematic investigation of the rotational bands in nuclei with Z ≈ 100 using a particle-number conserving method based on a cranked shell model NUCLEAR STRUCTURE 240,242,244,246,248,250,252Cm, 242,244,246,248,250,252,254Cf, 244,246,248,250,252,254,256Fm, 246,248,250,252,254,256,258No, 250Bk; calculated quadrupole deformation parameters β2, β4, moment of inertia plots, alignments, occupation probabilities, contribution of neutron and proton major shells to angular momentum alignments. 245Cm, 250Fm; calculated energies of Nilsson orbitals. 241,243,245,247,249Cm, 243,245,247,249,251Cf, 245,247,249,251,253Fm, 247,249,251,253,255No, 243,245,247,249,251Bk, 245,247,249,251,253Es, 247,249,251,253,255Md, 255Lr; calculated bandhead energies of low-lying one-quasiparticle bands, moments of inertia plots of g.s. and excited bands, alignments, occupation probabilities, contribution of neutron and proton major shells to angular momentum alignments. Cranked shell model (CSM), particle-number conserving (PNC) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.014324
2012ZH02 Phys.Rev. C 85, 014325 (2012) H.F.Zhang, Y.Gao, N.Wang, J.Q.Li, E.G.Zhao, G.Royer Double magic nuclei for Z>82 and N>126 NUCLEAR STRUCTURE Z=101-118, N=140-194; calculated binding energies, Q(α). Z=101-129, N=162, 184; calculated S(p), Q(α) using Macroscopic-microscopic model (MMM). 270Hs, 298Fl; calculated potential energy in the constrained relativistic mean-field (CRMF) theory with effective interaction NL3. Comparison with experimental data. RADIOACTIVITY 269Sg, 274Bh, 273Hs, 278Mt, 277,281Ds, 282Rg, 281,285Cn, 285,286Nh, 285,288,289Fl, 289,290Mc, 293,294Ts(α); Z=108, N=148-172(α); Z=114, N=160-190(α); calculated α decay half-lives. Macroscopic-microscopic model (MMM). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.014325
2012ZH45 Phys.Rev. C 86, 057304 (2012) J.Zhao, B.-N.Lu, E.-G.Zhao, S.-G.Zhou Nonaxial-octupole Y32 correlations in N=150 isotones from multidimensional constrained covariant density functional theories NUCLEAR STRUCTURE 246Cm, 248Cf, 250Fm, 252No; calculated quadrupole, non-axial octupole and hexadecapole deformations, binding energies, single-particle levels near the Fermi surface for protons and neutrons. Multidimensional constrained covariant density functional theories with DD-PC1 parameter set. Comparison with experimental data. Nonaxial reflection-asymmetric (β32 octupole) effects.
doi: 10.1103/PhysRevC.86.057304
2011DO19 Chin.Phys.Lett. 28, 122401 (2011) Nuclear Dynamical Quadrupole Deformations in Heavy-Ion Reactions NUCLEAR REACTIONS 48Ca(40Ca, X), E(cm)=60 MeV; 90Zr(40Ca, X), E(cm)=108 MeV; calculated quadrupole deformations and energies for projectile and target nuclei; deduced prolate deformation parameters. Quantum molecular dynamics model.
doi: 10.1088/0256-307X/28/12/122401
2011LU16 Phys.Rev. C 84, 014328 (2011) Quadrupole deformation (β, γ) of light Λ hypernuclei in a constrained relativistic mean field model: Shape evolution and shape polarization effect of the Λ hyperon NUCLEAR STRUCTURE 10,11,12,13,14,15,16,17,18,19,20,21,22,23C; calculated binding energies, rms radii, β and γ deformation parameters, potential-energy surfaces (PES) for hypernuclei. 26,27Mg, 22,23,24,25,26,27,28,29,30,31,32,33,34,35Si; calculated potential energy surfaces (PES) for hypernuclei. Constrained relativistic mean field model with PK1-Y1 and NLSH-A parameter sets.
doi: 10.1103/PhysRevC.84.014328
2011ZH03 Phys.Rev. C 83, 011304 (2011) Z.Zhang, J.Zeng, E.Zhao, S.Zhou Particle-number conserving analysis of rotational bands in 247, 249Cm and 249Cf NUCLEAR STRUCTURE 247,249Cm, 249Cf; analyzed rotational bands, moments of inertia and alignments and their variations with the rotational frequency, level crossings and upbendings using cranked-shell model with the pairing correlations treated by particle-number conserving method (PNC-CSM). Role of the intruder proton (N=6) i13/2 proton orbitals and absence of alignment of j15/2 neutrons discussed. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.011304
2011ZH55 J.Phys.:Conf.Ser. 312, 092067 (2011) S.G.Zhou, J.Meng, P.Ring, E.G.Zhao Neutron halo in deformed nuclei from a relativistic Hartree-Bogoliubov model in a Woods-Saxon basis NUCLEAR STRUCTURE 44Mg; calculated density distribution, neutron halo using fully self-consistent deformed Hartree-Bogoliubov model in spherical Woods-Saxon basis.
doi: 10.1088/1742-6596/312/9/092067
2010LI11 Int.J.Mod.Phys. E19, 359 (2010) L.-L.Li, S.-G.Zhou, E.-G.Zhao, W.Scheid A new barrier penetration formula and its application to α-decay half-lives NUCLEAR STRUCTURE Z=52-84, A=106-206; calculated Coulomb barrier; deduced barrier penetration formula. Comparison with WKB method.
doi: 10.1142/S0218301310014790
2010WA15 Chin.Phys.Lett. 27, 062502 (2010) N.Wang, L.Dou, E.-G.Zhao, W.Scheid Nuclear Hexadecapole Deformation Effects on the Production of Super-Heavy Elements NUCLEAR REACTIONS 209Bi(58Fe, X)267Mt, 208Pb(64Ni, X)272Ds, 209Bi(70Zn, X)279Nh, 209Bi(74Ge, X)283Mc, 208Pb(86Se, X)294Lv, 208Pb(90Kr, X)298Og, E not given; calculated interaction and driving potentials, fusion probabilities; deduced impact of nuclear hexadecapole deformation for production of super-heavy elements.
doi: 10.1088/0256-307X/27/6/062502
2010YU04 Nucl.Phys. A834, 97c (2010) Z.Yu, G.-Z.Liu, M.-F.Zhu, Y.Xu, E.-G.Zhao Thermal neutron stars including the hyperon-hyperon interactions
doi: 10.1016/j.nuclphysa.2010.01.029
2010ZH10 Phys.Rev. C 81, 044313 (2010) S.S.Zhang, L.G.Cao, U.Lombardo, E.G.Zhao, S.G.Zhou Isospin-dependent pairing interaction from nuclear matter calculations
doi: 10.1103/PhysRevC.81.044313
2010ZH23 Phys.Rev. C 82, 011301 (2010) S.-G.Zhou, J.Meng, P.Ring, E.-G.Zhao Neutron halo in deformed nuclei NUCLEAR STRUCTURE 36,38Ne, 44Mg; calculated proton and neutron density distributions, densities of the neutron core and neutron halo, single neutron levels for the core using deformed relativistic Hartree Bogoliubov (DRHB) theory. Halo phenomenon in deformed nuclei.
doi: 10.1103/PhysRevC.82.011301
2009HE02 Nucl.Phys. A817, 45 (2009) X.-t.He, Z.-z.Ren, S-x.Liu, E.-g.Zhao Influence of high-j intruder orbitals in odd mass transfermium nuclei 253No and 251Md NUCLEAR STRUCTURE 251Md, 253No; calculated rotational band properties, configurations using a cranked shell model and comparison with data.
doi: 10.1016/j.nuclphysa.2008.12.003
2009LI55 Phys.Rev. C 80, 064607 (2009) L.L.Li, Z.H.Li, E.G.Zhao, S.G.Zhou, W.Zuo, A.Bonaccorso, U.Lombardo Isospin splitting of the nucleon-nucleus optical potential NUCLEAR REACTIONS 28Si, 90Zr, 208Pb(n, n)(p, p), (n, γ), (p, γ), E<100 MeV; calculated volume term of the optical model potential and isospin splitting using the Brueckner-Hartree-Fock approach with three-body force.
doi: 10.1103/PhysRevC.80.064607
2009YU08 Chin.Phys.C 33, Supplement 1, 70 (2009) Z.Yu, G.-Z.Liu, M.-F.Zhu, W.-B.Ding, E.-G.Zhao Thermal protoneutron stars with hyperons
doi: 10.1088/1674-1137/33/S1/023
2008BA52 Eur.Phys.J. A 38, 287 (2008) T.Bao, G.-Z.Liu, E.-G.Zhao, M.-F.Zhu Self-consistently thermodynamic treatment for strange quark matter in the effective mass bag model
doi: 10.1140/epja/i2008-10682-6
2008SH26 Int.J.Mod.Phys. E17, Supplement 1, 66 (2008) C.W.Shen, Y.Abe, D.Boilley, G.Kosenko, E.Zhao Isospin dependence of reactions 48Ca+243-251Bk NUCLEAR REACTIONS 243,244,245,246,247,248,249,250,251Bk(48Ca, X), E(cm)=203.3 MeV; calculated fusion σ. Two-step model, KEWPIE code.
doi: 10.1142/S0218301308011768
2008WA02 Chin.Phys.Lett. 25, 77 (2008) Shell Correction and Pairing Energies in the Dinuclear System Model NUCLEAR REACTIONS 208Pb(76Ge, X), (86Kr, X), E not given; calculated fusion probabilities, compound nuclei survival probability, and evaporation residue cross sections.
doi: 10.1088/0256-307X/25/1/022
2008WA20 Phys.Rev. C 78, 054607 (2008) Orientation effects of deformed nuclei on the production of superheavy elements NUCLEAR REACTIONS 208Pb(58Fe, X), (70Zn, X), (82Se, X), (86Kr, X), E=10-18 MeV; calculated potential energy surfaces, interaction potentials, σ, fission barriers. Dinuclear system model.
doi: 10.1103/PhysRevC.78.054607
2008ZH03 Phys.Rev. C 77, 014312 (2008) L.Zhang, S.-G.Zhou, J.Meng, E.-G.Zhao Real stabilization method for nuclear single-particle resonances NUCLEAR STRUCTURE 120Sn; calculated excitation energies and level widths using Relativistic Mean Field theory.
doi: 10.1103/PhysRevC.77.014312
2008ZH27 Int.J.Mod.Phys. E17, 1937 (2008) E.G.Zhao, N.Wang, Z.Q.Feng, J.Q.Li, S.G.Zhou, W.Scheid The isotopic and nuclear orientation effects on the production of super-heavy elements NUCLEAR REACTIONS 208Pb(48Ca, X), (56Fe, X), (70Zn, X), (82Se, X), (86Kr, X), E not given; 236,237,238,239,240,241,242,243,244Pu(48Ca, X), E not given; calculated fusion evaporation cross sections for super heavy element formations.
doi: 10.1142/S021830130801091X
2007LI22 Phys.Rev. C 75, 048801 (2007) B.Liu, M.Di Toro, V.Greco, C.W.Shen, E.G.Zhao, B.X.Sun Application of density dependent parametrization models to asymmetric nuclear matter
doi: 10.1103/PhysRevC.75.048801
2007PE30 Phys.Rev. C 76, 044326 (2007) J.C.Pei, F.R.Xu, Z.J.Lin, E.G.Zhao α-decay calculations of heavy and superheavy nuclei using effective mean-field potentials RADIOACTIVITY 166,168,170,172,174,176,178,180,182Pt, 172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194,210Pb, 188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 210,212,214,216,218,220,222,224,226,228,230Th, 218,220,222,224,226,228,230,232,234,236U, 228,230,232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 254,256,258Rf, 258,260,262Sg, 264,266,270Hs, 270Ds, 286,288Fl, 292Lv, 294Og(α); calculated half-lives, deformation parameters, α-clustering spectroscopic factors, comparisons with experimental half-lives.
doi: 10.1103/PhysRevC.76.044326
2007WA23 Chin.Phys.Lett. 24, 2219 (2007) N.Wang, J.-Q.Li, E.-G.Zhao, Z.-Q.Feng Nuclear Potential and Fusion Cross Sections for Synthesizing Super-Heavy Elements in Di-nuclear Systems NUCLEAR REACTIONS 208Pb(54Cr, X), (58Fe, X), (64Ni, X), (82Se, X), E not given; calculated interaction potentials, fusion probability and evaporation residue cross sections using a double folding method with simplified Skyrme type nucleon-nucleon interaction.
doi: 10.1088/0256-307X/24/8/018
2007ZH35 Phys.Rev. C 76, 034312 (2007) X.-R.Zhou, H.-J.Schulze, H.Sagawa, C.-X.Wu, E.-G.Zhao Hypernuclei in the deformed Skyrme-Hartree-Fock approach NUCLEAR STRUCTURE 7,8,9,10Be, 8,9,10,11B, 11,12,13C, 27,28Si, 50,51V, 88,89Y, 207,208Pb; calculated binding energies and deformation parameters using a deformed Hartree-Fock approach for Λ hypernuclei.
doi: 10.1103/PhysRevC.76.034312
2006GE03 J.Phys.(London) G32, 573 (2006) The stability and the shape of the heaviest nuclei NUCLEAR STRUCTURE Z=101-120; calculated binding energies, deformation parameters. Relativistic mean-field model, comparison with other models.
doi: 10.1088/0954-3899/32/4/013
2006GU16 Int.J.Mod.Phys. E15, 1141 (2006) L.Guo, F.Sakata, E.-G.Zhao, J.A.Maruhn To what extent does the self-consistent mean-field exist?
doi: 10.1142/S0218301306004739
2006HE18 Eur.Phys.J. A 28, 265 (2006) X.T.He, S.G.Zhou, J.Meng, E.G.Zhao, W.Scheid Test of spin symmetry in anti-nucleon spectra NUCLEAR STRUCTURE 40Ca, 90Zr, 124Sn, 208Pb; calculated radial wave functions of antineutron spin doublets. Relativistic mean-field model.
doi: 10.1140/epja/i2006-10066-0
2006HE28 Int.J.Mod.Phys. E15, 1823 (2006) Study of parity doublets in odd-A nuclei NUCLEAR STRUCTURE 221,223Ra; calculated parity doublet rotational bands level energies. Di-nuclear system model.
doi: 10.1142/S0218301306005332
2006LI09 Nucl.Phys. A768, 80 (2006) M.Liu, N.Wang, Z.Li, X.Wu, E.Zhao Applications of Skyrme energy-density functional to fusion reactions spanning the fusion barriers NUCLEAR REACTIONS 92Zr(12C, X), E(cm) ≈ 24-48 MeV; 70,72,73,74,76Ge, 92Zr, 112Cd, 144Nd, 144,147,148,149,150,154Sm, 166Er, 186W, 208Pb, 232Th(16O, X), E(cm) ≈ 30-160; 144Sm(17O, X), E(cm) ≈ 50-100 MeV; 197Au, 208Pb(19F, X), E(cm) ≈ 70-150 MeV; 70,72,73,74,76Ge(27Al, X), E(cm) ≈ 45-65 MeV; 28Si, 92Zr, 178Hf(28Si, X), E(cm) ≈ 20-150 MeV; 186W(30Si, X), E(cm) ≈ 105-165 MeV; 175Lu(31P, X), E(cm) ≈ 100-150 MeV; 154Sm, 181Ta, 182W(32S, X), E(cm) ≈ 120-200 MeV; 90,92Zr(33S, X), E(cm) ≈ 70-100 MeV; 54Fe, 92Zr(35Cl, X), E(cm) ≈ 50-100 MeV; 90Zr(50Ti, X), E(cm) ≈ 90-130 MeV; 64Ni(132Sn, X), E(cm) ≈ 140-180 MeV; analyzed fusion excitation functions, fusion barrier features. Extended semi-classical Thomas-Fermi method, suppression and enhancement effects discussed.
doi: 10.1016/j.nuclphysa.2006.01.011
2006LI35 J.Phys.(London) G32, 1143 (2006) W.Li, N.Wang, F.Jia, H.Xu, W.Zuo, Q.Li, E.Zhao, J.Li, W.Scheid Particle transfer and fusion cross-section for super-heavy nuclei in dinuclear system NUCLEAR REACTIONS 208Pb(70Zn, X), E* ≈ 10 MeV; calculated fusion probability, angular momentum dependence, related features. Other compound nuclei discussed.
doi: 10.1088/0954-3899/32/8/006
2006ZH45 Int.J.Mod.Phys. E15, 1813 (2006) R.R.Zheng, S.Q.Zhu, Y.C.Yang, J.Y.Zeng, S.X.Liu, E.G.Zhao Angular momentum projection after variation for cranking shell model
doi: 10.1142/S0218301306005393
2005GU04 Phys.Rev. C 71, 024315 (2005) Applicability of self-consistent mean-field theory NUCLEAR STRUCTURE 66Se; calculated binding energy, deformation, related features. Analytic condition for applicability of self-consistent mean-field theory derived.
doi: 10.1103/PhysRevC.71.024315
2005GU14 Nucl.Phys. A753, 136 (2005) L.Guo, J.Meng, E.-G.Zhao, F.Sakata Rotational damping in a multi-j shell particles-rotor model
doi: 10.1016/j.nuclphysa.2005.02.106
2005HE01 Eur.Phys.J. A 23, 217 (2005) X.T.He, S.X.Liu, S.Y.Yu, J.Y.Zeng, E.G.Zhao The i13/2 proton intruder orbital and the identical superdeformed bands in 193, 194, 195Tl NUCLEAR STRUCTURE 193,194,195Tl; calculated superdeformed bands energies, configurations; deduced role of proton blocking. Particle-number-conserving cranked mean-field approach, comparison with data.
doi: 10.1140/epja/i2004-10092-x
2005HE21 Nucl.Phys. A760, 263 (2005) X.T.He, S.Y.Yu, J.Y.Zeng, E.G.Zhao The intruder orbitals in superdeformed bands and alignment additivity of odd-odd nuclei in the A ∼ 190 region NUCLEAR STRUCTURE 191,192,193Tl, 191,193,194Hg; calculated superdeformed bands configurations, moments of inertia, angular momentum alignment. Particle-number-conserving cranked mean field approach.
doi: 10.1016/j.nuclphysa.2005.06.006
2005LI16 Eur.Phys.J. A 24, 223 (2005) Q.Li, W.Zuo, W.Li, N.Wang, E.Zhao, J.Li, W.Scheid Deformation and orientation effects in the driving potential of the dinuclear model NUCLEAR REACTIONS 244Es(28Na, X), 198Hg(74Zn, X), 208Pb(64Ni, X), E not given; calculated Coulomb and nuclear driving potentials, deformation and orientation effects.
doi: 10.1140/epja/i2004-10138-1
2005LI21 Phys.Rev. C 71, 054907 (2005) Σ-/Σ+ ratio as a candidate for probing the density dependence of the symmetry potential at high nuclear densities NUCLEAR REACTIONS 132Sn(132Sn, X), E=1.5, 2.5, 3.5 GeV/nucleon; calculated pion and hyperon yield ratios, role of symmetry potential. Ultrarelativistic quantum molecular dynamics model.
doi: 10.1103/PhysRevC.71.054907
2005ZO03 Phys.Rev. C 72, 035202 (2005) H.-s.Zong, F.-y.Hou, W.-m.Sun, J.-l.Ping, E.-g.Zhao Modified approach for calculating vacuum susceptibility
doi: 10.1103/PhysRevC.72.035202
2004GU13 Nucl.Phys. A740, 59 (2004) Characteristic feature of self-consistent mean-field in level crossing region NUCLEAR STRUCTURE 70,72,74,76Ge; calculated potential energy surfaces, binding energies, deformation parameters, level energies. Constrained Hartree-Fock-Bogoliubov approach, adiabatic assumption.
doi: 10.1016/j.nuclphysa.2004.04.117
2004HE11 Chin.Phys.Lett. 21, 813 (2004) X.-T.He, S.-Y.Yu, S.-X.Liu, Y.-X.Liu, E.-G.Zhao Identical Bands and Alignment in 193, 194Tl NUCLEAR STRUCTURE 193,194Tl; analyzed superdeformed bands moments of inertia, relative alignments; deduced role of blocking in identical band mechanism.
doi: 10.1088/0256-307X/21/5/014
2004LI10 Phys.Rev. C 69, 017601 (2004) Density and temperature dependence of nucleon-nucleon elastic cross section
doi: 10.1103/PhysRevC.69.017601
2004LI32 Chin.Phys.Lett. 21, 636 (2004) W.-F.Li, Z.-Z.Wang, H.-S.Xu, Y.Ma, H.-F.Zhang, W.Zuo, J.-Q.Li, N.Wang, E.-G.Zhao, W.Scheid Odd-Even Effects of the Survival Probability for Superheavy Compound Nuclei NUCLEAR STRUCTURE 284,285,286,287,288,289,290,291Fl; calculated neutron separation energies, fission barriers, survival probability for neutron evaporation; deduced odd-even effects. Statistical model. NUCLEAR REACTIONS 241,242,243Pu(48Ca, X), E not given; calculated driving potential vs mass asymmetry.
doi: 10.1088/0256-307X/21/4/013
2004PA20 Phys.Rev. C 69, 065207 (2004) H.Pang, J.Ping, F.Wang, T.Goldman, E.Zhao High strangeness dibaryons in the extended quark delocalization, color screening model
doi: 10.1103/PhysRevC.69.065207
2004SU13 Phys.Lett. B 589, 83 (2004) Y.Sun, X.-R.Zhou, G.-L.Long, E.-G.Zhao, P.M.Walker Nuclear structure of 178Hf related to the spin-16, 31-year isomer NUCLEAR STRUCTURE 178Hf; calculated levels, J, π, rotational bands, deformation; deduced high-spin isomer features. Projected shell model, comparison with data.
doi: 10.1016/j.physletb.2004.03.066
2004XU04 Phys.Rev.Lett. 92, 252501 (2004) F.R.Xu, E.G.Zhao, R.Wyss, P.M.Walker Enhanced Stability of Superheavy Nuclei Due to High-Spin Isomerism NUCLEAR STRUCTURE Z=100-120; calculated two-quasiparticle excitation energies. 270Ds, 266Hs, 250,256Fm, 254No; analyzed data; deduced level configurations. 256Fm; calculated energy vs deformation. Configuration-constrained potential-energy surface calculations.
doi: 10.1103/PhysRevLett.92.252501
2004ZH36 Phys.Rev. C 70, 048802 (2004) X.-R.Zhou, H.-J.Schulze, E.-G.Zhao, F.Pan, J.P.Draayer Pairing gaps in neutron stars
doi: 10.1103/PhysRevC.70.048802
2004ZO01 Chin.Phys.Lett. 21, 43 (2004) H.-S.Zong, X.-H.Wu, F.-Y.Hou, E.-G.Zhao Explicit and Dynamical Chiral Symmetry Breaking in an Effective Quark-Quark Interaction Model
doi: 10.1088/0256-307X/21/1/013
2003LI59 Europhys.Lett. 64, 750 (2003) W.Li, N.Wang, J.F.Li, H.Xu, W.Zuo, E.Zhao, J.Q.Li, W.Scheid Fusion probability in heavy-ion collisions by a dinuclear-system model NUCLEAR REACTIONS 208Pb(50Ti, X), (54Cr, X), (58Fe, X), (64Ni, X), (68Zn, X), (76Ge, X), (82Ge, X), (82Se, X), (86Kr, X), E* ≈ 11-16 MeV; calculated fusion probabilities, optimal excitation energies. Dinuclear-system model.
doi: 10.1209/epl/i2003-00622-0
2003SU20 Int.J.Mod.Phys. E12, 543 (2003) B.-X.Sun, S.-F.Lu, P.-N.Shen, E.-G.Zhao Relativistic mean-field approximation with density-dependent screening meson masses in nuclear matter
doi: 10.1142/S0218301303001363
2003WA12 Chin.Phys.Lett. 20, 635 (2003) N.Wang, E.-G.Zhao, J.-F.Li, W.-F.Li, H.-S.Xu, W.Zuo, J.-Q.Li Influence of Nuclear Deformation on the Potential Energy Surface in Di-Nuclear Model NUCLEAR REACTIONS 208Pb(54Cr, X), (28Al, X), 227Np(35Al, X), E not given; calculated interaction potentials, deformation effects.
doi: 10.1088/0256-307X/20/5/313
2003WU06 Chin.Phys.Lett. 20, 1702 (2003) Z.-Y.Wu, F.-R.Xu, E.-G.Zhao, C.-K.Zheng Spherical and Deformed Shell Closures in Superheavy nuclei NUCLEAR STRUCTURE 270Hs, 298Fl, 306Og; calculated energy vs deformation. 250,252,254,256Fm, 252,254,256No, 256Rf, 260Sg, 264Hs; calculated binding energies. 270,288Hs, 298Fl, 304120; calculated single-particle levels. 250,252,254,256Fm, 252,254,256No, 256,262Rf, 260,266Sg, 264,266,270Hs, 270,280Ds, 284,286Cn, 288,290,292,298Fl, 292,294Lv, 292,294Og; calculated deformation, α-decay energy, T1/2. Macroscopic-microscopic model, comparisons with data.
doi: 10.1088/0256-307X/20/10/314
2003ZH22 Nucl.Phys. A723, 375 (2003) X.R.Zhou, E.G.Zhao, B.G.Dong, X.Z.Zhang, G.L.Long Collective properties of low-lying octupole excitations in 20882Pb126, 6020Ca40 and 288O20 NUCLEAR STRUCTURE 28O, 60Ca, 208Pb; calculated isoscalar and isovector octupole strength distributions, transition densities, giant resonance features. Self-consistent Hartree-Fock approach, RPA, particle-vibration coupling.
doi: 10.1016/S0375-9474(03)01366-6
2002LI50 Phys.Rev. C66, 024320 (2002) Microscopic mechanism of identical superdeformed bands in 192, 193, 194Hg NUCLEAR STRUCTURE 192,193,194Hg; calculated superdeformed bands moments of inertia, related features; deduced mechanisms for identical band phenomena.
doi: 10.1103/PhysRevC.66.024320
2002SU08 Phys.Rev. C65, 054301 (2002) Perturbative Calculation of the Excluded Volume Effect for Nuclear Matter in a Relativistic Mean-Field Approximation
doi: 10.1103/PhysRevC.65.054301
2002ZH03 Chin.Phys.Lett. 19, 184 (2002) Spectral Statistics in the Cranking Model
doi: 10.1088/0256-307X/19/2/313
2002ZH31 Chin.Phys.Lett. 19, 1274 (2002) X.-R.Zhou, Y.Sun, G.-L.Long, E.-G.Zhao Projected Shell Model Analysis of Multi-Quasiparticle High-K Isomers in 174Hf NUCLEAR STRUCTURE 174Hf; calculated levels, J, π, rotational bands, configurations. Projected shell model, comparison with data.
doi: 10.1088/0256-307X/19/9/317
2002ZO02 Phys.Rev. C66, 015201 (2002) H.-S.Zong, X.-S.Chen, F.Wang, C.-H.Chang, E.-G.Zhao Nonperturbative Aspects of Axial Vector Vertex in the Global Color Symmetry Model
doi: 10.1103/PhysRevC.66.015201
2001JI08 Chin.Phys.Lett. 18, 1571 (2001) H.-Y.Jia, B.-X.Sun, J.Meng, E.-G.Zhao How and When Will a Neutron Star Become a Hyperon Star ?
doi: 10.1088/0256-307X/18/12/309
2001LI25 Phys.Rev. C63, 054314 (2001) Y.-X.Liu, D.Sun, J.-J.Wang, E.-G.Zhao Description of Superdeformed Identical Bands of Odd-A Nuclei in the A ∼ 190 Mass Region NUCLEAR STRUCTURE 191,193Hg, 193Tl; calculated superdeformed bands transition energies, identical bands features. Supersymmetry scheme, comparisons with data.
doi: 10.1103/PhysRevC.63.054314
2000SH31 Chin.Phys.Lett. 17, 488 (2000) C.-W.Shen, Y.-S.Chen, E.-G.Zhao Prediction of Triaxial Superdeformation in the A ∼ 160, 80 Region NUCLEAR STRUCTURE 155,157,159,161Ho, 157,159,161,163Tm, 159,161,163,165,167,169Lu, 163,165,171Ta, 72,74Ni, 76Zn, 76Ge, 78,80Se, 80Kr, 86Zr, 88,90Mo, 90Ru; calculated total Routhian surfaces; deduced deformation parameters, triaxial superdeformation. Cranked mean-field approach.
2000YA17 Nucl.Phys. A675, 379c (2000) Chiral Quark Model with Topological Ghost
doi: 10.1016/S0375-9474(00)00293-1
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
1999JI06 Nucl.Phys. A658, 197 (1999) H.Y.Ji, G.L.Long, E.G.Zhao, S.W.Xu Studies of the Electric Dipole Transition of Deformed Rare-Earth Nuclei NUCLEAR STRUCTURE 152Sm; calculated levels, J, π, B(E1), γ decay relative intensities. 154Sm, 156,158,160Gd, 160,162Dy; calculated levels B(E1), γ decay relative intensities. Interacting Boson Model.
doi: 10.1016/S0375-9474(99)00335-8
1999LI11 Phys.Rev. C59, 2511 (1999) Systematic Description of the Superdeformed Bands of the Odd-A Nuclei in the A = 150 Region NUCLEAR STRUCTURE 147,149Gd, 151Tb, 151,153Dy; calculated superdeformed bands transitions Eγ, moments of inertia; deduced possible mechanism for ΔI=4 bifurcation. Supersymmetry scheme.
doi: 10.1103/PhysRevC.59.2511
1999LO18 Chin.Phys.Lett. 16, 870 (1999) Comprehensive Evidence of Octupole Vibration in 158Gd NUCLEAR STRUCTURE 158Gd; calculated levels J, π, B(E2) for intraband transitions, B(E2), B(E1), and relative intensities for interband transitions. Comparison with data. IBM calculations.
doi: 10.1088/0256-307X/16/12/005
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
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
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
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
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
1998LI02 J.Phys.(London) G24, 117 (1998) Y.Liu, J.Song, H.-Z.Sun, J.-J.Wang, E.-G.Zhao Description of the Turnover of the Dynamical Moment of Inertia of the Superdeformed Nuclear State NUCLEAR STRUCTURE 192,194Hg, 152,154Dy; calculated superdeformed bands transitions energies, dynamic moments of inertia; deduced spin-dependent interaction strength. Interacting boson model. Comparison with data.
doi: 10.1088/0954-3899/24/1/015
1998LO07 Phys.Rev. C57, 2301 (1998) G.L.Long, T.Y.Shen, H.Y.Ji, E.G.Zhao Analytical Expressions for Electromagnetic Transition Rates in the SU(3) Limit of the spdf Interacting Boson Model NUCLEAR STRUCTURE 152,154,156,158Sm, 230,232,234,238U; calculated transitions B(E1), intensities. IBM calculations, analytical expressions.
doi: 10.1103/PhysRevC.57.2301
1998LU10 Phys.Rev. C58, 1195 (1998) X.-F.Lu, Y.-X.Liu, H.-S.Zong, E.-G.Zhao Calculation of Some Properties of π and σ Mesons in the Global Color Symmetry Model
doi: 10.1103/PhysRevC.58.1195
1998LU17 Eur.Phys.J. A 3, 377 (1998) X.-F.Lu, B.S.Zou, H.-M.Ding, Y.-X.Liu, E.-G.Zhao Contribution of the σ Meson Exchange to Pionic Double Charge Exchange Reaction NUCLEAR REACTIONS 14C(π+, π-), E < 300 MeV; calculated forward excitation function; deduced sigma-meson exchange contribution.
doi: 10.1007/s100500050192
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
1997LI21 Phys.Rev. C56, 1370 (1997) Y.-X.Liu, J.-G.Song, H.-Z.Sun, E.-G.Zhao Description of Superdeformed Nuclear States in the Interacting Boson Model NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196,198Pb, 148,150Gd, 152,154Dy; calculated superdeformed states transition energies, rotational properties. Interacting boson model, comparison with experiment.
doi: 10.1103/PhysRevC.56.1370
1997LI28 Chin.Phys.Lett. 14, 641 (1997) Y.-X.Liu, J.-G.Song, H.-Z.Sun, J.-J.Wang, E.-G.Zhao Competition Between Pairing and Anti-Pairing Correlations in the Superdeformed Nuclear States in A ∼ 190 and 150 Ranges NUCLEAR STRUCTURE 152Dy, 192,194Hg; calculated superdeformed bands moments of inertia; deduced pairing, anti-pairing roles. Interacting boson model.
1997MA10 Phys.Rev. C55, 792 (1997) Medium Effects on the Double-Δ Production and Absorption Cross Section
doi: 10.1103/PhysRevC.55.792
1996MA24 Phys.Lett. 378B, 5 (1996) Study of In-Medium ΔΔ Elastic Scattering Cross Section
doi: 10.1016/0370-2693(96)00347-4
1995ZE05 Phys.Rev. C52, 1864 (1995) Two-Parameter Formula for Rotational Spectra NUCLEAR STRUCTURE 174,166,168,170,176Yb, 154Sm, 156Dy, 164,166Er, 168,170,172,174,176,178Hf, 182W, 178Os, 226Ra, 228,230,232Th, 230,232,234,236,238U, 236,238,240,242,244Pu, 248Cm; calculated levels. New two-parameter formula.
doi: 10.1103/PhysRevC.52.1864
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