NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = L.Mao Found 5 matches. 2018TU03 Phys.Rev. C 97, 014321 (2018) X.L.Tu, X.C.Chen, J.T.Zhang, P.Shuai, K.Yue, X.Xu, C.Y.Fu, Q.Zeng, X.Zhou, Y.M.Xing, J.X.Wu, R.S.Mao, L.J.Mao, K.H.Fang, Z.Y.Sun, M.Wang, J.C.Yang, Yu.A.Litvinov, K.Blaum, Y.H.Zhang, Y.J.Yuan, X.W.Ma, X.H.Zhou, H.S.Xu First application of combined isochronous and Schottky mass spectrometry: Half-lives of fully ionized 49Cr24+ and 53Fe26+ atoms RADIOACTIVITY 49Cr, 53Fe(β+)[from 9Be(58Ni, X), E=430.8 MeV/nucleon followed by separation of fragments using projectile fragment separator RIBLL2]; measured half-life of bare (fully-ionized) ions by isochronous and Schottky mass spectrometry technique using experimental cooler storage ring (CSRe) at the Heavy Ion Research Facility, Lanzhou (HIRFL-CSR). Comparison with half-lives of neutral atoms.
doi: 10.1103/PhysRevC.97.014321
2015MA27 Phys.Rev. C 91, 044604 (2015) Dynamical and statistical description of multifragmentation in heavy-ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=80 MeV; 46Ti(16O, X), E(cm)=38 MeV; 92Zr(16O, X), E(cm)=50 MeV; calculated excitation energy and density distributions of fragments. 197Au(197Au, X), E=35 MeV/nucleon; calculated excitation energies per nucleon, and charge distributions of fragments. Hybrid model of improved quantum molecular dynamics (ImQMD) model plus the statistical model GEMINI. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.044604
2015MA67 Phys.Scr. T166, 014012 (2015) X.Ma, W.Q.Wen, Z.K.Huang, H.B.Wang, Y.J.Yuan, M.Wang, Z.Y.Sun, L.J.Mao, J.C.Yang, H.S.Xu, G.Q.Xiao, W.L.Zhan Proposal for precision determination of 7.8 eV isomeric state in 229Th at heavy ion storage ring
doi: 10.1088/0031-8949/2015/T166/014012
2015WE01 Nucl.Phys. A933, 114 (2015) D.Wei, L.Mao, N.Wang, M.Liu, L.Ou Further study on mechanism of production of light complex particles in nucleon-induced reactions NUCLEAR REACTIONS 27Al(p, d), (p, t), (p, 3He), (p, α), E=62 MeV;56Fe(n, d), (n, 3H), (n, 3He), (n, α), E=62, 175 MeV;58Ni(p, d), (p, t), (p, 3He), (p, α), E=1200 MeV;58Ni(p, p'), (p, n), (p, d), (p, t), (p, 3He), (p, α), E=175 MeV;63Cu(n, d), (n, 3H), E=317, 383, 477, 542 MeV;197Au(p, d), (p, t), (p, 3He), (p, α), E=1200 MeV; calculated σ(θ, Eout) using transport model and statistical model. Compared with available data.
doi: 10.1016/j.nuclphysa.2014.10.020
2009WA05 Int.J.Mod.Phys. E18, 352 (2009) M.Wang, H.S.Xu, J.W.Xia, X.L.Tu, R.S.Mao, Y.J.Yuan, Z.G.Hu, Y.Liu, H.B.Zhang, Y.D.Zang, T.C.Zhao, X.Y.Zhang, F.Fu, J.C.Yang, L.J.Mao, C.Xiao, G.Q.Xiao, H.W.Zhao, W.L.Zhan First isochronous mass measurements at CSRe
doi: 10.1142/S0218301309012380
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