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NSR database version of May 10, 2024.

Search: Author = X.Yu

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2024YU04      Eur.Phys.J. A 60, 22 (2024)

X.Yu, L.Wu, L.Yu, X.Wang

Exploring the chiral and deconfinement phase transitions in a self-consistent PNJL model

doi: 10.1140/epja/s10050-024-01239-0
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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
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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
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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
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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
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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
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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
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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
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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
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2021HE09      Chin.Phys.C 45, 014110 (2021)

Y.He, X.Yu, H.-F.Zhang

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
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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
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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
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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
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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
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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
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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
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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
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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
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2016YU02      Nucl.Phys. A949, 1 (2016)

X.Yu, L.Zamick

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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