NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = X.Yu Found 47 matches. 2024YU04 Eur.Phys.J. A 60, 22 (2024) Exploring the chiral and deconfinement phase transitions in a self-consistent PNJL model
doi: 10.1140/epja/s10050-024-01239-0
2024ZH15 Nucl.Instrum.Methods Phys.Res. A1059, 168983 (2024) H.Q.Zhang, P.Kuang, X.T.Yu, P.Zhang, F.Y.Liu, R.S.Yu, X.Z.Cao, B.Y.Wang Development of novel positron lifetime measurement system for potential liquid material inspection
doi: 10.1016/j.nima.2023.168983
2023DO01 Appl.Radiat.Isot. 193, 110647 (2023) J.Dong, T.Bai, Y.Hu, X.Zhang, J.Fan, Y.Dai, L.Miao, X.Yu, Z.Li Determination of the half-life of 161Tb RADIOACTIVITY 161Tb(β-); measured decay products, Eγ, Iγ; deduced T1/2 and uncertainties. Comparison with available data.
doi: 10.1016/j.apradiso.2022.110647
2023LU04 Phys.Rev. C 108, 014302 (2023) H.Y.Lu, Z.Liu, Z.H.Li, X.Wang, J.Li, H.Hua, H.Huang, W.Q.Zhang, Q.B.Zeng, X.H.Yu, T.H.Huang, M.D.Sun, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, C.J.Lin, L.J.Sun, N.R.Ma, H.S.Xu, X.H.Zhou, G.Q.Xiao, F.S.Zhang Reinvestigation of 222U in high-precision digital α-decay spectroscopy: Solution to the reduced decay-width anomaly RADIOACTIVITY 222U(α) [from 186W(40Ar, 4n), E=80 MeV, followed by separation of fragments using SHANS separator at HRIFL-Lanzhou]; 218Th, 214Ra(α)[from 222U α decay chain]; measured Eα, Iα, evaporation residues (ER)-α correlations, T1/2 using DSSD detectors; deduced reduced α-decay width, and analyzed using NpNn scheme. 218Ac, 219Th, 220Pa(α); measured Eα, and T1/2. Systematics of reduced α-decay widths for g.s. to g.s. α transitions in even-even Z=84-92, N≥126 isotopes as function of NpNn. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.108.014302
2022HU09 Phys.Lett. B 833, 137345 (2022) H.Huang, W.Q.Zhang, A.N.Andreyev, Z.Liu, D.Seweryniak, Z.H.Li, C.Y.Guo, A.E.Barzakh, P.Van Duppen, B.Andel, S.Antalic, M.Block, A.Bronis, M.P.Carpenter, P.Copp, J.G.Cubiss, B.Ding, D.T.Doherty, Z.Favier, F.Giacoppo, T.H.Huang, B.Kindler, F.G.Kondev, T.Lauritsen, J.G.Li, G.S.Li, B.Lommel, H.Y.Lu, M.Al Monthery, P.Mosat, Y.F.Niu, C.Raison, W.Reviol, G.Savard, S.Stolze, G.L.Wilson, H.Y.Wu, Z.H.Wang, F.R.Xu, Q.B.Zeng, X.H.Yu, F.F.Zeng, X.H.Zhou First observation of the decay of the 13/2+ isomer in 183Hg and B(M2) systematics of neutron transitions across the nuclear chart RADIOACTIVITY 183Hg(α) [from 187Pb α decay]; 187mPb(α) [from 142Nd(50Cr, 3n2pγ), E=255 MeV, followed by separation of fragments using Argonne gas-filled analyzer (AGFA) at the ATLAS-ANL facility]; measured reaction products, evaporation residues (EVRs), Eα, Iα, (EVR)α-correlations, αγ(t), Eγ, Iγ, x rays, T1/2 using double-sided silicon strip detector (DSSD), and four HPGe clover detectors. 183,183mHg; deduced levels, isomer, J, π, T1/2 of g.s. and isomer, α branching ratio, K-conversion coefficient, multipolarity, B(M2), Nilsson configurations. 187mPb; deduced T1/2. Systematics of decay schemes of 13/2+ isomers in 175,177,179,181,183,185Hg. Systematics of B(M2) values for 7/2-, 9/2+, 11/2- and 13/2+ isomers in even-Z, odd-N nuclei: 25Mg, 33Si, 33,35S, 37Ar, 39Ca, 59Cr, 61Fe, 63,67Ni, 63,65,67Zn, 67,69,71Ge, 69,71Se, 97,99Mo, 99,101,103Ru, 103,105Pd, 107,109Cd, 109,111,113,115Sn, 153Yb, 161Hf, 163W, 163Os, 171,189,191Pt, 181,183,201,203,205Hg, 209Pb, 205,207,211Po, 207,209,213Rn, 209,211Ra, 211,213Th.
doi: 10.1016/j.physletb.2022.137345
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
2022ZE02 Phys.Rev. C 106, 034307 (2022) Q.B.Zeng, S.Guo, Z.Liu, J.G.Li, H.H.Li, J.G.Wang, Z.Y.Zhang, L.Ma, Y.H.Qiang, M.H.Huang, G.S.Li, Y.D.Fang, M.L.Liu, B.Ding, Y.Zheng, J.H.Li, H.Y.Lu, W.Q.Zhang, K.L.Wang, X.Y.Liu, H.Huang, F.F.Zeng, X.H.Yu, A.Rohilla, J.F.Huang, H.L.Fan, C.Qi, C.X.Yuan, C.M.Petrache, E.A.Lawrie, W.Zuo, Z.G.Gan, X.H.Zhou Configurations of the low-lying states in 146Eu RADIOACTIVITY 146mEu(IT) [from 124Sn(27Al, 5n), E=127 MeV, followed by mass-separation of evaporation residues (ERs) using the SHANS separator at the Sector-Focusing Cyclotron (SFC) of HIRFL-Lanzhou]; measured Eγ, Iγ, γγ-coin, isomer and level T1/2 by γ(t) and γγ(t) fast-timing method using three LaBr3(Ce) detectors, one coaxial and one Clover HPGe detectors, and analyzed using mirror symmetric centroid difference (MSCD) method. 146Eu; deduced levels, J, π, T1/2 of 6- levels and a 9+ isomer, multipolarities, upper limits of multipole mixing ratios, B(M1), spherical configurations. 146Sm; measured level T1/2 of the first 2+ state as a test case for measurements of short half-lives for levels in 146Eu. Comparison with shell model calculations using several different effective interactions, and with previous experimental results. Systematics of levels and B(M1) values in N=83 isotones 142Pr, 144Pm, 146Eu.
doi: 10.1103/PhysRevC.106.034307
2022ZH22 Phys.Lett. B 829, 137129 (2022) W.Q.Zhang, A.N.Andreyev, Z.Liu, D.Seweryniak, H.Huang, Z.H.Li, J.G.Li, C.Y.Guo, D.T.Doherty, A.E.Barzakh, P.Van Duppen, J.G.Cubiss, B.Andel, S.Antalic, M.Block, A.Bronis, M.P.Carpenter, P.Copp, B.Ding, Z.Favier, F.Giacoppo, T.H.Huang, X.H.Yu, B.Kindler, F.G.Kondev, T.Lauritsen, G.S.Li, B.Lommel, H.Y.Lu, M.Al Monthery, P.Mosat, Y.F.Niu, C.Raison, W.Reviol, G.Savard, S.Stolze, G.L.Wilson, H.Y.Wu, Z.H.Wang, F.R.Xu, Q.B.Zeng, X.H.Zhou First observation of a shape isomer and a low-lying strongly-coupled prolate band in neutron-deficient semi-magic 187Pb NUCLEAR REACTIONS 142Nd(50Cr, 3n2p)187Pb, E=255 MeV beam from ATLAS-ANL facility, followed by separation of evaporation residues (EVRs) using Argonne Gas-Filled Analyzer; measured Eα, Eγ, Iγ, x rays, αγ-coin, γγ-coin, T1/2 of a new low-energy microsec-isomer by αγ(t) using Gammasphere for γ detection and double-sided silicon strip detector (DSSD) for EVRs and α particles. Recoil-decay tagging (RDT) and isomer-decay tagging (IDT) methods. 187Pb; deduced high-spin levels, J, π, isomer, K-conversion coefficient, multipolarity, bands, B(E2), B(M1)/B(E2), triple-shape coexistence at low energy. Comparison with band structure in 185Hg. Systematics of aligned angular momenta plots and experimental Routhians for bands in 183,185Hg, 187Pb. 184Hg, 186Pb, 187Tl; observed γ rays. 186,187m,188Pb; observed α-decay peaks.
doi: 10.1016/j.physletb.2022.137129
2022ZH46 Phys.Rev. C 106, 024317 (2022) W.Q.Zhang, A.N.Andreyev, Z.Liu, D.Seweryniak, H.Huang, Z.H.Li, J.G.Li, C.Y.Guo, A.E.Barzakh, P.Van Duppen, M.Al Monthery, B.Andel, S.Antalic, M.Block, A.Bronis, M.P.Carpenter, P.Copp, J.G.Cubiss, B.Ding, D.T.Doherty, Z.Favier, F.Giacoppo, T.H.Huang, B.Kindler, F.G.Kondev, T.Lauritsen, G.S.Li, B.Lommel, H.Y.Lu, P.Mosat, Y.F.Niu, C.Raison, W.Reviol, G.Savard, S.Stolze, G.L.Wilson, H.Y.Wu, Z.H.Wang, F.R.Xu, X.H.Yu, Q.B.Zeng, X.H.Zhou Identification of excited states in 188Bi and 188Po NUCLEAR REACTIONS 142Nd(50Cr, 3np)188Bi, (50Cr, 4n)188Po, E=255 MeV; measured evaporation residues (EVRs), Eα, Eγ, Iγ, x rays, (EVR)γ-coin, αγ-coin, γγ-coin, using four clover HPGe detectors, Gammasphere array with 64 Compton-suppressed HPGe detectors, and DSSD and DSSD+Sibox at the ATLAS-ANL accelerator facility. 186,187,187m,188Pb, 189,189mBi; deduced recoil-decay tagging (RDT) γ-ray yields. 188Bi; deduced levels, J, π, isomer, T1/2 and decay modes of isomer, K-conversion coefficients, multipolarities, configurations. 188Po; deduced energy of the first 2+ level. 186Pb; deduced levels, J, π. 183,184,186Hg, 186,187,187m,188Pb, 188,189,189mBi; observed Eα. Systematics of 9/2-, 1/2+, 7/2- and 13/2+ level energies in 185,187,189,191,193,195Bi, and those of first 2+, 4+, 6+ and 8+, second 0+, 2+ and 4+ in 188,190,192,194,196,198,200,202,204,206,208,210Po.
doi: 10.1103/PhysRevC.106.024317
2021HE09 Chin.Phys.C 45, 014110 (2021) Improved empirical formula for α particle preformation factor RADIOACTIVITY 186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220Po, 191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221At, 194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226Rn, 206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225Ac, 209Th, 224,225,226,227,228,229,230,231,232Th, 217,218,219,220,221,222,223,224,225,226,227,228,229,230,231Pa, 219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238U, 229,230,231,232,233,234,235,236,237,238,239,240,241,242,243Am, 233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250Cm, 245,247Bk, 237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255Cf, 246,247,248,249,250,251,252,253,254,255Es, 244,245,246,247,248,249,250,251,252,253,254,255,256,257Fm, 247,248,249,250,251,252,253,254,255,256,257Md, 251,252,253,254,255,256,257,258No, 253,255,257,259Lr(α); calculated T1/2. Comparison with available data.
doi: 10.1088/1674-1137/abc684
2018KI20 Int.J.Mod.Phys. E27, 1850090 (2018) A.Kingan, M.Quinonez, X.Yu, L.Zamick The spin and orbital contributions to magnetic dipole transitions NUCLEAR STRUCTURE 44,46Ti, 48Cr; analyzed available data; deduced J, π, B(M1).
doi: 10.1142/S0218301318500908
2018LI33 Phys.Rev. C 98, 014618 (2018) F.Li, L.Zhu, Z.-H.Wu, X.-B.Yu, J.Su, C.-C.Guo Predictions for the synthesis of superheavy elements Z=119 and 120 NUCLEAR REACTIONS 238U, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-60 MeV; calculated evaporation residue σ(E), and compared with available experimental data. 252Es(40Ca, 3n), E(cm)=204.08 MeV; 252Es(42Ca, 3n), E(cm)=203.00 MeV; 249Cf(45Sc, 3n), E(cm)=211.09 MeV; 255Es(40Ca, 4n), E(cm)=207.02 MeV; 254Es(40Ca, 3n), E(cm)=203.60 MeV; 247Bk(47Ti, 3n), E(cm)=219.19 MeV; 248Bk(46Ti, 3n), E(cm)=217.76 MeV; 242Cm(51V, 2n), E(cm)=225.86 MeV; 248Cf(45Sc, 2n), E(cm)=209.29 MeV; 241Am(52Cr, 2n), E(cm)=231.94 MeV; 252Es(44Ca, 3n), E(cm)=204.27 MeV; 253Es(43Ca, 3n), E(cm)=202.49 MeV; 254Es(42Ca, 3n), E(cm)=201.65 MeV; 251Cf(45Sc, 3n), E(cm)=210.03 MeV; 249Bk(47Ti, 3n), E(cm)=217.18 MeV; 248Bk(48Ti, 3n), E(cm)=219.47 MeV; 245Cm(51V, 3n), E(cm)=229.29 MeV; 247Bk(49Ti, 3n), E(cm)=222.17 MeV; 246Cm(50V, 3n), E(cm)=225.70 MeV; 244Cm(51V, 2n), E(cm)=224.00 MeV; 255Es(42Ca, 4n), E(cm)=205.95 MeV; 243Am(53Cr, 3n), E(cm)=236.20 MeV; 254Es(43Ca, 4n), E(cm)=206.90 MeV; 253Es(44Ca, 4n), E(cm)=210.94 MeV; 243Am(52Cr, 2n), E(cm)=229.49 MeV; 254Es(44Ca, 3n), E(cm)=201.64 MeV; 255Es(43Ca, 3n), E(cm)=201.49 MeV; 255Es(44Ca, 4n), E(cm)=207.59 MeV; 252Es(46Ca, 3n), E(cm)=206.00 MeV; 248Bk(50Ti, 3n), E(cm)=222.48 MeV; 247Cm(51V, 3n), E(cm)=226.83 MeV; 254Cf(45Sc, 4n), E(cm)=211.93 MeV; 249Bk(49Ti, 3n), E(cm)=218.88 MeV; 254Es(46Ca, 3n), E(cm)=203.64 MeV; 255Es(46Ca, 4n), E(cm)=210.13 MeV; 252Es(48Ca, 3n), E(cm)=208.42 MeV; 255Es(46Ca, 3n), E(cm)=204.13; 254Es(48Ca, 3n), E(cm)=205.96 MeV; 255Es(48Ca, 4n), E(cm)=212.72 MeV; 242Cm(50Cr, 2n), E(cm)=234.22 MeV; 249Cf(46Ti, 3n), E(cm)=222.89 MeV; 248Cf(46Ti, 2n), E(cm)=219.12 MeV; 257Fm(40Ca, 5n), E(cm)=222.66 MeV; 257Fm(40Ca, 4n), E(cm)=211.66 MeV; 257Fm(40Ca, 3n), E(cm)=205.66 MeV; 251Cf(46Ti, 3n), E(cm)=220.39 MeV; 252Es(45Sc, 3n), E(cm)=214.17 MeV; 250Cf(46Sc, 2n), E(cm)=218.88 MeV; 247Bk(50V, 3n), E(cm)=231.13 MeV; 244Cm(52Cr, 2n), E(cm)=234.88 MeV; 245Cm(52Cr, 3n), E(cm)=240.80 MeV; 243Cm(53Cr, 2n), E(cm)=236.02 MeV; 247Cm(50Cr, 3n), E(cm)=235.12 MeV; 257Fm(42Ca, 3n), E(cm)=205.29 MeV; 254Es(45Sc, 3n), E(cm)=213.40 MeV; 257Fm(43Ca, 4n), E(cm)=210.97 MeV; 257Fm(44Ca, 3n), E(cm)=205.27 MeV; 257Fm(46Ca, 3n), E(cm)=207.84 MeV; 250Cm(53Cr, 3n), E(cm)=234.59 MeV; 257Fm(48Ca, 3n), E(cm)=211.07 MeV; calculated production σ for Z=119 and 120 superheavy isotopes. Dinuclear system (DNS) model.
doi: 10.1103/PhysRevC.98.014618
2018WU06 Phys.Rev. C 97, 064609 (2018) Z.-H.Wu, L.Zhu, F.Li, X.-B.Yu, J.Su, C.-C.Guo Synthesis of neutron-rich superheavy nuclei with radioactive beams within the dinuclear system model NUCLEAR REACTIONS 242,244Pu, 243Am, 245,248,250Cm, 249Bk, 250,251Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-60 MeV; 234Th(42S, 2n), (42S, 3n), (42S, 4n), (42S, 5n), E*=20-65 MeV; 234Th, 244Pu(46Ar, 2n), (46Ar, 3n), (46Ar, 4n), (46Ar, 5n), E*=20-65 MeV; 234Th, 238U, 248Cm, 255Es(44Cl, 2n), (44Cl, 3n), (44Cl, 4n), (44Cl, 5n), E*=20-65 MeV; 228Ra(45Cl, 2n), (45Cl, 3n), (45Cl, 4n), (45Cl, 5n), E*=20-65 MeV; 244Pu, 248Cm(43Cl, 2n), (43Cl, 3n), (43Cl, 4n), (43Cl, 5n), E*=20-65 MeV; 244Pu, 254Cf, 255Es(41S, 2n), (41S, 3n), (41S, 4n), (41S, 5n), E*=20-65 MeV; 257Fm(42Ar, 2n), (42Ar, 3n), (42Ar, 4n), (42Ar, 5n), E*=20-65 MeV; 260Md(38Cl, 2n), (38Cl, 3n), (38Cl, 4n), (38Cl, 5n), E*=20-65 MeV; calculated evaporation residue σ. 228Ra(45Cl, 2n), E*=36.0 MeV; 228Ra(46Cl, 3n), E*=46.0 MeV; 226Ra(47Cl, 2n), E*=36.0 MeV; 234Th(42S, 4n), E*=43.0 MeV; 228Ra(46Ar, 2n), E*=34.0 MeV; 234Th(43S, 5n), E*=51.0 MeV; 234Th(42S, 3n), E*=41.0 MeV; 234Th(43S, 4n), E*=46.0 MeV; 234Th(44S, 5n), E*=59.0 MeV; 234Th(44Cl, 2n), E*=37.0 MeV; 234Th(45Cl, 3n), E*=44.0 MeV; 228Ra(50K, 2n), E*=36.0 MeV; 234Th(46Ar, 2n), E*=34.0 MeV; 238U(43S, 3n), E*=41.0 MeV; 238U(42S, 2n), E*=37.0 MeV; 238U(44Cl, 3n), E*=38.0 MeV; 238U(43Cl, 2n), E*=36.0 MeV; 238U(43S, 3n), E*=41.0 MeV; 234Th(47K, 2n), E*=33.0 MeV; 244Pu(41S, 3n), E*=38.0 MeV; 244Pu(42S, 4n), E*=42.0 MeV; 238U(46Ar, 2n), E*=33.0 MeV; 244Pu(43Cl, 4n), E*=44.0 MeV; 242Pu(44Cl, 3n), E*=37.0 MeV; 244Pu(42Cl, 3n), E*=38.0 MeV; 244Pu(46Ar, 4n), E*=38.0 MeV; 244Pu(45Ar, 3n), E*=44.0 MeV; 242Pu(46Ar, 2n), E*=33.0 MeV; 248Cm(43Cl, 4n), E*=38.0 MeV; 250Cm(42Cl, 5n), E*=43.0 MeV; 248Cm(44Cl, 5n), E*=43.0 MeV; 248Cm(44Cl, 4n), E*=38.0 MeV; 250Cm(42Cl, 4n), E*=39.0 MeV; 250Cm(43Cl, 5n), E*=45.0 MeV; 254Cf(41S, 5n), E*=40.0 MeV; 253Cf(42S, 5n), E*=40.0 MeV; 250Cm(44Ar, 4n), E*=37.0 MeV; 255Es(41S, 5n), E*=40.0 MeV; 254Cf(42Cl, 5n), E*=40.0 MeV; 253Cf(43Cl, 5n), E*=39.0 MeV; 255Es(41S, 4n), E*=37.0 MeV; 253Cf(43Cl, 4n), E*=36.0 MeV; 254Cf(42Cl, 4n), E*=37.0 MeV; 250Cm(48Ca, 4n), E*=35.0 MeV; 248Cm(48Ca, 2n), E*=31.0 MeV; 250Cm(46Ca, 2n), E*=35.0 MeV; 255Es(44Cl, 5n), E*=40.0 MeV; 254Cf(44Ar, 4n), E*=36.0 MeV; 257Fm(41S, 4n), E*=37.0 MeV; 250Cm(48Ca, 3n), E*=31.0 MeV; 255Es(44Cl, 4n), E*=36.0 MeV; 253Cf(46Ar, 4n), E*=34.0 MeV; 254Cf(46Ar, 5n), E*=41.0 MeV; 250Cf(48Ca, 3n), E*=34.0 MeV; 250Cm(49Ti, 4n), E*=42.0 MeV; 252Cf(46Ca, 3n), E*=36.0 MeV; 260Md(38Cl, 3n), E*=41.0 MeV; 260Md(39Cl, 4n), E*=42.0 MeV; 257Fm(42Ar, 4n), E*=41.0 MeV; 251Cf(48Ca, 3n), E*=30.0 MeV; 252Cf(48Ca, 4n), E*=38.0 MeV; 250Cm(49Ti, 3n), E*=34.0 MeV; 257Fm(42Ar, 3n), E*=33.0 MeV; 257Fm(43Ar, 4n), E*=38.0 MeV; 260Md(39Cl, 3n), E*=37.0 MeV; 244Pu(43Cl, n), E*=40.0 MeV; 238Cm(48Ca, 2np), E*=41.0 MeV; 254Cf(41S, 5n), E*=40.0 MeV; 248Cm(48Ca, 2nα), E*=46.0 MeV; 248Cm(43Cl, 4n), E*=38.0 MeV; 242Pu(48Ca, 2np), E*=35.0 MeV; 248Cm(44Cl, 4n), E*=38.0 MeV; 242Pu(48Ca, np), E*=40.0 MeV; 244Pu(48Ca, 3np), E*=45.0 MeV; 255Es(41S, 5n), E*=40.0 MeV; 245Cm(48Ca, np), E*=32.0 MeV; 249Bk(48Ca, 2nα), E*=37.0 MeV; 255Es(41S, 4n), E*=37.0 MeV; 248Cm(48Ca, 3np), E*=44.0 MeV; 249Bk(48Ca, nα), E*=32.0 MeV; calculated evaporation residue σ, and optimal incident beam energies. 48Ca(238U, 2n), (238U, 3n), (238U, 4n), E(cm)=184.13-214.13 MeV; calculated evaporation residue σ, potential energy surface, driving potential, survival and complete fusion probabilities, and capture σ. Dinuclear system model. 271Db, 272,273Sg, 276Bh, 278Hs, 279Mt, 282Ds, 283Rg, 286Cn, 287,288Nh, 290Fl, 291,292Mc, 294,295Lv, 295,296Og; calculated evaporation residue σ, and optimal incident beam energies for various reactions. Comparison with available experimental data. Relevance to synthesis of neutron-rich superheavy nuclei using radioactive ion beams, such as those at ATLAS-ANL.
doi: 10.1103/PhysRevC.97.064609
2018YU01 Chin.Phys.C 42, 034103 (2018) X.-R.Yu, J.Hu, X.-X.Li, S.-Y.An, Y.Zhang Effects of single particle on shape phase transitions and phase coexistence in odd-even nuclei
doi: 10.1088/1674-1137/42/3/034103
2017SH11 Int.J.Mod.Phys. E26, 1730017 (2017) S.Shen, X.Yu, J.Shen, S.Shi, J.Liu, W.Li, Y.Li, Y.Yan Uncertainties on gamma-ray energies and intensities measured in the decay of 83Sr RADIOACTIVITY 83Sr(β+), (EC); analyzed decay products, Eγ, Iγ; deduced uncertainties on γ-ray energies and intensities.
doi: 10.1142/S0218301317500173
2016HE05 Phys.Rev. C 93, 055804 (2016) J.J.He, B.L.Jia, S.W.Xu, S.Z.Chen, S.B.Ma, S.Q.Hou, J.Hu, L.Y.Zhang, X.Q.Yu Direct measurement of 11B(p, γ)12C astrophysical S factors at low energies NUCLEAR REACTIONS 11B(p, γ)12C, E(cm)=130-257 keV; measured Eγ, Iγ, excitation functions, cross section at IMP-Lanzhou; deduced astrophysical S factors. Comparison with previous experimental results and with data in NACREII database.
doi: 10.1103/PhysRevC.93.055804
2016LI51 Chin.Phys.C 40, 114104 (2016) E.T.Li, B.Guo, Z.H.Li, Y.B.Wang, Y.J.Li, Z.D.Wu, J.Su, D.Y.Pang, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, Z.Y.Han, X.Hao, S.P.Hu, J.J.He, L.Jing, S.J.Jin, L.Li, X.Y.Li, Z.C.Li, G.Lian, J.C.Liu, Q.Luo, L.H.Qiao, Y.P.Shen, H.B.Sun, S.Q.Yan, X.Q.Yu, S.Zeng, D.H.Zhang, L.Y.Zhang, W.J.Zhang, Y.Zhou, W.P.Liu Radii of the bound states in 16N from the asymptotic normalization coefficients RADIOACTIVITY 16N(n) [from 15N(7Li, 6Li)16N, E=44 MeV]; analyzed available data; deduced asymptotic normalization coefficients (ANCs), rms radii of the valence neutron, probabilities of the valence neutron staying out of the core potentials.
doi: 10.1088/1674-1137/40/11/114104
2016NI15 Int.J.Mod.Phys. E25, 1650083 (2016) T.Ning, S.Y.An, X.X.Li, X.R.Yu, Y.Zhang Triaxial models description of the low-lying properties in 192Os NUCLEAR STRUCTURE 192Os; calculated energy levels, J, π, B(E2), γ-bands; deduced γ-rigid triaxiality. Triaxial models.
doi: 10.1142/S021830131650083X
2016YU02 Nucl.Phys. A949, 1 (2016) Surface delta interaction in the g7/2 - d5/2 model space NUCLEAR STRUCTURE 112,114,116,118,120,122,124,126Sn; calculated 2+, 4+, 6+ state energies, g-factors using known data and assuming 2 neutron particle (or 2 n hole) states and cancellation of the spin parts. 107,109,111,113,125,127Sn; calculated magnetic g-factors using single-energy splittigs between teo orbits.
doi: 10.1016/j.nuclphysa.2016.02.020
2014GU02 Phys.Rev. C 89, 012801 (2014) B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, S.Q.Yan, Z.D.Wu, E.T.Li, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, J.J.He, S.J.Jin, L.Jing, L.Li, Z.C.Li, G.Lian, J.C.Liu, Y.P.Shen, Y.B.Wang, X.Q.Yu, S.Zeng, L.Y.Zhang, W.J.Zhang, W.P.Liu Spectroscopic factors for low-lying 16N levels and the astrophysical 15N(n, γ)16N NUCLEAR REACTIONS 15N(7Li, 6Li)16N, E=44 MeV; measured 6Li spectrum, σ(θ) using Q3D magnetic spectrograph at CIAE's HI-13 tandem accelerator facility. 16N; deduced levels, J, π, configurations, spectroscopic factors for ground and first three excited states. DWBA analysis. Comparison with shell model calculations. 15N(n, γ)16N, at T=0.01-3 GK; deduced astrophysical reaction rates. Comparison with previous experimental and theoretical results.
doi: 10.1103/PhysRevC.89.012801
2014LI49 Phys.Rev. C 90, 067601 (2014) E.T.Li, Z.H.Li, Y.J.Li, B.Guo, Y.B.Wang, D.Y.Pang, J.Su, S.Q.Yan, S.Zeng, L.Gan, Z.C.Li, J.C.Liu, X.X.Bai, Z.D.Wu, S.J.Jin, L.Y.Zhang, X.Q.Yu, L.Li, H.B.Sun, G.Lian, Q.W.Fan, W.P.Liu Proton spectroscopic factor of the 12C ground state from the 12C(11B, 12C) 11B elastic transfer reaction NUCLEAR REACTIONS 12C(11B, 11B), (11B, 12C)11B, E=50 MeV; measured particle spectra, angular distributions using Q3D magnetic spectrometer at the HI-13 tandem accelerator of CIAE facility. 12C; deduced optical potential parameters, proton spectroscopic factor for 12C g.s., DWBA calculations. Comparison with previous experimental and theoretical results.
doi: 10.1103/PhysRevC.90.067601
2014WU03 Phys.Rev. C 89, 054315 (2014) Z.D.Wu, B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, S.Q.Yan, E.T.Li, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, J.J.He, S.J.Jin, L.Jing, L.Li, Z.C.Li, G.Lian, J.C.Liu, Y.P.Shen, Y.B.Wang, X.Q.Yu, S.Zeng, D.H.Zhang, L.Y.Zhang, W.J.Zhang, W.P.Liu Proton widths of the low-lying 16F states from the 15N(7Li, 6Li)16N reaction NUCLEAR REACTIONS 15N(7Li, 7Li), (7Li, 6Li), E=34.5, 44 MeV; measured particle spectra, elastic and inelastic σ(θ) using Q3D magnetic spectrograph at CIAE facility. 16N; deduced levels, J, π, asymptotic normalization coefficients (ANCs), spectroscopic factors. DWBA analysis. 16F; deduced proton and single-particle widths, spectroscopic factors for first four levels from mirror analogy with 16N. Comparison with previous experimental results and compilation.
doi: 10.1103/PhysRevC.89.054315
2013HE21 Phys.Lett. B 725, 287 (2013) J.J.He, S.Z.Chen, C.E.Rolfs, S.W.Xu, J.Hu, X.W.Ma, M.Wiescher, R.J.de Boer, T.Kajino, M.Kusakabe, L.Y.Zhang, S.Q.Hou, X.Q.Yu, N.T.Zhang, G.Lian, Y.H.Zhang, X.H.Zhou, H.S.Xu, G.Q.Xiao, W.L.Zhan A drop in the 6Li(p, γ)7Be reaction at low energies NUCLEAR REACTIONS 6Li(p, γ), E(cm)<1 MeV; measured reaction products, Eγ, Iγ; deduced S-factors, positive-parity resonance. Comparison with available data, SUSY assisted Big-bang Nucleosynthesis models.
doi: 10.1016/j.physletb.2013.07.044
2012LI14 Eur.Phys.J. A 48, 13 (2012); Erratum Eur.Phys.J. A 49, 106 (2013) Y.J.Li, Z.H.Li, E.T.Li, X.X.Bai, J.Su, B.Guo, B.X.Wang, S.Q.Yan, S.Zeng, Z.C.Li, J.C.Liu, X.Liu, S.J.Jin, Y.B.Wang, L.Y.Zhang, X.Q.Yu, L.Li, G.Lian, Q.W.Fan, W.P.Liu New determination of the astrophysical 13C(p, γ)14N S(E) factors and reaction rates via the 13C(7Li, 6He)14N reaction NUCLEAR REACTIONS 13C(7Li, 6He), (7Li, 7Li), E=34 MeV; measured reaction products using Q3D magnetic spectrometer; deduced astrophysical S-factor, σ(θ), spectroscopic factors, potential parameters, resonance parameters; calculated spectroscopic factors, reaction rates using DWBA code PTOLEMY. Comparison with other data.
doi: 10.1140/epja/i2012-12013-x
2011HE07 Int.J.Mod.Phys. E20, 747 (2011) J.J.He, L.Li, J.Hu, L.Y.Zhang, S.W.Xu, X.Q.Yu, M.L.Liu Development of a Lorentzian-Function approximation utilizing in the charge-particle-induced nonresonant reaction rate
doi: 10.1142/S0218301311018204
2011HE09 Eur.Phys.J. A 47, 67 (2011) J.J.He, J.Hu, S.W.Xu, Z.Q.Chen, X.Y.Zhang, J.S.Wang, H.W.Wang, W.D.Tian, X.Q.Yu, L.Y.Zhang, L.Li, Y.Y.Yang, P.Ma, X.H.Zhang, J.Su, E.T.Li, Z.G.Hu, Z.Y.Guo, X.Xu, X.H.Yuan, W.Lu, Y.H.Yu, Y.D.Zang, S.W.Ye, R.P.Ye, J.D.Chen, S.L.Jin, C.M.Du, S.T.Wang, J.B.Ma, L.X.Liu, Z.Bai, X.Q.Li, X.G.Lei, Z.Y.Sun, Y.H.Zhang, X.H.Zhou, H.S.Xu Study of proton resonances in 18Ne via resonant elastic scattering of 17F + p and its astrophysical implication in the stellar reaction of 14O(α, p)17F NUCLEAR REACTIONS 1H, 12C(17F, X), E=4.22 MeV/nucleon; measured E(particle), I(particle, θ); deduced σ(θ), R-matrix resonance parameters; calculated σ(θ), α spectroscopic factors, resonant reaction rates using multichannel R-matrix.
doi: 10.1140/epja/i2011-11067-6
2002LI41 Appl.Radiat.Isot. 57, 399 (2002) Y.Li, S.Shen, S.Shi, J.Gu, X.Yu, J.Liu, J.Zeng A Decay Study of 70As RADIOACTIVITY 70As(EC), (β+) [from 70Ge(p, n)]; measured Eγ, Iγ, γγ-coin. 70Ge deduced levels, J, π.
doi: 10.1016/S0969-8043(02)00126-4
2000SH48 J.Radioanal.Nucl.Chem. 246, 423 (2000) S.Shen, J.Liu, J.Gu, X.Yu, Y.Li, D.Yin, S.Shi 188Os Low Excited Levels RADIOACTIVITY 188Re(β-); measured Eγ, Iγ(t), γγ-coin; deduced β-branching ratios. 188Os deduced levels, J, π.
doi: 10.1023/A:1006728104225
2000SH49 Eur.Phys.J. A 9, 463 (2000) S.Shen, X.Yu, S.Shi, J.Gu, J.Liu, Y.Li, Z.Zhu Decay of 83Sr and Level Structure of 83Rb RADIOACTIVITY 83Sr(β+), (EC) [from 85Rb(p, 3n)]; measured Eγ, Iγ, γγ-coin. 83Rb deduced levels, J, π, branching ratios, log ft. Comparison with shell model calculations.
doi: 10.1007/s100500070004
2000YU03 Int.J.Mod.Phys. E9, 471 (2000) X.Yu, S.Shi, J.Gu, J.Liu, W.Li, S.Shen, Y.Li Low-Spin States of 83Rb Excited in the 83Sr(β+ + EC)83Rb Decay RADIOACTIVITY 83Sr(β+), (EC) [from 85Rb(p, 3n)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 83Rb deduced levels, J, π. Radiochemical separation.
doi: 10.1142/S0218301300000350
1999FA20 High Energy Phys. and Nucl.Phys. (China) 23, 820 (1999) K.Fang, J.Liu, S.Shi, J.Gu, J.Zeng, X.Yu, S.Shen, Y.Li Decay of 95Ru
1999LI56 High Energy Phys. and Nucl.Phys. (China) 23, 320 (1999) Y.Li, J.Gu, X.Yu, J.Liu, Y.Cao, J.Zeng, W.Li, S.Shi Study of the Low Excited States of 72Ge
1998YE01 J.Nucl.Sci.Technol.(Tokyo) 35, 1 (1998) B.Ye, R.Han, Z.Wang, Y.Fan, X.Yu, H.Du, Z.Xiao Measurement of Alpha-Particles Emitted from Interaction of 14.6 MeV Neutrons with Elemental Nickel NUCLEAR REACTIONS Ni(n, xα), E=14.6 MeV; measured σ(Eα, θ); deduced total α-emission σ. Thick target, comparison with previous results.
doi: 10.1080/18811248.1998.9733813
1998YU07 High Energy Phys. and Nucl.Phys. (China) 22, 1082 (1998) X.Yu, S.Shi, J.Gu, J.Liu, W.Li, J.Zeng, J.Tian, Y.Li, J.Zhou Low-lying level structure of 83Rb
1997YE06 Nucl.Instrum.Methods Phys.Res. A398, 224 (1997) B.Ye, X.Yu, Y.Fan, Z.Wang, S.Jin, R.Han, H.Du, Z.Xiao Particle Identification in the Measurement of Differential (n, x) Cross Sections NUCLEAR REACTIONS Ni(n, X), E=14.6 MeV; measured p-, α-spectra; deduced detector system perfomance.
doi: 10.1016/S0168-9002(97)00325-2
1997ZH44 High Energy Phys. and Nucl.Phys. (China) 21, 201 (1997) X.Zhang, S.Yuan, W.Yang, Z.Li, W.Mou, X.Yu, Y.Luo, T.Guo Internal conversion effect applications in identifying new neutron-rich nuclides in the rare-earth region
1996ZH03 Z.Phys. A353, 353 (1996) X.Zhang, S.Yuan, W.Yang, Z.Li, W.Mou, X.Yu, J.Zhong The γ-Decay of a New Neutron-Rich Nucleus 175Er NUCLEAR REACTIONS 176Yb(n, 2p), E=14 MeV; measured γγ-, γ(X-ray)-coin, Eγ, Iγ. RADIOACTIVITY 175Er(β-) [from 176Yb(n, 2p), E=14 MeV]; measured γγ-, γ(X-ray)-coin, Eγ, Iγ; deduced T1/2. 175Tm deduced levels, J, π, band structure.
1996ZH39 High Energy Phys. and Nucl.Phys. (China) 20, 673 (1996) X.Zhang, S.Yuan, W.Yang, W.Mou, X.Yu, Z.Li, T.Guo, Y.Du, X.Luo The Decay Scheme of 175Er
1995LI54 Chin.J.Nucl.Phys. 17, No 1, 21 (1995) G.-X.Liu, K.-L.Chen, X.Yu, J.-W.Zheng, W.-Y.Jin, T.-Y.Sun, D.-Q.Wu, L.-L.Zhao, X.Zang, X.-M.Yin, Z.Qin Fragment Angular Distributions for 40Ar + 197Au Reaction NUCLEAR REACTIONS 197Au(40Ar, X), E=600 MeV; measured Eγ, Iγ; deduced σ(fragment θ), reaction mechanism. Off-line γ-spectroscopy.
1995LI55 Chin.J.Nucl.Phys. 17, No 1, 24 (1995) G.-X.Liu, G.-X.Dai, K.-L.Chen, X.Yu Angular Distributions of Projectile Fragmentation in the 600 MeV 40Ar + 197Au Reaction NUCLEAR REACTIONS 197Au(40Ar, X), E=600 MeV; measured σ(fragment θ) for X=7Be, 24Na, 28Mg. Glauber statistical model. Off-line γ-spectroscopy.
1995YA22 High Energy Phys. and Nucl.Phys. (China) 19, 479 (1995) W.Yang, S.Yuan, W.Mou, X.Zhang, Z.Li, X.Yu, Z.Gan, H.Liu, Y.Guo, J.Zhao, X.Lei, J.Guo, Y.Du, L.Zhao, X.Zhang A New Heavy Neutron-Rich Isotope 239Pa
1995YA23 High Energy Phys. and Nucl.Phys. (China) 19, 959 (1995) W.Yang, S.Yuan, X.Zhang, X.Yu, W.Mou, Z.Li, Z.Gan, H.Liu, J.Guo, J.Zhong, X.Sun The Synthesis and γ Decay of New Heavy Neutron-Rich Nuclide 175Er
1995YU01 Z.Phys. A352, 235 (1995) S.Yuan, W.Yang, W.Mou, X.Zhang, Z.Li, X.Yu, J.Gu, Y.Guo, Z.Gan, H.Liu, J.Guo A New Isotope of Protactinium: 239Pa NUCLEAR REACTIONS U(18O, X), E=50 MeV/nucleon; measured Eγ, Iγ, γγ(X-ray)-coin, γγ(X-ray)(t); deduced evidence for 239Pa. RADIOACTIVITY 239Pa(β-) [from U(18O, X), E=50 MeV/nucleon]; measured Eγ, Iγ, γγ(X-ray)-coin, γγ(X-ray)(t); deduced T1/2. 239U deduced transitions.
doi: 10.1007/BF01289491
1994YE09 Nucl.Instrum.Methods Phys.Res. A345, 115 (1994) B.Ye, W.Fan, Y.Fan, X.Yu, W.Mei, Z.Wang, R.Han, Z.Xiao Development of a Pulse Shape Discrimination Circuit NUCLEAR REACTIONS 6Li(d, p), (d, α), E=0.15 MeV; 1H(n, p), E=14 MeV; measured Ep, Eα, γ spectra; deduced pulse shape discrimination circuit features.
doi: 10.1016/0168-9002(94)90979-2
1993JO01 Phys.Rev. C47, 110 (1993) C.E.Jones, E.J.Beise, J.E.Belz, R.W.Carr, B.W.Filippone, W.Lorenzon, R.D.McKeown, B.A.Mueller, T.G.O'Neill, G.W.Dodson, K.Dow, M.Farkhondeh, S.Kowalski, K.Lee, N.Makins, R.Milner, A.Thompson, D.Tieger, J.F.van den Brand, A.Young, X.Yu, J.D.Zumbro 3He(pol)(e(pol), e') Quasielastic Asymmetry NUCLEAR REACTIONS 3He(polarized e, e'), E=574 MeV; measured spin-dependent asymmetry. Model comparison. Longitudinal beam polarization, polarized target.
doi: 10.1103/PhysRevC.47.110
1991JO06 Phys.Rev. C44, R571 (1991) C.E.Jones-Woodward, E.J.Beise, J.E.Belz, R.W.Carr, B.W.Filippone, W.Lorenzon, R.D.McKeown, B.A.Mueller, T.G.O'Neill, G.Dodson, K.Dow, M.Farkhondeh, S.Kowalski, K.Lee, N.Makins, R.Milner, A.Thompson, D.Tieger, J.F.J.van den Brand, A.Young, X.Yu, J.D.Zumbro Determination of the Neutron Electric Form Factor in Quasielastic Scattering of Polarized Electrons from Polarized 3He NUCLEAR REACTIONS 3He(polarized e, e'), E=574 MeV; measured spin dependent asymmetry. 1n deduced electric form factor. Polarized target.
doi: 10.1103/PhysRevC.44.R571
1991WO02 Nucl.Phys. A527, 367c (1991) C.Woodward, E.Beise, J.E.Belz, R.Carr, B.Filippone, W.Lorenzon, R.McKeown, B.Mueller, T.O'Neill, G.Dodson, K.Dow, M.Farkhondeh, S.Kowalski, K.Lee, N.Makins, R.Milner, A.Thompson, D.Tieger, J.van den Brand, A.Young, X.Yu, J.Zumbro Measurement of Inclusive Quasielastic Scattering of Polarized Electrons from Polarized 3He NUCLEAR REACTIONS 3He(polarized e, e), E=574 MeV; measured asymmetry, quasielastic scattering. Polarized target, longitudinal beam polarization.
doi: 10.1016/0375-9474(91)90126-Q
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