NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Z.Cheng Found 15 matches. 2024CO01 Phys.Rev. C 109, 014301 (2024) L.Coraggio, N.Itaco, G.De Gregorio, A.Gargano, Z.H.Cheng, Y.Z.Ma, F.R.Xu, M.Viviani The renormalization of the shell-model Gamow-Teller operator starting from effective field theory for nuclear systems
doi: 10.1103/PhysRevC.109.014301
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
2023XU10 Phys.Rev. C 108, L031301 (2023) Z.C.Xu, S.Zhang, J.G.Li, S.L.Jin, Q.Yuan, Z.H.Cheng, N.Michel, F.R.Xu Complex valence-space effective operators for observables: The Gamow-Teller transition
doi: 10.1103/PhysRevC.108.L031301
2023ZH48 Phys.Rev. C 108, 064316 (2023) S.Zhang, F.R.Xu, J.G.Li, B.S.Hu, Z.H.Cheng, N.Michel, Y.Z.Ma, Q.Yuan, Y.H.Zhang Ab initio descriptions of A=16 mirror nuclei with resonance and continuum coupling
doi: 10.1103/PhysRevC.108.064316
2022CH42 Chin.Phys.C 46, 094102 (2022) Possibilities of synthesizing new proton-rich nuclei with 40 ≤ Z ≤ 60 using multinucleon transfer reactions NUCLEAR REACTIONS 130Te(64Ni, X), E(cm)=184.27 MeV; analyzed available data; deduced mass distributions of final fragments using the DNS model+GEMINI++.
doi: 10.1088/1674-1137/ac6ed3
2022ZH57 Phys.Lett. B 827, 136958 (2022) S.Zhang, Y.Z.Ma, J.G.Li, B.S.Hu, Q.Yuan, Z.H.Cheng, F.R.Xu The roles of three-nucleon force and continuum coupling in mirror symmetry breaking of oxygen mass region NUCLEAR STRUCTURE 17,18,19,20,21,22,23,24,25,26,27,28O; calculated g.s. energies, energy levels, J, π, using the complex-energy ab initio Gamow shell model with a core. Comparison with available data.
doi: 10.1016/j.physletb.2022.136958
2021CH10 Phys.Rev. C 103, 024613 (2021) Formation of heavy neutron-rich nuclei by 48Ca-induced multinucleon transfer reactions NUCLEAR REACTIONS 238U(48Ca, X), E=195.0 MeV; 248Cm(48Ca, X), E=226.41 MeV; calculated transfer σ for production of Z=81-91 nuclei for 238U+48Ca reaction, and Z=84-95 nuclei for 248Cm+48Ca reaction in transfer of up to 12 protons from the target nuclei. 208Pb(136Xe, X), E=450.0 MeV; 238U(48Ca, X), E=195.0 MeV; calculated production σ for the production of Z=83-91 and Z=70-81 neutron-rich nuclei in multinucleon transfer reactions. Improved dinuclear system model+GEMINI++. Comparison with available experimental data.
doi: 10.1103/PhysRevC.103.024613
2021CH27 Phys.Rev. C 103, 064613 (2021) Influence of entrance channel on multinucleon transfer cross sections NUCLEAR REACTIONS 208Pb(58Ni, X), E(cm)=269.77 MeV; 208Pb(64Ni, X), E(cm)=267.64 MeV; 208Pb(64Ni, X), E(cm)=244.40 MeV; 198Pt(58Ni, X), (64Ni, X), (70Ni, X), E not given; 208Pb(86Kr, X), (91Kr, X), (102Kr, X), E not given; calculated production cross sections of target-like fragments (TLF) by the removal of 1-18 protons and by addition of 0-7 protons, maximum cross sections of multinucleon transfer (MNT) products as a function of their proton number Z, mass distributions of final products. Improved dinuclear system (DNS) model + GEMINI++. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.064613
2019SU03 Phys.Rev. C 99, 024605 (2019) Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, D.Yan, B.H.Sun, J.W.Zhao, Y.P.Xu, D.Y.Pang, Y.H.Yu, K.Yue, S.W.Tang, C.Dong, Y.X.Zhao, F.Fang, Y.Sun, Z.H.Cheng, X.M.Liu, P.Ma, H.R.Yang, C.G.Lu, L.M.Duan Two-neutron removal cross sections from 15, 16C at around 240 MeV/nucleon NUCLEAR REACTIONS 12C(15C, X), (15C, 13C), (16C, X), (16C, 14C)8Li/10Be/11Be/12B/13B/15C/16C/17N, E=237, 239 MeV/nucleon, [secondary 15,16C beams from 9Be(18O, X), E=280 MeV/nucleon primary reaction followed by in-flight fragment separator RIBLL2 at HIRFL-Lanzhou]; measured reaction products, particle identification spectra, time of flight of fragments, and two-neutron removal σ(E) using multiwire drift chambers for particle detection and identification, and plastic scintillators for time of flight measurements. Comparison with previous experimental values, and theoretical calculations for two-neutron removal σ based on eikonal-model and shell-model structure information. Systematics of odd-even staggering in two-neutron removal σ from 15,16,17,18,19,20C projectiles.
doi: 10.1103/PhysRevC.99.024605
2019ZH46 Phys.Rev. C 100, 044609 (2019) Y.X.Zhao, Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, D.Yan, D.Y.Pang, P.Ma, Y.H.Yu, K.Yue, S.W.Tang, S.M.Wang, F.Fang, Y.Sun, Z.H.Cheng, X.M.Liu, H.R.Yang, C.G.Lu, L.M.Duan One-proton knockout from 16C at around 240 MeV/nucleon NUCLEAR REACTIONS 12C(16C, 15B), E=239 MeV/nucleon, [secondary16O beam from 9Be(18O, X)8Li/10Be/11Be/13B/16C, E=280 MeV/nucleon primary reaction using RIBLL2 at HRIFL-Lanzhou facility]; measured reaction products by magnetic rigidity (Bρ), time of flight (TOF), and energy loss (ΔE), mass yields. 16C, 15B; deduced σ for one-proton knockout, spectroscopic reduction factor. Comparison to predictions based on the eikonal reaction model with shell-model structure inputs, and with previous experimental data for 9Be(16C, 15B), E=75 MeV/nucleon reaction. Discussed energy dependence of the spectroscopic reduction factor, and the role of surface neutrons as spectators.
doi: 10.1103/PhysRevC.100.044609
2013XI08 Appl.Radiat.Isot. 80, 56 (2013) F.Xie, W.Jiang, X.He, X.Li, Z.Cheng, S.Wang, Q.Li, Q.L.Shi, Y.Chang Measurement of absolute gamma-ray emission probabilities from decay of 138Xe RADIOACTIVITY 138Xe(β-); measured decay products, Eγ, Iγ; deduced emission probabilities and their uncertainties. Comparison with available data.
doi: 10.1016/j.apradiso.2013.06.006
1997CH34 Chin.Phys.Lett. 14, 387 (1997) Z.-H.Cheng, B.-G.Shen, J.-X.Zhang, M.-X.Mao, J.-J.Sun, C.-L.Yang, F.-S.Li, Y.-D.Zhang Mossbauer Spectroscopy and X-Ray Diffraction Studies of the Phase Composition of Crystallized Nd(x)Fe(81.5-x)B(18.5) Alloys with 7 ≤ x ≤ 15 NUCLEAR REACTIONS 58Fe(γ, γ), E=14.4 keV; measured Mossbauer spectra; deduced crystallized Nd2Fe(81.5-x)-B(18.5) alloy phase composition. Data on X-ray diffraction also studied.
1994CH62 J.Phys.Condens.Matter 6, 3109 (1994) Z.-H.Cheng, M.-X.Mao, C.-L.Yang, F.-S.Li, B.-G.Shen, Y.-D.Zhang Magnetism and Hyperfine Fields in YFe10V2: A combined nuclear magnetic resonance and Mossbauer study NUCLEAR REACTIONS 57Fe(γ, γ), E=14.4 keV; measured Mossbauer spectra; deduced hyperfine filed characteristics. NMR data input, YFe10V2 sample. NUCLEAR MOMENTS 57Fe, 89Y, 51V; measured NMR; deduced hyperfine field characteristics. Mossbauer data input, YFe10V2 sample.
doi: 10.1088/0953-8984/6/16/016
1994CH64 J.Phys.Condens.Matter 6, 7437 (1994) Z.-H.Cheng, M.-X.Mao, J.-J.Sun, B.-G.Shen, F.-W.Wang, C.-L.Yang, F.-S.Li, Y.-D.Zhang The Effect of Gd Substitution on the Magnetic Properties and Hyperfine Fields of Melt-Spun Ns4Fe(77.5)B(18.5) Alloys NUCLEAR MOMENTS 11B, 57Fe; measured NMR spectra; deduced Gd substitution role in magnetic properties, hyperfine fields. Melt-spun Nd4Fe(77.5)B(18.5) alloys.
doi: 10.1088/0953-8984/6/36/023
1986CH17 Radiat.Eff. 94, 97 (1986) Y.Chang, Z.Cheng, C.Yan, G.Shi, D.Qiao Determination of x-, and Gamma-Ray Emission Probabilities in the Decay of Np-239 RADIOACTIVITY 239Np(β-); measured Eγ, Iγ, E X-ray, I X-ray. 239Pu levels deduced γ-emission probabilities per parent decay.
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