NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Z.Yuan Found 16 matches. 2024YA08 Phys.Rev.Lett. 132, 152502 (2024) X.Yan, Zh.Cheng, A.Abdukerim, Z.Bo, W.Chen, X.Chen, Ch.Cheng, X.Cui, Y.Fan, D.Fang, Ch.Fu, M.Fu, L.Geng, K.Giboni, L.Gu, X.Guo, Ch.Han, K.Han, Ch.He, J.He, D.Huang, Y.Huang, J.Huang, Zh.Huang, R.Hou, Y.Hou, X.Ji, Y.Ju, Ch.Li, J.Li, M.Li, Sh.Li, T.Li, Q.Lin, J.Liu, X.Lu, C.Lu, L.Luo, Y.Luo, W.Ma, Y.Ma, Y.Mao, Y.Meng, X.Ning, B.Pang, N.Qi, Zh.Qian, X.Ren, N.Shaheed, X.Shang, X.Shao, G.Shen, L.Si, W.Sun, A.Tan, Y.Tao, A.Wang, M.Wang, Q.Wang, Sh.Wang, S.Wang, W.Wang, X.Wang, Zh.Wang, Y.Wei, M.Wu, W.Wu, J.Xia, M.Xiao, X.Xiao, P.Xie, B.Yan, J.Yang, Y.Yang, Y.Yao, Ch.Yu, Y.Yuan, Zh.Yuan, X.Zeng, D.Zhang, M.Zhang, P.Zhang, Sh.Zhang, Sh.Zhang, T.Zhang, W.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, L.Zhao, Q.Zheng, J.Zhou, N.Zhou, X.Zhou, Y.Zhou, Y.Zhou, for the PandaX Collaboration Searching for Two-Neutrino and Neutrinoless Double Beta Decay of 134Xe with the PandaX-4T Experiment RADIOACTIVITY 134Xe(2β-); measured decay products, Eβ, Iβ; deduced two-neutrino and neutrinoless T1/2 limits. Comparison with available data. The cylindrical active volume PandaX-4T dual-phase TPC.
doi: 10.1103/PhysRevLett.132.152502
2024YU05 Eur.Phys.J. A 60, (2024) Z.Yuan, D.Bai, Zh.Wang, Zh.Ren Improved formulas of spontaneous fission half-lives for heavy and superheavy nuclei RADIOACTIVITY 232Th, 232,234,236,238U, 236,238,240,242,244Pu, 240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254,256Cf, 246,248,250,252,254,256Fm, 252,254,256,258,260No, 256,258Rf, 260,262Sg, 264,266Hs, 280Ds, 284Cn, 286Fl(SF); calculated T1/2. Comparison with available data.
doi: 10.1140/epja/s10050-024-01280-z
2024YU06 Phys.Rev. C 109, L031903 (2024) Z.Yuan, A.Huang, W.-H.Zhou, G.-L.Ma, M.Huang Evolution of topological charge through chiral anomaly transport
doi: 10.1103/PhysRevC.109.L031903
2022YU01 Chin.Phys.C 46, 024101 (2022) Theoretical predictions on α-decay properties of some unknown neutron-deficient actinide nuclei using machine learning RADIOACTIVITY 204Ac, 206,207,208,209Th, 210Pa, 222Pa, 216,213,214,217,220U, 217,218Np, 221Np, 217,218,219,220,221,222,223,224,225,226,227Pu(α); calculated T1/2, Q-values. Comparison with available data.
doi: 10.1088/1674-1137/ac321c
2021YU06 Chin.Phys.C 45, 124107 (2021) Magnetic moment predictions of odd-A nuclei with the Bayesian neural network approach NUCLEAR MOMENTS 207,209Pb, 209Bi, 207Tl, Cd, Cs, 23F, 23Si, 37S, 39Sc, 53K, 41Ti, 53,61Co, 79Cu, 59Zn, 81Ge, 93Mo, 93Ru, 97Pd, 99,103,129In, 101Sn, 113,135Sb, 181Tl, 197,215Bi; analyzed available data; deduced nuclear magnetic moments using the BNN-I4 approach. Bayesian neural network (BNN).
doi: 10.1088/1674-1137/ac28f9
2020YU02 J.Radioanal.Nucl.Chem. 324, 277 (2020) Measurement of the 238U(n, γ)239U reaction cross sections in the energy range of 2.0-5.0 MeV by using a neutron activation technique NUCLEAR REACTIONS 238U(n, γ), E=2-5 MeV; measured reaction products, Eγ, Iγ; deduced σ and uncertainties. Comparison with ENDF/B-VII, JENDL-4, CENDL-3.1 libraries and TALYS calculations.
doi: 10.1007/s10967-020-07046-3
2007ZH42 Appl.Radiat.Isot. 65, 1314 (2007) P.Zhu, Z.Yuan, J.Chen, Z.Liu, G.Zhang, Z.Shi, H.Lu Measurement of neutron capture cross sections for 141Pr from 0.5 to 1.6 MeV NUCLEAR REACTIONS 141Pr(n, γ), E=0.54, 1.09, 1.59 MeV; measured Eγ, Iγ, cross sections using the activation method. Compared results to model calculations.
doi: 10.1016/j.apradiso.2007.07.015
1993HO20 Phys.Rev. C48, 2277 (1993) Y.-K.Ho, Z.-S.Yuan, B.-H.Zhang, Z.-Y.Pan Self-Consistent Description for X-Ray, Auger Electron, and Nuclear Excitation by Electron Transition Processes NUCLEAR STRUCTURE 189Os, 197Au, 237Np; calculated electron transition induced nuclear excitation probability. Self-consistent, unified nonrelativistic approach, X-ray, Auger electron emission also considered.
doi: 10.1103/PhysRevC.48.2277
1993YU02 Phys.Rev. C47, 323 (1993) First-Principles Calculation of the Cross Sections for Nuclear Excitation by Electron Capture of Channeled Nuclei NUCLEAR STRUCTURE 165Ho, 173Yb, 187,185Re, 185Pt; calculated σ for excitation by electron capture. Highly stripped nuclei, channelling along Si <110> crystal axis.
doi: 10.1103/PhysRevC.47.323
1992HO11 Phys.Rev. C46, 1425 (1992) Intermediate-Energy Proton Direct Capture Populating Continuum States NUCLEAR REACTIONS 11B(p, γ), E=10-70 MeV; calculated σ(θ) vs E. Direct capture continuum states population.
doi: 10.1103/PhysRevC.46.1425
1991HO02 Phys.Rev. C43, 709 (1991) Mass, Shell, and Even-Odd Effects in Radiative Capture Reaction NUCLEAR STRUCTURE A=27-197; analyzed (n, γ) data; deduced mass, shell, even-odd effects role.
doi: 10.1103/PhysRevC.43.709
1991HO17 Phys.Rev. C44, 1910 (1991) Y.-K.Ho, B.-H.Zhang, Z.-S.Yuan Probability and Selection Rule for Nuclear Excitation by Electron Transition NUCLEAR STRUCTURE 189Os, 197Au, 237Np; calculated nuclear excitation by electron transition probability; deduced selection rule. Quantum mechanical formalism.
doi: 10.1103/PhysRevC.44.1910
1991YU01 Phys.Rev. C43, 2765 (1991) Unified Formalism to Study Nonstatistical Effects in Radiative Capture Reactions NUCLEAR REACTIONS 55Mn, 89Y, 208Pb, 27Al(n, γ), E < 20 MeV; calculated capture σ(E). Unified formalism, nonstatistical effects.
doi: 10.1103/PhysRevC.43.2765
1989HO09 Phys.Rev. C39, 1691 (1989) Strong Nonstatistical Effects in Neutron Capture at the 2p Size Resonance Region NUCLEAR REACTIONS 27Al, 28Si(n, γ), E=thermal-2 MeV; calculated σ(E); deduced nonstatistical fractions, reaction mechanisms.
doi: 10.1103/PhysRevC.39.1691
1989HO21 Phys.Rev. C40, 2541 (1989) Averaged Nonstatistical Effects in the 3s Region for Capture Reactions NUCLEAR REACTIONS 55Mn(n, γ), E ≤ 2 MeV; calculated σ(E). Statistical, nonstatistical contributions. NUCLEAR STRUCTURE A=30-70; calculated neutron capture σ(E). Averaged nonstatistical effects.
doi: 10.1103/PhysRevC.40.2541
1986ZH11 Chin.J.Nucl.Phys. 8, 140 (1986) Zheng Guotong, Wang Yansen, Yuan Zhushu, Qiu Zhihong The Effects of Quadrupole Vibration of the Fragments on μ- Final-State Probabilities NUCLEAR REACTIONS 238U(μ-, F), E not given; calculated muon final state probabilities following fission. Linear combination of atomic obital method.
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