NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = Li Guangwei Found 100 matches. 2024LI24 Phys.Rev. D 109, 055012 (2024) Complementary LHC searches for UV resonances of the 0νββ decay operators
doi: 10.1103/PhysRevD.109.055012
2023HA40 Commun. Phys. 6, 220 (2023) J.Han, Y.Ye, J.Lou, X.Yang, Q.Li, Z.Yang, Y.Yang, J.Wang, J.Xu, Y.Ge, H.Hua, Z.Li, B.Yang, Y.Liu, S.Bai, K.Ma, J.Chen, G.Li, Z.Hu, H.Yu, Z.Tan, L.Yang, S.Wang, L.Tao, W.Liu, Y.Jiang, J.Li, D.Wang, S.Huang, Y.Chen, W.L.Pu, K.Wei, J.Ma, H.Yang, P.Ma, S.Xu, Z.Bai, S.Jin, F.Duan, Y.Song, L.Hu, Y.Li, J.Li, S.Zhang, M.Huang, D.Wang, Z.Li Nuclear linear-chain structure arises in carbon-14 RADIOACTIVITY 14C(α) [from 1H(14C, 14C'), E=23 MeV/nucleon]; measured decay products, Eα, Iα. 14C; deduced Q-value, excitation energy spectra, resonant states in 14C, J, π, widths, σ(θ). Comparison with the antisymmetrized molecular dynamics (AMD) calculations. The Radioactive Ion Beam Line at the Heavy Ion Research Facility in Lanzhou (HIRFL-RIBLL1).
doi: 10.1038/s42005-023-01342-6
2023LI12 Phys.Rev. C 107, 024611 (2023) Theoretical calculations for the capture cross section of the formation of heavy and superheavy nuclei NUCLEAR REACTIONS 204,206,208Pb, 194,198Pt(12C, X), E(cm)=45-95 MeV;204,206,208Pb(36S, X), E(cm)=130-180 MeV;208Pb(40Ca, X), (48Ca, X), E(cm)=160-210 MeV;238U(12C, X), 232Th(14N, X), 209Bi(15N, X), E(cm)=55-105 MeV;237Np(12C, X), E(cm)=45-105 MeV;238U(14N, X), 204,208Pb(16O, X), 208Pb(18O, X), E(cm)=65-115 MeV;208Pb(19F, X), E(cm)=75-120 MeV;208Pb(26Mg, X), E(cm)=100-150 MeV; 208Pb(28Si, X), E(cm)=120-160 MeV;208Pb(32S, X), 204,206,208Pb(34S, X), E(cm)=135-180 MeV; 192Os, 194Pt(40Ca, X), E(cm)=160-200 MeV;197Au(40Ca, X), (48Ca, X), E(cm)=165-210 MeV;168Er, 170Er(48Ca, X), E(cm)=140-200 MeV;186Os, 194Pt, 197Au(16O, X), E(cm)=60-110;209Bi, 232Th, 238U(16O, X), E(cm)=65-125;208Pb(28Si, X), E(cm)=110-160 MeV;204,206,208Pb(34S, X), 208Pb(32S, X), E(cm)=130-180 MeV;188Os, 197Au, 209Bi(19F, X), E(cm)=72-120 MeV;238U(20Ne, X), E(cm)=90-145 MeV;197Au(27Al, X), (29Al, X), (31Al, X), E(cm)=72-120 MeV;198Pt(28Si, X), E(cm)=115-160 MeV;186W(30Si, X), E(cm)=105-150 MeV;182,184W(32S, X), E(cm)=120-175 MeV;168Er(34S, X), E(cm)=110-150 MeV;180Hf(40Ar, X), E(cm)=135-200 MeV;181Ta(39K, X), (46K, X), E(cm)=140-190 MeV;208Pb(50Ti, X), E(cm)=180-230 MeV;208Pb(52Cr, X), E(cm)=200-250 MeV;238U(36S, X), E(cm)=140-180 MeV;238U(40Ca, X), (48Ca, X), E(cm)=170-220 MeV;246Cm, 248Cm, (48Ca, X), E(cm)=180-230 MeV;209Bi(50Ti, X), E(cm)=190-230 MeV;244Pu(50Ti, X), E(cm)=200-250 MeV;248Cm(26Mg, X), E(cm)=110-150;238U(27Al, X), (30Si, X), E(cm)=120-170 MeV;238U(32S, X), E(cm)=140-195 MeV;238U(35Cl, X), E(cm)=160-210 MeV; calculated capture σ(E) for formation of compound nucleus. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.024611
2023LI14 Phys.Rev. C 107, 025205 (2023) J.-F.Li, C.Chen, G.Li, C.-S.An, C.-R.Deng, J.-J.Xie Quark orbital angular momentum of ground-state octet baryons
doi: 10.1103/PhysRevC.107.025205
2023LI64 Nucl.Instrum.Methods Phys.Res. A1057, 168780 (2023) G.Li, S.Chen, Sh.Jia, Zh.Lu, J.Cai, S.Jiang, Y.Cao, P.Sun, H.Xu, J.Fan, J.Li, S.Jing Prediction of explosives by a de-broadening model based on RBF neural network NUCLEAR REACTIONS C, N, O(n, n'), E not given; analyzed available data; deduced identification in previous explosives identification researches by choosing the inelastic scattering peaks. The radial basis function network (RBF network).
doi: 10.1016/j.nima.2023.168780
2023MA57 Chin.Phys.C 47, 114001 (2023) K.Ma, Y.-L.Ye, Ch.-J.Lin, J.-H.Chen, D.-X.Wang, J.-X.Han, H.-M.Jia, L.Yang, L.-Sh.Yang, Z.-Y.Hu, Y.Chen, W.-L.Pu, G.Li, Zh.-W.Tan, D.-H.Huang, T.-P.Luo, Sh.-H.Zhong, J.-L.Lou, X.-F.Yang, Zh.-H.Li, Q.-T.Li, J.-Y.Xu, Z.-H.Yang, K.Wei New measurement of 4He and proton decays from resonant states in 19Ne RADIOACTIVITY 19N(p), (α) [from 6Li(16O, X)19Ne, E=96 MeV]; measured decay products, Ep, Ip, Eα, Iα; deduced excitation-energy spectra, level energies, resonance parameters for astrophysical applications. The HI-13 tandem accelerator facility at the China Institute of Atomic Energy, Beijing.
doi: 10.1088/1674-1137/acc16f
2023WA01 Chin.Phys.C 47, 014001 (2023) D.-X.Wang, Y.-L.Ye, C.-J.Lin, J.-H.Chen, K.Ma, J.-X.Han, H.-M.Jia, L.Yang, L.-S.Yang, Z.-Y.Hu, Y.Chen, W.-L.Pu, G.Li, Z.-W.Tan, H.-Y.Zhu, T.-P.Luo, S.-H.Zhong, D.-H.Huang, J.-L.Lou, X.-F.Yang, Q.-T.Li, J.-Y.Xu, Z.-H.Yang, K.Wei α-cluster decay from 24Mg resonances produced in the 12C(16O, 24Mg)α reaction RADIOACTIVITY 24Mg(α) [from 12C(16O, 24Mg), E=96 MeV]; measured decay products, Eα, Iα; deduced resonant states, the energy-momentum of a 20Ne fragment, resonance parameters. Comparison with available data, theoretical calculations. The HI-13 tandem accelerator at the China Institute of Atomic Energy (CIAE) in Beijing.
doi: 10.1088/1674-1137/ac9e9a
2023WA35 Eur.Phys.J. A 59, 224 (2023) J.Wang, J.Ren, W.Jiang, X.Ruan, Q.Sun, J.Hu, B.Jiang, J.Bao, Q.Zhang, G.Luan, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, J.Bai, P.Cao, Q.Chen, Y.Chen, Z.Chen, Z.Cui, A.Fan, R.Fan, C.Feng, F.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, Y.Hu, W.Jia, H.Jiang, Z.Jiang, Z.Jin, L.Kang, B.Li, C.Li, G.Li, J.Li, Q.Li, Y.Li, J.Liu, R.Liu, S.Liu, C.Ning, B.Qi, Z.Ren, Z.Song, K.Sun, Z.Tan, J.Tang, S.Tang, L.Wang, P.Wang, Z.Wang, Z.Wen, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, Y.Yu, G.Zhang, L.Zhang, M.Zhang, X.Zhang, Y.Zhang, Y.Zhang, Z.Zhang, M.Zhao, L.Zhou, K.Zhu, J.Zhang Determination of the 232Th(n, γ) cross section from 10 to 200 keV at the Back-n facility at CSNS NUCLEAR REACTIONS 232Th, 197Au(n, γ), E=10-200 keV; measured reaction products, En, In, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VIII.0, CENDL-3.2, JENDL-5 libraries and TALYS 1.96 calculations. The back-streaming white neutron beam-line (Back-n) of China Spallation Neutron Source (CSNS).
doi: 10.1140/epja/s10050-023-01126-0
2023XI11 Phys.Rev. C 108, 064605 (2023) B.L.Xia, J.L.Lou, Y.L.Ye, Z.H.Li, Q.T.Li, H.Hua, X.F.Yang, J.Y.Xu, W.Liu, H.J.Ong, D.T.Tran, N.Aoi, E.Ideguchi, D.Y.Pang, C.X.Yuan, Y.Jiang, B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, G.Li, K.Ma, Z.W.Tan, H.Y.Zhu, H.Y.Ge, W.W.Wan Search for the missing d-wave neutron excitation states in 13B
doi: 10.1103/PhysRevC.108.064605
2023XI12 Phys.Rev. C 108, 065204 (2023) J.-X.Xie, J.-F.Li, Ch.-Sh.An, Ch.-R.Deng, G.Li, J.-J.Xie Intrinsic sea content of the ground state decuplet baryons in the extended chiral constituent quark model
doi: 10.1103/PhysRevC.108.065204
2023ZH17 Phys.Rev. C 107, 045809 (2023) S.Zhang, G.Li, W.Jiang, D.X.Wang, J.Ren, M.Huang, E.T.Li, J.Y.Tang, X.C.Ruan, H.W.Wang, Z.H.Li, Y.S.Chen, L.X.Liu, X.X.Li, Q.W.Fan, R.R.Fan, X.R.Hu, J.C.Wang, X.Li, D.D.Niu, N.Song, M.Gu Measurement of the 159Tb (n, γ) cross section at the CSNS Back-n facility NUCLEAR REACTIONS 159Tb(n, γ), E=0.002-1 MeV; measured neutron Time-of-Flight, Eγ, Iγ; deduced σ(E), resonance parameters, Maxwellian-averaged σ (kT=5-100 keV), astrophysical reaction rate. R-matrix analysis (SAMMY code) to obtain resonance parameters and compare to JEFF-3.3 evaluations, recommended data from Mughabghab and ENDF/B-VIII.0. Comparison of cross-section data to other experimental results, TALYS-1.9 calculations, data from KADoNiS-v0.3, KADoNiS-v1.0, JEFF-3.3, ENDF/B-VIII.0. Analyzed impact of the obtained data on the time evolution of nuclear abundances of 159Tb, 160Tb, 160Dy, 161Dy, 162Dy, 163Dy, 164Dy, 163Ho, 165Ho, 164Er, 166Er, 167Er. Four C6D6 detectors. Neutron beam from Back-n Facility of the China spallation neutron source (CSNS).
doi: 10.1103/PhysRevC.107.045809
2022CH55 Phys.Rev. C 106, 064312 (2022) J.Chen, B.P.Kay, T.L.Tang, I.A.Tolstukhin, C.R.Hoffman, H.Li, P.Yin, X.Zhao, P.Maris, J.P.Vary, G.Li, J.L.Lou, M.L.Avila, Y.Ayyad, S.Bennett, D.Bazin, J.A.Clark, S.J.Freeman, H.Jayatissa, C.Muller-Gatermann, A.Munoz-Ramos, D.Santiago-Gonzalez, D.K.Sharp, A.H.Wuosmaa, C.X.Yuan Probing the quadrupole transition strength of 15C via deuteron inelastic scattering NUCLEAR REACTIONS 1H(15C, p), 2H(15C, d);E=7.1 MeV/nucleon; measured reaction products, Ep, Ip, deuteron spectrum; deduced elastic and inelastic scattering σ(θ). 15C; deduced B(E2), proton quadrupole matrix element, ratio of neutron and proton matrix elements, proton deformation length, core polarization parameters, neutron effective charge; calculated levels, J, π, B(E2), magnetic dipole moments. Comparison to data on 17O and other C isotopes. Ab initio no-core configuration interaction (NCCI) calculations with Daejeon16 interaction. HELIOS spectrometer at ATLAS in-flight facility (Argonne National Laboratory).
doi: 10.1103/PhysRevC.106.064312
2022HA10 Phys.Rev. C 105, 044302 (2022) J.X.Han, Y.Liu, Y.L.Ye, J.L.Lou, X.F.Yang, T.Baba, M.Kimura, B.Yang, Z.H.Li, Q.T.Li, J.Y.Xu, Y.C.Ge, H.Hua, Z.H.Yang, J.S.Wang, Y.Y.Yang, P.Ma, Z.Bai, Q.Hu, W.Liu, K.Ma, L.C.Tao, Y.Jiang, L.Y.Hu, H.L.Zang, J.Feng, H.Y.Wu, S.W.Bai, G.Li, H.Z.Yu, S.W.Huang, Z.Q.Chen, X.H.Sun, J.J.Li, Z.W.Tan, Z.H.Gao, F.F.Duan, J.H.Tan, S.Q.Sun, Y.S.Song Observation of the π2σ2-bond linear-chain molecular structure in 16C NUCLEAR REACTIONS 2H(16C, X)16C/2H/1H/2H/3H/3He/4He/5He/6He/6Li/7Li/8Li/9Li/7Be/8Be/9Be/10Be/11Be/12Be, E=23.5 MeV/nucleon; measured reaction products, recoil 2H, 8Be and other outgoing particles; deduced Q-value spectra for breakup of excited states of 16C into 4He+12Be and 6He+10Be channels, angular correlation between 4He and 12Be decay fragments from the 16.5 MeV resonance in 16C, and 6He and 10Be fragments from the 19.4 MeV resonance in 16C. 16C; deduced excitation energy spectra reconstructed from 4He+12Be+2 H and 6He+10Be+2H channels, levels, resonances, total width. Comparison with previous experimental data, and with antisymmetrized molecular dynamics (AMD) theoretical calculations. Secondary 16C beam produced in 9Be(18O, X), E=59.6 MeV/nucleon primary reaction at the HIRFL-RIBLL facility in Lanzhou.
doi: 10.1103/PhysRevC.105.044302
2022LI15 Phys.Rev. C 105, 034613 (2022) W.Liu, J.L.Lou, Y.L.Ye, S.M.Wang, Z.W.Tan, Z.H.Li, Q.T.Li, H.Hua, X.F.Yang, J.Y.Xu, H.J.Ong, D.T.Tran, N.Aoi, E.Ideguchi, D.Y.Pang, C.X.Yuan, Y.Jiang, B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, G.Li, K.Ma, H.Y.Zhu, B.L.Xia New investigation of low-lying states in 12Be via a 2H(13B, 3He) reaction NUCLEAR REACTIONS 2H(13B, d), (13B, 3He), E=23 MeV/nucleon; measured reaction products, deuteron spectra, 3He spectra, angular distributions; deduced σ(θ), optical potential parameters. 12Be; deduced levels, J, π, spectroscopic factors, resonance widths. DWBA analysis. Comparison to various calculations in particular to one using the shell model with the YSOX interaction and Gamow coupled-channel (GCC) approach (for the resonance widths). Secondary beam from 18O(9Be, X), E=60 MeV/nucleon (RCNP, Osaka).
doi: 10.1103/PhysRevC.105.034613
2022OR04 Phys.Rev. C 106, 064301 (2022) R.Orlandi, H.Makii, K.Nishio, K.Hirose, M.Asai, K.Tsukada, T.K.Sato, Y.Ito, F.Suzaki, Y.Nagame, A.N.Andreyev, E.Ideguchi, N.Aoi, T.T.Pham, S.Q.Yan, Y.P.Shen, B.Gao, G.Li New K isomers in 248Cf NUCLEAR REACTIONS 249Cf(18O, 19O)248Cf, E=140.4 MeV; measured reaction products, Eγ, Iγ, γγ-coin, particleγ-coin. 248Cf; deduced levels, J, π, transitions from isomeric states, T1/2 for 2 low-ling transitions, B(E1). Discussed possible configuration of newly observed isomeric state at 950 keV to be two-quasineutron K=8- and the two-quasiproton K=5-. Comparison to other experimental data. Radioactive target. Si-detectors array combined with γ-ray detector array consisted of 4 Ge detectors and 4 4x5 inch LaBr3 scintillators at Tokai Tandem accelerator facility of the Japan Atomic Energy Agency (JAEA).
doi: 10.1103/PhysRevC.106.064301
2022QI02 Phys.Rev. C 105, 065204 (2022) R.Qi, J.-B.Wang, G.Li, C.-S.An, C.-R.Deng, J.-J.Xie Investigations on the flavor-dependent axial charges of the octet baryons
doi: 10.1103/PhysRevC.105.065204
2022RE10 Phys.Rev. C 106, 014320 (2022) K.Rezynkina, D.D.Dao, G.Duchene, J.Dudouet, F.Nowacki, E.Clement, A.Lemasson, C.Andreoiu, A.Astier, G.de Angelis, G.de France, C.Delafosse, I.Deloncle, F.Didierjean, Z.Dombradi, C.Ducoin, A.Gadea, A.Gottardo, D.Guinet, B.Jacquot, P.Jones, T.Konstantinopoulos, I.Kuti, A.Korichi, S.M.Lenzi, G.Li, F.Le Blanc, C.Lizarazo, R.Lozeva, G.Maquart, B.Million, C.Michelagnoli, D.R.Napoli, A.Navin, R.M.Perez-Vidal, C.M.Petrache, N.Pietralla, D.Ralet, M.Ramdhane, M.Rejmund, O.Stezowski, C.Schmitt, D.Sohler, D.Verney Structure of 83As, 85As, and 87As: From semimagicity to γ softness NUCLEAR REACTIONS 9Be(238U, X)83As/85As/87As, E=6.2 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin, γγ-coin using the VAMOS++ spectrometer for particle detection and AGATA array for γ radiation at GANIL facility. 83,85,87As; deduced levels, J, π, collectivity in a prolate deformed, γ-soft regime in the open shell nuclei. Comparison with shell-model calculations. Systematics of energies of 9/2+ states in 83,85,87,89As, 85,87,89,91Br, 87,89,91,93Rb, 89,91,93,95Y from experimental data and large-scale shell-model calculations. NUCLEAR STRUCTURE 85,87As; calculated levels, J, π, potential energy surfaces (PES) in (β, γ) planes, wave functions amplitudes in K-quantum numbers. Large-scale shell-model calculations, SU3 symmetries, and beyond mean-field calculations.
doi: 10.1103/PhysRevC.106.014320
2022TA09 Chin.Phys.C 46, 054001 (2022) Z.W.Tan, J.L.Lou, Y.L.Ye, Y.Liu, D.Y.Pang, C.X.Yuan, J.G.Li, W.Liu, Y.Jiang, B.Yang, L.C.Tao, K.Ma, Z.H.Li, Q.T.Li, X.F.Yang, J.Y.Xu, H.Z.Yu, J.X.Han, S.W.Bai, S.W.Huang, G.Li, H.Y.Wu, H.L.Zang, J.Feng, J.S.Wang, Y.Y.Yang, P.Ma, Q.Hu, Z.Bai, Z.H.Gao, F.F.Duan, L.Y.Hu, J.H.Tan, S.Q.Sun, Y.S.Song, H.J.Ong, D.T.Tran, H.Y.Zhu, B.L.Xia Investigation of negative-parity states in 16C via deuteron inelastic scattering NUCLEAR REACTIONS 16C(d, d'), E=59.6 MeV/nucleon; measured reaction products; deduced σ(θ), optical model potentials, deformation lengths, energy levels, J, π. Comparison with the distorted-wave Born approximation (DWBA) and shell model calculations. The Radioactive Ion Beam Line in Lanzhou (RIBLL), Institute of Modern Physics (IMP), China.
doi: 10.1088/1674-1137/ac488b
2022YA30 Fusion Sci. Technol. 78, 164 (2022) W.Yang, G.Li, X.Gong, X.Gao, X.Li, H.Li, S.Liu Effect of the Fusion Fuels' Polarization on Neutron Wall Loading DistrIbution in CFETR NUCLEAR REACTIONS 3H(polarized d, n), (d, n), E not given; analyzed available data; calculated the neutron source and neutron wall loading (NWL) distributions and investigate the effect of spin polarization on them. The China Fusion Engineering Test Reactor (CFETR) is a new superconducting tokamak device being designed in China, aiming to bridge the gaps between ITER and future fusion power plants.
doi: 10.1080/15361055.2021.1969064
2021LI64 Phys.Rev. C 104, 064605 (2021) W.Liu, J.L.Lou, Y.L.Ye, Z.H.Li, Q.T.Li, H.Hua, X.F.Yang, J.Y.Xu, H.J.Ong, D.T.Tran, N.Aoi, E.Ideguchi, D.Y.Pang, C.X.Yuan, S.M.Wang, Y.Jiang, B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, G.Li, K.Ma, Z.W.Tan, H.Y.Zhu, B.L.Xia s- and d-wave intruder strengths in 13Bg.s. via the 1H(13B, d)12B reaction NUCLEAR REACTIONS 1H(13B, p), (13B, d)12B, E=23 MeV/nucleon, [13B secondary beam from 9Be(18O, X), E=58 MeV/nucleon]; measured reaction products, E(d), I(d), E(p), I(p), σ(θ), (particle)(particle)-coin using four sets of charged-particle telescopes of double-sided silicon strip (DSSD) detectors at RCNP-Osaka accelerator facility. 12,13B; analyzed optical potential parameters for low energy elastic scattering and single-neutron transfer reaction. 13B; deduced levels, J, π, L-transfers from σ(θ) distributions relative spectroscopic factors, s- and d-wave intruder strengths in the ground state; calculated p-, s-, and d-wave intensities from the shell model with the YSOX interaction and Gamow coupled-channel (GCC) approach. Comparison with systematics of p-, s-, and d-wave intensities in the ground state of 12Be, 13B and 14C.
doi: 10.1103/PhysRevC.104.064605
2021YU05 Phys.Rev. C 104, 035201 (2021) Z.Yu, M.Song, J.-Y.Guo, Y.Zhang, G.Li Probing double hadron resonances by the complex scaling method
doi: 10.1103/PhysRevC.104.035201
2020LI01 Ann.Nucl.Energy 135, 106932 (2020) G.Li, G.Bentoumi, K.Hartling, I.Molnar, C.Neggers, R.Rogge, Z.Yamani Validation of ENDF/B-VIII thermal neutron scattering data of heavy water by differential cross section measurements at various temperatures NUCLEAR REACTIONS 2H, O(n, n), E thermal; measured reaction products, En, In; deduced temperature-dependent thermal neutron differential scattering cross sections for heavy water (D2O). Comparison with the D2O data libraries from the ENDF/B-VII.1 evaluation and the recently released ENDF/B-VIII.0 evaluation.
doi: 10.1016/j.anucene.2019.07.034
2020LI14 Phys.Rev.Lett. 124, 192501 (2020) Y.Liu, Y.L.Ye, J.L.Lou, X.F.Yang, T.Baba, M.Kimura, B.Yang, Z.H.Li, Q.T.Li, J.Y.Xu, Y.C.Ge, H.Hua, J.S.Wang, Y.Y.Yang, P.Ma, Z.Bai, Q.Hu, W.Liu, K.Ma, L.C.Tao, Y.Jiang, L.Y.Hu, H.L.Zang, J.Feng, H.Y.Wu, J.X.Han, S.W.Bai, G.Li, H.Z.Yu, S.W.Huang, Z.Q.Chen, X.H.Sun, J.J.Li, Z.W.Tan, Z.H.Gao, F.F.Duan, J.H.Tan, S.Q.Sun, Y.S.Song Positive-Parity Linear-Chain Molecular Band in 16C NUCLEAR REACTIONS 2H(16C, X)2H, E=23.5 MeV/nucleon; measured reaction products, Eα, Iα. 16C; deduced excitation energies, spin parities, total decay widths of the resonances in 16C. Comparison with AMD calculations.
doi: 10.1103/PhysRevLett.124.192501
2019DU18 Phys.Rev. C 100, 011301 (2019) J.Dudouet, A.Lemasson, G.Maquart, F.Nowacki, D.Verney, M.Rejmund, G.Duchene, O.Stezowski, E.Clement, C.Michelagnoli, A.Korichi, C.Andreoiu, A.Astier, G.de Angelis, G.de France, C.Delafosse, I.Deloncle, F.Didierjean, Z.Dombradi, C.Ducoin, A.Gadea, A.Gottardo, D.Guinet, B.Jacquot, P.Jones, T.Konstantinopoulos, I.Kuti, F.Le Blanc, S.M.Lenzi, G.Li, R.Lozeva, B.Million, D.R.Napoli, A.Navin, R.M.Perez-Vidal, C.M.Petrache, D.Ralet, M.Ramdhane, N.Redon, C.Schmitt, D.Sohler Excitations of the magic N=50 neutron-core revealed in 81Ga NUCLEAR REACTIONS 9Be(238U, F)72Ga/73Ga/74Ga/75Ga/76Ga/77Ga/78Ga/79Ga/80Ga/81Ga/82Ga/83Ga/81Ge/81As/81Se, E=6.2 MeV/nucleon; measured yields of fission fragments, Eγ, Iγ, (fragment)γ- and γγ-coin using the VAMOS++ spectrometer for fragment identification and AGATA array for γ detection at GANIL. 81Ga; deduced high-spin levels, J, π. Systematics of shell gap in N=50 isotones: 78Ni, 79Cu, 80Zn, 81Ga, 82Ge, 83As, 84Se. Comparison with state-of-the-art large-scale shell model (LSSM) calculations. NUCLEAR STRUCTURE 78Ni, 81Ga; calculated levels, J, π and decomposition of the wave functions for states in the two nuclide. Large-scale shell model (LSSM) calculations.
doi: 10.1103/PhysRevC.100.011301
2018AN13 Phys.Rev. C 98, 045201 (2018) Decay patterns of low-lying Nss-bar states via strangeness channels
doi: 10.1103/PhysRevC.98.045201
2018CH38 Phys.Rev. C 98, 014616 (2018) J.Chen, J.L.Lou, Y.L.Ye, Z.H.Li, D.Y.Pang, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, F.R.Xu, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, Y.Zhang, G.Li, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki Low-lying states in 12Be using one-neutron transfer reaction NUCLEAR REACTIONS 1,2H(11Be, 11Be), (11Be, p), E=26.9 MeV/nucleon; measured recoils, Ep, Ip, p(θ), Eγ and Iγ from decay of recoils, (recoil)p-coin, differential σ(θ) for low-lying 0+, 2+ and 1- states in 12Be, half-life of excited 0+ isomer by decay-tagging method using (CH2)n and (CD2)n targets, annular silicon detectors (ADSSD) for protons, detector telescopes for charged particle detection, and scintillation detectors for γ detection, and isomer-tagging method at RCNP-Osaka. DWBA analysis of σ(θ) data. 12Be; deduced levels, J, π, spectroscopic factors, single-particle components in the g.s. and excited 0+ state. Comparison with shell-model calculations, and with previous experimental results. 11,12Be; calculated B(E2), B(E1), S(n) and S(2n) from shell-model, and compared with experimental data in literature.
doi: 10.1103/PhysRevC.98.014616
2018JI04 Chin.Phys.Lett. 35, 082501 (2018) Y.Jiang, J.-L.Lou, Y.-L.Ye, D.-Y.Pang, J.Chen, Z.-H.Li, Y.-C.Ge, Q.-T.Li, J.Li, W.Jiang, Y.-Le.Sun, H.-L.Zang, Y.Zhang, W.Liu, Y.-D.Chen, G.Li, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.-N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki, T.T.Nguyen A New Measurement of 11Be(p, d) Transfer Reaction NUCLEAR REACTIONS 1H(11Be, d), E=26.9 MeV/nucleon; measured reaction products. 10Be; deduced Q-value spectrum, σ(θ), spectroscopic factors to 0+ and 2+. Comparison with theoretical calculations.
doi: 10.1088/0256-307X/35/8/082501
2017DU05 Phys.Rev.Lett. 118, 162501 (2017) J.Dudouet, A.Lemasson, G.Duchene, M.Rejmund, E.Clement, C.Michelagnoli, F.Didierjean, A.Korichi, G.Maquart, O.Stezowski, C.Lizarazo, R.M.Perez-Vidal, C.Andreoiu, G.de Angelis, A.Astier, C.Delafosse, I.Deloncle, Z.Dombradi, G.de France, A.Gadea, A.Gottardo, B.Jacquot, P.Jones, T.Konstantinopoulos, I.Kuti, F.Le Blanc, S.M.Lenzi, G.Li, R.Lozeva, B.Million, D.R.Napoli, A.Navin, C.M.Petrache, N.Pietralla, D.Ralet, M.Ramdhane, N.Redon, C.Schmitt, D.Sohler, D.Verney, D.Barrientos, B.Birkenbach, I.Burrows, L.Charles, J.Collado, D.M.Cullen, P.Desesquelles, C.Domingo Pardo, V.Gonzalez, L.Harkness-Brennan, H.Hess, D.S.Judson, M.Karolak, W.Korten, M.Labiche, J.Ljungvall, R.Menegazzo, D.Mengoni, A.Pullia, F.Recchia, P.Reiter, M.D.Salsac, E.Sanchis, Ch.Theisen, J.J.Valiente-Dobon, M.Zielinska 9636Kr60-Low-Z Boundary of the Island of Deformation at N=60 NUCLEAR REACTIONS 9Be(238U, X)96Kr, E=6.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, R4/2. Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.118.162501
2017WA32 Phys.Rev. C 96, 034611 (2017) T.Wang, G.Li, L.Zhu, O.Hen, G.Zhang, Q.Meng, L.Wang, H.Han, H.Xia Aspects of charge distribution measurement for 252Cf(sf) RADIOACTIVITY 252Cf(SF); measured charge distribution and yields of fission fragments of Z=33-43, charge dispersion of A=101 nuclei 101Y, 101Zr, 101Nb, 101Mo, and 101Tc using grid-ionization chamber (GIC) and a gas ΔE-E detector coupled with a surface-barrier detector; deduced kinetic energy averaged widths as function of atomic mass A, widths of charge distributions, Charge polarization as a function of the mass number of primary fission fragments, average most probable charge as a function of mass number of light fragments. Comparison with theoretical calculations.
doi: 10.1103/PhysRevC.96.034611
2016WA03 Phys.Rev. C 93, 014606 (2016) T.Wang, G.Li, L.Zhu, Q.Meng, L.Wang, H.Han, W.Zhang, H.Xia, L.Hou, R.Vogt, J.Randrup Correlations of neutron multiplicity and γ-ray multiplicity with fragment mass and total kinetic energy in spontaneous fission of 252Cf RADIOACTIVITY 252Cf(SF); measured E(n), I(n), Eγ, Iγ; deduced total kinetic energy (TKE), neutron and γ-ray multiplicities, correlations of neutron and γ-ray multiplicities, ratio of average γ-ray yield to the average neutron multiplicity as function of fragment mass, γ-ray multiplicity as a function of the total fragment kinetic energy TKE.
doi: 10.1103/PhysRevC.93.014606
2016WA27 Phys.Rev. C 94, 044913 (2016) R.-Q.Wang, J.Song, K.-J.Sun, L.-W.Chen, G.Li, F.-L.Shao Hidden-charm pentaquark states in heavy ion collisions at energies available at the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.94.044913
2016WE06 Ann.Nucl.Energy 94, 576 (2016) Nuclear emulsion measuring the prompt fission neutron spectrum of 238U induced by 2.8 MeV neutrons NUCLEAR REACTIONS 238U(n, F), E=2.8 MeV; measured reaction products, Ep, Ip; deduced prompt fission neutron spectrum. Comparison with calculations using Maxwell and Watt models.
doi: 10.1016/j.anucene.2016.03.017
2015FA06 Hyperfine Interactions 230, 155 (2015) P.Fan, H.Zhang, D.Yuan, Y.Zheng, Y.Zuo, Q.Zhang, X.Ma, X.Wu, G.Li, L.Zhu, Q.Fan, J.Liang, X.Zhang, S.Zhu g-factor measurements of high spin states in 108Cd NUCLEAR REACTIONS 76Ge(37Cl, 4np), E=135 MeV; measured reaction products, Eγ, Iγ; deduced energy levels, J, π, g-factors. Comparison with theoretical calculations.
doi: 10.1007/s10751-015-1123-2
2015LI46 Sci. Rep. 5, 15790 (2015) High-Gain High-Field Fusion Plasma
doi: 10.1038/srep15790
2015ST15 Phys.Rev.Lett. 115, 182501 (2015) M.G.Sternberg, R.Segel, N.D.Scielzo, G.Savard, J.A.Clark, P.F.Bertone, F.Buchinger, M.Burkey, S.Caldwell, A.Chaudhuri, J.E.Crawford, C.M.Deibel, J.Greene, S.Gulick, D.Lascar, A.F.Levand, G.Li, A.Perez Galvan, K.S.Sharma, J.Van Schelt, R.M.Yee, B.J.Zabransky Limit on Tensor Currents from 8Li β Decay RADIOACTIVITY 8Li(β-) [from 7Li(d, p), E not given]; measured decay products, Eβ, Iβ, Eα, Iα. 6He; deduced β-ν-α correlations. Comparison with available data.
doi: 10.1103/PhysRevLett.115.182501
2014SC11 Nucl.Data Sheets 120, 70 (2014) N.D.Scielzo, R.M.Yee, P.F.Bertone, F.Buchinger, S.A.Caldwell, J.A.Clark, A.Czeszumska, C.M.Deibel, J.P.Greene, S.Gulick, D.Lascar, A.F.Levand, G.Li, E.B.Norman, S.Padgett, M.Pedretti, A.Perez Galvan, G.Savard, R.E.Segel, K.S.Sharma, M.G.Sternberg, J.Van Schelt, B.J.Zabransky A Novel Approach to β-delayed Neutron Spectroscopy Using the Beta-decay Paul Trap RADIOACTIVITY 137I(β-); measured decay products, Eβ, Iβ.; deduced neutron energy spectrum and branching ratio. Comparison with available data.
doi: 10.1016/j.nds.2014.07.009
2014YA19 J.Phys.(London) G41, 105104 (2014) H.Yang, L.Ma, Z.Zhang, L.Yu, G.Jia, M.Huang, Z.Gan, T.Huang, G.Li, X.Wu, Y.Fang, Z.Wang, B.Gao, W.Hua Experiment for synthesis of neutron-deficient protactinium isotopes NUCLEAR REACTIONS 175,176Lu(40Ca, X)201Po/203At/205Rn/206Rn/207Rn/208Rn/206Fr/207Fr/208Fr/209Fr/210Fr/211Fr/209Ra/210Ra/211Ra/212Ra/210Ac/211Ac/212Ac/212Pa/214Pa/211Th/214Th/216TH, E=193 MeV; measured reaction products, Eα, Iα; deduced α-particles energies, σ. Comparison with available data. RADIOACTIVITY 208,209,210,211,212Ac, 212,214Pa, 211,214,216Th(α); measured decay products, Eα, Iα; deduced T1/2. Comparison with available data.
doi: 10.1088/0954-3899/41/10/105104
2013HE08 Phys.Rev. C 87, 034320 (2013), Erratum Phys.Rev. C 102, 029903 (2020) C.He, S.Shen, S.Wen, L.Zhu, X.Wu, G.Li, Y.Zhao, Y.Yan, Z.Bai, Y.Wu, Y.Li, G.Li, S.Yan, M.Oshima, Y.Toh, A.Osa, M.Koizumi, Y.Hatsukawa, M.Matsuda, T.Hagakawa Signature splitting inversion and backbending in 80Rb NUCLEAR REACTIONS 65Cu(19F, 3np), E=75 MeV; 66Zn(18O, 3np), E=76 MeV; 68Zn(16O, 3np), E=80 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) at CIAE and JAERI facilities. 80Rb; deduced high-spin levels, J, π, bands, alignments, signature splitting and inversion. Comparison with structures of 78Rb and 82Y nuclei. Calculated total Routhian surface (TRS) plots. Projected shell-model calculations.
doi: 10.1103/PhysRevC.87.034320
2013LI12 Phys.Rev.Lett. 110, 092502 (2013) G.Li, R.Segel, N.D.Scielzo, P.F.Bertone, F.Buchinger, S.Caldwell, A.Chaudhuri, J.A.Clark, J.E.Crawford, C.M.Deibel, J.Fallis, S.Gulick, G.Gwinner, D.Lascar, A.F.Levand, M.Pedretti, G.Savard, K.S.Sharma, M.G.Sternberg, T.Sun, J.Van Schelt, R.M.Yee, B.J.Zabransky Tensor Interaction Limit Derived From the α-β-ν(bar) Correlation in Trapped 8Li Ions RADIOACTIVITY 8Li(β-) [from 7Li(d, p), E=24 MeV]; measured decay products, Eα, Iα; deduced α-β-ν correlation in the Gamow-Teller decay, limit on tensor component contribution.
doi: 10.1103/PhysRevLett.110.092502
2013SH50 Sci. Rep. 3, 2740 (2013) S.Shen, G.Han, S.Wen, X.Kang, Y.Yan, Z.Bai, Y.Wu, X.Wu, L.Zhu, G.Li, C.He High-Spin States and Level Structure in Stable Nucleus Strontium-84 NUCLEAR REACTIONS 70Zn(18O, 4n)84Sr, E=75 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies and relative intensities, J, π, directional correlations of oriented states (DCO) ratios, partial level scheme. Comparison with total-Routhian-surface (TRS) calculations. HI-13 Tandem Accelerator at China Institute of Atomic Energy (CIAE).
doi: 10.1038/srep02740
2013VA12 Phys.Rev.Lett. 111, 061102 (2013) J.Van Schelt, D.Lascar, G.Savard, J.A.Clark, P.F.Bertone, S.Caldwell, A.Chaudhuri, A.F.Levand, G.Li, G.E.Morgan, R.Orford, R.E.Segel, K.S.Sharma, M.G.Sternberg First Results from the CARIBU Facility: Mass Measurements on the r-Process Path ATOMIC MASSES 130,131In, 130,131,132,133,134,135Sn, 131,132,133,134,135,136,137Sb, 133,135,136,137,138,139,140Te, 133,134,135,139,140,141I, 142,143,144,145,146Cs; measured TOF ion cyclotron resonances, cyclotron frequency; deduced mass excess. Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.111.061102
2013YE02 Phys.Rev.Lett. 110, 092501 (2013) R.M.Yee, N.D.Scielzo, P.F.Bertone, F.Buchinger, S.Caldwell, J.A.Clark, C.M.Deibel, J.Fallis, J.P.Greene, S.Gulick, D.Lascar, A.F.Levand, G.Li, E.B.Norman, M.Pedretti, G.Savard, R.E.Segel, K.S.Sharma, M.G.Sternberg, J.Van Schelt, B.J.Zabransky β-Delayed Neutron Spectroscopy Using Trapped Radioactive Ions RADIOACTIVITY 137I(β-n) [from 252Cf(SF)];measured decay products, TOF, Eβ, Iβ, Eγ, Iγ, En, In; deduced βn branching ratios. Linear Paul trap.
doi: 10.1103/PhysRevLett.110.092501
2012SC09 Nucl.Instrum.Methods Phys.Res. A681, 94 (2012) N.D.Scielzo, G.Li, M.G.Sternberg, G.Savard, P.F.Bertone, F.Buchinger, S.Caldwell, J.A.Clark, J.Crawford, C.M.Deibel, J.Fallis, J.P.Greene, S.Gulick, A.A.Hecht, D.Lascar, J.K.P.Lee, A.F.Levand, M.Pedretti, R.E.Segel, H.Sharma, K.S.Sharma, I.Tanihata, J.Van Schelt, R.M.Yee, B.J.Zabransky The β-decay Paul trap: A radiofrequency-quadrupole ion trap for precision β-decay studies RADIOACTIVITY 8Li(β-), (α); measured decay products, Eβ, Iβ, Eα, Iα, nuclear recoils; deduced technique for the β-ν angular correlations.
doi: 10.1016/j.nima.2012.04.035
2012VA02 Phys.Rev. C 85, 045805 (2012) J.Van Schelt, D.Lascar, G.Savard, J.A.Clark, S.Caldwell, A.Chaudhuri, J.Fallis, J.P.Greene, A.F.Levand, G.Li, K.S.Sharma, M.G.Sternberg, T.Sun, B.J.Zabransky Mass measurements near the r-process path using the Canadian Penning Trap mass spectrometer ATOMIC MASSES 133,134Sb, 134,135,136,137Te, 135,136,137,138,139I, 137,138,139,140,141Xe, 141,142Cs, 153,155Pr, 153,155,157Nd, 153,155,156,157,158,159Pm, 155,157,158,159,160,161Sm, 158,159,160,161Eu, 163Gd; measured cyclotron frequency ratios; deduced mass excess, atomic masses. Canadian Penning Trap mass spectrometer at ANL. Comparison with AME-2003 evaluation and theoretical mass models. Systematics of S(2n) values.
doi: 10.1103/PhysRevC.85.045805
2011CH66 J.Phys.:Conf.Ser. 312, 042009 (2011) A.Chaudhuri, P.F.Bertone, F.Buchinger, S.Caldwell, J.A.Clark, J.E.Crawford, C.M.Deibel, S.Gulick, D.Lascar, A.F.Levand, G.Li, G.Savard, R.E.Segel, K.S.Sharma, M.G.Sternberg, T.Sun, J.Van Schelt Studies of neutron-rich nuclei using the CPT mass spectrometer at CARIBU
doi: 10.1088/1742-6596/312/4/042009
2011FA10 Phys.Rev. C 84, 045807 (2011) J.Fallis, J.A.Clark, K.S.Sharma, G.Savard, F.Buchinger, S.Caldwell, A.Chaudhuri, J.E.Crawford, C.M.Deibel, S.Gulick, A.A.Hecht, D.Lascar, J.K.P.Lee, A.F.Levand, G.Li, B.F.Lundgren, A.Parikh, S.Russell, M.Scholte-van de Vorst, N.D.Scielzo, R.E.Segel, H.Sharma, S.Sinha, M.G.Sternberg, T.Sun, I.Tanihata, J.Van Schelt, J.C.Wang, Y.Wang, C.Wrede, Z.Zhou Mass measurements of isotopes of Nb, Mo, Tc, Ru, and Rh along the Νp- and rp-process paths using the Canadian Penning trap mass spectrometer ATOMIC MASSES 87Nb, 87,90,91,92Mo, 90,91,92,93Tc, 90,91,92,93,94Ru, 92,93,94,95Rh; measured cyclotron frequency ratios using Canadian Penning trap mass spectrometer; deduced mass excesses. 88Tc; deduced S(p). Comparison with previous measurements and AME-2003. Z=42-47, A=87-96; analyzed systematics of S(2p) values. Z=42-45, N=45-52; analyzed systematics of S(2n) values. Z=42-45, A=87-95; analyzed systematics of S(p) values. 94mAg; discussed 2p decay mode of 21+ isomer. NUCLEAR REACTIONS 58Ni(40Ca, X)87Nb/87Mo/90Mo/92Mo/90Tc/90Tc/92Tc/93Tc/90Ru/91Ru/92Ru/93Ru/92Rh/93Rh/94Rh, E=185, 190, 200 MeV; 58Ni(36Ar, X)91Tc/91Ru, E=125 MeV; Ni(36Ar, X)90Mo/91Mo/90Tc/91Tc/92Tc/91Ru/92Ru, E=130, 150 MeV; Ni(40Ca, X)93Tc/93Ru/94Ru/94Rh/95Rh, E=170 MeV; measured yields at ATLAS facility.
doi: 10.1103/PhysRevC.84.045807
2010FA08 Nucl.Phys. A834, 107c (2010) P.Fan, D.Yuan, Y.Zheng, Y.Zuo, D.Zhou, X.Wu, Gu.Li, L.Zhu, G.Xu, Q.Fan, X.Zhang, S.Zhu Experimental and Theoretical Study of Quasi-Particle Alignment in 82Sr NUCLEAR REACTIONS 58Ni(28Si, 4p), E=110 MeV; measured Eγ, Iγ. 82Sr; deduced g factor, rotational bands. Comparison with particle rotor model with Nilsson potential.
doi: 10.1016/j.nuclphysa.2010.01.032
2010SH12 Phys.Rev. C 82, 014306 (2010), Erratum Phys.Rev. C 91, 029902 (2015) S.Shen, G.Han, S.Wen, F.Pan, J.Zhu, J.Gu, J.P.Draayer, X.Wu, L.Zhu, C.He, G.Li, B.Yu, T.Wen, Y.Yan High-spin states and level structure in 84Rb NUCLEAR REACTIONS 70Zn(18O, 3np), E=75 MeV; measured Eγ, Iγ, γγ-coin, DCO. 84Rb; deduced levels, J, π, multipolarities, bands, configurations, kinematic moments of inertia. Total Routhian surface calculations. Comparison with projected shell-model calculations, and with structures of 80,82Rb.
doi: 10.1103/PhysRevC.82.014306
2009SC19 Phys.Rev. C 80, 025501 (2009) N.D.Scielzo, S.Caldwell, G.Savard, J.A.Clark, C.M.Deibel, J.Fallis, S.Gulick, D.Lascar, A.F.Levand, G.Li, J.Mintz, E.B.Norman, K.S.Sharma, M.Sternberg, T.Sun, J.Van Schelt Double-β-decay Q values of 130Te, 128Te, and 120Te ATOMIC MASSES 128,129,130,131,132Xe, 120,128,130Te, 120Sn; measured mass differences of 120Te-120Sn, 128Te-128Xe, 130Te-130Xe and 132Xe-129Xe pairs using Penning Trap mass spectrometer. RADIOACTIVITY 120Te(2β+); 128,130Te(2β-); measured parent-daughter mass differences by Penning-trap spectrometer; deduced Q values.
doi: 10.1103/PhysRevC.80.025501
2008FA11 Phys.Rev. C 78, 022801 (2008) J.Fallis, J.A.Clark, K.S.Sharma, G.Savard, F.Buchinger, S.Caldwell, J.E.Crawford, C.M.Deibel, J.L.Fisker, S.Gulick, A.A.Hecht, D.Lascar, J.K.P.Lee, A.F.Levand, G.Li, B.F.Lundgren, A.Parikh, S.Russell, M.Scholte-van de Vorst, N.D.Scielzo, R.E.Segel, H.Sharma, S.Sinha, M.Sternberg, T.Sun, I.Tanihata, J.Van Schelt, J.C.Wang, Y.Wang, C.Wrede, Z.Zhou Determination of the proton separation energy of 93Rh from mass measurements ATOMIC MASSES 92Ru, 93Rh; measured masses; deduced mass excesses, proton separation energies. Penning trap method.
doi: 10.1103/PhysRevC.78.022801
2007YU03 Hyperfine Interactions 180, 49 (2007) D.Yuan, Y.Zheng, D.Zhou, Y.Zuo, P.Fan, M.Liu, X.Wu, L.Zhu, G.Li, G.Xu, Q.Fan, X.Zhang, S.Zhu g-Factors of magnetic-rotational states in 85Zr NUCLEAR REACTIONS 60Ni(28Si, n2p), E=98 MeV; measured Eγ, Iγ(θ), g-factors for high spin states.
doi: 10.1007/s10751-008-9684-y
2005LI63 Phys.Rev. C 72, 067301 (2005) G.Liang, S.Wang, Y.Liu, Y.Ma, J.Lu, M.Li, X.Cui, G.Zhao, X.Li, X.Wu, L.Zhu, G.Li, S.Wen, C.Yang Gallagher-Moszkowski (GM) doublet bands in 162Ho NUCLEAR REACTIONS 160Gd(7Li, 5n), E=49 MeV; measured Eγ, Iγ, γγ-coin. 162Ho deduced high-spin levels, J, π, B(M1)/B(E2), configurations.
doi: 10.1103/PhysRevC.72.067301
2002LI20 Appl.Radiat.Isot. 56, 731 (2002) G.Li, Z.Pu, X.Kong, F.Zhang, X.Zhu Cross Section Measurements for (n, 3n) Reactions Induced by 14.8 MeV Neutrons NUCLEAR REACTIONS 209Bi, 191Ir, 151Eu, 185Re(n, 3n), E=14.8 MeV; measured σ. Activation technique.
doi: 10.1016/S0969-8043(01)00247-0
2001YI03 Eur.Phys.J. A 11, 379 (2001) L.Yin, Y.Liu, J.Lu, G.Zhao, X.Li, X.Wu, G.Li, S.Wen, C.Yang High-Spin States in 160Lu NUCLEAR REACTIONS 144Sm(19F, 3n), E=90 MeV; measured Eγ, γγ-coin. 160Lu deduced high-spin levels, J, π, band features, B(M1), B(E2). Comparison with neighboring nuclides.
doi: 10.1007/s100500170049
2000LU15 Phys.Rev. C62, 057304 (2000) J.Lu, Y.Liu, L.Yin, G.Zhao, F.Zhang, X.Li, R.Meng, Z.Wang, Y.Ma, Z.Wang, J.Huo, X.Wu, S.Wen, G.Li, C.Yang Spin Assignment for the πh11/2 (x) νh11/2 Yrast Band in Odd-Odd 124Cs NUCLEAR REACTIONS 116Sn(11B, 3n), E=45 MeV; measured Eγ, Iγ, γγ-coin. 124Cs deduced high-spin levels, J, π, configurations.
doi: 10.1103/PhysRevC.62.057304
2000ZH51 Eur.Phys.J. A 9, 299 (2000) G.Zhao, Y.Liu, J.Lu, Y.Ma, L.Yin, X.Li, Z.Li, X.Wu, G.Li, S.Wen, C.Yang High-Spin States in 166Lu NUCLEAR REACTIONS 152Sm(19F, 5n), E=97 MeV; measured Eγ, Iγ, γγ-coin. 166Lu deduced high-spin levels, J, π, rotational bands configuration, alignment. NUCLEAR STRUCTURE 162,164Tm, 166,168,170Lu, 170,172,174,176Ta, 176,178Re, 180Ir; compiled, analyzed rotational band signature splitting based on π[541]1/2 coupled to ν i13/2 orbitals; deduced N and Z dependence.
doi: 10.1007/s100500070012
1999HA67 High Energy Phys. and Nucl.Phys. (China) 23, 601 (1999) G.Han, S.Wen, X.Liu, X.Wu, G.Li, G.Yuan, P.Weng, C.Yang, Y.Ma, J.-b.Lu Study of the High Spin States of Stable 84Sr
1999HA68 High Energy Phys. and Nucl.Phys. (China) 23, 890 (1999) G.Han, S.Wen, X.Liu, X.Wu, G.Li, G.Yuan, P.Weng, C.Yang, D.Tong, Y.Ma, J.Lu High Spin States in 84Rb
1999HO17 Phys.Rev.Lett. 82, 5198 (1999) Nucleosynthesis in Supernovae NUCLEAR REACTIONS 1n(ν, e), 1H(ν, e+), E ≈ 10-25 MeV; analyzed σ in supernova environment; deduced implications for nucleosynthesis.
doi: 10.1103/PhysRevLett.82.5198
1999LI28 Nucl.Instrum.Methods Phys.Res. A431, 194 (1999) G.Li, T.Zhang, Z.Li, Y.Su, S.Zhang Neutrons Around Thick Target Bombarded by 50 MeV/u 18O-Ion Beam NUCLEAR REACTIONS Be, Cu, 197Au(18O, nX), E=50 MeV/nucleon; measured neutron spectra, thick target yields, angular distributions.
doi: 10.1016/S0168-9002(99)00150-3
1999LU03 Phys.Rev. C59, 3461 (1999) J.Lu, Y.Liu, X.Wu, Y.Ma, G.Zhao, H.Sun, J.Huo, S.Wen, G.Li, C.Yang High-Spin States in Doubly Odd 158Ho NUCLEAR REACTIONS 152Sm(11B, 5n), E=60 MeV; measured Eγ, Iγ, γγ-coin. 158Ho deduced high-spin levels, J, π, configurations, B(M1)/B(E2).
doi: 10.1103/PhysRevC.59.3461
1998HE21 Eur.Phys.J. C 4, 301 (1998) Z.He, X.Yao, C.Duan, G.Li, H.Peng Double Q2-Rescaling Model and the Nuclear Effect of the Parton Distribution Functions NUCLEAR STRUCTURE 12C, 40Ca, 56Fe, 119Sn; calculated parton distribution, average structure functions F2. Double Q2-rescaling model. Comparison with lepton-nucleus deep inelastic scattering data.
doi: 10.1007/s100520050208
1998LI18 Nucl.Instrum.Methods Phys.Res. A404, 349 (1998) G.Li, T.Zhang, Z.Li, Y.Su, S.Zhang Neutron Yields and Emission Rates of 50 MeV/u 18O-Ion on Thick Be, Cu and Au Targets NUCLEAR REACTIONS Be, Cu, 197Au(18O, X), E=50 MeV/nucleon; measured thick-target neutron yields, angular distributions. Activation technique.
doi: 10.1016/S0168-9002(97)01104-2
1998LI62 High Energy Phys. and Nucl.Phys. (China) 22, 299 (1998) G.Li, Z.Dai, X.Liu, L.Zhang, S.Wen, G.Yuan, X.Wu, P.Weng, S.Li, C.Yang Lifetime measurements of the states around the backbend in 126Ba
1998TA17 Phys.Scr. 58, 193 (1998) Approximate Bounds to the Average Electron Momentum Density for Atomic Systems ATOMIC PHYSICS Z=1-36; calculated average electron momentum density approximate bounds. Hartree-Fock approach.
doi: 10.1088/0031-8949/58/3/001
1997KO59 Ann.Rev.Nucl.Part.Sci. 47, 505 (1997) Properties of Hadrons in the Nuclear Medium
1997LI45 High Energy Phys. and Nucl.Phys. (China) 21, 881 (1997) Z.Liu, X.Sun, Y.Guo, X.Lei, X.Chen, X.Zhou, Y.Zhang, H.Jin, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang, X.Liu Lifetime measurement of the negative-parity isomers in 117Xe
1996DU11 Nucl.Instrum.Methods Phys.Res. A369, 424 (1996) H.Du, Y.Liu, J.Li, S.Yan, G.Li, Y.Zhu, L.Yao Progress in Preparation 4πβ Quantitative Sources RADIOACTIVITY 60Co(β-); measured βγ-coin; deduced detector plateau-characteristics.
doi: 10.1016/S0168-9002(96)80023-4
1996ZH40 High Energy Phys. and Nucl.Phys. (China) 20, 769 (1996) X.Zhou, X.Sun, Y.Guo, X.Lei, Z.Liu, Y.Zhang, X.Chen, H.Jin, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang High-Spin States in 198Bi
1995LI67 High Energy Phys. and Nucl.Phys. (China) 19, 106 (1995) Z.Liu, X.Sun, X.Zhou, X.Lei, H.Jin, Y.Guo, Q.Pan, Y.Zhang, X.Chen, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang Identification of Excited States in 117Xe
1995LI68 High Energy Phys. and Nucl.Phys. (China) 19, 1057 (1995) G.Li, Z.Dai, S.Wen, S.Li, P.Weng, L.Zhang, G.Yuan, C.Yang Lifetime Measurement of the 16+ Yrast State in 128Ce
1995MA46 J.Phys.(London) G21, 937 (1995) Y.Ma, H.Sun, Y.Liu, S.Wen, H.Zheng, S.Li, G.Li, G.Yuan, P.Weng, C.Yang High-Spin States in 159Lu NUCLEAR REACTIONS 144Sm(19F, 4n), E=105 MeV; measured Eγ, γγ-coin. 159Lu deduced high-spin levels, J, π. Enriched targets, array of escape-suppressed spectrometers (hyperpure Ge, BGO detectors). Systematics of first i13/2 band-crossing frequency and signature splitting for odd-Z-even-N nuclei in 159Lu region discussed.
doi: 10.1088/0954-3899/21/7/006
1995SU07 Z.Phys. A351, 241 (1995); see 1995Su11 H.Sun, Y.Ma, H.Zheng, J.Zhang, Y.Ma, Y.Liu, C.Yang, S.Wen, G.Yuan, G.Li First Identification of High Spin States in 160Lu
doi: 10.1007/BF01290902
1995SU08 Phys.Rev. C51, 2803 (1995) X.Sun, Z.Liu, X.Zhou, X.Lei, H.Jin, Q.Pan, Y.Zhang, Y.Guo, Y.Luo, S.Wen, G.Yuan, G.Li, C.X.Yang, Z.Xing, X.Q.Chen Observation of a Possible πh11/2 Band in 117Cs NUCLEAR REACTIONS 92Mo(28Si, X), E=115 MeV; measured Eγ, Iγ(E), γγ-coin. 117Cs deduced high-spin levels, J, π. Particle-plus-traxial rotor calculations.
doi: 10.1103/PhysRevC.51.2803
1995SU11 Z.Phys. A351, 241 (1995) H.Sun, Y.Ma, H.Zheng, J.Zhang, Y.Ma, Y.Liu, C.Yang, S.Wen, G.Yuan, G.Li First Identification of High Spin States in 160Lu NUCLEAR REACTIONS 144Sm(19F, 3n), E=90 MeV; measured γγ-coin. 160Lu deduced high-spin levels, J, π, configuration, band structure.
doi: 10.1007/BF01290902
1995SU12 Z.Phys. A352, 115 (1995) H.Sun, Y.Ma, J.Zhang, H.Zheng, S.Zhou, Y.Liu, S.Wen, G.Li, G.Yuan, C.Yang Study of the Yrast Band in the Doubly Odd 156Tm NUCLEAR REACTIONS 144Sm(19F, 5n2p), E=105 MeV; measured Eγ, Iγ, γγ-coin. 156Tm deduced high-spin levels, J, π, configuration.
doi: 10.1007/BF01298894
1995ZH08 Chin.Phys.Lett. 12, 4 (1995) X.Zhou, X.Sun, X.Lei, H.Jin, Z.Liu, Y.Zhang, Q.Pan, Y.Guo, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang On Beam Study of 198Bi Decay NUCLEAR REACTIONS 187Re(16O, 5n), E=100 MeV; measured γγ(t). RADIOACTIVITY 198Bi(β+), (EC) [from 187Re(16O, 5n), E=100 MeV]; measured γγ(t). 198Pb deduced levels, T1/2, γ-multipolarity.
1995ZH59 High Energy Phys. and Nucl.Phys. (China) 19, 961 (1995) X.Zhou, X.Sun, Y.Guo, X.Lei, Z.Liu, X.Chen, Y.Zhang, H.Jin, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang Study of Excited States in Neutron-Deficient 197Bi
1994SU13 J.Phys.(London) G20, 991 (1994) H.Sun, X.Wan, Y.Liu, S.Wen, H.Zheng, S.Li, G.Li, G.Yuan, P.Hua, P.Weng, L.Zhang, B.Yu, C.Yang Band Crossing Frequencies of Strongly Populated Bands in 174Ta NUCLEAR REACTIONS 160Gd(19F, 5n), E=87 MeV; measured γγ-coin. 174Ta deduced levels, J, π, band structure. Hyperpure Ge, BGO Compton-suppressed spectrometers.
doi: 10.1088/0954-3899/20/6/013
1994ZH47 High Energy Phys. and Nucl.Phys. (China), Supplement 1, 18, 28 (1994) X.Zhou, X.Sun, X.Lei, H.Jin, Z.Liu, Y.Zhang, Q.Pan, Y.Guo, X.Chen, Y.Luo, S.Wen, G.Yuan, G.Li, C.Yang Study of Low-lying Level Structure in 198Pb
1993LI50 Chin.Phys.Lett. 10, 648 (1993) Unified Description of the EMC Effect and Nuclear Shadowing Effect NUCLEAR STRUCTURE 2H, 40Ca; calculated average structure function rario; deduced no need for nuclear shadowing factor. Parton evolution model.
doi: 10.1088/0256-307X/10/11/003
1993XU06 High Energy Phys. and Nucl.Phys. (China) 17, 577 (1993) X.Xu, J.Guo, Z.Hu, X.Zhou, R.Ma, H.Liu, G.Li, Y.Du A New Decay Channel Discovered in β-Delayed α Decay of 20Na
1992LI03 J.Phys.(London) G18, 291 (1992) G.Li, Y.Lotfy, S.W.Huang, A.Faessler Self-Consistent Quantum Molecular Dynamics Description of Photon Production in Nucleus-Nucleus Reactions NUCLEAR REACTIONS 40Ca(40Ca, X), E=84, 200 MeV/nucleon; Tb(p, X), E=168 MeV; calculated γ-production σ(θ) vs Eγ. Self-consistent quantum molecular dynamics approach.
doi: 10.1088/0954-3899/18/2/011
1992LI13 Chin.J.Nucl.Phys. 14, No 1, 1 (1992) G.Li, L.Zhu, S.Wen, S.Li, P.Weng, P.Yu, G.Yuan, L.Zhang, P.Hua, C.Yang Spectroscopic Study of High Spin States in 163Lu NUCLEAR REACTIONS 148Sm(19F, 4n), E=92 MeV; measured γγ(t). 163Lu deduced levels, J, π, band structure.
1991LI33 Nucl.Phys. A534, 697 (1991) G.Li, D.T.Khoa, T.Maruyama, S.W.Huang, N.Ohtsuka, A.Faessler, J.Aichelin Subthreshold Pion Production in Nucleus-Nucleus Collisions within the Quantum Molecular Dynamics Approach NUCLEAR REACTIONS 12C(12C, X), Ca(Ca, X), 93Nb(93Nb, X), E=200 MeV/nucleon; 20Ne(20Ne, X), E=183 MeV/nucleon; 64Cu(20Ne, X), E=250 MeV/nucleon; calculated pion production σ(θ, E(π)). Quantum molecular dynamics model.
doi: 10.1016/0375-9474(91)90467-K
1990CA19 Z.Phys. A336, 97 (1990) The Role of Nucleon-Nucleon Short-Range Correlations in the Nuclear Structure Function in the x > 1 Region NUCLEAR STRUCTURE 12C; calculated structure function; deduced nucleon-nucleon short-range correlations role.
1990LI24 Chin.J.Nucl.Phys. 12, No.2, 139 (1990) The Transition Density and Transition Current Density of Giant Resonances NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb, 120Sn; calculated giant resonance transition current densities.
1990LI35 Chin.J.Nucl.Phys. 12, No 3, 219 (1990) Temperature Dependence of Nucleus-Nucleus Optical Potentials and Fusion Barrier NUCLEAR REACTIONS 120Sn, 40Ca(40Ca, 40Ca), 90Zr(90Zr, 90Zr), E not given; calculated potential parameters, fusion barriers.
1990LI43 Chin.J.Nucl.Phys. 12, No 4, 325 (1990) Self-Consistent Semiclassical Sum Rule Approach to Nuclear Giant Octupole Resonances NUCLEAR STRUCTURE 40Ca, 60Ni, 90Zr, 120Sn, 208Pb; calculated giant octupole resonances, nucleon rms radii. Self-consistent semi-classical sum rule approach.
1989YU03 Chin.J.Nucl.Phys. 11, No.1, 1 (1989) G.Yuan, G.Li, S.Wen, S.Li, P.Hua, L.Zhou, P.Wu, L.Zhang, Z.Yu, P.Yu, P.Weng, C.Yang, J.N.Mo Study of the (1/2)[541] Rotational Band in 169Ta NUCLEAR REACTIONS 155Gd(19F, 5n), E=85.5-100 MeV; measured γ-spectra, γγ-coin. 169Ta deduced levels, J, π, band structure. Cranked shell model.
1989ZE02 Chin.J.Nucl.Phys. 11, No.2, 43 (1989) X.Zeng, Z.Shi, M.Zhang, G.Li, D.Ding Study of the Thermal Neutron Radiative Capture 31P(n, γ) Reaction NUCLEAR REACTIONS 31P(n, γ), E=thermal; measured Eγ, Iγ; deduced neutron separation energy, reaction mechanism. 32P deduced levels.
1988YU02 Chin.J.Nucl.Phys. 10, 97 (1988) Yuan Guanjun, Li Guangsheng, Wen Shuxian, Li Shenggang, Hua Pengfei, Zhou Ling, Wu Ping, Zhang Lankuan, Yu Zhikang, Yu Panshui, Weng Peikun, Yang Chunxiang, J.N.Mo Study of the (1/2)[541] Rotational Band and the Band Crossing Frequency of 169Ta NUCLEAR REACTIONS 155Gd(19F, 5n), E=85.5-100 MeV; measured Eγ, Iγ, σ(Eγ, E), γγ-coin. 169Ta deduced levels, J, π, band structure.
1987ZH12 Chin.J.Nucl.Phys. 9, 307 (1987) Zhang Ming, Shi Zongren, Zeng Xiantang, Li Guohua, Ding Dazhao Study of Thermal Neutron Capture in 23Na NUCLEAR REACTIONS 23Na(n, γ), E=thermal; measured Eγ, Iγ, σ. 24Na deduced levels, level density parameters, neutron binding energy. Ge(Li) detector. Back-shift Fermi gas model. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30778. 1986LI21 Chin.J.Nucl.Phys. 8, 64 (1986) Li Guangsheng, Liu Fengying, Wen Shuxian, Han Benhua, Lu Xiane, Weng Peikun Level Structure of 128Xe NUCLEAR REACTIONS 126Te(α, 2nγ), E=26 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 128Xe deduced levels, J, π. Enriched target, Ge(Li) detectors. Interacting boson model calculations.
1986LI23 Chin.J.Nucl.Phys. 8, 97 (1986) Li Guangsheng, Liu Fengying, Wen Shuxian, Han Benhua, Lu Xiane, Weng Peikun In-Beam γ-Ray Spectroscopy on 132Xe NUCLEAR REACTIONS 130Te(α, 2nγ), E=26 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 132Xe deduced levels, J, π, configuration. In-beam γ-ray spectroscopy.
1985GU20 Chin.J.Nucl.Phys. 7, 50 (1985) Guo Taichang, Shi Zongren, Zeng Xiantang, Li Guohua, Ding Dazhao The Study of Thermal Neutron Capture of 32S NUCLEAR REACTIONS 32S(n, γ), E=thermal; measured Eγ, Iγ; deduced capture σ(E). 33S deduced neutron separation energy, levels, E1 transitions, γ-branching ratios. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30710. 1983LI16 Chin.J.Nucl.Phys. 5, 217 (1983) Li Guangsheng, L.Cleemann, J.Eberth, T.Heck, W.Neumann, M.Nolte, J.Roth In-Beam Gamma Spectroscopic Investigation of 73Se NUCLEAR REACTIONS 58Ni(19F, n3p), E=56-68 MeV; measured Eγ, Iγ, σ(Eγ, E), γ(θ), γγ-, nγ-coin, recoil distance. 73Se deduced levels, J, π, band structure. Strong coupling rotation model.
1980CH38 Chin.J.Nucl.Phys. 2, 382 (1980) Chen Shiping, Liu Fengying, Zhou Ling, Yang Chunxiang, Li Guangsheng, Weng Peikun, Zhang Youfang γ-Ray Spectrum from 147Nd Decay RADIOACTIVITY 147Nd; measured Eγ, Iγ. 147Pm deduced levels, γ-branching. Ge(Li) spectrometers.
1980YA10 Chin.J.Nucl.Phys. 2, 41 (1980) Yang Chunxiang, Li Guangsheng, Weng Peikun, Cheng Shiping, Liou Fengyeng, Zhou Ling, Zhang Youfang The Decay of 99Mo RADIOACTIVITY 99Mo; measured Eγ, Iγ; deduced β-branching. 99Tc levels deduced γ-branching.
1980YU01 Chin.J.Nucl.Phys. 2, 19 (1980) Yu Jusheng, Wang Sufang, Tian Yuhong, Hou Mingdong, Miao Degui, Zeng Wenbing, Li Guangwei Study of the Fission of the Excited Nuclei near Radium NUCLEAR REACTIONS, Fission 197Au, Pb, 209Bi(12C, F), E=72.5 MeV; measured (fragment)(fragment)-coin; deduced symmetric fission dominance, fragment shape at scission.
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