NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = W.Ye Found 52 matches. 2024YE01 Phys.Rev. C 109, L021603 (2024) Odd-even stagger in dissipative fission of excited nuclear systems
doi: 10.1103/PhysRevC.109.L021603
2023WA19 Phys.Lett. B 843, 138010 (2023) Stringent constraints on nuclear dissipation by second-chance survival probability RADIOACTIVITY 231,232Cf, 229,230Cm, 215,216U(SF); calculated fission barriers, second-chance survival probabilities in the framework of the dynamical Langevin equation coupled to a statistical model of particle emission; deduced a new and sensitive observable the friction strength β. Comparison with available data.
doi: 10.1016/j.physletb.2023.138010
2023YE03 Phys.Rev. C 107, 044302 (2023) Multiple constraints on nuclear mass formulas for reliable extrapolations ATOMIC MASSES 160Nd, 164Sm; calculated binding energies. Multiobjective optimization of the Bethe-Weizsacker–type and the Duflo-Zucker (DZ) mass models usingα-decay energy and the Garvey-Kelson relations. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.044302
2022YE01 Nucl.Phys. A1024, 122477 (2022) Effects of isospin and shell on probing nuclear dissipation with survival probabilities of heavy systems NUCLEAR STRUCTURE 228,234,240U; calculated the survival probability using the Langevin model. Comparison with available data.
doi: 10.1016/j.nuclphysa.2022.122477
2022YE02 Phys.Rev. C 106, 024318 (2022) Accuracy versus predictive power in nuclear mass tabulations ATOMIC MASSES Z=8-120, N=8-256; calculated masses, S(2n) of even-even by the multi-objective optimization (MOO)-constrained Dulfo-Zuker model (DZ10) formulas with possible Pareto front (PF) solutions, and compared with AME2020 evaluation. 208Pb; calculated slope parameter and the neutron skin thickness using the symmetry energy coefficient of the DZ10 mass formula after the multi-objective optimization.
doi: 10.1103/PhysRevC.106.024318
2022YE03 Phys.Rev. C 106, 034603 (2022) Isospin effect on first-chance fission probability NUCLEAR STRUCTURE 220,230,240U, 240Cm; calculated first-chance fission probability as a function of the presaddle dissipation strength at 45 evin model calculations. NUCLEAR REACTIONS 206Pb(32S, X)238Cf, E=193.2 MeV; 206Pb(28Si, X)234Cm, E=172.6 MeV; 204Pb(26Mg, X)230Pu, E=143.9 MeV; 184W(40Ar, X)224U, E=202.6 MeV; 204Pb(30S, X)234Cf, E=174.2 MeV; 204Pb(26Si, X)230Cm, E=151 MeV; calculated first-chance fission probability as a function of the presaddle dissipation strength. Stochastic Langevin model calculations.
doi: 10.1103/PhysRevC.106.034603
2021WA13 Phys.Rev. C 103, 024611 (2021) Fission cross sections of heavy nuclei as a probe of nuclear dissipation NUCLEAR STRUCTURE 226,234,242U, 190,200,210Tl; calculated lowering of fission cross sections caused by friction with respect to its standard statistical-model value as a function of the presaddle dissipation strength, fission barriers as function of angular momentum for 226,234,242U using dynamical Langevin equations. Relevance to fission cross sections for high-isospin and low-spin heavy fissioning systems by light radioactive nuclear beams.
doi: 10.1103/PhysRevC.103.024611
2021YE01 Phys.Rev. C 104, 064308 (2021) Refining the nuclear mass model via the α decay energy ATOMIC MASSES A=100-275; analyzed difference between experimental values and theoretical evaluations obtained from the Duflo-Zuker DZ10 mass model for three different kinds of parameters, corresponding correspond to Q(α) and the binding energies for heavy nuclei above A=100. 208Pb; deduced symmetry energy coefficient in the equation of state (EOS), and neutron skin thickness.
doi: 10.1103/PhysRevC.104.064308
2018WA02 Phys.Rev. C 97, 014603 (2018) Probing nuclear dissipation with first-chance fission probability NUCLEAR REACTIONS 235U(3He, F)238Pu*, E=41.9 MeV; 235U(α, F)239Pu*, E=66.4 MeV; 239Pu(3He, F)242Cm*, E=42.8 MeV; 239Pu(α, F)243Cm*, E=67.3 MeV; 241Am(3He, F)244Bk*, E=43.1 MeV; 241Am(α, F)245Bk*, E=67.6 MeV; 248Cm(3He, F)251Cf*, E=42.9 MeV; 248Cm(α, F)252Cf*, E=67.3 MeV; calculated average angular momentum contributing to fission using fusion spin distribution formula and the scaling formulas for critical angular momentum and diffuseness for fusion. 220Th, 240Cf; calculated influence of dissipation on first-chance fission probability as a function of the presaddle friction strength at excitation energies of 50 MeV and 80 MeV for 220Th and 240Cf. Stochastic Langevin model.
doi: 10.1103/PhysRevC.97.014603
2018WA27 Phys.Rev. C 98, 034614 (2018) Probing postsaddle dissipation with light-particle multiplicity of hot heavy nuclear systems NUCLEAR STRUCTURE 240Am; calculated proton, neutron, and α-particle multiplicity as a function of postsaddle dissipation strength and angular momenta, for fission of compound nucleus 240Am at an angular momentum of 40 units and at excitation energies of E*=60, 120, and 250 MeV, and fission barrier strength. Dynamical Langevin equations coupled to a statistical decay model.
doi: 10.1103/PhysRevC.98.034614
2017TI02 Phys.Rev. C 95, 041601 (2017) Constraining presaddle dissipation with fission cross sections of light nuclear systems NUCLEAR STRUCTURE 205Bi, 215Fr, 225Pa, 230Np; calculated drop of fission cross sections over the statistical model values at different angular momenta and excitation energies using stochastic Langevin model.
doi: 10.1103/PhysRevC.95.041601
2017UM01 Phys.Rev. C 96, 024625 (2017) Transport properties of isospin asymmetric nuclear matter using the time-dependent Hartree-Fock method NUCLEAR REACTIONS 208Pb(78Kr, X), (92Kr, X), E=8.5 MeV/nucleon; calculated impact parameter and energy-loss dependence of relevant observables, neutron and proton numbers transferred to and from the projectile-like fragments (PLFs), neutron and proton numbers of the PLFs as a function of impact parameter and the angle representing initial orientation of deformed projectile with respect to the beam axis, deflection functions, final kinetic energy versus the scattering angle for the reactions, sticking time as a function of impact parameter, N/Z values for PLFs and target-like fragments (TLFs) as a function of energy loss, (N-Z)/A values of primary PLFs and TLFs as function of contact time between the collision partners, distribution of PLF neutron and proton numbers in the N-Z plane, percent of total excitation energy carried by the PLFs as a function of energy loss. Time-dependent density-constrained Hartree-Fock (TDHF) method in full three dimensions.
doi: 10.1103/PhysRevC.96.024625
2016TI05 Phys.Rev. C 94, 021601 (2016) Isospin effect on probing nuclear dissipation with fission cross sections NUCLEAR REACTIONS 208Pb, 209Bi(p, F), E*=60-210 MeV; calculated fission cross sections at different friction strengths using stochastic Langevin model; deduced isospin effects. Comparison with experimental data. 195,202,209Bi; calculated dynamical drop of fission cross sections at excitation energies of 50-200 MeV.
doi: 10.1103/PhysRevC.94.021601
2016TI07 Chin.Phys.C 40, 094103 (2016) Effect of pre-equilibrium emission on probing postsaddle nuclear dissipation with neutrons NUCLEAR REACTIONS 238U(18O, X)256Fm, E=159 MeV; 208Pb(40Ar, X)248Fm, E=249 MeV; calculated neutron multiplicity, α-particle binding energies using deformation parameters of heavy fissioning systems 248,256Fm.
doi: 10.1088/1674-1137/40/9/094103
2016YE01 Phys.Rev. C 93, 044603 (2016) Probing postsaddle nuclear dissipation with excitation energy at scission NUCLEAR REACTIONS 238U(16O, F)254Fm*, E=288 MeV; 238U(18O, F)256Fm*, E=159 MeV; 159Tb(20Ne, F)179Re*, E=8-16 MeV/nucleon; calculated excitation energy at scission, prescission neutron multiplicity and compared to experimental data. 238U(16O, F)254Fm*, E=288 MeV; calculated postsaddle neutron multiplicity as a function of postsaddle dissipation strength. 246Cf at E(*)=50, 80, 180 MeV; calculated postsaddle neutron multiplicity, excitation energy at scission versus postsaddle friction strength. Stochastic Langevin model coupled with statistical decay model. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.044603
2015TI01 Chin.Phys.C 39, 034102 (2015) Langevin analysis of fission excitation functions induced by protons NUCLEAR REACTIONS 206Pb, 209Bi(p, F), E<200 MeV; analyzed available data; deduced fits to measured excitation function data of fission σ.
doi: 10.1088/1674-1137/39/3/034102
2015YE01 Phys.Rev. C 91, 064603 (2015) Spallation reaction versus heavy-ion fusion: Fission excitation functions as a fundamental probe of presaddle nuclear dissipation NUCLEAR STRUCTURE 224Th; calculated drop of fission σfdrop as function of presaddle dissipation strength in spallation and heavy-ion fusion reactions for the production of 224Th compound nucleus at E(*)=100-300 MeV and angular momentum l=10-30 ~h. Comparison of dynamical drop of fission cross section relative to statistical-model values. Combination of dynamical Langevin equations with a statistical decay model (CDSM).
doi: 10.1103/PhysRevC.91.064603
2014YE07 Phys.Rev. C 90, 041604 (2014) Probing nuclear dissipation with particle multiplicity in heavy-ion-induced light fissioning systems NUCLEAR STRUCTURE 200Pb, 251Es; calculated postsaddle multiplicities and change in binding energies of neutrons, protons, and α particles as a function of deformation parameter and angular momentum at excitation energy 120 MeV for 200Pb and 70 MeV for 251Es in the framework of Langevin models coupled to a statistical decay model.
doi: 10.1103/PhysRevC.90.041604
2013WA14 Phys.Rev. C 87, 051601 (2013) Exploring postsaddle nuclear dissipation with light-particle multiplicity at high energy NUCLEAR REACTIONS 232Th(19F, X)251Es*, E=100-140 MeV; 232Th (20Ne, X)252Fm*, E=215 MeV; 197Au(18O, X)215Fr*, E=159 MeV; 238U(18O, X)256Fm*, E=159 MeV; 208Pb(40Ar, X)248Fm*, E=249 MeV; 197Au(16O, X)213Fr*, E=288 MeV; 184W(16O, X)200Pb*, E=288 MeV; analyzed prescission neutron yields, and multiplicities of neutrons, protons, and α particles as function of postsaddle friction strength. Stochastic Langevin equation coupled with a statistical decay model.
doi: 10.1103/PhysRevC.87.051601
2013YE01 Phys.Rev. C 87, 014610 (2013) Significant role of level-density parameters in probing nuclear dissipation with light-ion-induced fission excitation functions NUCLEAR REACTIONS 197Au, 208Pb(3He, X), E*=50-150 MeV; analyzed fission σ(E), presaddle neutron probability. Bohr-Wheeler theory and Langevin approach.
doi: 10.1103/PhysRevC.87.014610
2013YE07 Phys.Rev. C 88, 054606 (2013) Roles of system size and excitation energy in probing nuclear dissipation with giant dipole resonance γ rays NUCLEAR STRUCTURE 200Pb, 224Th, 240Cf; calculated presaddle multiplicity of neutrons and GDR γ rays, multiplicities of postsaddle neutrons, protons and α particles, change of postsaddle GDR γ multiplicity Mγ as function of postsaddle friction β at different excitation energies of the fissioning system. Stochastic Langevin equation coupled to a statistical model of particle emission.
doi: 10.1103/PhysRevC.88.054606
2012YE01 Phys.Rev. C 85, 011601 (2012) Spallation reactions induced by high energy protons: A possible way to probe dissipation in nuclear fission with excitation energy at scission NUCLEAR STRUCTURE 200Hg; calculated excitation energy at scission of the compound nucleus at E*=100, 350, 450 MeV, negative entropies, level density parameters, evaporated multiplicities of prescission neutrons and protons and α particles. Stochastic dynamical approach to the fission process, Langevin model.
doi: 10.1103/PhysRevC.85.011601
2012YE08 Phys.Rev. C 86, 034605 (2012) Robustness of the excitation energy at scission as a novel probe of nuclear dissipation at high energy NUCLEAR STRUCTURE 194,200,206Hg, 200Rn, 240Cf; calculated excitation energy of compound nuclei at scission, evaporated multiplicities of prescission neutrons, protons and α particles, fission barriers, emission barriers of protons and α particles of the fissioning systems. Langevin model with statistical description of particle evaporation from fissioning compound nuclei.
doi: 10.1103/PhysRevC.86.034605
2011YE01 Nucl.Phys. A853, 61 (2011) Fissility effects on evaporation residue spin distributions NUCLEAR STRUCTURE 190Os, 210Po; calculated pre-scission multiplicities of neutrons, protons and α particles, pre-saddle multiplicities of neutrons, and evaporation residue spin distributions using dynamical Langevin model. Comparison with 175Os and 193Po. Fission of compound nuclei at high excitation energies and angular momenta and role of fissility and pre-saddle friction strength.
doi: 10.1016/j.nuclphysa.2011.01.023
2011YE02 Phys.Rev. C 83, 044611 (2011) Excitation energy and nuclear dissipation probed with evaporation-residue cross sections NUCLEAR STRUCTURE 200Hg; calculated σ for excess of evaporation residues over standard-statistical values versus dissipation strength at different excitation energies and low- and high-angular momentum values, and ratio of level density parameter at saddle to that at ground-state configurations from 200Hg compound nucleus using dynamical Langevin equations with a statistical decay model.
doi: 10.1103/PhysRevC.83.044611
2011YE04 Phys.Rev. C 84, 034617 (2011) Heavy-ion versus 3He/4He fusion-fission reactions: Angular momentum dependence of dissipation in nuclear fission NUCLEAR REACTIONS 181Ta(16O, F)197Tl, 197Au(3He, F)200Tl, 197Au(α, F)201Tl, E=60-140 MeV; analyzed precision neutron yields, spin distributions, negative entropies using Stochastic Langevin model. Comparison with fission width formula. Dependence on angular momentum, and nonaxiality in the study of the nuclear fission process.
doi: 10.1103/PhysRevC.84.034617
2010YE01 Phys.Rev. C 81, 011603 (2010) Significant role of fissility in evaporation residue cross sections as a probe of presaddle nuclear dissipation NUCLEAR STRUCTURE 175,190Os, 193,210Po; calculated multiplicities of precission and presaddle neutrons and α particles, dynamical excess of residue cross sections, fission barriers using Langevin model calculations. Discussed effects of fissility in presaddle nuclear dissipation. Fission of compound nuclei at high excitation energies and angular momenta.
doi: 10.1103/PhysRevC.81.011603
2010YE04 Phys.Rev. C 81, 054609 (2010) Significant role of deformation in probing postsaddle nuclear dissipation with light particle emission RADIOACTIVITY 240Cf(SF); calculated binding energies, emission barrier, neutron, proton and α multiplicities, GDR γ multiplicity using a one-dimensional Langevin model.
doi: 10.1103/PhysRevC.81.054609
2010YE05 Chin.Phys.C 34, 45 (2010) Surveying post-saddle nuclear dissipation with protons and α particles as probes NUCLEAR STRUCTURE 234,240,246Cf, 240U; calculated post-saddle proton and α-particle multiplicities, fission barriers; deduced isospin dependence. Langevin model.
doi: 10.1088/1674-1137/34/1/008
2009YE01 Phys.Rev. C 79, 031601 (2009) Isospin effects on neutrons as a probe of nuclear dissipation NUCLEAR STRUCTURE 240,246,252Cf, 240U; calculated excess prescission neutron multiplicity as a function of postsaddle dissipation strength, fission barriers in the framework of dynamical Langevin equation coupled with statistical decay model. Comparisons with standard statistical models.
doi: 10.1103/PhysRevC.79.031601
2009YE02 Phys.Rev. C 80, 011601 (2009) Isospin effects on light charged particles as probes of nuclear dissipation RADIOACTIVITY 234,240,246Cf, 240U(SF); calculated postsaddle dissipation strengths and neutron, proton and α multiplicities in the framework of a dynamical Langevin model coupled with a statistical decay model.
doi: 10.1103/PhysRevC.80.011601
2008YE01 Phys.Rev. C 77, 011302 (2008) Isospin effects on the evaporation residue spin distribution NUCLEAR REACTIONS 184W(16O, X)200Pb, E=84, 92, 100, 108, 116, 120 MeV; calculated evaporation residue spin distributions, emitted neutrons. 194,206Pb, 200Os; calculated evaporation residue spin distributions.
doi: 10.1103/PhysRevC.77.011302
2007YE01 Phys.Lett. B 647, 118 (2007) Isospin effect on pre-scission γ emission NUCLEAR STRUCTURE 200Os, 194,200,206Pb; calculated pre-scission γ and particle multiplicities from excited nuclei, viscosity dependence; deduced isospin effect. Langevin equation.
doi: 10.1016/j.physletb.2007.01.065
2007YE03 Phys.Rev. C 76, 021604 (2007); Erratum Phys.Rev. C 77, 029904 (2008) Effect of isospin on the evaporation residue cross section NUCLEAR STRUCTURE 194,200,206Pb; calculated excess of evaporation residue cross sections, excess of presaddle neutrons and fission barrier distributions using a combination of Langevin equation and a statistical decay model.
doi: 10.1103/PhysRevC.76.021604
2007YE04 Phys.Rev. C 76, 041601 (2007); Erratum Phys.Rev. C 77, 029903 (2008) Significant role of angular momentum in probing nuclear dissipation NUCLEAR STRUCTURE 200Pb; calculated role of angular momentum in CDSM model, evaporation residue, cross section, nuclear dissipation strength.
doi: 10.1103/PhysRevC.76.041601
2006YE01 J.Phys.(London) G32, B7 (2006) Deformation effects on the isospin dependence of particle emission NUCLEAR STRUCTURE 178Pb; calculated pre-scission neutron, proton, and α multiplicities from excited nucleus, deformation and viscosity dependence. Diffusion model.
doi: 10.1088/0954-3899/32/5/B01
2004YE02 J.Phys.(London) G30, B21 (2004) Influence of excitation energy and angular momentum on the isospin dependence of particle emission NUCLEAR STRUCTURE 189,202,212Po, 202Fr, 202Tl; calculated pre-scission particle multiplicity vs excitation energy and angular momentum.
doi: 10.1088/0954-3899/30/7/B02
2003YE01 Chin.Phys.Lett. 20, 482 (2003) Influence of Neutron Shell Closure (Nc=126) on Prescission Particle Emission of Fissioning Systems 216, 224Th NUCLEAR STRUCTURE 216,224Th; calculated pre-scission neutron multiplicities vs excitation energy, spin; deduced shell effects.
doi: 10.1088/0256-307X/20/4/312
2003YE04 J.Phys.(London) G29, 2125 (2003) Shell effects on pre-scission particle emission NUCLEAR STRUCTURE 132Sn, 208Pb; calculated pre-scission particle emission multiplicity vs excitation energy, angular momentum; deduced shell effects.
doi: 10.1088/0954-3899/29/9/308
2003YE05 Prog.Theor.Phys.(Kyoto) 109, 933 (2003) Isospin Effect on Pre-Scission Particle Emission NUCLEAR STRUCTURE 189,202,212Po, 202Tl, 202Fr, 110,117,124In, 110Tc, 110Pd; calculated pre-scission particle multiplicities from excited compound nuclei; deduced isospin effects. Smoluchowski equation.
doi: 10.1143/PTP.109.933
2003YE06 Eur.Phys.J. A 18, 571 (2003) Effects of the N/Z of fissioning systems on the multiplicity of pre-scission particles NUCLEAR STRUCTURE 189,202,212Po, 202Tl, 202Fr; calculated pre-scission neutron, proton, and α multiplicities vs excitation energy, angular momentum, viscosity coefficient. NUCLEAR REACTIONS 168Er, 181Ta(20Ne, X), E=148 MeV; 164,170Er(28Si, X), E=132-168 MeV; 170Er(30Si, X), E=158 MeV; calculated pre-scission neutron multiplicities. Comparison with data.
doi: 10.1140/epja/i2003-10100-9
2003YE07 Int.J.Mod.Phys. E12, 817 (2003) Influence of isospin on prescission particle emission of light fissioning systems NUCLEAR STRUCTURE 110Tc, 110Pd, 110,117,124In; calculated prescission particle multiplicity from excited nuclei; deduced isospin effects. Diffusion model.
doi: 10.1142/S0218301303001600
1998CA23 Phys.Rev. C58, 572 (1998) X.Cai, J.Feng, W.Shen, Y.Ma, J.Wang, W.Ye In-Medium Nucleon-Nucleon Cross Section and Its Effect on Total Nuclear Reaction Cross Section NUCLEAR REACTIONS 12C, 27Al(12C, X), E=10-1000 MeV/nucleon; 12C(Li, X), (Be, X), E=790 MeV/nucleon; calculated reaction σ; deduced medium effects. Phenomenological model, Coulomb-modified Glauber model. Comparisons with data.
doi: 10.1103/PhysRevC.58.572
1998CA37 Chin.Phys.Lett. 15, 642 (1998) Y.-H.Cai, J.-S.Wang, W.-Q.Shen, Y.-G.Ma, J.Feng, W.Ye, X.-Z.Cai, D.-Q.Fang Study of Giant Dipole Resonance of Super Heavy Compound System NUCLEAR REACTIONS 197Au(197Au, X), U(Xe, X), E not given; calculated GDR γ spectra vs temperature; deduced residual interaction role, deformation effects. Microscopic semiclassical approach.
doi: 10.1088/0256-307X/15/9/007
1997SH31 Phys.Rev. C56, 1996 (1997) W.Q.Shen, W.Ye, Y.G.Ma, J.Feng, J.S.Wang, K.Yuasa-Nakagawa, T.Nakagawa, K.Yoshida, J.Kasagi, Y.Futami, S.M.Lee, K.Furutaka, K.Matsuda Azimuthal Distribution, Azimuthal Correlation, and Reaction Plane Dispersion in the Reaction of 10.6 MeV/nucleon 84Kr on 27Al NUCLEAR REACTIONS 27Al(84Kr, X), E=10.6 MeV/nucleon; measured proton σ(θ) vs fragment mass, pp(φ), pα(φ), αα(φ) vs fragment mass; deduced correlation coefficients, reaction mechanism features.
doi: 10.1103/PhysRevC.56.1996
1997YE05 Z.Phys. A359, 385 (1997) W.Ye, W.Q.Shen, Z.D.Lu, J.Feng, Y.G.Ma, J.S.Wang, K.Yuasa-Nakagawa, T.Nakagawa Angular Momentum Effect in Prescission Particle Multiplicities for a Light System by Diffusion Model NUCLEAR REACTIONS 84Kr(27Al, F), E=10.6 MeV/nucleon; 56Fe(58Ni, F), E=10 MeV/nucleon; 109Ag(16O, F), E=18 MeV/nucleon; calculated prescission particle emission multiplicity; deduced angular momentum dependence.
doi: 10.1007/s002180050418
1988YA04 Chin.J.Nucl.Phys. 10, 166 (1988) Yan Yiming, Zhou Hongyu, Tang Lin, Wen Chenlin, Zhang Shengji, Hua Ming, Ding Xiaoji, Rong Yaning, Liu Shuzhen, Fu Jingquan, Lu Ting, Wang Qi, Sun Suxu, Lan Liqiao, Xu Jinkui, Wang Wanhong, Yang Hua, Han Chongzhan, He Peilun, Ye Wenxiang, Han Xiuqing A Facility for Measurements of γ-Ray Production Cross Sections from (n, xγ) Reactions using the Pulsed Neutron Source NUCLEAR REACTIONS 56Fe(n, n'γ), E=14.9 MeV; measured γγ(t), nγ(t); deduced γ production σ. Pulsed beam. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30904. 1987YU02 Chin.J.Nucl.Phys. 9, 316 (1987) Yuan Haiji, Ye Weilei, Gao Qin, Shen Qingbiao, Zhuo Yizhong Microscopic Calculations of Single-Particle Spreading Width II. In Finite Nuclei NUCLEAR STRUCTURE 12C, 16O, 40Ca, 90Zr, 120Sn, 208Pb; calculated single particle spreading widths. Local density approximation.
1986YE01 Chin.J.Nucl.Phys. 8, 15 (1986) Ye Weilei, Yuan Haiji, Gao Qin, Shen Qingbiao, Zhuo Yizhong The Calculations of Charge Density Distribution and Charge Radii for Spherical Nuclei using the Hartree-Fock Method with Skyrme Forces NUCLEAR STRUCTURE 48Ca, 90Zr; calculated levels. 16O, 40,48Ca, 90Zr; calculated charge density distributions. 16O, 28Si, 32S, 40,48Ca, 60Ni, 90Zr, 120Sn; calculated charge rms radii. Hartree-Fock method.
1986YE02 Chin.J.Nucl.Phys. 8, 214 (1986) Ye Weilei, Yuan Haiji, Gao Qin, Zheng Chunkai, Tian Ye, Shen Qingbiao Calculations of Neutron Skin for Spherical Nuclei using the Hartree-Fock Method with Skyrme Forces NUCLEAR STRUCTURE 16O, 28Si, 32S, 40,48Ca, 60Ni, 90Zr, 120Sn; calculated proton, neutron density distributions, rms radii. Hartree-Fock method, Skyrme force.
1985YE02 Chin.J.Nucl.Phys. 7, 166 (1985) Ye Weilei, Yuan Haiji, Gao Qin, Shen Qingbiao, Zhang Jingshang, Liu Ruizhe, Gu Yingqi Hartree-Fock Calculations with Extended Skyrme Force for 16O and 40Ca NUCLEAR STRUCTURE 16O, 40Ca; calculated single particle energies. Hartree-Fock method, extended Skyrme force.
1982YE01 Chin.J.Nucl.Phys. 4, 216 (1982) Ye Wenchuan, Zhao Xuan, Zeng Fanan Edge and Cluster Effects in Precompound Nuclear Reactions NUCLEAR REACTIONS 12C, 54Fe, 209Bi(p, X), (p, p'), E=62 MeV; calculated σ(total), σ(θp'). Intranuclear cascade model, edge, α-cluster effects, Monte Carlo simulation.
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