NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = Z.An Found 27 matches. 2023AN14 Sci. Rep. 13, 12657 (2023) Z.An, W.Qiu, W.Jiang, G.Yang, X.Li, Z.Liao, Z.Zhuang, X.Zhang, S.Chen, C.Guo, E.Xiao, X.Fang, X.Li, H.Wang, X.Hu, Bi.Jiang, W.Shen, J.Wang, J.Ren, X.Ruan, D.Wang, S.-Y.Zhang, W.Luo, Z.Zhu, H.Lan, Z.Cao, X.Ma, Y.Liu, P.Wang, Y.Yang, P.Su, X.Deng, W.He, Y.Ma, C.Ma, Y.Wang, P.He, R.Tang, T.Zhou, J.Wang, H.Yi, Y.Zhang, Y.Chen, R.Fan, K.Gao, Q.Li, K.Sun, Z.Tan, M.Gu, H.Jing, J.Tang Measurement of the 181Ta(n, γ) cross sections up to stellar s-process temperatures at the CSNS Back-n NUCLEAR REACTIONS 181Ta(n, γ), E=0.001-800 keV; measured reaction products, En, In, TOF; deduced σ, resonance parameters using the R-Matrix code SAMMY, Maxwellian average cross sections (MACS). Comparison with available data. The back-streaming white neutron facility (Back-n) of China spallation neutron source (CSNS).
doi: 10.1038/s41598-023-39603-7
2023RU05 Phys.Rev. C 107, 065803 (2023) L.H.Ru, D.H.Xie, T.Y.Jiao, Z.An, F.Bai, J.W.Cai, X.Fang, Y.H.Fan, Y.X.Fan, B.S.Gao, Y.Z.Li, W.P.Lin, G.Liu, L.Ma, H.J.Ong, X.D.Tang, P.Wang, X.Zhang Strength of the resonance of the 13C(α, n)16O reaction at Eα = 1055.63 keV NUCLEAR REACTIONS 13C(α, n), E=960-1150 keV; measured In; deduced σ(E), resonance strengths at 1055.63 keV (used for neutron detector arrays calibration), resonance parameters for Eα= 1334.64 and 1338.27 keV. Comparison to previous experimental results and ENDF/B-VIII.0 evaluation. Low background neutron detector array consisting of 24 cylindrical 3He-filled proportional counters at 3 MV Tandetron accelerator (Sichuan University).
doi: 10.1103/PhysRevC.107.065803
2022LI28 Few-Body Systems 63, 43 (2022) W.P.Liu, Z.H.Li, J.J.He, X.D.Tang, G.Lian, J.Su, Y.P.Shen, Z.An, F.Q.Chao, J.J.Chang, L.H.Chen, H.Chen, X.J.Chen, Y.H.Chen, Z.J.Chen, B.Q.Cui, X.C.Du, X.Fang, C.B.Fu, L.Gan, B.Guo, Z.Y.Han, X.Y.Guo, G.Z.He, J.R.He, A.Heger, S.Q.Hou, H.X.Huang, N.Huang, B.L.Jia, L.Y.Jiang, S.Kubono, J.M.Li, M.C.Li, K.A.Li, E.T.Li, T.Li, Y.J.Li, M.Lugaro, X.B.Luo, H.Y.Ma, S.B.Ma, D.M.Mei, W.Nan, W.K.Nan, N.C.Qi, Y.Z.Qian, J.C.Qin, J.Ren, C.S.Shang, L.T.Sun, W.L.Sun, W.P.Tan, I.Tanihata, S.Wang, P.Wang, Y.B.Wang, Q.Wu, S.W.Xu, S.Q.Yan, L.T.Yang, Y.Yang, X.Q.Yu, Q.Yue, S.Zeng, L.Zhang, H.Zhang, H.Y.Zhang, L.Y.Zhang, N.T.Zhang, P.Zhang, Q.W.Zhang, T.Zhang, X.P.Zhang, X.Z.Zhang, W.Zhao, J.F.Zhou, Y.Zho Progress of Underground Nuclear Astrophysics Experiment JUNA in China NUCLEAR REACTIONS 12C(α, γ), 13C(α, n), 25Mg(p, γ), 19F(p, α), E(cm)<600 keV; measured reaction products; deduced yields near the Gamow window. Comparison with available data.
doi: 10.1007/s00601-022-01735-3
2022LI72 Phys.Rev. C 106, 065804 (2022) X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, D.X.Wang, S.Y.Zhang, G.L.Yang, X.K.Li, Z.D.An, J.J.He, W.Luo, X.G.Cao, L.L.Song, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, Y.D.Liu, C.W.Ma, Y.T.Wang, J.Su, L.Y.Zhang, Y.X.Yang, S.Feng, W.B.Liu, W.Q.Su, S.Jin, K.J.Chen Experimental determination of the neutron resonance peak of 162Er at 67.8 eV NUCLEAR REACTIONS 162Er(n, γ), E=20-100 eV; measured Eγ, Iγ; deduced neutron-capture yield, resonances, decay widths. Resonance parameters at 67.8 eV are extracted for the first time. R-matrix analysis. Comparison to other experimental results and ENDF/B-VIII.0 data. 4 C6D6 detectors. Neutron beam from Back-n Facility of the CSNS.
doi: 10.1103/PhysRevC.106.065804
2022WU02 Nucl.Phys. A1017, 122357 (2022) D.Wu, B.Guo, C.Y.He, W.P.Lin, Z.An, T.L.Ma, F.L.Liu, W.S.Yang, J.H.Wei, Y.C.Li, Y.P.Shen, Q.W.Fan, X.G.Wu, Y.Zheng, T.X.Li, F.Bai, P.Wang, M.L.Qiu, N.Y.Wang Determination of the 74Ge(p, γ)75As reaction rates in p-process nucleosynthesis with in-beam γ spectroscopy NUCLEAR REACTIONS 74Ge(p, γ), E=2.5-4.3 MeV; measured reaction products, Eγ, Iγ; deduced σ, reaction rates. Comparison with TALYS and EMPIRE nuclear reaction codes calculations. The 3 MV tandem accelerator of the Institute of Nuclear Science and Technology, Sichuan University.
doi: 10.1016/j.nuclphysa.2021.122357
2021LI46 Nucl.Instrum.Methods Phys.Res. B506, 15 (2021) L.Li, Z.An, J.Zhu, W.Lin, S.Williams Absolute measurements of bremsstrahlung double differential cross sections of C and Al atoms by 5-25 keV electron impact NUCLEAR REACTIONS C, 27Al(e-, e-'), E=5-25 keV; measured reaction products, Eγ, Iγ; deduced σ(θ, E) bremsstrahlung. Comparison with theoretical calculations.
doi: 10.1016/j.nimb.2021.09.001
2021LI61 Phys.Rev. C 104, 054302 (2021) X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, X.G.Cao, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, J.C.Wang, D.X.Wang, S.Y.Zhang, Y.D.Liu, X.Ma, C.W.Ma, Y.T.Wang, Z.D.An, J.J.He, J.Su, L.Y.Zhang, Y.X.Yang, W.B.Liu, W.Q.Su New experimental measurement of natEr(n, γ) cross sections between 1 and 100 eV NUCLEAR REACTIONS 162,164,166,167,168,170Er, 12,13C, 197Au(n, γ), E=0.001-100 keV; measured E(n), I(n), Eγ, Iγ using C6D6 liquid scintillator and a silicon monitor and natural Er, C and Au targets at the China spallation neutron source (CSNS) facility; deduced neutron-capture σ(E), capture yields as function of E(n), neutron resonances in Er isotopes in the 1-100 eV region. 162,164,166,167,168Er; deduced energies of 43 neutron resonances (nine for 162Er, five for 164Er, three for 166Er, 25 for 167Er, one for 168Er), cross sections, widths Γγ and Γn by R-matrix analysis. Comparison with previous experimental data, and with data in evaluated databases ENDF/B-VIII.0, ENDF/B-VII.1, JENDL-4.0, and ROSFOND-2010.
doi: 10.1103/PhysRevC.104.054302
2019GU08 Phys.Rev. C 99, 044607 (2019) C.-C.Guo, Y.-G.Ma, Z.-D.An, B.-S.Huang Influence of α-clustering configurations in 16O + 197Au collisions at Fermi energy NUCLEAR REACTIONS 197Au(16O, X), E=40 MeV/nucleon; calculated contour plots of nucleon density, directed flow and flow parameters of free protons as function of rapidity with the chain and a tetrahedron α configurations of 16O projectile, and transverse momentum dependence of flow parameters. 197Au(12C, X), (14N, X), (36Ar, X), E=30, 35, 40 MeV/nucleon; calculated charge multiplicity distributions. Extended quantum molecular dynamics model (ImQMD). Comparison with available experimental data. Relevance to α-clustering configurations in light nuclei.
doi: 10.1103/PhysRevC.99.044607
2019LI12 Nucl.Instrum.Methods Phys.Res. B445, 13 (2019) Experimental thick target bremsstrahlung spectra produced by 5-25 keV electrons for 6 ≤ Z ≤ 82 and comparison with Monte Carlo PENELOPE simulations NUCLEAR REACTIONS C, Ti, Zr, Nb, W, Pb(E, γ), E=5-25 keV; measured reaction products, X-rays; deduced thick target yields, bremsstrahlung spectra. Comparison with theoretical calculations.
doi: 10.1016/j.nimb.2019.02.025
2019SH11 Phys.Rev. C 99, 025805 (2019) Y.P.Shen, B.Guo, Z.H.Li, Y.J.Li, D.Y.Pang, S.Adhikari, Z.D.An, J.Su, S.Q.Yan, X.C.Du, Q.W.Fan, L.Gan, Z.Y.Han, D.H.Li, E.T.Li, X.Y.Li, G.Lian, J.C.Liu, T.L.Ma, C.J.Pei, Y.Su, Y.B.Wang, S.Zeng, Y.Zhou, W.P.Liu Astrophysical SE2 factor of the 12C (α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction NUCLEAR REACTIONS 12C(11B, 7Li), (11B, 11B), E=50 MeV; 16O(7Li, 7Li), E=26 MeV; measured charged-particle spectra, differential σ(θ) using the Q3D magnetic spectrograph at the HI-13 tandem accelerator of the CIAE-Beijing. 12C(α, γ), E(cm)<5 MeV; deduced astrophysical SE2(300) factor of the ground state. 16O; deduced asymptotic normalization coefficient (ANC) and reduced α width of the 6.917-MeV level from finite-range distorted wave Born approximation (FRDWBA) and coupled-reaction-channel (CRC) analysis using FRESCO code. Comparison with previous experimental values, and with theoretical model predictions. R-matrix analysis of scattering data.
doi: 10.1103/PhysRevC.99.025805
2019SH37 Phys.Lett. B 797, 134820 (2019) Y.P.Shen, B.Guo, T.L.Ma, D.Y.Pang, D.D.Ni, Z.Z.Ren, Y.J.Li, Z.D.An, J.Su, J.C.Liu, Q.W.Fan, Z.Y.Han, X.Y.Li, Z.H.Li, G.Lian, Y.Su, Y.B.Wang, S.Q.Yan, S.Zeng, W.P.Liu First experimental constraint of the spectroscopic amplitudes for the α-cluster in the 11B ground state NUCLEAR REACTIONS 7Li(6Li, d), E=24 MeV; measured reaction products; deduced spectroscopic amplitudes (SA) for the α-cluster in the 11B ground state. Comparison with available data.
doi: 10.1016/j.physletb.2019.134820
2018HA06 Nucl.Instrum.Methods Phys.Res. B418, 68 (2018) J.Han, Z.An, G.Zheng, F.Bai, Z.Li, P.Wang, X.Liao, M.Liu, S.Chen, M.Song, J.Zhang An ion beam facility based on a 3 MV tandetron accelerator in Sichuan University, China NUCLEAR REACTIONS 55Mn(p, X), E=2 MeV; measured reaction products, Eγ, Iγ, X-rays; deduced X-ray production yields for PIXE. High-precision ion implantation.
doi: 10.1016/j.nimb.2018.01.002
2016AN01 Astrophys.J. 817, L5 (2016); Erratum Astrophys.J. 877, L42 (2019) Z.-D.An, Y.-G.Ma, G.-T.Fan, Y.-Ji.Li, Z.-P.Chen, Y.-Y.Sun New Astrophysical Reaction Rate for the 12C(α, γ)16O Reaction NUCLEAR REACTIONS 12C(α, γ), E(cm)<7.5 MeV; analyzed available data; deduced reaction rate probability density functions, fractional contributions of different J, π. Comparison with available data.
doi: 10.3847/2041-8205/817/1/L5
2015AN15 Phys.Rev. C 92, 045802 (2015) Z.-D.An, Z.-P.Chen, Y.-G.Ma, J.-K.Yu, Y.-Y.Sun, G.-T.Fan, Y.-J.Li, H.-H.Xu, B.-S.Huang, K.Wang Astrophysical S factor of the 12C(α, γ)16O reaction calculated with reduced R-matrix theory NUCLEAR REACTIONS 12C(α, γ)16O, E(cm)<10 MeV; 12C(α, α), E(cm)=1.1-6.2 MeV; analyzed σ(E, θ) data using reduced R-matrix theory based on the classical R-matrix theory of Lane and Thomas; deduced accurate, and self-consistent astrophysical S factor. 16O; deduced particle partial widths for levels, and radiation widths for the γ-ray transitions from R-matrix fits. Comparison of widths to literature values.
doi: 10.1103/PhysRevC.92.045802
2014LI20 Nucl.Instrum.Methods Phys.Res. B333, 106 (2014) X.L.Li, J.L.Zhao, L.X.Tian, Z.An, J.J.Zhu, M.T.Liu Measurements of inner-shell characteristic X-ray yields of thick W, Mo and Zr targets by low-energy electron impact and comparison with Monte Carlo simulations NUCLEAR REACTIONS W, Mo, Zr(E, X), E=5-29 keV; measured reaction products, X-rays; deduced X-ray thick target yields. Monte Carlo simulations.
doi: 10.1016/j.nimb.2014.04.017
2012CA01 Nucl.Phys. A874, 1 (2012) X.L.Cai, W.Xu, W.Luo, L.F.Yang, G.T.Fan, B.J.Xu, Y.J.Li, Z.D.An, Z.Yan, Q.Y.Pan Experimental study for measuring the decay branching ratio for nuclear excitation by electron transition in 189Os NUCLEAR REACTIONS 189Os(X-ray, X), E=69.535 keV; measured Eγ, Iγ, X-ray using Si(Li) detector; analyzed feasibility of deducing branching ratio for populating isomeric state. Synchrotron radiation.
doi: 10.1016/j.nuclphysa.2011.09.011
2012WU01 Can.J.Phys. 90, 125 (2012) Y.Wu, Z.An, Y.M.Duan, M.T.Liu, X.P.Ouyang K-shell ionization cross sections of K and Lα X-ray production cross sections of I by 10-30 keV electron impact NUCLEAR REACTIONS I(e, X), E=10-30 keV; measured characteristic X-rays; deduced σ. Comparison with DWBA and PWBA-C-Ex calculations.
doi: 10.1139/p11-149
2010WU03 Nucl.Instrum.Methods Phys.Res. B268, 2473 (2010) Measurements of Lα, Lβ X-ray production cross sections of Bi by 17-0 keV electron impact
doi: 10.1016/j.nimb.2010.05.060
2003AN11 Chin.Phys.Lett. 20, 478 (2003) Z.An, Q.Chen, Y-H.Cheng, D.-J.Shen, G.Guo Properties of the First 1/2+ Excitation State of 13C by 22 MeV Proton Inelastic Scattering NUCLEAR REACTIONS 12,13C(p, p), E=22 MeV; 13C(p, p'), E=22 MeV; measured σ(θ). 13C level deduced neutron halo structure, related features. Microscopic DWBA analysis, comparison with related data.
doi: 10.1088/0256-307X/20/4/311
1999AN32 J.Phys.(London) G25, 1693 (1999) Low-Energy Nucleon Scattering and Halderson's Effective NN Interaction NUCLEAR REACTIONS 12C(p, p'), E=62 MeV; analyzed σ(θ). 12C(p, n), E=50-80 MeV; analyzed zero-degree transverse polarization. Comparison of effective interactions.
doi: 10.1088/0954-3899/25/8/311
1996AN24 Phys.Rev. A54, 3067 (1996) Z.An, T.H.Li, L.M.Wang, X.Y.Xia, Z.M.Luo Correction of Substrate Effect in the Measurement of 8-25-keV Electron-Impact K-Shell Ionization Cross Sections of Cu and Co Elements ATOMIC PHYSICS Cu, 59Co(e, X), E=8-25 keV; measured K-shell ionization σ. Thin targets substrate influence corrected. NUCLEAR REACTIONS Cu, 59Co(e, X), E=8-25 keV; measured K-shell ionization σ. Thin targets substrate influence corrected.
doi: 10.1103/PhysRevA.54.3067
1996HE16 Chin.Phys.Lett. 13, 175 (1996) F.-Q.He, X.-G.Long, X.-F.Peng, Z.-M.Luo, Z.An K-Shell Ionization of Molybdenum and Iron by Electron Bombardment NUCLEAR REACTIONS Mo, Fe(e, X), E ≤ 50 keV; measured K-shell ionization σ. ATOMIC PHYSICS Mo, Fe(e, X), E ≤ 50 keV; measured K-shell ionization σ.
doi: 10.1088/0256-307X/13/3/005
1996HE35 Nucl.Instrum.Methods Phys.Res. B114, 213 (1996) F.Q.He, X.G.Long, X.F.Peng, Z.M.Luo, Z.An K-Shell Ionization of Molybdenum by Electron Bombardment
doi: 10.1016/0168-583X(96)00193-0
1996LU17 J.Phys.(London) B29, 4001 (1996) Z.Luo, Z.An, F.He, T.Li, X.Long, X.Peng Correction of the Influence of the Substrate Upon the Measurement of K-Shell Ioniziation Cross Sections ATOMIC PHYSICS Ni, Cr(e, X), E ≤ 34 keV; measured K-shell ionization σ. NUCLEAR REACTIONS Ni, Cr(e, X), E ≤ 34 keV; measured K-shell ionization σ.
doi: 10.1088/0953-4075/29/17/020
1995AN28 Chin.Phys.Lett. 12, 649 (1995) Verification of the Orbital Character of Low-Lying M1 Excitation Mode in 160Gd by 22 MeV Proton Inelastic Scattering at a Forward Angle NUCLEAR REACTIONS 160Gd(p, p'), E=22 MeV; measured σ(θ), σ(Ep). 160Gd deduced levels, J, π, deformation length, M1 transition characteristics.
1995AN32 Chin.J.Nucl.Phys. 17, No 2, 124 (1995) Microscopic Analysis of Inelastic Proton Scattering Off 28Si NUCLEAR REACTIONS 28Si(p, p), (p, p'), E=22 MeV; measured σ(θ). Local momentum approximation, nucleon-nucleon effective interaction.
1994AN33 Chin.Phys.Lett. 11, 401 (1994) Z.An, Q.Chen, D.Ding, Z.Shi, S.Wan, K.Gao Empirical Effective Interaction in 22 MeV Proton Scattering NUCLEAR REACTIONS 28Si(p, p), (p, p'), E=22 MeV; measured σ(θ); deduced effective interaction parameters. DWBA approach.
doi: 10.1088/0256-307X/11/7/001
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