NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = Zhuo Yizhong Found 41 matches. 1997LI22 Phys.Rev. C56, 1570 (1997) Z.Li, G.Mao, Y.Zhuo, W.Greiner Transition to Δ Matter from Hot, Dense Nuclear Matter within a Relativistic Mean Field Formulation of the Nonlinear σ and ω Model
doi: 10.1103/PhysRevC.56.1570
1997MA10 Phys.Rev. C55, 792 (1997) Medium Effects on the Double-Δ Production and Absorption Cross Section
doi: 10.1103/PhysRevC.55.792
1997WA18 Phys.Rev. C55, 3159 (1997) Running Coupling Constants in the Walecka Model and Renormalization-Group Equations
doi: 10.1103/PhysRevC.55.3159
1997WA26 Z.Phys. A358, 451 (1997) Quark Condensates in Nuclear Matter with Vacuum Effects
doi: 10.1007/s002180050354
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
1996MA19 Phys.Rev. C53, 2933 (1996) Self-Consistent Relativistic Boltzmann-Uehling-Uhlenbeck Equation for the Δ Distribution Function
doi: 10.1103/PhysRevC.53.2933
1996MA24 Phys.Lett. 378B, 5 (1996) Study of In-Medium ΔΔ Elastic Scattering Cross Section
doi: 10.1016/0370-2693(96)00347-4
1996WU03 Phys.Rev. C53, 1233 (1996) X.Wu, F.Sakata, Y.Zhuo, Z.Li, D.D.Nguyen Dynamic Realization of Statistical State in Finite Systems
doi: 10.1103/PhysRevC.53.1233
1995BA47 Z.Phys. A352, 321 (1995) Systematic Studies of Fission Fragment Kinetic Energy Distributrions by Langevin Simulations NUCLEAR STRUCTURE 233Pu, 234Th, 218Pa, 256,254Fm, 239Es; calculated fission fragment kinetic energy, variances; deduced scission condition finite neck radius. Langevin Monte Carlo simulation of fission fluctuation-Dissipation dynamics.
doi: 10.1007/BF01289505
1994BA18 Z.Phys. A347, 217 (1994) Kramers Rate Formula with Coordinate-Dependent Mass NUCLEAR STRUCTURE 248Cf; calculated stationary, time-dependent fission rates vs temperature. 230Th; calculated symmetric fission rate. Kramers rate formula, coordinate-dependent mass.
doi: 10.1007/BF01292379
1994HA30 Phys.Rev. C50, 961 (1994) Effective Nucleon-Nucleon Cross Sections Based on Skyrme Interactions
doi: 10.1103/PhysRevC.50.961
1994LI44 J.Phys.(London) G20, 1829 (1994) Further Studies of the Equilibration Process in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS Ca(Ca, X), 20Ne(20Ne, X), 139La(139La, X), E=1-2 GeV/nucleon; calculated average density time evolution, relativistic collision. Relativistic Boltzmann-Uehling-Uhlenbeck model, local equilibration process.
doi: 10.1088/0954-3899/20/11/011
1994MA09 Z.Phys. A347, 173 (1994) G.Mao, Z.Li, Y.Zhuo, Y.Han, Z.Yu, M.Sano Density and Momentum Dependence of the Coupling Strengths for Scalar and Vector Fields
1994MA22 Phys.Rev. C49, 3137 (1994) G.Mao, Z.Li, Y.Zhuo, Y.Han, Z.Yu Study of In-Medium NN Inelastic Cross Section from Relativistic Boltzmann-Uehling-Uhlenbeck Approach NUCLEAR REACTIONS 1H(p, pπ0), (p, pπ+), E=high; calculated σ. In-medium NN-inelastic σ from relativistic Boltzmann-Uehling-Uhlenbeck approach.
doi: 10.1103/PhysRevC.49.3137
1994MA28 Phys.Lett. 327B, 183 (1994) Medium Effects on the NN Inelastic Cross Section in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 1H(p, pπ0), E not given; calculated σ vs E. In-medium σ(NN → NΔ), relativistic Boltzmann-Uehling-Uhlenbeck approach.
doi: 10.1016/0370-2693(94)90715-3
1994ZH22 Phys.Rev. C50, R2664 (1994) Momentum Dependent Vlasov-Uehling-Uhlenbeck Calculation of Mass Dependence of the Flow Disappearance in Heavy-Ion Collisions
doi: 10.1103/PhysRevC.50.R2664
1994ZH25 Nucl.Phys. A580, 627 (1994) Probing the EOS and nn Cross Section by Analyzing the Collective Flow at High and Intermediate Energy in the RVUU Approach NUCLEAR REACTIONS 51V(40Ar, X), E=80-140 MeV/nucleon; calculated collective flow vs E, σ(NN); deduced effective mass preferred value. Relativistic Vlasov-Uehling-Uhlenbeck approach, Waleckas' quantum hadrodynamics model.
doi: 10.1016/0375-9474(94)90785-4
1993ZH23 Phys.Lett. 318B, 19 (1993) Analysis of Flow Disappearance in the RVUU Approach NUCLEAR REACTIONS 51V(40Ar, X), E=80-140 MeV; calculated in-plane mean fragment transverse momentum rapidity distribution, reduced flow vs E; deduced effective nucleon-nucleon σ. Relativistic Vlasov-Uehling-Uhlenbeck approach.
doi: 10.1016/0370-2693(93)91776-J
1991CA21 Nucl.Sci.Eng. 109, 142 (1991) Comparisons of Global Phenomenological and Microscopic Optical Potentials for Nuclear Data Predictions NUCLEAR REACTIONS 59Co(n, n), (n, n'), E ≤ 20 MeV; calculated σ(E). 59Co(n, n), E=2.47, 8 MeV; calculated σ(θ). 98Mo(n, p), (n, nα), (n, γ), (n, np), (n, α), E=threshold-20 MeV; 100Mo(n, 2n), E ≈ 8.5-20 MeV; calculated σ(E). Optical model from other data analysis.
doi: 10.13182/NSE91-A28513
1991CA26 Chin.J.Nucl.Phys. 13, No 1, 45 (1991) C.Cai, D.Liu, Q.Shen, Y.Tian, Y.Zhuo Comparison between Phenomenological and Microscopic Optical Potential in Nuclear Data Evaluations NUCLEAR REACTIONS 27Al, 31P, S, Cl, K, Ca, Fe, 59Co, Cu, Ag, In, Sb, W, Pb(n, n), E ≈ 0.083-24 MeV; calculated σ. Comparison with data. Different models chi square fits, phenomenological optimal, global and microscopic optical potentials.
1989ZH14 Chin.J.Nucl.Phys. 11, No.3, 39 (1989) Relativistic Microscopic Optical Potentials for Nucleon-Asymmetric Nuclei NUCLEAR REACTIONS 58Ni, 90Zr, 118Sn, 208Pb(polarized p, p), E=65 MeV; 90Zr, 208Pb(polarized p, p), E=80-182 MeV; analyzed σ(θ), polarization observables data. Relativistic microscopic optical potentials.
1988CH46 Chin.J.Nucl.Phys. 10, 320 (1988) Chen Bin, Zhang Jingshang, Lu Zhongdao, Han Huiyi, Zhuo Yizhong Difference of Fission Behaviors at Saddle and Scission Points and the Neutron Multiplicity Prior to Fission NUCLEAR STRUCTURE 240Pu; calculated fission rates neutron multiplicity. Diffusion model.
1988HU13 Chin.J.Nucl.Phys. 10, 314 (1988) Huang Hanchen, Wu Xizhen, Zhuo Yizhong, Han Huiyi Calculation of Potential Energy Surface and Spontaneous Fission Lifetimes of Heavy Nuclei Using Two-Center Shell Model NUCLEAR STRUCTURE 254,256,258Fm, 258No; calculated potential energy surfaces, SF-decay T1/2.
1988LU05 Chin.J.Nucl.Phys. 10, 328 (1988) Theoretical Explaination for the Large Amount of Light Particle Emission in Fission Induced by Heavy Ion Reactions NUCLEAR STRUCTURE 240Pu; calculated fission rate, probability, Γn/ΓF. Smoluchowski equation.
1988SU08 Chin.J.Nucl.Phys. 10, 31 (1988) Study of Complex Particle Emission in the Preequilibrium Exciton Model NUCLEAR REACTIONS 12C, 54Fe(α, α'), E=58 MeV; 206Pb(α, α'), E=55 MeV; 197Au(α, α'), E=42-90 MeV; calculated angle integrated σ. Exciton model.
1988ZH04 Prog.Theor.Phys.(Kyoto) 79, 110 (1988) Zhuo Yizhong, Han Yin-lu, Wu Xi-zhen Further Investigation on Temperature-Dependent Optical Potential and Mean Free Path NUCLEAR REACTIONS 40Ca, 208Pb(p, p), (n, n), E=-30-60 MeV; calculated optical potential parameters.
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.
1986GE09 Nucl.Phys. A459, 77 (1986) Temperature-Dependent Optical Potential and Mean Free Path Based on Skyrme Interactions NUCLEAR REACTIONS 40Ca, 208Pb(n, n), E=10, 30, 50 MeV; calculated real, imaginary parts of optical potential, mean free path vs E, temperature, separation distance. Effective Skyrme interactions.
doi: 10.1016/0375-9474(86)90057-6
1986LU05 Z.Phys. A323, 477 (1986) Lu Zhongdao, Zhang Jingshang, Feng Renfa, Zhuo Yizhong Competition between Fission and Neutron Emission by Diffusion Model NUCLEAR STRUCTURE 240Pu; calculated average fission rate, fission probability, Γn/Γf; deduced fission potential height, nuclear temperature dependence. Diffusion model.
1986TI05 Chin.J.Nucl.Phys. 8, 28 (1986) Tian Ye, Wang Chang, Han Yinlu, Shen Qingbiao, Zhuo Yizhong An Application of the Microscopic Optical Potential (S-MOP) to Non Even-Even Nuclei in Calculations of Cross Sections NUCLEAR REACTIONS 6,7Li, 9Be, 10,11B, 14N, 23Na, 27Al, 51V, 53Cr, 55Mn, 59Co, 63,65Cu, 93Nb, 181Ta, 197Au, 235U, 239Pu(n, n), E ≈ 1-200 MeV; calculated total σ, σ(θ). Microscopic optical potential.
1986WE10 Z.Phys. A324, 325 (1986) Wen Yuanqi, Shi Xiangjun, Yan Shiwei, Zhuo Yizhong, Han Huiyi A Semi-Classical Model of Multi-Step Direct and Compound Nuclear Reactions NUCLEAR REACTIONS 197Au, 120Sn(p, p'), E=62 MeV; 93Nb(n, n'), E=14.6 MeV; calculated σ(θ, Ep), σ(θ, En). Semi-classical model, multi-step direct, compound nuclear reactions.
1986WE14 Chin.J.Nucl.Phys. 8, 9 (1986) Wen Yuanqi, Han Huiyi, Shi Xiangjun, Yan Shiwei, Zhuo Yizhong The Multi-Step Energy Correlation of Exciton Model and the Calculation of Double Differential Cross Section NUCLEAR REACTIONS 93Nb(n, n'), E=15 MeV; 120Sn, 197Au(p, p'), E=62 MeV; calculated σ(θn, En), σ(θp, Ep). Exciton model, multi-step energy correlation.
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.
1985TI06 Chin.J.Nucl.Phys. 7, 207 (1985) Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin Lifei A Global Analysis of Proton Differential Elastic Cross Section Calculations with the Microscopic Optical Potential S-MOP NUCLEAR REACTIONS 184W, 120Sn, 90Zr, 58,60,62,64Ni(p, p), E=16 MeV; 120Sn, 60Ni, 56Fe(p, p), E=30.3 MeV; 90Zr, 58Ni, 40Ca(p, p), E=40 MeV; 68Zn, 58Ni, 40Ca, 12C(p, p), E=61.4 MeV; 208Pb(p, p), E=16-61.4 MeV; analyzed σ(θ). Microscopic optical potential, extended Skyrme force.
1985TI07 Chin.J.Nucl.Phys. 7, 154 (1985) Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin, Li Fei A Global Analysis of Integral Cross Section Calculations with the Microscopic Optical Potential NUCLEAR REACTIONS 12C(n, n), E ≤ 100 MeV; 44,40Ca(n, n), E ≤ 15 MeV; 60Ni(n, n), E ≤ 30 MeV; 242Pu, 98Mo(n, n), E ≤ 100 MeV; 140Ce(n, n), E ≤ 60 MeV; 238U, 232Th(n, n), E ≤ 15 MeV; calculated elastic, nonelastic, total σ(E). Effective Skyrme force, microscopic optical potential.
1985TI08 Chin.J.Nucl.Phys. 7, 344 (1985) Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin, Li Fei A Global Analysis of Neutron Differential Elastic Cross Section Calculations with the Microscopic Optical Potential NUCLEAR REACTIONS 4He, 12C, 16O, 24Mg, 28Si, 32S, 40Ca, 50,52,54Cr, 54,56Fe, 58,60,62,64Ni, 64,66,68Zn, 90,92,94Zr, 92,94,96,98,100Mo, 118,120,122,124Sn, 182,184,186W, 208Pb, 232Th, 238U, 240Pu(n, n), E=1-26 MeV; calculated σ(θ). Microscopic optical potential.
1984SH38 Chin.J.Nucl.Phys. 6, 245 (1984) Shen Qingbiao, Tian Ye, Wang Shunuan, Gao Liangjun, Zhuo Yizhong, Zhao Fujian Exciton Transition Rate Calculations Based on the Optical Model Potentials NUCLEAR STRUCTURE 40Ca, 120Sn, 238U; calculated exciton transition rates. Optical potential, Skyrme interaction.
1982MA46 Chin.J.Nucl.Phys. 4, 97 (1982) Ma Zhongyu, Wu Xizhen, Zhang Jingshang, Zhuo Yizhong Calculation of Muon Final Probabilities After Muon-Induced Fission in Four-State Basis NUCLEAR REACTIONS 238U(μ-, F), E at rest; calculated light fission fragment muon capture probability.
1982WA22 Chin.J.Nucl.Phys. 4, 104 (1982) Wang Shunuan, Sun Ziyang, Zhang Jingshang, Gao Liangjun, Zhuo Yizhong Angular Distribution Calculation for Both the Preequilibrium and Equilibrium Decay by Considering the Influence of the Pauli Exclusion Principle NUCLEAR REACTIONS 93Nb(n, n'), E=15 MeV; calculated σ(θ, En'). Equilibrium, preequilibrium decay, Pauli effect, closed form exciton model.
1982ZI01 Z.Phys. A305, 61 (1982) S.Ziyang, W.Shunuan, Z.Jingshang, Z.Yizhong Angular Distribution Calculation Based on the Exciton Model Taking Account of the Influence of the Fermi Motion and the Pauli Principle NUCLEAR REACTIONS 93Nb(n, n'), E=15 MeV; calculated σ(θ, En'). Exciton model, Fermi motion, Pauli principle.
1981MA36 Chin.J.Nucl.Phys. 3, 217 (1981) Ma Zhongyu, Sun Ziyang, Zhang Jingshang, Zhuo Yizhong, Ding Dazhao Pre-Equilibrium Exciton-Phonon Coupling Model for (n, γ) Reaction NUCLEAR REACTIONS 238U, 56Fe, 208Pb(n, γ), E=5-19 MeV; calculated σ(E). Preequilibrium exciton-phonon coupling model.
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