NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Y.Tian Found 68 matches. 2024SA20 Phys.Rev.Lett. 132, 162501 (2024) S.N.Santiesteban, S.Li, D.Abrams, S.Alsalmi, D.Androic, K.Aniol, J.Arrington, T.Averett, C.Ayerbe Gayoso, J.Bane, S.Barcus, J.Barrow, A.Beck, V.Bellini, H.Bhatt, D.Bhetuwal, D.Biswas, A.Camsonne, J.Castellanos, J.Chen, J.-P.Chen, D.Chrisman, M.E.Christy, C.Clarke, S.Covrig, R.Cruz-Torres, D.Day, D.Dutta, E.Fuchey, C.Gal, F.Garibaldi, T.N.Gautam, T.Gogami, J.Gomez, P.Gueye, T.J.Hague, J.O.Hansen, F.Hauenstein, W.Henry, D.W.Higinbotham, R.J.Holt, C.Hyde, K.Itabashi, M.Kaneta, A.Karki, A.T.Katramatou, C.E.Keppel, P.M.King, L.Kurbany, T.Kutz, N.Lashley-Colthirst, W.B.Li, H.Liu, N.Liyanage, E.Long, A.Lovato, J.Mammei, P.Markowitz, R.E.McClellan, F.Meddi, D.Meekins, R.Michaels, M.Mihovilovic, A.Moyer, S.Nagao, D.Nguyen, M.Nycz, M.Olson, L.Ou, V.Owen, C.Palatchi, B.Pandey, A.Papadopoulou, S.Park, T.Petkovic, S.Premathilake, V.Punjabi, R.D.Ransome, P.E.Reimer, J.Reinhold, S.Riordan, N.Rocco, V.M.Rodriguez, A.Schmidt, B.Schmookler, E.P.Segarra, A.Shahinyan, S.Sirca, K.Slifer, P.Solvignon, T.Su, R.Suleiman, L.Tang, Y.Tian, W.Tireman, F.Tortorici, Y.Toyama, K.Uehara, G.M.Urciuoli, D.Votaw, J.Williamson, B.Wojtsekhowski, S.Wood, Z.H.Ye, J.Zhang, X.Zheng Novel Measurement of the Neutron Magnetic Form Factor from A=3 Mirror Nuclei NUCLEAR REACTIONS 3H, 3He(e-, e-), E=2.222, 4.323 GeV; measured reaction products; deduced σ(θ, E), the neutron magnetic form factor using quasielastic scattering from the mirror nuclei. Comparison with available data. Hall A at Jefferson Lab (JLab).
doi: 10.1103/PhysRevLett.132.162501
2024WA14 Phys.Lett. B 850, 138503 (2024) J.G.Wang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, H.B.Yang, C.L.Yang, Y.H.Qiang, X.Y.Huang, Z.Zhao, S.Y.Xu, Z.C.Li, L.X.Chen, L.C.Sun, H.Zhou, X.Zhang, X.L.Wu, Y.L.Tian, Y.S.Wang, J.Y.Wang, W.X.Huang, M.L.Liu, Z.W.Lu, Y.He, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov α-decay properties of new neutron-deficient isotope 203Ac RADIOACTIVITY 203Ac, 199Fr, 195At, 191Bi(α) [from 169Tm(40Ca, 6n)203Ac, E=226 MeV]; measured decay products, Eα, Iα; deduced α-particle energies, transitions T1/2, J, π, partial decay scheme, reduced α-decay widths, proton separation energies, the onset of deformation in neutron-deficient Ac isotopes. Comparison with systematics. The superconducting linear accelerator, China Accelerator Facility for superheavy Elements (CAFE2) at Institute of Modern Physics, Chinese Academy of Sciences.
doi: 10.1016/j.physletb.2024.138503
2024YA04 Phys.Rev.Lett. 132, 072502 (2024) H.B.Yang, Z.G.Gan, Y.J.Li, M.L.Liu, S.Y.Xu, C.Liu, M.M.Zhang, Z.Y.Zhang, M.H.Huang, C.X.Yuan, S.Y.Wang, L.Ma, J.G.Wang, X.C.Han, A.Rohilla, S.Q.Zuo, X.Xiao, X.B.Zhang, L.Zhu, Z.F.Yue, Y.L.Tian, Y.S.Wang, C.L.Yang, Z.Zhao, X.Y.Huang, Z.C.Li, L.C.Sun, J.Y.Wang, H.R.Yang, Z.W.Lu, W.Q.Yang, X.H.Zhou, W.X.Huang, N.Wang, S.G.Zhou, Z.Z.Ren, H.S.Xu Discovery of New Isotopes 160Os and 156W: Revealing Enhanced Stability of the N=82 Shell Closure on the Neutron-Deficient Side NUCLEAR REACTIONS 106Cd(58Ni, 4n)160Os, E=335 MeV; measured reaction products; deduced new isotopes, σ. The Spectrometer for Heavy Atoms and Nuclear Structure (SHANS), the Sector Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL), China. RADIOACTIVITY 160Os(α), 156W(β+); measured decay products, Eα, Iα; deduced α-particles energies, Q-values, T1/2, α-decay reduced widths, N=82 shell closure toward the proton drip line. Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.132.072502
2024ZH04 Phys.Rev. C 109, 014608 (2024) M.M.Zhang, Z.Y.Zhang, Z.G.Gan, N.Wang, H.Yao, J.G.Wang, M.H.Huang, L.Ma, H.B.Yang, C.L.Yang, Y.L.Tian, Y.S.Wang, J.Y.Wang, Y.H.Qiang, X.L.Wu, S.Y.Xu, X.Y.Huang, Z.C.Li, Z.Zhao, L.C.Sun, H.Zhou, X.Zhang, G.Xie, L.Zhu, J.H.Zheng, Y.J.Li, F.Guan, Z.W.Lu, W.X.Huang, Y.He, H.S.Xu, Z.Z.Ren, S.G.Zhou Experimental cross section study of 40Ca + 175Lu: Searching for new neutron-deficient Pa isotopes
doi: 10.1103/PhysRevC.109.014608
2024ZH19 Phys.Rev. C 109, 034314 (2024) Z.Zhao, Z.G.Gan, Z.Y.Zhang, J.G.Wang, M.H.Huang, L.Ma, H.B.Yang, M.M.Zhang, C.L.Yang, S.Y.Xu, X.Y.Huang, Z.C.Li, L.C.Sun, X.L.Wu, Y.S.Wang, Y.L.Tian, Y.H.Qiang, J.Y.Wang, W.X.Huang, Y.He, L.T.Sun, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov Reinvestigation of the decay properties of 261, 262Bh at the gas-filled recoil separator SHANS2
doi: 10.1103/PhysRevC.109.034314
2023CH23 Phys.Rev. C 107, 054306 (2023) J.Chen, M.Liu, C.Yuan, S.Chen, N.Shimizu, X.Sun, R.Xu, Y.Tian Shell-model-based investigation on level density of Xe and Ba isotopes NUCLEAR STRUCTURE 131,132,133,134Sn, 132,133,134,135Sb, 133,134,135,136Te, 134,135,136,137I, 135,136,137,138Xe, 136,137,138,139Cs, 137,138,139,140Ba; calculated one-neutron separation energy S(n). 132,133,134Sn, 132,133,134,135Sb, 134,135,136Te, 135,136,137I, 136,137,138Xe, 137,138,139Cs, 138,139,140Ba; calculated two-neutron separation energies S(2n). 134, ,136,138Xe, 134,136,138,140Ba, 128,129,130,134,135,136Sn, 131,135Sb, 132,134,136Te, 133,135,137I, 135,137,139Cs, 139La; calculated levels, J, π. 133,134,135,136,137Xe, 134,135,136,137,138,139Ba; calculated nuclear level densities (NLD), cumulative number of levels spin distributions. 134Te, 135I, 136Xe, 137Cs, 138Ba, 139La; calculated effective single particle energy for proton and neutron orbits with and without the consideration of tensor part in two-body matrix elements. 133,134,135,136,137Xe; calculated spin distribution , parity ratios, spin cut-off parameter. Configuration-interaction shell model with a unified effective nuclear force. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.054306
2023TI01 Phys.Rev. C 107, 015201 (2023) Y.Tian, for the CLAS Collaboration Exclusive π- electroproduction off the neutron in deuterium in the resonance region NUCLEAR REACTIONS 2H(e, e'pπ-), E=2.039 GeV; measured reaction products; deduced σ(θ), kinematically defined final-state-interaction contribution factor, exclusive structure functions, Legendre moments of the exclusive structure functions. CEBAF Large Acceptance Spectrometer (CLAS) detector at JLAB.
doi: 10.1103/PhysRevC.107.015201
2022HU12 Phys.Lett. B 834, 137484 (2022) M.H.Huang, Z.G.Gan, Z.Y.Zhang, L.Ma, J.G.Wang, M.M.Zhang, H.B.Yang, C.L.Yang, X.Y.Huang, Z.Zhao, S.Y.Xu, L.X.Chen, X.J.Wen, Y.F.Niu, C.X.Yuan, Y.L.Tian, Y.S.Wang, J.Y.Wang, M.L.Liu, Y.H.Qiang, W.Q.Yang, H.B.Zhang, Z.W.Lu, S.Guo, W.X.Huang, Y.He, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov α decay of the new isotope 204Ac RADIOACTIVITY 204,205Ac(α) [from 169Tm(40Ca, xn), E=202, 210, 212, 214 MeV using SHANS2 separator at CAFE2 and SHANS separator at HRIFL, Lanzhou accelerator facility]; 200Fr, 196At(α) [from 204Ac α-decay chain]; measured evaporation residues (ERs), Eα, (ER)α-α-α correlated events, production cross sections, T1/2 of decays using two multiwire proportional counters for implanted events, double-sided silicon strip detectors (DSSSDs) for α particles, and a segmented clover Ge detector for γ radiation. 204,205Ac, 200Fr, 196At; deduced T1/2 of decays of ground-state decays, and Eα values, reduced α-width in Rasmussen formalism, favored α decay for 204Ac decay. 204Ac(p); no proton decay events observed. 201,201m,202,202m,203,204,205Fr, 204,205,206Ra(α); observed α spectra, (ERs)-α-α-correlated events. Comparison with previous available experimental results. Systematics of experimental and theoretical T1/2 and Q(α) values for 196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211At, 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213Fr, 203,204,205,206,207,208,209,210,211,212,213,214,215Ac, 211,212,213,214,215,216,217Pa, using Hartree-Fock-BCS (HFBSC) method, and macroscopic-microscopic (MM) mass formula for theory.
doi: 10.1016/j.physletb.2022.137484
2022MA45 Phys.Rev. C 106, 064316 (2022) L.Ma, H.B.Yang, Z.Y.Zhang, J.C.Pei, M.H.Huang, M.M.Zhang, C.Y.Qiao, X.J.Bao, Y.L.Tian, C.L.Yang, Y.S.Wang, Z.Zhao, X.Y.Huang, S.Y.Xu, W.X.Huang, Z.Liu, X.H.Zhou, Z.G.Gan Attempts to produce new americium isotopes near N=126 NUCLEAR REACTIONS 191,193Ir(40Ar, xn)231Am*/233Am*, E=190-204 MeV; measured reaction products, Eα, (recoils)α-α-α correlated events, using SHANS gas-filled recoil separator, 16 position-sensitive Si-strip detectors (PSSDs) for evaporation residues, and eight side silicon detectors (SSDs) for α particles at the HRIFL-Lanzhou facility. 226,227,228Am; no evidence found for the detection of these nuclides, with upper limits of cross sections determined for the production of the compound nuclei of 231Am and 233Am; discussed nonobservation of new americium isotopes in terms of reduced survival probabilities of compound nuclei 231Am and 233Am due to their low fission barriers at high excitations. NUCLEAR STRUCTURE 226,227,228,229Am; calculated excitation functions for the production of these nuclides in 191,193Ir(40Ar, xn) using the statistical model code HIVAP. 230,231,232,233,234,235,236Am; evaluated shell correction energies and fission barriers from FRDM2012, KTUY2005, and WS2010. 226U, 227Np, 231,233Am; calculated fission barrier heights as functions of excitation energy and quadrupole deformation parameter β2 using microscopic finite-temperature Skyrme Hartree-Fock+BCS theory.
doi: 10.1103/PhysRevC.106.034316
2022SU03 Prog.Theor.Exp.Phys. 2022, 013D01 (2022) K.N.Suzuki, T.Gogami, B.Pandey, K.Itabashi, S.Nagao, K.Okuyama, S.N.Nakamura, L.Tang, D.Abrams, T.Akiyama, D.Androic, K.Aniol, C.Ayerbe Gayoso, J.Bane, S.Barcus, J.Barrow, V.Bellini, H.Bhatt, D.Bhetuwal, D.Biswas, A.Camsonne, J.Castellanos, J.-P.Chen, J.Chen, S.Covrig, D.Chrisman, R.Cruz-Torres, R.Das, E.Fuchey, K.Gnanvo, F.Garibaldi, T.Gautam, J.Gomez, P.Gueye, T.J.Hague, O.Hansen, W.Henry, F.Hauenstein, D.W.Higinbotham, C.E.Hyde, M.Kaneta, C.Keppel, T.Kutz, N.Lashley-Colthirst, S.Li, H.Liu, J.Mammei, P.Markowitz, R.E.McClellan, F.Meddi, D.Meekins, R.Michaels, M.Mihovilovic, A.Moyer, D.Nguyen, M.Nycz, V.Owen, C.Palatchi, S.Park, T.Petkovic, S.Premathilake, P.E.Reimer, J.Reinhold, S.Riordan, V.Rodriguez, C.Samanta, S.N.Santiesteban, B.Sawatzky, S.Sirca, K.Slifer, T.Su, Y.Tian, Y.Toyama, K.Uehara, G.M.Urciuoli, D.Votaw, J.Williamson, B.Wojtsekhowski, S.A.Wood, B.Yale, Z.Ye, J.Zhang, X.Zheng The cross-section measurement for the 3H(e, e'K+)nnΛ reaction NUCLEAR REACTIONS 3H(e-, e-'K+), E not given; measured reaction products; deduced σ(θ), missing mass. Comparison with Monte Carlo simulations.
doi: 10.1093/ptep/ptab158
2022TI01 Nucl.Instrum.Methods Phys.Res. A1026, 166151 (2022) Yu.E.Titarenko, V.F.Batyaev, K.V.Pavlov, A.Yu.Titarenko, S.V.Malinovskiy, V.I.Rogov, V.M.Zhivun, T.V.Kulevoy, M.V.Chauzova, R.S.Khalikov, A.V.Ignatyuk, V.Yu.Blandinskiy, A.A.Kovalishin, M.I.Baznat, A.Yu.Stankovskiy, A.I.Dubrouski, H.I.Kiyavitskaya, T.Xue, Y.Tian, M.Zeng, Z.Zeng, O.Normahmedov, T.Sato 206, 207, 208, natPb(p, x)194Hg and 209Bi(p, x)194Hg excitation functions in the energy range 0.04-2.6 GeV NUCLEAR REACTIONS Pb, 209Bi(p, X)194Hg, E=0.04-2.6 GeV; measured reaction products, Eγ, Iγ; deduced production σ. Comparison with theoretical calculations.
doi: 10.1016/j.nima.2021.166151
2022YA15 Phys.Rev. C 105, L051302 (2022) H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, C.X.Yuan, Y.F.Niu, C.L.Yang, Y.L.Tian, L.Guo, Y.S.Wang, J.G.Wang, H.B.Zhou, X.J.Wen, H.R.Yang, X.H.Zhou, Y.H.Zhang, W.X.Huang, Z.Liu, S.G.Zhou, Z.Z.Ren, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, D.I.Solovyev New isotope 207Th and odd-even staggering in α-decay energies for nuclei with Z > 82 and N < 126 RADIOACTIVITY 207Th(α)[from 176Hf(36Ar, 5n), E=197-199 MeV]; 208Th(α)[from 176Hf(36Ar, 4n), E=197-199 MeV]; 203Ra, 199Rn, 195Po(α)[from 207Th α-decay chain]; 204Ra, 200Rn, 196Po(α)[from 208Th α-decay chain]; measured evaporation residues (ERs), Eα, and ER-α1-α2-α3-α4 correlated α-decay chain from the decays of 207Th and208Th. 207,208Th; deduced α-decay T1/2, production σ. Z=84-92, N=102-126; discussed systematics of experimental and theoretically calculated (by relativistic Hartree-Fock-Bogoliubov and large-scale shell-model approaches) odd-even staggering (OES) of Q(α), Q(proton) and Q(neutron). Position-sensitive silicon strip detectors (PSSDs), non-position sensitive Si detectors, and SHANS gas-filled recoil separator at the sector focusing cyclotron facility of HIRFL, Lanzhou.
doi: 10.1103/PhysRevC.105.L051302
2022YA27 Phys.Rev. C 106, 064311 (2022) H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, C.L.Yang, Y.L.Tian, Y.S.Wang, H.B.Zhou, X.J.Wen, J.G.Wang, Z.Zhao, S.Y.Xu, L.X.Chen, X.Y.Huang, C.X.Yuan, Y.F.Niu, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, S.G.Zhou, Z.Z.Ren, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, D.I.Solovyev Examining the impact of α-decay energies on the odd-even staggering in half-lives: α-decay spectroscopy of 207-209Ac RADIOACTIVITY 207,208,208m,209Ac(α)[from 176Hf(36Ar, X), E=197-199 MeV]; measured evaporation residues (ER), Eα, Iα, αα-coin, (ER)αα-coin; deduced T1/2, Q values, decay branches. 204mFr(IT) [from 208Ac(α)]; deduced T1/2, isomer level energy, tentative J and π for the newly found 80-keV isomer. 204Fr(α)[from 208,208mAc(α)]; deduced T1/2. Found new α-decay branching 208Ac and assigned to the transition from ground state to the excited (2+, 4+) state. Comparison to the calculations performed in the framework of Wentzel-Kramers-Brillouin approximation. Spectrometer for Heavy Atoms and Nuclear Structure (SHANS) at Sector Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL).
doi: 10.1103/PhysRevC.106.064311
2022ZH07 Phys.Rev. C 105, 024328 (2022) H.B.Zhou, Z.Y.Li, Z.G.Gan, Z.Y.Zhang, H.Yao, N.Wang, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, X.H.Zhou, J.L.Tian Modeling the fusion process with a modified Woods-Saxon potential in 40Ar-induced fusion reactions NUCLEAR REACTIONS 176Hf(40Ar, 2np)212Ac, (40Ar, 3np)213Ac, (40Ar, 2nα)209Ra, (40Ar, 3nα)210Ra, E=183, 190 MeV; measured reaction products, Eα, Iα; deduced σ(E), theory evaluation factors. Observed α peaks from decays of 211,212,213,213Ra, 214,215Ac. Comparison to density-constrained time-dependent Hartree-Fock theory calculations. Beam from Sector-Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL). 165Ho(40Ar, 4n), E(cm)=130-160 MeV; 169Tm(40Ar, 4n), E(cm)=130-170 MeV; 174Yb(40Ar, 4n), (40Ar, 5n), E(cm)=130-170 MeV; 175Lu(40Ar, 4n), (40Ar, 5n), E(cm)=130-170 MeV; 176Hf(40Ar, 4n), (40Ar, 5n), E(cm)=135-165 MeV; 181Ta(40Ar, 4n), E(cm)=130-160 MeV; analyzed σ(E) from 1984VE09.
doi: 10.1103/PhysRevC.105.024328
2022ZH45 Phys.Rev. C 106, 024305 (2022) M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Zhang, Z.G.Gan, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, J.G.Wang, C.X.Yuan, C.Qi, A.N.Andreyev, X.Y.Huang, S.Y.Xu, Z.Zhao, L.X.Chen, J.Y.Wang, M.L.Liu, Y.H.Qiang, G.S.Li, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Y.F.Niu, L.Guo, Z.Z.Ren, S.G.Zhou Fine structure in the α decay of the 8+ isomer in 216, 218U RADIOACTIVITY 216,216m,218,218mU(α)[218U from 182W(40Ar, 4n), E=190 MeV, 184W(40Ca, 2nα), E=206 MeV, 216U from 180W(40Ar, 4n), E=191 MeV]; measured evaporation residues (EVRs), Eα, Iα, (EVR)α1-α2-correlations, T1/2 using position-sensitive strip detectors (PSSDs) for α detection, and SHANS separator at HIRFL-Lanzhou. 216,216m,218,218mU; deduced T1/2, Q-values, α-branching ratio, α-decay hindrance factors. 204Rn, 208,210Ra, 212,214Th(α)[from 216,218U α-decay chains]; measured Eα, T1/2. 212Th; deduced level, J, π, identification of the first 2+ state. 215Ra, 212,213,216Ac, 211,212,213,214,216,216m,217Th, 216,217,217m,218Pa, 217,218,219U; observed Eα from their decays from (EVR)α-correlations. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.106.024305
2021HU18 Chin.Phys.C 45, 044001 (2021) W.Hua, Z.Zhang, L.Ma, Z.Gan, H.Yang, C.Yuan, M.Huang, C.Yang, M.Zhang, Y.Tian, X.Zhou Fine structure of α decay in 222Pa RADIOACTIVITY 222Pa, 218Ac, 214Fr(α) [from 186W(40Ar, X)222Pa, E=198.7 MeV]; measured decay products, Eα, Iα; deduced Q-values, T1/2. Comparison with available data.
doi: 10.1088/1674-1137/abdea8
2021HU19 Chin.Phys.C 45, 044003 (2021) W.Hua, Z.Zhang, L.Ma, Z.Gan, H.Yang, M.Huang, C.Yang, M.Zhang, Y.Tian, X.Zhou, C.Yuan, C.Shen, L.Zhu α-decay study of 218Ac and 221Th in 40Ar+186W reaction RADIOACTIVITY 218Ac, 221Th, 217Ra, 213Rn(α) [from 186W(40Ar, X)221Th/218Ac, E=198.7 MeV]; measured decay products, Eα, Iα; deduced Q-values, T1/2. Comparison with available data.
doi: 10.1088/1674-1137/abe0bd
2021MA66 Phys.Rev. C 104, 044310 (2021) L.Ma, Z.Y.Zhang, H.B.Yang, M.H.Huang, M.M.Zhang, Y.L.Tian, C.L.Yang, Y.S.Wang, Z.Zhao, W.X.Huang, Z.Liu, X.H.Zhou, Z.G.Gan α-decay properties of 220Pa RADIOACTIVITY 220,220mPa(α)[from 187Re(40Ar, 3nα), E=198.7 MeV]; 216Ac(α)[from 220Pa(α)]; measured Eα, Iα, half-lives of decays of 220,220mPa using position-sensitive 16-strip detectors (PSSDs) at the Sector-Focusing Cyclotron and SHANS recoil separator of HIRF-Lanzhou. 220Pa, 216Ac; deduced levels, J, π, Q(α), reduced α-width, new isomer in 220Pa. Comparison with previous experimental data. Systematics of reduced α widths of N=129, Z=84-93 isotones.
doi: 10.1103/PhysRevC.104.044310
2021ZH22 Phys.Rev.Lett. 126, 152502 (2021) Z.Y.Zhang, H.B.Yang, M.H.Huang, Z.G.Gan, C.X.Yuan, C.Qi, A.N.Andreyev, M.L.Liu, L.Ma, M.M.Zhang, Y.L.Tian, Y.S.Wang, J.G.Wang, C.L.Yang, G.S.Li, Y.H.Qiang, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Z.Z.Ren, S.G.Zhou New α-Emitting Isotope 214U and Abnormal Enhancement of α-Particle Clustering in Lightest Uranium Isotopes RADIOACTIVITY 214,216,218U(α) [from 180,182W(36Ar, 4n), 184W(40Ca, 2nα), E<200 MeV]; measured decay products, Eα, Iα; deduced α-decay Q-values and reduced widths, T1/2, abnormal enhancement by the strong monopole interaction between the valence protons and neutrons. Comparison withavailable data, calculations.
doi: 10.1103/PhysRevLett.126.152502
2021ZH24 Phys.Rev. C 103, 044314 (2021) H.B.Zhou, Z.G.Gan, N.Wang, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Li, C.X.Yuan, S.Huang, X.J.Sun, H.Y.Peng, L.Ou, X.H.Zhou Lifetime measurement for the isomeric state in 213Th NUCLEAR REACTIONS 176Hf(40Ar, xn)213Th/214Th/215Th, E=183, 190 MeV beam from Sector-Focusing Cyclotron of HIRFL-Lanzhou facility, followed by the separation of evaporation residues (ERs) by the SHANS separator and implanted in three position-sensitive silicon strip detectors (PSSDs); measured position, time, and energy of the ERs, Eα, Iα, Eγ, Iγ, (ER)α-, (ER)γ- and (ER)αγ-correlated events. Enriched target. 213,214,215Th; deduced levels, J, π, isomers, half-lives of the isomers in 213,214,215Th. Comparison with previous experimental results for isomer half-lives. Systematics of 13/2+ isomers in N=123 isotones 207Po, 209Rn, 211Ra and 213Th. RADIOACTIVITY 209,210,211,213Ra, 212,213,215Ac, 211,212,213,214,215,216Th(α)[from 176,177,178,179,180Hf(40Ar, xnyp), E=183, 190 MeV, enriched 176Hf with small abundance of other Hf isotopes]; measured Eα, Iα, αγ-correlations.
doi: 10.1103/PhysRevC.103.044314
2020KA09 Nucl.Data Sheets 163, 109 (2020) T.Kawano, Y.S.Cho, P.Dimitriou, D.Filipescu, N.Iwamoto, V.Plujko, X.Tao, H.Utsunomiya, V.Varlamov, R.Xu, R.Capote, I.Gheorghe, O.Gorbachenko, Y.L.Jin, T.Renstrom, M.Sin, K.Stopani, Y.Tian, G.M.Tveten, J.M.Wang, T.Belgya, R.Firestone, S.Goriely, J.Kopecky, M.Krticka, R.Schwengner, S.Siem, M.Wiedeking IAEA Photonuclear Data Library 2019
doi: 10.1016/j.nds.2019.12.002
2020MA27 Phys.Rev.Lett. 125, 032502 (2020) L.Ma, Z.Y.Zhang, Z.G.Gan, X.H.Zhou, H.B.Yang, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, H.B.Zhou, X.T.He, Y.C.Mao, W.Hua, L.M.Duan, W.X.Huang, Z.Liu, X.X.Xu, Z.Z.Ren, S.G.Zhou, H.S.Xu Short-Lived α-Emitting Isotope 222Np and the Stability of the N = 126 Magic Shell NUCLEAR REACTIONS 187Re(40Ar, 5N)222Np, E=198.7 MeV; measured reaction products, Eα, Iα. 220Pa, 219Th; deduced Q-values, T1/2. Comparison with systematics.
doi: 10.1103/PhysRevLett.125.032502
2020SU07 Phys.Rev. C 101, 034302 (2020) X.Sun, R.Xu, Y.Tian, Z.Ma, Z.Zhang, Z.Ge, H.Zhang, E.N.E.van Dalen, H.Muther Relativistic mean-field approach in nuclear systems NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,132Sn, 208Pb; calculated binding energy per nucleon, charge radii, charge density distribution, single particle energies, spin-orbit splitting in 16O, scalar and vector potentials for neutrons and protons as a function of isospin asymmetry using both local density approximation (LDA) and improved LDA, based on Dirac-Brueckner-Hartree-Fock (DBHF) approach starting from a realistic nucleon-nucleon interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.034302
2020TI03 Nucl.Instrum.Methods Phys.Res. A984, 164635 (2020) Y.E.Titarenko, V.F.Batyaev, K.V.Pavlov, A.Y.Titarenko, S.V.Malinovskiy, V.I.Rogov, V.M.Zhivun, T.V.Kulevoy, M.V.Chauzova, S.V.Lushin, A.S.Busygin, A.V.Ignatyuk, P.N.Alekseev, V.Y.Blandinskiy, A.A.Kovalishin, S.I.Tyutyunnikov, A.A.Baldin, A.N.Sosnin, M.I.Baznat, A.Y.Stankovskiy, A.I.Dubrouski, H.I.Kiyavitskaya, T.Xue, Y.Tian, M.Zeng, Z.Zeng, T.Sato 208, 207, 206, natPb(p, x)207Bi and 209Bi (p, x)207Bi excitation functions in the energy range of 0.04 - 2.6 GeV NUCLEAR REACTIONS 206,207,208Pb, Pb, 209Bi(p, X)207Bi, E=0.04-2.6 GeV; measured reaction products, Eγ, Iγ; deduced σ and uncertainties. Comparison with MCNP-6.1, PHITS, Geant4 and TENDL-2019 calculations.
doi: 10.1016/j.nima.2020.164635
2020WU05 Phys.Lett. B 805, 135431 (2020) D.Wu, N.Y.Wang, B.Guo, C.Y.He, Y.Tian, X.Tao, T.L.Ma, F.L.Liu, W.S.Yang, J.H.Wei, Y.P.Shen, S.L.Guo, Q.W.Fan, X.G.Wu, Y.Zheng, T.X.Li, Z.Q.Wang, H.L.Luo, Y.N.Liu, M.L.Qiu New measurement of the 74Ge(p, γ)75As reaction cross sections in the p-process nucleosynthesis NUCLEAR REACTIONS 74Ge(p, γ), E(cm)=1-4.5 MeV; measured reaction products, Eγ, Iγ; deduced σ, reaction rates. Comparison with EMPIRE and TALYS nuclear model codes calculations.
doi: 10.1016/j.physletb.2020.135431
2020ZH01 Phys.Lett. B 800, 135102 (2020) M.M.Zhang, H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, C.L.Yang, C.X.Yuan, Y.S.Wang, Y.L.Tian, H.B.Zhou, S.Huang, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, X.X.Xu, J.G.Wang, H.R.Yang, L.M.Duan, W.Q.Yang, S.G.Zhou, Z.Z.Ren, X.H.Zhou, H.S.Xu, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, M.V.Shumeiko A new isomeric state in 218Pa RADIOACTIVITY 218Pa(α) [from 182W(40Ar, 3np)218Pa, E=190 MeV]; measured decay products, Eα, Iα, Eγ, Iγ; deduced ground and isomeric states T1/2, α and γ-ray energies and intensities, J, π.
doi: 10.1016/j.physletb.2019.135102
2019CH34 At.Data Nucl.Data Tables 129-130, 101278 (2019) Z.-B.Chen, Y.-S.Tian, C.-C.Sang, X.-L.Wang, K.Wang, X.-L.Guo Energies and transition parameters of fusion interest in Cr-like ions between Hf XLIX and Au LVI ATOMIC PHYSICS Z=72-79; calculated energies, wavelengths, and T1/2.
doi: 10.1016/j.adt.2019.03.003
2019TI10 Chin.Phys.C 43, 114102 (2019) Y.Tian, X.Tao, J.Wang, X.Ke, R.Xu, Z.Ge Giant dipole resonance parameters from photoabsorption cross-sections NUCLEAR STRUCTURE 34S, 40Ar, 40,42,44,46,48Ca, 48Ti, 51V, 52Cr, 90,91,92,94Zr, 112,114,116,117,118,119,120,122,124Sn, 138Ba, 208Pb, 209Bi, 23Na, 24,25Mg, 27Al, 28,29Si, 63,65Cu, 80Se, 127I, 133Cs, 159Tb, 181Ta, 182,184,186W, 186,188,189,190,192Os, 235U; analyzed available data; deduced systematic GDR parameters.
doi: 10.1088/1674-1137/43/11/114102
2019ZH23 Phys.Rev.Lett. 122, 192503 (2019) Z.Y.Zhang, Z.G.Gan, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, M.D.Sun, H.Y.Lu, W.Q.Zhang, H.B.Zhou, X.Wang, C.G.Wu, L.M.Duan, W.X.Huang, Z.Liu, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, Yu.S.Tsyganov, A.A.Voinov, A.N.Polyakov New Isotope 220Np: Probing the Robustness of the N=126 Shell Closure in Neptunium RADIOACTIVITY 220Np, 216Pa, 212Ac, 208Fr(α) [from 185Re(40Ar, 5n)220Np/216Pa/212Ac/208Fr, E=201 MeV]; measured decay products, Eα, Iα; deduced T1/2, Q-values. Comparison with systematics.
doi: 10.1103/PhysRevLett.122.192503
2019ZH39 Nucl.Phys. A990, 1 (2019) Z.Zhang, R.R.Xu, Z.Y.Ma, Z.G.Ge, Y.Tian, D.Y.Pang, X.D.Sun, Y.L.Jin, X.Tao, Y.Zhang, J.M.Wang Global α-nucleus optical model based on an Dirac Brueckner Hartree Fock approach
doi: 10.1016/j.nuclphysa.2019.06.013
2019ZH54 Phys.Rev. C 100, 064317 (2019) M.M.Zhang, Y.L.Tian, Y.S.Wang, X.H.Zhou, Z.Y.Zhang, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, Z.G.Gan, J.G.Wang, H.B.Zhou, S.Huang, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, X.X.Xu, L.M.Duan, Z.Z.Ren, S.G.Zhou, H.S.Xu Fine structure in the α decay of 219U RADIOACTIVITY 219U(α)[from 183W(40Ar, 4n), E=190 MeV]; measured Eα, Iα, αα-coin, (recoils)ααα-correlations, half-life of 219U decay, production σ of 219U using position-sensitive strip detectors (PSSDs) for α detection, and the SHANS separator at the Heavy Ion Research Facility (HIRFL) in Lanzhou. 215Th; deduced levels, J, π, α-branching ratios, α-decay reduced widths. 216,216m,217,219Th, 220Pa(α)[from 183W(40Ar, X), E=190 MeV]; 215Th, 211Ra[from 219U α decay]; measured Eα, half-lives of decays of the isotopes. Discussed α-decay systematics in neighboring nuclides. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.100.064317
2018TI06 Phys.Rev. C 97, 064615 (2018) Effects of nonlocality of nuclear potentials on direct capture reactions NUCLEAR REACTIONS 48Ca(n, γ), E=0.01-0.4 MeV; 7Li(n, γ), E=0.01-2 MeV; 12C(p, γ), E=0-1.2 MeV; calculated local and non-local potential parameters, s-wave phase shifts of target nuclides as function of incident energy, and σ(E) with the Perey-Buck-type nonlocal potentials using a potential model; deduced effects of potential nonlocality in direct radiative capture reactions. Comparison with experimental values.
doi: 10.1103/PhysRevC.97.064615
2018YA01 Phys.Lett. B 777, 212 (2018) H.B.Yang, L.Ma, Z.Y.Zhang, C.L.Yang, Z.G.Gan, M.M.Zhang, M.H.Huang, L.Yu, J.Jiang, Y.L.Tian, Y.S.Wang, J.G.Wang, Z.Liu, M.L.Liu, L.M.Duan, S.G.Zhou, Z.Z.Ren, X.H.Zhou, H.S.Xu, G.Q.Xiao Alpha decay properties of the semi-magic nucleus 219Np RADIOACTIVITY 219Np(α) [from 187Re(36Ar, 4n), E=191.5 MeV]; 218,218U, 215Pa(α); measured decay products, Eα, Iα; deduced α-particle energy, T1/2, Q-value. Comparison with available data.
doi: 10.1016/j.physletb.2017.12.017
2017GU19 Chin.Phys.C 41, 084105 (2017) R.-J.Guo, Z.-Q.Li, C.Liu, Y.-H.Tian, S.-Y.Wang Shell-model calculations for the semi-magic nucleus 85Br and systematic features of the N = 50 odd-A isotones* NUCLEAR STRUCTURE 85Br; calculated energy levels, J, π. Shell-model code nushellx within a large model space containing the neutron-core excitations across the N = 50 closed shell.
doi: 10.1088/1674-1137/41/8/084105
2017TI04 Chin.Phys.C 41, 044104 (2017) Y.-J.Tian, T.-H.Heng, Z.-M.Niu, Q.Liu, J.-Y.Guo Exploration of resonances by using complex momentum representation NUCLEAR STRUCTURE 17O; calculated the bound states and resonant states using the complex momentum representation in comparison with those obtained in coordinate representation by the complex scaling method for resonances.
doi: 10.1088/1674-1137/41/4/044104
2017TI05 Phys.Rev. C 95, 064329 (2017) Y.-J.Tian, Q.Liu, T.-H.Heng, J.-Y.Guo Research on the halo in 31Ne with the complex momentum representation method NUCLEAR STRUCTURE 31Ne; calculated single-particle spectra for several different deformations, neutron single-particle levels and resonances as a function of quadrupole deformation β2, occupation probabilities, widths of resonant states. Scattering phase shift approach or complex scaling method to explore the physical mechanism of a deformed halo in 31Ne.
doi: 10.1103/PhysRevC.95.064329
2016XU07 Phys.Rev. C 94, 034606 (2016) R.Xu, Z.Ma, Y.Zhang, Y.Tian, E.N.E.van Dalen, H.Muther Global analysis of isospin dependent microscopic nucleon-nucleus optical potentials in a Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 40Ca(n, n), E=2.06-185.0 MeV; 208Pb(n, n), E=1.8-155.0 MeV; 12C(n, n), E=1.04-225.0 MeV; 56Fe(n, n), E=1.8-75.0 MeV; 98Mo(n, n), E=1.5-26.0 MeV; 103Rh(n, n), E=4.51-10.0 MeV; 28Si, 90Zr, 120Sn(n, n), E=65 MeV; 27Al(n, n), E=3.2-26.0 MeV; 40Ca, 56Fe(p, p), E=61.5, 65 MeV; 28Si(p, p), E=14.26-250.0 MeV; 58Ni(p, p), E=7.0-250.0 MeV; 90Zr(p, p), E=9.7-185.0 MeV; 208Pb(p, p), E=16.0-201.0 MeV; calculated σ(θ, E). 12C, 40Ca(polarized n, n), E=10.9 MeV; 58Ni(polarized n, n), E=9.92 MeV; 208Pb(polarized n, n), E=9.97 MeV; 56Fe(polarized p, p), E=16.0-65.0 MeV; 58Ni(polarized p, p), E=16.0-250.0 MeV; 208Pb(polarized p, p), E=80, 200 MeV; calculated analyzing powers Ay(θ, E). 12C, 56Fe, 208Pb(n, X), 40Ca, 120Sn, 208Pb(p, X), E<200 MeV; calculated reaction σ(E). Global analysis of the isospin dependent nucleon-nucleus microscopic optical potential (MOP) based on the DBHF calculation in symmetric and asymmetric nuclear matter; deduced relativistic MOP for nucleon-nucleus scattering. Comparisons with experimental data, and with results from phenomenological Koning-Delaroche global potential. Compiled bibliographic information for experimental (n, n) data for 12C, 14N, 16O, 23Na, 24Mg, 27Al, 28Si, 31P, 32S, 39K, 40Ca, 48Ti, 52Cr, 55Mn, 56Fe, 59Co, 58Ni, 63Cu, 80Se, 88Sr, 89Y, 90Zr, 93Nb, 98Mo, 103Rh, 115In, 120Sn, 197Au, 208Pb, 209Bi targets, and experimental (p, p) data for 12C, 27Al, 28Si, 40Ca, 56Fe, 58Ni, 90Zr, 120Sn, 208Pb targets.
doi: 10.1103/PhysRevC.94.034606
2016ZH33 Yuan.Wul.Ping. 33, 217 (2016); Nucl.Phys.Rev. 33, 217 (2016) Z.Zhang, Z.Gan, L.Ma, H.Yang, J.Wang, L.Yu, J.Jiang, Y.Tian, B.Ding, S.Guo, Y.Wang, T.Huang, M.Sun, K.Wang Alpha Decay of the Neutron-deficient Isotopes 215, 216U RADIOACTIVITY 215,216U(α) [from 180W(40Ar, xn), E=189.5, 204.5, 207.6 MeV]; measured decay products, Eα, Iα; deduced energy levels, J, π, T1/2. Comparison with systematics.
doi: 10.11804/NuclPhysRev.33.02.217
2015MA37 Phys.Rev. C 91, 051302 (2015) L.Ma, Z.Y.Zhang, Z.G.Gan, H.B.Yang, L.Yu, J.Jiang, J.G.Wang, Y.L.Tian, Y.S.Wang, S.Guo, B.Ding, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, G.Q.Xiao α-decay properties of the new isotope 216U RADIOACTIVITY 216,216m,218,218mU(α)[from 180W(40Ar, xn), E=189.5 MeV]; measured evaporation residues (ER), Eα, Iα, correlated ER-α1-α2 events, α-decay half-lives using SHANS spectrometer at HIRFL-Lanzhou facility; deduced 216U new isotope and its isomeric state, and α-reduced widths. 212,214Th, 208,210Ra(α); measured Eα, Iα, α-decay half-lives, α-reduced widths. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.051302
2015YA13 Eur.Phys.J. A 51, 88 (2015) H.B.Yang, Z.Y.Zhang, J.G.Wang, Z.G.Gan, L.Ma, L.Yu, J.Jiang, Y.L.Tian, B.Ding, S.Guo, Y.S.Wang, T.H.Huang, M.D.Sun, K.L.Wang, S.G.Zhou, Z.Z.Ren, X.H.Zhou, H.S.Xu, G.Q.Xiao Alpha decay of the new isotope 215U RADIOACTIVITY 215U(α)[from 180W(40Ar, 5n)]; measured sequential α emission Eα, Iα(t), αα-coin; deduced α-decay energy, T1/2. NUCLEAR REACTIONS 180W(40Ar, 5n), E=205.5 MeV; measured reaction products; deduced σ. 180W(40Ar, xn), E=170-220 MeV; calculated σ for x=3-6 using HIVAP code. Compared with one other experimental point.
doi: 10.1140/epja/i2015-15088-9
2014ZH03 Phys.Rev. C 89, 014308 (2014) Z.Y.Zhang, Z.G.Gan, L.Ma, L.Yu, H.B.Yang, T.H.Huang, G.S.Li, Y.L.Tian, Y.S.Wang, X.X.Xu, X.L.Wu, M.H.Huang, C.Luo, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, G.Q.Xiao α decay of the new neutron-deficient isotope 205Ac RADIOACTIVITY 205,206Ac(α)[from 169Tm(40Ca, 4n), (40Ca, 3n), E=196 MeV, and subsequent α decays]; measured Eα, Iα, (evaporation residues)αα-correlations, half-lives, production σ using gas-filled separator SHANS at HIRFL-Lanzhou facility; discussed J, π of parent states. 198At, 202Fr(α); measured Eα, half-lives. Comparison with previous measurements. 200Po, 201,202,202m,203At, 202,203,204,205,206Fr, 203,204,205Rn, 205Ra, 205mRa(α); observed Eα, (evaporation residues)α-correlations. 205,206,207,208,209,210,211,212,213,214,215Ac; systematics of Q(α) and half-lives.
doi: 10.1103/PhysRevC.89.014308
2013TI03 Phys.Rev. C 87, 057305 (2013) Systematics of nuclear ground-state properties of Sr isotopes by covariant density functional theory NUCLEAR STRUCTURE 82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104Sr; calculated rms charge radii, S(2n), three-point neutron pairing energies of ground states. Density functional theory with parameter set DD-PC1. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.057305
2010MA35 Nucl.Phys. A834, 50c (2010) Density functional theory with a separable pairing force in finite nuclei NUCLEAR STRUCTURE 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sn; calculated E2, B(E2), pairing gap using separable and Gogny D1S forces. 128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Sm; calculated deformation using RMF+BCS, HFB, RHB (relativistic Hartree-Bogoliubov). Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.015
2010NI06 Phys.Rev. C 81, 054318 (2010) T.Niksic, P.Ring, D.Vretenar, Y.Tian, Z.-y.Ma 3D relativistic Hartree-Bogoliubov model with a separable pairing interaction: Triaxial ground-state shapes NUCLEAR STRUCTURE 134,136,138,140,142,144,146,148,150,152,154,156Sm, 190,192,194,196,198,200Pt; calculated triaxial quadrupole binding-energy contour maps, neutron and proton pairing energy maps in β-γ plane, quadrupole deformations. 192Pt; calculated proton and neutron canonical single-particle energy levels. Relativistic Hartree-Bogoliubov (RHB) model.
doi: 10.1103/PhysRevC.81.054318
2010YA20 Phys.Rev. C 82, 054305 (2010) D.Yang, L.-G.Cao, Y.Tian, Z.-Y.Ma Importance of self-consistency in relativistic continuum random-phase approximation calculations NUCLEAR STRUCTURE 40Ca, 132Sn, 208Pb; calculated inverse energy-weighted moments and strength distributions of isoscalar giant-monopole resonances (ISGMR), isovector giant-monopole resonances (IVGMR), isoscalar giant-quadrupole resonances (ISGQR), isovector giant-quadrupole resonances (IVGQR) using relativistic continuum random phase approximation (RCRPA) method.
doi: 10.1103/PhysRevC.82.054305
2010ZO02 Chin.Phys.C 34, 56 (2010) W.-H.Zou, Y.Tian, S.-F.Shen, J.-Z.Gu, B.-B.Peng, D.-D.Zhang, Z.-Y.Ma Nuclear structure around 80Zr NUCLEAR STRUCTURE 80,82,84Zr; calculated potential energy surfaces, ground state bands. Projected shell model (PSM) and relativistic Hartee-Bogoliubov (RHB) theory.
doi: 10.1088/1674-1137/34/1/010
2010ZO03 Phys.Rev. C 82, 024309 (2010) W.-h.Zou, Y.Tian, J.-z.Gu, S.-f.Shen, J.-m.Yao, B.-b.Peng, Z.-y.Ma Microscopic description of nuclear structure around 80Zr NUCLEAR STRUCTURE 80,82,84Zr; calculated ground-state total binding energies and angular momentum projected potential energy surfaces (AMPPES) using projected shell model with a quadrupole constrained relativistic Hartree-Bogoliubov (RHB) theory and NL3 effective interaction and Gogny D1S interaction for the pairing force. Shape coexistence and shape transitions, and decay out of superdeformed rotational bands.
doi: 10.1103/PhysRevC.82.024309
2009HU20 Chin.Phys.C 33, Supplement 1, 193 (2009) W.-X.Huang, J.-Y.Wang, Y.Wang, Y.-L.Tian, Z.-C.Zhu, H.-S.Xu, G.-Q.Xiao Simulation of the Lanzhou Penning Trap LPT
doi: 10.1088/1674-1137/33/S1/062
2009LI51 Phys.Rev. C 80, 054315 (2009) Z.H.Li, J.L.Lou, Y.L.Ye, H.Hua, D.X.Jiang, X.Q.Li, S.Q.Zhang, T.Zheng, Y.C.Ge, Z.Kong, L.H.Lv, C.Li, F.Lu, F.Y.Fan, Z.Y.Li, Z.X.Cao, L.Y.Ma, Q.Faisal, H.S.Xu, Z.G.Hu, M.Wang, X.G.Lei, L.M.Duan, Z.G.Xiao, W.L.Zhan, G.Q.Xiao, T.H.Huang, F.Fu, X.H.Zhang, C.Zheng, Y.H.Yu, X.L.Tu, Y.P.Zhang, Y.Y.Yang, H.B.Zhang, B.Thang, Y.L.Tian, Z.Ouang, M.R.Huang, Z.G.Xu, K.Yue, Q.Gao Experimental study of the β-delayed neutron decay of 21N RADIOACTIVITY 21N(β-), (β-n) [from 9Be(26Mg, X), E=68.8 MeV]; measured Eγ, Iγ, Eβ, Iβ, En, In, βn-, βγ-, βγn-coin, half-lives and. delayed-neutron emission probabilities. 20,21O; deduced levels, J, π, branching ratios, logft values and B(GT). Comparison with shell model calculations. 20,21F, 20,21O(β-); measured Eγ. NUCLEAR REACTIONS 9Be(26Mg, X), E=68.8 MeV; measured isotopic yields. 6He, 7,8,9Li, 9,10,11,12Be, 12,13,14,15,17B, 15,16,17,18,19C, 19,20,21N, 22,23O; measured yields.
doi: 10.1103/PhysRevC.80.054315
2009LO07 Chin.Phys.C 33, Supplement 1, 202 (2009) J.-L.Lou, H.-Z.Li, Y.-L.Ye, D.-X.Jiang, H.Hua, X.-Q.Li, S.-Q.Zhang, T.Zheng, Y.-C.Ge, Z.Kong, L.-H.Lu, C.Li, F.Lu, F.-Y.Fan, Z.-Y.Li, Z.-X.Cao, Y.-L.Ma, J.Q.Faisal, H.-S.Xu, Z.-G.Hu, M.Wang, X.-G.Lei, L.-M.Duan, Z.-H.Xiao, W.-L.Zhan, G.-Q.Xiao, T.-H.Huang, F.Fu, X.H.Zhang, C.Zheng, Y.-H.Yu, X.-L.Tu, Y.-P.Zhang, Y.-Y.Yang, B.-H.Zhang, B.Tang, Y.-L.Tian, Z.Ouyang, M.-R.Huang, Z.-G.Xu, K.Yue, Q.Gao Characteristics of a 4-fold segmented clover detectore
doi: 10.1088/1674-1137/33/S1/065
2009TI03 Phys.Lett. B 676, 44 (2009) A finite range pairing force for density functional theory in superfluid nuclei NUCLEAR STRUCTURE Sn, Pb; calculated pairing energy and associated matrix elements using the relativistic Hartree?Bogoliubov approach.
doi: 10.1016/j.physletb.2009.04.067
2009TI04 Phys.Rev. C 79, 064301 (2009) Separable pairing force for relativistic quasiparticle random-phase approximation NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sn, 122Zr, 124Mo, 126Ru, 128Pd, 130Cd, 132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb; calculated energies of first 2+, first and second 3-, B(E2), proton average gap, and isoscalar giant monopole resonance (ISGMR) using Relativistic Hartree-Bogoliubov (RHB) and relativistic quasiparticle random phase approximation (RQRPA). Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064301
2009TI07 Phys.Rev. C 80, 024313 (2009) Axially deformed relativistic Hartree Bogoliubov theory with a separable pairing force NUCLEAR STRUCTURE 164Er, 128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Sm, 240Pu; calculated binding energies, neutron and proton pairing energies using axially symmetric relativistic Hartree-Bogoliubov calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024313
2008LO06 Chin.Phys.Lett. 25, 1992 (2008) J.-L.Lou, Z.-H.Li, Y.-L.Ye, D.-X.Jiang, H.Hua, X.-Q.Li, S.-Q.Zhang, T.Zheng, Y.-C.Ge, Z.Kong, L.-H.Lv, C.Li, F.Lu, F.-Y.Fan, Z.-Y.Li, Z.-X.Cao, L.-Y.Ma, Faisal, H.-S.Xu, Z.-G.Hu, M.Wang, X.-G.Lei, L.-M.Duan, Z.-G.Xiao, W.-L.Zhan, G.-Q.Xiao, T.-H.Huang, F.Fu, X.-H.Zhang, C.Zheng, Y.-H.Yu, X.-L.Tu, Y.-P.Zhang, Y.-Y.Yang, H.-B.Zhang, B.Tang, Y.-L.Tian, Y.-Z.Ou, M.-R.Huang, Z.-G.Xu, K.Yue, Q.Gao The β Decay of 21N RADIOACTIVITY 21N(β-) [from 9Be(26Mg, X), E=68.8 MeV/nucleon]; measured T1/2, Eβ, Iβ, Eγ, Iγ, En, In, βγ-, (n)β-coin.
doi: 10.1088/0256-307X/25/6/019
2008ZO03 Phys.Rev. C 78, 064613 (2008) Microscopic optical potential for α-nucleus elastic scattering in a Dirac-Brueckner-Hartree-Fock approach NUCLEAR REACTIONS 12C(α, α), E=104, 120, 145, 166, 172.5 MeV; 16O(α, α), E=48.7, 54.1, 69.5, 80.7, 104 MeV; 28Si(α, α), E=104, 166, 240 MeV; 40Ca(α, α), E=40.05, 47, 53.9, 80, 104, 141.7 MeV; calculated density dependence of optical model potentials, normalization factors, σ(θ). DBHF calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.064613
2007MA02 Chin.Phys.Lett. 24, 69 (2007) Influence of D-state in 4He on S Factor for the 2H(d, γ)4He Reaction NUCLEAR REACTIONS 2H(d, γ), E(cm)=10-1000 keV; calculated astrophysical S-factors; deduced sensitivity to 4He D-state.
doi: 10.1088/0256-307X/24/1/019
2006TI10 Chin.Phys.Lett. 23, 3226 (2006) A Separable Pairing Force in Nuclear Matter
doi: 10.1088/0256-307X/23/12/029
1991CA26 Chin.J.Nucl.Phys. 13, No 1, 45 (1991) C.Cai, D.Liu, Q.Shen, Y.Tian, Y.Zhuo Comparison between Phenomenological and Microscopic Optical Potential in Nuclear Data Evaluations NUCLEAR REACTIONS 27Al, 31P, S, Cl, K, Ca, Fe, 59Co, Cu, Ag, In, Sb, W, Pb(n, n), E ≈ 0.083-24 MeV; calculated σ. Comparison with data. Different models chi square fits, phenomenological optimal, global and microscopic optical potentials.
1988TI04 Chin.J.Nucl.Phys. 10, 183 (1988) Tian Ye, Han Yinlu, Shen Qingbiao, Cai Chonghai Calculation and Analysis of Fast Neutron Cross Sections on Mo with Microscopic Optical Potential NUCLEAR REACTIONS 98Mo(n, p), (n, γ), (n, α), (n, np), 100Mo(n, 2n), E=threshold-20 MeV; calculated σ(E). 98Mo(n, n), E=0.5-26 MeV; calculated σ(θ). Hauser-Feshbach, preequilibrium exciton (with evaporation) models, microscopic optical potential.
1986SH37 Chin.J.Nucl.Phys. 8, 376 (1986) Empirical Formula of Nuclear Density fitting Experimental Data of Charge Radii and Charge Distributions NUCLEAR STRUCTURE A ≤ 208; calculated charge radii, distributions; deduced model parameters. Fermi type empirical formula.
1986TI05 Chin.J.Nucl.Phys. 8, 28 (1986) Tian Ye, Wang Chang, Han Yinlu, Shen Qingbiao, Zhuo Yizhong An Application of the Microscopic Optical Potential (S-MOP) to Non Even-Even Nuclei in Calculations of Cross Sections NUCLEAR REACTIONS 6,7Li, 9Be, 10,11B, 14N, 23Na, 27Al, 51V, 53Cr, 55Mn, 59Co, 63,65Cu, 93Nb, 181Ta, 197Au, 235U, 239Pu(n, n), E ≈ 1-200 MeV; calculated total σ, σ(θ). Microscopic optical potential.
1986YE02 Chin.J.Nucl.Phys. 8, 214 (1986) Ye Weilei, Yuan Haiji, Gao Qin, Zheng Chunkai, Tian Ye, Shen Qingbiao Calculations of Neutron Skin for Spherical Nuclei using the Hartree-Fock Method with Skyrme Forces NUCLEAR STRUCTURE 16O, 28Si, 32S, 40,48Ca, 60Ni, 90Zr, 120Sn; calculated proton, neutron density distributions, rms radii. Hartree-Fock method, Skyrme force.
1985TA26 Chin.J.Nucl.Phys. 7, 263 (1985) Tang Xuetian, Gao Liangjun, Tian Ye Generalization of the Goldhaber Theory NUCLEAR STRUCTURE 11C, 19O; calculated momentum distribution widths. Generalized Goldhaber theory.
1985TI06 Chin.J.Nucl.Phys. 7, 207 (1985) Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin Lifei A Global Analysis of Proton Differential Elastic Cross Section Calculations with the Microscopic Optical Potential S-MOP NUCLEAR REACTIONS 184W, 120Sn, 90Zr, 58,60,62,64Ni(p, p), E=16 MeV; 120Sn, 60Ni, 56Fe(p, p), E=30.3 MeV; 90Zr, 58Ni, 40Ca(p, p), E=40 MeV; 68Zn, 58Ni, 40Ca, 12C(p, p), E=61.4 MeV; 208Pb(p, p), E=16-61.4 MeV; analyzed σ(θ). Microscopic optical potential, extended Skyrme force.
1985TI07 Chin.J.Nucl.Phys. 7, 154 (1985) Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin, Li Fei A Global Analysis of Integral Cross Section Calculations with the Microscopic Optical Potential NUCLEAR REACTIONS 12C(n, n), E ≤ 100 MeV; 44,40Ca(n, n), E ≤ 15 MeV; 60Ni(n, n), E ≤ 30 MeV; 242Pu, 98Mo(n, n), E ≤ 100 MeV; 140Ce(n, n), E ≤ 60 MeV; 238U, 232Th(n, n), E ≤ 15 MeV; calculated elastic, nonelastic, total σ(E). Effective Skyrme force, microscopic optical potential.
1985TI08 Chin.J.Nucl.Phys. 7, 344 (1985) Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin, Li Fei A Global Analysis of Neutron Differential Elastic Cross Section Calculations with the Microscopic Optical Potential NUCLEAR REACTIONS 4He, 12C, 16O, 24Mg, 28Si, 32S, 40Ca, 50,52,54Cr, 54,56Fe, 58,60,62,64Ni, 64,66,68Zn, 90,92,94Zr, 92,94,96,98,100Mo, 118,120,122,124Sn, 182,184,186W, 208Pb, 232Th, 238U, 240Pu(n, n), E=1-26 MeV; calculated σ(θ). Microscopic optical potential.
1984SH38 Chin.J.Nucl.Phys. 6, 245 (1984) Shen Qingbiao, Tian Ye, Wang Shunuan, Gao Liangjun, Zhuo Yizhong, Zhao Fujian Exciton Transition Rate Calculations Based on the Optical Model Potentials NUCLEAR STRUCTURE 40Ca, 120Sn, 238U; calculated exciton transition rates. Optical potential, Skyrme interaction.
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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