NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = T.Li Found 94 matches. 2024LI17 Phys.Rev. C 109, 034310 (2024) C.B.Li, Y.Zheng, T.X.Li, X.G.Wu, H.Y.Wu, M.Zheng, Z.H.Zhao, Y.Q.Li, R.Hong, Z.Y.He, J.Z.Li, J.L.Wang, C.Y.Guo, Z.X.Zhou, L.Ni, G.S.Li, X.H.Zhou, B.Guo, S.Y.Wang, M.L.Liu, Y.H.Zhang, C.Y.He, F.L.Liu, S.Wang, L.H.Zhu Lifetime measurements of the first 2+ states in 116, 118Te
doi: 10.1103/PhysRevC.109.034310
2024YA08 Phys.Rev.Lett. 132, 152502 (2024) X.Yan, Zh.Cheng, A.Abdukerim, Z.Bo, W.Chen, X.Chen, Ch.Cheng, X.Cui, Y.Fan, D.Fang, Ch.Fu, M.Fu, L.Geng, K.Giboni, L.Gu, X.Guo, Ch.Han, K.Han, Ch.He, J.He, D.Huang, Y.Huang, J.Huang, Zh.Huang, R.Hou, Y.Hou, X.Ji, Y.Ju, Ch.Li, J.Li, M.Li, Sh.Li, T.Li, Q.Lin, J.Liu, X.Lu, C.Lu, L.Luo, Y.Luo, W.Ma, Y.Ma, Y.Mao, Y.Meng, X.Ning, B.Pang, N.Qi, Zh.Qian, X.Ren, N.Shaheed, X.Shang, X.Shao, G.Shen, L.Si, W.Sun, A.Tan, Y.Tao, A.Wang, M.Wang, Q.Wang, Sh.Wang, S.Wang, W.Wang, X.Wang, Zh.Wang, Y.Wei, M.Wu, W.Wu, J.Xia, M.Xiao, X.Xiao, P.Xie, B.Yan, J.Yang, Y.Yang, Y.Yao, Ch.Yu, Y.Yuan, Zh.Yuan, X.Zeng, D.Zhang, M.Zhang, P.Zhang, Sh.Zhang, Sh.Zhang, T.Zhang, W.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, L.Zhao, Q.Zheng, J.Zhou, N.Zhou, X.Zhou, Y.Zhou, Y.Zhou, for the PandaX Collaboration Searching for Two-Neutrino and Neutrinoless Double Beta Decay of 134Xe with the PandaX-4T Experiment RADIOACTIVITY 134Xe(2β-); measured decay products, Eβ, Iβ; deduced two-neutrino and neutrinoless T1/2 limits. Comparison with available data. The cylindrical active volume PandaX-4T dual-phase TPC.
doi: 10.1103/PhysRevLett.132.152502
2023LI05 Phys.Rev. C 107, 014307 (2023) J.Lin, Y.K.Wang, C.Xu, Z.H.Li, H.Hua, S.Q.Zhang, D.W.Luo, H.Y.Wu, J.Meng, X.G.Wu, Y.Zheng, C.B.Li, T.X.Li, Z.Y.Huang, H.Cheng, C.Y.Guo, Z.X.Zhou, Z.Q.Chen, C.G.Wang Possible coexistence of magnetic and antimagnetic rotations in 61Ni NUCLEAR REACTIONS 54Cr(11B, 4n)61Ni, E=54 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 61Ni; deduced levels, J, π, asymmetric angular distributions from oriented states (ADO), dipole and quadrupole bands structures, configurations, high-spin states. Study provides evidence for possible coexistence of magnetic and antimagnetic rotations in the region around A=60. Comparison with calculations using the microscopic tilted axis cranking covariant density functional theory (TAC-CDFT). Detector array consisted of 6 HPGe with BGO anti-Compton suppressors, 1 clover HPGe detector 2 planar HPGe detectors at HI-13 Tandem Accelerator of the China Institute of Atomic Energy (CIAE).
doi: 10.1103/PhysRevC.107.014307
2023LI49 Phys.Rev. C 108, L041602 (2023) Theory of Coulomb excitation of the 229Th nucleus by protons
doi: 10.1103/PhysRevC.108.L041602
2023RO06 Appl.Radiat.Isot. 199, 110863 (2023) A.Rohilla, J.G.Wang, G.S.Li, S.K.Ghorui, X.H.Zhou, M.L.Liu, Y.H.Qiang, S.Guo, Y.D.Fang, B.Ding, W.Q.Zhang, S.Huang, Y.Zheng, T.X.Li, W.Hua, H.Cheng Occupancy of orbitals and the quadrupole collectivity in 45Sc nucleus NUCLEAR REACTIONS 12C(36Ar, 3p)45Sc, E=145 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, partial level scheme, negative parity yrast band, B(E2), lifetimes. Comparison with large-scale shell model calculations, involving different interactions like: GX1A, GX1J, FPD6, KB3 and ZBM2. KB3 and FPD6 interactions. Doppler Shift Attenuation method (DSAM). The Heavy Ion Research Facility in Lanzhou (HIRFL), China.
doi: 10.1016/j.apradiso.2023.110863
2023XI14 J.Phys.(London) G50, 125103 (2023) Sh.Xia, S.Huang, K.Xu, T.Li, X.Chen, K.Han, Sh.Wang Optimization of convolutional neural networks for background suppression in the PandaX-III experiment RADIOACTIVITY 136Xe(2β-); analyzed available data with optimized the convolutional neural network based on the Monte Carlo simulation data to improve the signal-background discrimination power; deduced EfficientNet as the baseline model and the optimization is performed by tuning the hyperparameters. The PandaX-III experiment.
doi: 10.1088/1361-6471/acfe24
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
2022WU02 Nucl.Phys. A1017, 122357 (2022) D.Wu, B.Guo, C.Y.He, W.P.Lin, Z.An, T.L.Ma, F.L.Liu, W.S.Yang, J.H.Wei, Y.C.Li, Y.P.Shen, Q.W.Fan, X.G.Wu, Y.Zheng, T.X.Li, F.Bai, P.Wang, M.L.Qiu, N.Y.Wang Determination of the 74Ge(p, γ)75As reaction rates in p-process nucleosynthesis with in-beam γ spectroscopy NUCLEAR REACTIONS 74Ge(p, γ), E=2.5-4.3 MeV; measured reaction products, Eγ, Iγ; deduced σ, reaction rates. Comparison with TALYS and EMPIRE nuclear reaction codes calculations. The 3 MV tandem accelerator of the Institute of Nuclear Science and Technology, Sichuan University.
doi: 10.1016/j.nuclphysa.2021.122357
2022ZH23 J.Phys.(London) G49, 055103 (2022) Y.Zheng, C.B.Li, X.G.Wu, H.L.Ma, L.H.Zhu, T.X.Li, Z.Y.Huang, H.Chen, C.Y.He, Q.W.Fan, G.S.Li, Q.M.Chen, J.Zhong, S.P.Hu, H.W.Li, J.L.Wang, J.J.Liu, Y.H.Wu, P.W.Luo Fast-timing lifetime measurements of the 33/2+ and 25/2- states in 189Hg: oblate excitations NUCLEAR REACTIONS 175Lu(19F, 5n), E=100 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies, partial level scheme, J, π, level T1/2, B(E2), B(E1). Comparison with systematics, Nilsson-Strutinsky Bogoliubov (CNSB) model calculations. The fast-timing techniques with the HPGe and LaBr3:Ce array at the HI-13 tandem accelerator at the China Institute of Atomic Energy.
doi: 10.1088/1361-6471/ac58b0
2021CH14 Phys.Rev. C 103, 034303 (2021) M.Chen, T.Li, J.Dobaczewski, W.Nazarewicz Microscopic origin of reflection-asymmetric nuclear shapes NUCLEAR STRUCTURE 146Ba, 224Ra; calculated deformation energies, multipole components of the total deformation energy, isospin and neutron-proton components of the octupole energy as functions of β3 parameter. 138,140,142,144,146,148,150,152Ba, 166,168,170,172,174,176,178,180Yb, 214,216,218,220,222,224,226,228,230,232Ra, 216,218,220,222,224,226,228,230,232,234U; calculated equilibrium quadrupole deformations β20, deformation energies. 176Yb, 224Ra; calculated single-particle (canonical) neutron and proton SLy4-HFB levels as functions of β2. Axial reflection-asymmetric Hartree-Fock-Bogoliubov theory using SLy4 and UNEDF2 Skyrme energy-density functionals and density-dependent pairing force for the multipole expansion of interaction energies in isospin and neutron-proton schemes to investigate their role in the appearance of reflection-asymmetric deformations.
doi: 10.1103/PhysRevC.103.034303
2021CH36 Astrophys.J. 915, 78 (2021) H.Cheng, B.-H.Sun, L.-H.Zhu, M.Kusakabe, Y.Zheng, L.C.He, T.Kajino, Z.-M.Niu, T.-X.Li, C.-B.Li, D.-X.Wang, M.Wang, G.-S.Li, K.Wang, L.Song, G.Guo, Z.-Y.Huang, X.-L.Wei, F.-W.Zhao, X.-G.Wu, Y.Abulikemu, J.-C.Liu, P.Fan Measurements of 160Dy(p, γ) at Energies Relevant for the Astrophysical γ Process NUCLEAR REACTIONS 160Dy(p, γ), 161Dy(p, n), E=3.4-7 MeV; measured reaction products, Eγ, Iγ; deduced σ, S-factor, astrophysical reaction rates. Comparison with TALYS, NON-SMOKER calculations.
doi: 10.3847/1538-4357/ac00b1
2021HA29 Phys.Rev. C 104, 014327 (2021) X.C.Han, S.Y.Wang, B.Qi, C.Liu, S.Wang, D.P.Sun, Z.Q.Li, H.Jia, R.J.Guo, X.Xiao, L.Mu, X.Lu, Q.Wang, W.Z.Xu, H.W.Li, X.G.Wu, Y.Zheng, C.B.Li, T.X.Li, Z.Y.Huang, H.Y.Wu, D.W.Luo First observation of candidate chiral doublet bands in Z=37 Rb isotopes NUCLEAR REACTIONS 76Ge(11B, 3n)84Rb, E=36 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO ratios) using an array of six Compton-suppressed HPGe detectors and one clover detector at the HI-13 tandem accelerator of CIAE-Beijing. 84Rb; deduced high-spin levels, J, π, B(M1)/B(E2) ratios, chiral doublet bands, configurations, staggering parameters. Comparison with triaxial relativistic mean-field theory and triaxial particle-rotor model calculations. Systematics of positive-parity yrast states in 76,78,80,82,84Rb.
doi: 10.1103/PhysRevC.104.014327
2021JI07 Chin.Phys.C 45, 063101 (2021) Interpretation of the Galactic gamma-ray excess with the dark matter indicated by 8Be and 4He anomalous transitions
doi: 10.1088/1674-1137/abeda6
2021LI25 At.Data Nucl.Data Tables 140, 101440 (2021) Compilation of recent nuclear ground state charge radius measurements and tests for models COMPILATION Z=4-88; compiled root-mean-square (rms) charge radii measured by laser spectroscopy; deduced magic numbers, linear relationship between the difference of the mirror nuclear charge radii and the isospin asymmetry, accuracies and predictive powers of the WS* and HFB25 models.
doi: 10.1016/j.adt.2021.101440
2021LI36 Nucl.Phys. A1014, 122225 (2021) T.X.Li, C.B.Li, Y.Zheng, X.G.Wu, J.Zhong, B.J.Zhu, Q.W.Fan, Y.X.Gao, Y.J.Jin, G.S.Li, L.H.Zhu Lifetime measurements and the structure of some negative-parity states in 134Ce NUCLEAR REACTIONS 122Sn(16O, 4n), E=76 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, B(Eλ), lifetimes of negative-parity states. Comparison with cranked Nilsson-Strutinsky Bogoliubov (CNSB) model. Recoil-distance Doppler-shift technique.
doi: 10.1016/j.nuclphysa.2021.122225
2021LI39 J.Phys.(London) G48, 095105 (2021) Nonlinear optical effects in a nucleus NUCLEAR STRUCTURE 57Fe, 2H; calculated two-photon and three-photon σ(θ), integrated absorption rates.
doi: 10.1088/1361-6471/ac1712
2021RO03 Nucl.Phys. A1006, 122116 (2021) A.Rohilla, G.S.Li, Y.H.Qiang, M.L.Liu, X.H.Zhou, J.G.Wang, S.Guo, B.Ding, W.Q.Zhang, S.Huang, Y.Zheng, Y.D.Fang, S.K.Ghorui, T.X.Li, W.Hua, H.Cheng Quadrupole coherence enhancement in 46Ti: Mixing of f7/2 and p3/2 orbital NUCLEAR REACTIONS 12C(36Ar, 2p), E=145 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies, J, π, level lifetimes, B(E2). Doppler Shift Attenuation Method (DSAM). Heavy Ion Research Facility in Lanzhou (HIRFL), China.
doi: 10.1016/j.nuclphysa.2020.122116
2021ZH66 Nucl. Sci. Tech. 32, 107 (2021) J.Zhong, X.-G.Wu, S.-P.Hu, Y.-J.Ma, Y.Zheng, C.-B.Li, G.-S.Li, B.-J.Zhu, T.-X.Li, Y.-J.Jin, Y.-X.Gao, Q.-W.Fan, K.-Y.Ma, D.Yang, H.-B.Sun, H.-G.Zhao, L.Gan, Q.Luo, Z.X.Wu Lifetime measurements in 138Nd NUCLEAR REACTIONS 123Sb(19F, 4n), E=87 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, J, π, partial level scheme, level T1/2, B(E2). Comparison with Grodzins systematics and available data. The recoil distance Doppler shift technique in combination with the differential decay curve method. The HI-13 tandem accelerator of the China Institute of Atomic Energy (CIAE) in Beijing.
doi: 10.1007/s41365-021-00953-4
2020LI40 Phys.Rev. C 102, 044305 (2020) T.Li, M.Z.Chen, C.L.Zhang, W.Nazarewicz, M.Kortelainen Nucleon localization function in rotating nuclei NUCLEAR STRUCTURE 152Dy; calculated single-particle neutron and proton Routhians as functions of angular frequency using Skyrme interaction SkM* and the cranked Hartree-Fock (CHF), and cranked harmonic oscillator (CHO) methods for the SD band, current, spin, spin-kinetic and spin-current tensor densities for the SD band using CHF method; used the concept of nucleon localization function (NLF) to interpret the results from CHF method for fast rotation in nuclei. Discussed oscillating pattern of the NLF in terms of interference between kinetic-energy and particle densities, and nodal pattern of the NLF in terms of direction of major axis of a rotating nucleus, and aligned angular momentum.
doi: 10.1103/PhysRevC.102.044305
2020NE08 Phys.Rev. C 102, 034326 (2020) E.M.Ney, J.Engel, T.Li, N.Schunck Global description of β- decay with the axially deformed Skyrme finite-amplitude method: Extension to odd-mass and odd-odd nuclei RADIOACTIVITY Z=20, A=50-61(β-); Z=21, A=50-66(β-); Z=22, A=52-73(β-); Z=23, A=53-74(β-); Z=24, A=56-79(β-); Z=25, A=57-80(β-); Z=26, A=60-83(β-); Z=27, A=62-88(β-); Z=28, A=68-93(β-); Z=29, A=68-96(β-); Z=30, A=74-99(β-); Z=31, A=74-102(β-); Z=32, A=80-103(β-); Z=33, A=80-110(β-); Z=34, A=84-113(β-); Z=35, A=84-116(β-); Z=36, A=88-117(β-); Z=37, A=88-120(β-); Z=38, A=90-121(β-); Z=39, A=90-124(β-); Z=40, A=97-125(β-); Z=41, A=96-128(β-); Z=42, A=102-135(β-); Z=43, A=102-138(β-); Z=44, A=106-143(β-); Z=45, A=106-146(β-); Z=46, A=112-147(β-); Z=47, A=112-150(β-); Z=48, A=118-157(β-); Z=49, A=124-160(β-); Z=50, A=128-163(β-); Z=51, A=128-168(β-); Z=52, A=134-171(β-); Z=53, A=134-176(β-); Z=54, A=138-179(β-); Z=55, A=138-182(β-); Z=56, A=140-183(β-); Z=57, A=141-184(β-); Z=58, A=144-185(β-); Z=59, A=146-186(β-); Z=60, A=152-187(β-); Z=61, A=152-188(β-); Z=62, A=156-189(β-); Z=63, A=156-192(β-); Z=64, A=162-207(β-); Z=65, A=162-210(β-); Z=66, A=166-213(β-); Z=67, A=167-218(β-); Z=68, A=172-221(β-); Z=69, A=172-224(β-); Z=70, A=180-227(β-); Z=71, A=180-228(β-); Z=72, A=184-233(β-); Z=73, A=185-238(β-); Z=74, A=190-241(β-); Z=75, A=191-248(β-); Z=76, A=194-255(β-); Z=77, A=195-256(β-); Z=78, A=202-261(β-); Z=79, A=202-262(β-); Z=80, A=206-265(β-); Z=81, A=210-266(β-); Z=82, A=212-267(β-); Z=83, A=214-268(β-); Z=84, A=220-269(β-); Z=85, A=220-270(β-); Z=86, A=224-271(β-); Z=87, A=225-272(β-); Z=88, A=230-273(β-); Z=89, A=231-274(β-); Z=90, A=236-275(β-); Z=91, A=237-278(β-); Z=92, A=242-281(β-); Z=93, A=242-302(β-); Z=94, A=246-305(β-); Z=95, A=247-308(β-); Z=96, A=252-309(β-); Z=97, A=254-314(β-); Z=98, A=260-315(β-); Z=99, A=260-318(β-); Z=100, A=268-323(β-); Z=101, A=268-326(β-); Z=102, A=274-329(β-); Z=103, A=274-332(β-); Z=104, A=282-335(β-); Z=105, A=282-336(β-); Z=106, A=286-339(β-); Z=107, A=290-340(β-); Z=108, A=292-345(β-); Z=109, A=294-348(β-); Z=110, A=300-369(β-); calculated asymptotic quantum numbers of the blocked proton or neutron quasiparticle, HFB binding energy, β2 deformation parameter, β- decay half-lives of 3983 neutron-rich nuclei, Q(β-), percent first-forbidden rate, QRPA energy and B(GT) Gamow-Teller strength for selected nuclei. Statistical extension of the charge-changing Finite-amplitude method (FAM), with a global Skyrme density functional. Comparison with experimental data, and with other theoretical calculations. Relevance to r process in nucleosynthesis.
doi: 10.1103/PhysRevC.102.034326
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
2019GU11 Int.J.Mod.Phys. E28, 1950015 (2019) Calculation of charge form factor of elastic electron scattering based on Skyrme force and relativistic eikonal approximation NUCLEAR REACTIONS 12C, 16O, 24Mg, 27Al, 28Si, 32S, 40Ca, 208Pb(E, E), E=250, 500, 740 MeV; calculated charge form factors using relativistic eikonal approximation and the Skyrme–Hartree–Fock equation.
doi: 10.1142/S0218301319500150
2019QI03 Phys.Rev. C 99, 044610 (2019) J.Qi, T.Li, R.Xu, L.Fu, X.Wang α decay in intense laser fields: Calculations using realistic nuclear potentials RADIOACTIVITY 148Sm, 216Rn, 228Th(α); calculated potentials between the α particle and the daughter nuclei 144Nd, 212Po and 224Ra, time-dependent α penetrability of daughter nuclei in intense laser fields, angle-resolved and angle-integrated modifications to the α decay penetrability as a function of laser intensity. Realistic and quantitative nuclear potentials. Relevance to future experiments investigating laser-modified α-decay processes.
doi: 10.1103/PhysRevC.99.044610
2019ZH34 Phys.Rev. C 100, 014325 (2019) Y.Zheng, Y.H.Wu, X.G.Wu, C.B.Li, L.H.Zhu, T.X.Li, P.W.Luo, G.S.Li, C.Y.He, H.W.Li, S.P.Hu, J.J.Liu, J.L.Wang, S.H.Yao, Q.M.Chen, J.Zhong, J.B.Lu, K.Y.Ma, D.Yang Reinvestigation of the high-spin level structure of 92Nb: Excitations across the Z=38 and N=50 closed shells NUCLEAR REACTIONS 82Se(14N, 4n), E=54 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO) using Compton-suppressed HPGe array for γ detection at the HI-13 tandem accelerator of the CIAE-Beijing. 92Nb; deduced high-spin levels, J, π. Comparison with shell model calculations. NUCLEAR STRUCTURE 92Nb; calculated high-spin levels, J, π, partition of the wave functions, and seniority using shell model with NUSHELLX code, GWB model space and GWBXG interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.014325
2018LI14 Phys.Rev. C 97, 034331 (2018) C.B.Li, X.G.Wu, Y.Zheng, Y.J.Jin, H.L.Ma, G.S.Li, J.Zhong, B.J.Zhu, T.X.Li, Y.X.Gao, X.Guan, J.Q.Liu Level structure in the transitional nucleus 199Tl NUCLEAR REACTIONS 196Pt(7Li, 4n), E=40 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using eight Compton-suppressed HPGe detectors and two planar HPGe detectors at HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE). 199Tl; deduced high-spin levels, J, π, bands, multipolarities, configurations, alignments, oblate shapes, potential energy surfaces for 17/2- state. Comparison with cranked Nilsson-Strutinsky-Bogoliubov (CNSB) model calculations. Systematics of 13/2+ states in N=104-122 Tl and Bi nuclei. Systematics of negative-parity yrast states and positive-parity 3-qp yrast states in 195,197,199Tl.
doi: 10.1103/PhysRevC.97.034331
2016HU11 Phys.Rev. C 94, 014303 (2016) B.S.Hu, F.R.Xu, Z.H.Sun, J.P.Vary, T.Li Ab initio nuclear many-body perturbation calculations in the Hartree-Fock basis NUCLEAR STRUCTURE 4He, 16O; calculated binding energies and point-proton rms radii using ab initio many-body perturbation theory (MBPT), with realistic nuclear forces, chiral N3LO and JISP16. Comparison with experimental data.
doi: 10.1103/PhysRevC.94.014303
2014WA44 Chin.Phys.Lett. 31, 123201 (2014) Q.Wang, Y.-G.Lin, Y.Li, B.-K.Lin, F.Meng, E.-J.Zang, T.-C.Li, Z.-J.Fang Observation of Spin Polarized Clock Transition in 87Sr Optical Lattice Clock ATOMIC PHYSICS 87Sr; measured π-polarized clock transition spectrum of resolvable mF states; deduced spin polarized clock transition spectrum.
doi: 10.1088/0256-307X/31/12/123201
2013WA18 Phys.Rev. C 88, 011301 (2013) Shell and isospin effects in nuclear charge radii NUCLEAR STRUCTURE A>15, N=8-154; analyzed rms charge radii for 885 measured charge radii, and proposed a four-parameter phenomenological formula including shell correction and deformations from Weizsacker-Skyrme mass model and isospin dependent term. Comparison with HFB21 model calculations. Z=10-100; Z=20, N=18-32; Z=28, N=30-36; Z=40, N=46-62; Z=82, N=100-132; analyzed rms charge radii and compared with HFB21 and RMF model calculations. 30Si, 30S; analyzed nuclear symmetry energy, rms charge radii differences for mirror nuclei. A=254-310, Z=108, 112, 116, 120; predicted rms charge radii using the proposed formula, and compared with HFB21 model calculations.
doi: 10.1103/PhysRevC.88.011301
2011HU07 Chin.Phys.Lett. 28, 092102 (2011) L.-X.Huang, Y.-J.Qi, T.Li, S.-X.Liu The Plateau of Moment of Inertia and the Energy Gap in 161-168Yb NUCLEAR STRUCTURE 161,162,163,164,165,166,167,168Yb; calculated moments of inertia, Nilsson levels; deduced plateau of moment of inertia.
doi: 10.1088/0256-307X/28/9/092102
2010LI07 Phys.Rev. C 81, 034309 (2010) T.Li, U.Garg, Y.Liu, R.Marks, B.K.Nayak, P.V.Madhusudhana Rao, M.Fujiwara, H.Hashimoto, K.Nakanishi, S.Okumura, M.Yosoi, M.Ichikawa, M.Itoh, R.Matsuo, T.Terazono, M.Uchida, Y.Iwao, T.Kawabata, T.Murakami, H.Sakaguchi, S.Terashima, Y.Yasuda, J.Zenihiro, H.Akimune, K.Kawase, M.N.Harakeh Isoscalar giant resonances in the Sn nuclei and implications for the asymmetry term in the nuclear-matter incompressibility NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(α, α'), E=386 MeV; measured Eα, Iα, excitation energies, σ(θ), σ, angular distributions, differential cross section as function of excitation energy; deduced strengths distributions, widths and EWSR for isoscalar giant monopole resonance (ISGMR), isoscalar giant-dipole resonance (ISGDR), isoscalar giant quadrupole resonance (ISGQR), and high-energy octupole resonance (HEOR). Comparisons with theoretical predictions.
doi: 10.1103/PhysRevC.81.034309
2010PI13 J.Phys.:Conf.Ser. 205, 012036 (2010) N.Pietralla, T.C.Li, M.Fritzsche, M.W.Ahmed, D.Savran, A.P.Tonchev, W.Tornow, H.R.Weller, V.Werner Spin and parity assignments to dipole excitations of the odd-mass nucleus 207Pb from nuclear resonance fluorescence experiments with linearly-polarized γ-ray beams NUCLEAR REACTIONS Pb(polarized γ, γ'), E=5400-5700 keV; measured Eγ, Iγ(θ) using HIγS at DFELL. 206,207,208Pb deduced low-lying dipole-excited levels, J, π, E1 γ decay rate.
doi: 10.1088/1742-6596/205/1/012036
2009HU13 Phys.Rev. C 80, 044317 (2009) M.Hunyadi, H.Hashimoto, T.Li, H.Akimune, H.Fujimura, M.Fujiwara, Z.Gacsi, U.Garg, K.Hara, M.N.Harakeh, J.Hoffman, M.Itoh, T.Murakami, K.Nakanishi, B.K.Nayak, S.Okumura, H.Sakaguchi, S.Terashima, M.Uchida, Y.Yasuda, M.Yosoi Proton decay from the isoscalar giant dipole resonance in 58Ni NUCLEAR REACTIONS 58Ni(α, α'p), E=386 MeV; measured Eα, Iα, αp-coin, σ, σ(θ), and width. 58Ni; deduced isoscalar giant dipole resonance (ISGDR), associated resonance parameters and branching ratios for proton decays to 57Co; analyzed EWSR. 57Co; deduced levels, J, π. Grand Raiden spectrometer at RCNP facility. Proton branching ratios compared with continuum-RPA calculations.
doi: 10.1103/PhysRevC.80.044317
2009LI32 Nucl.Phys. A828, 125 (2009) Comprehensive calculations on the OZI-forbidden nonleptonic decays of orthoquarkonia J/ψ (Υ) ππ, ρπ
doi: 10.1016/j.nuclphysa.2009.06.021
2009LI43 Phys.Rev. C 80, 044329 (2009) Influence of the pairing interaction at ultrahigh spin NUCLEAR STRUCTURE 155Tb; analyzed proton alignments, moments of inertia, and influence of the pairing interaction near ultrahigh spins using the particle number-conserving (PNC) method of the cranked shell model.
doi: 10.1103/PhysRevC.80.044329
2009NA09 Phys.Lett. B 674, 281 (2009) B.K.Nayak, U.Garg, M.Koss, T.Li, E.Martis, H.Fujimura, M.Fujiwara, K.Hara, K.Kawase, K.Nakanishi, E.Obayashi, H.P.Yoshida, M.Itoh, S.Kishi, H.Sakaguchi, H.Takeda, M.Uchida, Y.Yasuda, M.Yosoi, R.G.T.Zegers, H.Akimune, M.N.Harakeh, M.Hunyadi Direct proton decay of the isoscalar giant dipole resonance in 208Pb NUCLEAR REACTIONS 208Pb(α, α'p), E=400 MeV; measured Eα, Iα, decay proton spectra, σ(E, θ); calculated σ(θ) via DWBA; deduced ISGDR proton-decay branching ratio. Comparison with continuum RPA calculations.
doi: 10.1016/j.physletb.2009.03.047
2009PI14 Phys.Lett. B 681, 134 (2009) N.Pietralla, T.C.Li, M.Fritzsche, M.W.Ahmed, T.Ahn, A.Costin, J.Enders, J.Li, S.Muller, P.von Neumann-Cosel, I.V.Pinayev, V.Yu.Ponomarev, D.Savran, A.P.Tonchev, W.Tornow, H.R.Weller, V.Werner, Y.K.Wu, A.Zilges Competition between excited core states and 1hω single-particle excitations at comparable energies in 207Pb from photon scattering NUCLEAR REACTIONS 208Pb(polarized γ, γ'), E=5.5, 5.6 MeV; measured Eγ, Iγ using the azimuthal nuclear resonance fluorescence intensity asymmetry technique. 206,207,208Pb; deduced levels, J, π.
doi: 10.1016/j.physletb.2009.09.059
2008MU18 Phys.Rev. C 78, 034311 (2008) S.Mukhopadhyay, D.Almehed, U.Garg, S.Frauendorf, T.Li, P.V.Madhusudhana Rao, X.Wang, S.S.Ghugre, M.P.Carpenter, S.Gros, A.Hecht, R.V.F.Janssens, F.G.Kondev, T.Lauritsen, D.Seweryniak, S.Zhu Electromagnetic transition rates in high-spin bands in 136Nd NUCLEAR REACTIONS 100Mo(40Ar, 4nγ), E=175 MeV; measured Eγ, Iγ, γγ-coin, half-lives using doppler shift attenuation method. 136Nd; deduced levels, J, π, bands, transition quadrupole moments, B(M1), B(E2), configurations. Comparisons with random phase approximations and tilted-axis cranking models.
doi: 10.1103/PhysRevC.78.034311
2007AH02 Phys.Rev. C 75, 014313 (2007) T.Ahn, N.Pietralla, G.Rainovski, A.Costin, K.Dusling, T.C.Li, A.Linnemann, S.Pontillo γ-ray multipolarimetry between low-spin states of 136Ce: Search for the 2+1, ms one-phonon mixed-symmetry state RADIOACTIVITY 136Pr(EC), (β+) [from 134Ba(6Li, 4n)]; measured Eγ, Iγ, γγ-coin. 136Ce deduced levels, J, π, δ, B(E2)/B(M1), possible mixed-symmetry state.
doi: 10.1103/PhysRevC.75.014313
2007GA44 Nucl.Phys. A788, 36c (2007) U.Garg, T.Li, S.Okumura, H.Akimune, M.Fujiwara, M.N.Harakeh, H.Hashimoto, M.Itoh, Y.Iwao, T.Kawabata, K.Kawase, Y.Liu, R.Marks, T.Murakami, K.Nakanishi, K.Nayak, P.V.Madhusudhana Rao, H.Sakaguchi, Y.Terashima, M.Uchida, Y.Yasuda, M.Yosoi, J.Zenihiro The Giant Monopole Resonance in the Sn Isotopes: Why is Tin so "Fluffy"? NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(α, α'), E=400 MeV; measured Eα, Iα, σ(E, θ). 112,114,116,118,120,122,124Sn deduced GMR energy, strength distributions, moment ratios. Comparison with other data and calculations.
doi: 10.1016/j.nuclphysa.2007.01.046
2007LI61 Phys.Rev.Lett. 99, 162503 (2007) T.Li, U.Garg, Y.Liu, R.Marks, B.K.Nayak, P.V.Madhusudhana Rao, M.Fujiwara, H.Hashimoto, K.Kawase, K.Nakanishi, S.Okumura, M.Yosoi, M.Itoh, M.Ichikawa, R.Matsuo, T.Terazono, M.Uchida, T.Kawabata, H.Akimune, Y.Iwao, T.Murakami, H.Sakaguchi, S.Terashima, Y.Yasuda, J.Zenihiro, M.N.Harakeh Isotopic Dependence of the Giant Monopole Resonance in the Even-A 112-124Sn Isotopes and the Asymmetry Term in Nuclear Incompressibility NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(α, α'), E=400 MeV; measured Eα, Iα. Deduced GMR strength distributions.
doi: 10.1103/PhysRevLett.99.162503
2007MU14 Phys.Rev.Lett. 99, 172501 (2007) S.Mukhopadhyay, D.Almehed, U.Garg, S.Frauendorf, T.Li, P.V.Madhusudhana Rao, X.Wang, S.S.Ghugre, M.P.Carpenter, S.Gros, A.Hecht, R.V.F.Janssens, F.G.Kondev, T.Lauritsen, D.Seweryniak, S.Zhu From Chiral Vibration to Static Chirality in 135Nd NUCLEAR REACTIONS 100Mo(40Ar, 5n), E=175 MeV; measured Eγ, Iγ, lifetimes. 135Nd deduced B(M1), B(E2).
doi: 10.1103/PhysRevLett.99.172501
2007PA22 Phys.Lett. B 647, 243 (2007) N.S.Pattabiraman, Y.Gu, S.Frauendorf, U.Garg, T.Li, B.K.Nayak, X.Wang, S.Zhu, S.S.Ghugre, R.V.F.Janssens, R.S.Chakrawarthy, M.Whitehead, A.O.Macchiavelli Evidence for particle-hole excitations in the triaxial strongly-deformed well of 163Tm NUCLEAR REACTIONS 130Te(37Cl, 4n), E=170 MeV; measured Eγ, Iγ, γγ-coin. 163Tm deduced high-spin levels, J, π, triaxial superdeformed bands, B(M1)/B(E2). Gammasphere array, potential energy surface calculations.
doi: 10.1016/j.physletb.2007.01.057
2007TI07 Phys.Rev. C 76, 024307 (2007) J.Timar, T.Koike, N.Pietralla, G.Rainovski, D.Sohler, T.Ahn, G.Berek, A.Costin, K.Dusling, T.C.Li, E.S.Paul, K.Starosta, C.Vaman High-spin structure of 105Ag: Search for chiral doublet bands NUCLEAR REACTIONS 100Mo(10B, 5n), E=58, 64 MeV; measured Eγ, Iγ, γγ-coinc. 105Ag deduced levels, J, π, multipolarities.
doi: 10.1103/PhysRevC.76.024307
2007WA21 Phys.Rev. C 75, 064315 (2007) X.Wang, R.V.F.Janssens, E.F.Moore, U.Garg, Y.Gu, S.Frauendorf, M.P.Carpenter, S.S.Ghugre, N.J.Hammond, T.Lauritsen, T.Li, G.Mukherjee, N.S.Pattabiraman, D.Seweryniak, S.Zhu Lifetime measurements of triaxial strongly deformed bands in 163Tm NUCLEAR REACTIONS 130Te(37Cl, 4n)163Tm, E=165 MeV; measured E\G, Iγ, γγ-coinc, mean lifetimes using DSAM and the Gammasphere array. 163Tm deduced quadrupole transition moments for proposed triaxial strongly deformed bands.
doi: 10.1103/PhysRevC.75.064315
2006CO20 Phys.Rev.C 74, 067301 (2006) A.Costin, T.Ahn, B.Bochev, K.Dusling, T.C.Li, N.Pietralla, G.Rainovski, W.Rother Lifetime measurement for the 21+ state of 170Hf NUCLEAR REACTIONS 158Gd(16O, 4n), E=80 MeV; measured prompt and delayed Eγ, Iγ. 170Hf levels deduced T1/2, B(E2). Pulsed beam, level systematics in neighboring nuclides discussed.
doi: 10.1103/PhysRevC.74.067301
2006DU02 Phys.Rev. C 73, 014317 (2006) K.Dusling, N.Pietralla, G.Rainovski, T.Ahn, B.Bochev, A.Costin, T.Koike, T.C.Li, A.Linnemann, S.Pontillo, C.Vaman Medium-spin γ-ray spectroscopy of the transitional nucleus 160Er NUCLEAR REACTIONS 159Tb(6Li, 5n), E=52 MeV; measured Eγ, Iγ, γγ-coin. 160Er deduced levels, J, π, δ, branching ratios, collective features. Constrained β-soft rotor model analysis.
doi: 10.1103/PhysRevC.73.014317
2006LI23 Phys.Rev. C 73, 054306 (2006) T.C.Li, N.Pietralla, A.P.Tonchev, M.W.Ahmed, T.Ahn, C.Angell, M.A.Blackston, A.Costin, K.J.Keeter, J.Li, A.Lisetskiy, S.Mikhailov, Y.Parpottas, B.A.Perdue, G.Rainovski, W.Tornow, H.R.Weller, Y.K.Wu First evidence for spin-flip M1 strength in 40Ar NUCLEAR REACTIONS 40Ar(polarized γ, γ'), E=7.7-11 MeV; measured Eγ, Iγ, asymmetry. 40Ar deduced levels, J, π, excitation B(E1), B(M1), spin-flip M1 strength. Comparison with shell model predictions.
doi: 10.1103/PhysRevC.73.054306
2006NA17 Phys.Lett. B 637, 43 (2006) B.K.Nayak, U.Garg, M.Hedden, M.Koss, T.Li, Y.Liu, P.V.Madhusudhana Rao, S.Zhu, M.Itoh, H.Sakaguchi, H.Takeda, M.Uchida, Y.Yasuda, M.Yosoi, H.Fujimura, M.Fujiwara, K.Hara, T.Kawabata, H.Akimune, M.N.Harakeh "Bi-modal" isoscalar giant dipole strength in 58Ni NUCLEAR REACTIONS 58Ni(α, α'), E=386 MeV; measured Eα, Iα, σ(θ), σ(E, θ). 58Ni deduced isoscalar GDR, GMR, and GQR parameters. Comparison with quasi-particle RPA calculations.
doi: 10.1016/j.physletb.2006.03.034
2005LI14 Phys.Rev. C 71, 044318 (2005) T.C.Li, N.Pietralla, C.Fransen, H.von Garrel, U.Kneissl, C.Kohstall, A.Linnemann, H.H.Pitz, G.Rainovski, A.Richter, M.Scheck, F.Stedile, P.von Brentano, P.von Neumann-Cosel, V.Werner One-phonon 2+1, ms mixed-symmetry state of 148Sm observed in nuclear resonance fluorescence NUCLEAR REACTIONS 148Sm(γ, γ'), E=3.2 MeV bremsstrahlung; measured Eγ, Iγ. 148Sm deduced levels, J, π, B(M1), B(E1), B(E2), mixed-symmetry state. Nuclear resonance fluorescence, interacting boson model.
doi: 10.1103/PhysRevC.71.044318
2000LI19 J.Phys.(London) G26, L111 (2000) Invariant Mass Dependence of Λ Polarization in pp → pΛK+π+π-π+π- NUCLEAR REACTIONS 1H(p, X), E at 27.5 GeV/c; calculated ΛK, ΛK2π, ΛK4π systems transverse and parallel momentum vs invariant mass; deduced invariant mass dependence of Λ polarization. Monte Carlo event generator.
doi: 10.1088/0954-3899/26/7/101
1997DE23 Phys.Rev. C56, 244 (1997) P.A.DeYoung, C.Dykstra, P.Gonthier, C.Mader, G.F.Peaslee, D.Peterson, R.Sedlar, S.Sundbeck, N.Shaw, G.Westfall, D.Craig, R.Lacey, T.Li, T.Reposeur, A.Vander Molen, J.Winfield, S.Yennello, A.Nadasen Sensitivity of Small-Angle Correlations of Light Charged Particles to Reaction Mechanisms in the 16O + 27Al Reaction at 40 MeV/nucleon NUCLEAR REACTIONS 27Al(16O, X), E=40 MeV/nucleon; measured pp-, pα-, dα, αα- correlation functions; deduced source lifetime features. 27Al, Ag, (32S, X), E=3.3-22.3 MeV; 12C, 27Al, 197Au(16O, X), E=5-94 MeV; 12C, Ag, 108Ag, 197Au(40Ar, X), E=8-60 MeV; 12C, 27Al, 59Co, 197Au(20Ne, X), E=30 MeV; 58Ni(α, X), E=30 MeV; 27Al, 122Sn(139Xe, X), E=31 MeV, 27Al, 197Au(14N, X), E=35-75 MeV; 58Ni, 115In, 197Au(12C, X), E=46.7 MeV; 108Ag(3He, X), E=66.7 MeV; 45Sc(36Ar, X), E=80-160 MeV; compiled small-angle correlation measurements. 4π CsI array.
doi: 10.1103/PhysRevC.56.244
1997GU32 Chin.J.Nucl.Phys. 19, 180 (1997) J.Guo, K.Zhao, X.Lu, Y.Cheng, T.Li, C.Fu, S.Li Mass Measurement of 122Cd and the New Levels of 120, 122Cd NUCLEAR REACTIONS 122,124Sn(18O, 20Ne), E=102 MeV; measured particle spectra. 122Cd deduced mass excess. 120,122Cd deduced levels.
1996AN24 Phys.Rev. A54, 3067 (1996) Z.An, T.H.Li, L.M.Wang, X.Y.Xia, Z.M.Luo Correction of Substrate Effect in the Measurement of 8-25-keV Electron-Impact K-Shell Ionization Cross Sections of Cu and Co Elements ATOMIC PHYSICS Cu, 59Co(e, X), E=8-25 keV; measured K-shell ionization σ. Thin targets substrate influence corrected. NUCLEAR REACTIONS Cu, 59Co(e, X), E=8-25 keV; measured K-shell ionization σ. Thin targets substrate influence corrected.
doi: 10.1103/PhysRevA.54.3067
1996LE22 Nucl.Instrum.Methods Phys.Res. A374, 299 (1996) M.J.Leitch, M.E.Anderson, J.Kapustinsky, T.K.Li, C.S.Mishra, J.C.Peng, J.E.Simmons, S.A.Dytman, J.G.Hardie, K.F.Von Reden, C.Smith Performance of a BGO-NaI η Spectrometer NUCLEAR REACTIONS 1H(π-, X), E at 200, 698 MeV/c; measured missing mass, invariant mass spectra for π0, η production. Performance of two-arm spectrometer with BGO actiuve converters discussed.
doi: 10.1016/0168-9002(96)00181-7
1996LU17 J.Phys.(London) B29, 4001 (1996) Z.Luo, Z.An, F.He, T.Li, X.Long, X.Peng Correction of the Influence of the Substrate Upon the Measurement of K-Shell Ioniziation Cross Sections ATOMIC PHYSICS Ni, Cr(e, X), E ≤ 34 keV; measured K-shell ionization σ. NUCLEAR REACTIONS Ni, Cr(e, X), E ≤ 34 keV; measured K-shell ionization σ.
doi: 10.1088/0953-4075/29/17/020
1995GU15 Phys.Lett. 357B, 7 (1995) E.E.Gualtieri, J.Yee, D.Craig, S.Hannuschke, R.A.Lacey, T.Li, W.J.Llope, A.Nadasen, E.Norbeck, R.Pak, N.T.B.Stone, A.M.Vander Molen, J.S.Winfield, G.D.Westfall, S.J.Yennello Absence of Saturation in Energy Deposition in 40Ar + 232Th Collisions at E = 15-115 A MeV NUCLEAR REACTIONS 232Th(40Ar, X), (40Ar, F), E=15-115 MeV/nucleon; measured fission, intermediate mass (fragment)(fragment)(θ), light charged particle production; deduced saturation absence in central collisions energy depositions. 4π detector.
doi: 10.1016/0370-2693(95)00901-V
1995HA32 Phys.Rev.Lett. 75, 2916 (1995) D.O.Handzy, W.Bauer, F.C.Daffin, S.J.Gaff, C.K.Gelbke, T.Glasmacher, E.Gualtieri, S.Hannuschke, M.J.Huang, G.J.Kunde, R.Lacey, T.Li, M.A.Lisa, W.J.Llope, W.G.Lynch, L.Martin, C.P.Montoya, R.Pak, G.F.Peaslee, S.Pratt, C.Schwarz, N.Stone, M.B.Tsang, A.M.Vander Molen, G.D.Westfall, J.Yee, S.J.Yennello Understanding Proton Emission in Central Heavy-Ion Collisions NUCLEAR REACTIONS 45Sc(36Ar, X), E=80-160 MeV/nucleon; measured σ(θ, Ep), pp-correlation function, central collisions; deduced proton emission from particle-unstable states possibility. BUU transport model.
doi: 10.1103/PhysRevLett.75.2916
1995LL01 Phys.Rev. C51, 1325 (1995) W.J.Llope, J.A.Conrad, C.M.Mader, G.Peilert, W.Bauer, D.Craig, E.Gualtieri, S.Hannuschke, R.A.Lacey, J.Lauret, T.Li, A.Nadasen, E.Norbeck, R.Pak, N.T.B.Stone, A.M.Vander Molen, G.D.Westfall, J.Yee, S.J.Yennello Autocorrelations and Intermediate-Mass-Fragment Multiplicities in Central Heavy-Ion Collisions NUCLEAR REACTIONS 27Al(20Ne, X), 45Sc(40Ar, X), 93Nb(84Kr, X), 139La(129Xe, X), E=15-155 MeV/nucleon; measured intermediate mass fragment average multiplicities; deduced model validities, autocorrelating centrality variables.
doi: 10.1103/PhysRevC.51.1325
1995LL02 Phys.Rev. C52, 1900 (1995) W.J.Llope, W.Bauer, D.Craig, E.E.Gualtieri, S.Hannuschke, R.A.Lacey, J.Lauret, T.Li, C.M.Mader, A.Nadasen, E.Norbeck, R.Pak, G.Peilert, N.T.B.Stone, A.M.Vander Molen, G.D.Westfall, J.Yee, S.J.Yennello The Sphericity of Central Heavy-Ion Reactions NUCLEAR REACTIONS 12C(12C, X), E=155 MeV/nucleon; 27Al(20Ne, X), E=140 MeV/nucleon; 45Sc(40Ar, X), E=115 MeV/nucleon; 93Nb(84Kr, X), E=75 MeV/nucleon; 139La(129Xe, X), E=60 MeV/nucleon; analyzed sphericity data. Dynamic, hybrid models.
doi: 10.1103/PhysRevC.52.1900
1995WE15 Chin.J.Nucl.Phys. 17, No 2, 106 (1995) Theoretical Calculation of the Asymmetrical Values on Z' Decay
1995WI19 Phys.Rev. C51, 3136 (1995) W.K.Wilson, W.Bauer, D.Cebra, M.Cronqvist, D.Krofcheck, R.Lacey, T.Li, A.Nadasen, E.Norbeck, T.Reposeur, A.Vander Molen, C.A.Ogilvie, G.D.Westfall, J.S.Winfield, J.Yee Azimuthal Distributions and Collective Motion in Intermediate Energy Heavy-Ion Collisions NUCLEAR REACTIONS 51V(40Ar, X), E=35-100 MeV/nucleon; measured light particle (Z=1, 2) azimuthal distribution; deduced mean field deflection associated anisotropy related features. Microscopic approach, mean-field mediated interactions plus NN-collisions.
doi: 10.1103/PhysRevC.51.3136
1995YE03 Phys.Lett. 356B, 191 (1995) J.Yee, E.E.Gualtieri, D.Craig, S.A.Hannuschke, T.Li, W.J.Llope, R.Pak, N.T.B.Stone, A.M.Vander Molen, G.D.Westfall, J.S.Winfield, S.J.Yennello, R.A.Lacey, A.Nadasen, E.Norbeck Tracking Fission-Like Processes in Central Collisions of 40Ar + 232Th; E = 15-115 A MeV NUCLEAR REACTIONS 232Th(40Ar, X), (40Ar, F), E=15-115 MeV/nucleon; measured fission fragment σ(θ), σ(φ), (fragment)(charged particle)-coin; deduced incomplete fusion followed by fission-like processes evidence.
doi: 10.1016/0370-2693(95)00805-U
1994HA29 Phys.Rev. C50, 858 (1994) D.O.Handzy, M.A.Lisa, C.K.Gelbke, W.Bauer, F.C.Daffin, P.Decowski, W.G.Gong, E.Gualtieri, S.Hannuschke, R.Lacey, T.Li, W.G.Lynch, C.M.Mader, G.F.Peaslee, T.Reposeur, S.Pratt, A.M.Vander Molen, G.D.Westfall, J.Yee, S.J.Yennello Two-Proton Correlation Functions for 36Ar + 45Sc at E/A = 80 MeV NUCLEAR REACTIONS 45Sc(36Ar, X), E=80 MeV/nucleon; measured 2p-correlation functions. Boltzmann-Uehling-Uhlenbeck transport model.
doi: 10.1103/PhysRevC.50.858
1994LA29 Phys.Lett. 339B, 22 (1994) J.Lauret, R.A.Lacey, A.Elmaani, A.Tsepetis, A.Moores, G.D.Westfall, D.Craig, E.Gualtieri, S.Hannuschke, T.Li, W.J.Llope, R.Pak, N.Stone, A.Vander Molen, J.Yee, A.Nadasen, R.S.Tickle, E.Norbeck High-Order Azimuthal Correlation Functions: Powerful probes for collective motion in heavy ion reactions NUCLEAR REACTIONS Sc(40Ar, X), E=35-115 MeV/nucleon; measured azimuthal correlation functions; deduced collective motion probing related features.
doi: 10.1016/0370-2693(94)91127-4
1994LI07 Phys.Rev. C49, 1630 (1994) T.Li, W.Bauer, D.Craig, E.Gualtieri, S.Hannuschke, R.Pak, A.M.Vander Molen, G.D.Westfall, J.S.Winfield, J.Yee, S.J.Yennello, R.Lacey, A.Nadasen, R.S.Tickle, E.Norbeck Mass Dependence of Critical Behavior in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 45Sc(40Ar, X), E=15-115 MeV/nucleon; measured fragment σ(Z); deduced critical behavior mass dependence. Percolation model.
doi: 10.1103/PhysRevC.49.1630
1994YE01 Phys.Lett. 321B, 15 (1994) S.J.Yennello, B.Young, J.Lee, J.A.Winger, J.S.Winfield, G.D.Westfall, A.Vander Molen, B.M.Sherrill, J.Shea, E.Norbeck, D.J.Morrissey, T.Li, E.Gualtieri, D.Craig, W.Benenson, D.Bazin The use of Radioactive Nuclear Beams to Study the Equilibration of the N/Z Degree of Freedom in Intermediate-Energy Heavy-Ion Reactions NUCLEAR REACTIONS 58Ni, 58Fe(40Ca, X), (40Ar, X), E=53 MeV/nucleon; 9Be(40Ar, X), E=80 MeV/nucleon; measured fragment spectra, isotope production ratio for fragment Z ≤ 5; deduced target, beam N/Z dependence.
doi: 10.1016/0370-2693(94)90321-2
1993BA19 Phys.Rev.Lett. 70, 3705 (1993) E.Bauge, A.Elmaani, R.A.Lacey, J.Lauret, N.N.Ajitanand, D.Craig, M.Cronqvist, E.Gualtieri, S.Hannuschke, T.Li, B.Llope, T.Reposeur, A.Vander Molen, G.D.Westfall, J.S.Winfield, J.Yee, S.Yennello, A.Nadasen, R.S.Tickle, E.Norbeck Observation of a Saturation in the Time Scale for Multifragment Emission in Symmetric Heavy-Ion Collisions NUCLEAR REACTIONS 93Nb(84Kr, X), E=35-75 MeV/nucleon; measured (fragment)(fragment) reduced velocity correlation functions; deduced intermediate mass fragment emission T1/2, time scale saturation.
doi: 10.1103/PhysRevLett.70.3705
1993LA02 Phys.Rev.Lett. 70, 1224 (1993) R.A.Lacey, A.Elmaani, J.Lauret, T.Li, W.Bauer, D.Craig, M.Cronqvist, E.Gualtieri, S.Hannuschke, T.Reposeur, A.Vander Molen, G.D.Westfall, W.K.Wilson, J.S.Winfield, J.Lee, S.Yennello, A.Nadasen, R.S.Tickle, E.Norbeck Multifragment Azimuthal Correlation Functions: Probes from reaction dynamics in collisions of intermediate energy heavy ions NUCLEAR REACTIONS 45Sc(40Ar, X), E=45 MeV/nucleon; measured (fragment)(fragment)(φ); deduced rotational collective motion, flow dominance, usefulness as reaction dynamics probe.
doi: 10.1103/PhysRevLett.70.1224
1993LI08 Phys.Rev.Lett. 70, 1924 (1993) T.Li, W.Bauer, D.Craig, M.Cronqvist, E.Gualtieri, S.Hannuschke, R.Lacey, W.J.Llope, T.Reposeur, A.M.Vander Molen, G.D.Westfall, W.K.Wilson, J.S.Winfield, J.Yee, S.J.Yennello, A.Nadasen, R.S.Tickle, E.Norbeck Intermediate Mass Fragment Production in Central Collisions of Intermediate Energy Heavy Ions NUCLEAR REACTIONS 45Sc(40Ar, X), E=35-115 MeV/nucleon; measured σ(fragment Z); deduced power-law parameter minimum.
doi: 10.1103/PhysRevLett.70.1924
1993LI16 Phys.Rev.Lett. 70, 3709 (1993) M.A.Lisa, C.K.Gelbke, W.Bauer, P.Decowski, W.G.Gong, E.Gualtieri, S.Hannuschke, R.Lacey, T.Li, W.G.Lynch, C.M.Mader, G.F.Peaslee, T.Reposeur, A.M.Vander Molen, G.D.Westfall, J.Yee, S.J.Yennello Impact-Parameter-Selected Two-Proton Intensity Interferometry for 36Ar + 45Sc at E/A = 80 MeV NUCLEAR REACTIONS 45Sc(36Ar, X), E=80 MeV/nucleon; measured (pp)(θ) vs momentum. Boltzmann-Uehling-Uhlenbeck theory.
doi: 10.1103/PhysRevLett.70.3709
1993LI37 Phys.Rev.Lett. 71, 2863 (1993) M.A.Lisa, C.K.Gelbke, P.Decowski, W.G.Gong, E.Gualtieri, S.Hannuschke, R.Lacey, T.Li, W.G.Lynch, G.F.Peaslee, S.Pratt, T.Reposeur, A.M.Vander Molen, G.D.Westfall, J.Yee, S.J.Yennello Observation of Lifetime Effects in Two-Proton Correlations for Well-Characterized Sources NUCLEAR REACTIONS 45Sc(36Ar, X), E=80 MeV/nucleon; measured pp-longitudinal, transverse correlation functions; deduced emitting source characteristic T1/2, other features.
doi: 10.1103/PhysRevLett.71.2863
1993WE09 Phys.Rev.Lett. 71, 1986 (1993) G.D.Westfall, W.Bauer, D.Craig, M.Cronqvist, E.Gualtieri, S.Hannuschke, D.Klakow, T.Li, T.Reposeur, A.M.Vander Molen, W.K.Wilson, J.S.Winfield, J.Yee, S.J.Yennello, R.Lacey, A.Elmaani, J.Lauret, A.Nadasen, E.Norbeck Mass Dependence of the Disappearance of Flow in Nuclear Collisions NUCLEAR REACTIONS 12C(12C, X), E=55-155 MeV/nucleon; 27Al(20Ne, X), E=55-140 MeV/nucleon; 41Sc(40Ar, X), E=35-115 MeV/nucleon; 93Nb(86Kr, X), E=35-75 MeV/nucleon; measured flow disappearance vs mass; deduced E(balance) dependence on mass. Boltzmann-Uehling-Uehlenbeck calculations.
doi: 10.1103/PhysRevLett.71.1986
1991KR01 Phys.Rev. C43, 350 (1991) D.Krofcheck, D.A.Cebra, M.Cronqvist, R.Lacey, T.Li, C.A.Ogilvie, A.Vander Molen, K.Tyson, G.D.Westfall, W.K.Wilson, J.S.Winfield, A.Nadasen, E.Norbeck Observation of a Minimum in Collective Flow for Ar + V Collisions NUCLEAR REACTIONS 51V(40Ar, X), E=100 MeV/nucleon; measured light charge particle spectra; deduced nuclear matter flow features. 4π solid angle array.
doi: 10.1103/PhysRevC.43.350
1991WI11 Phys.Rev. C43, 2696 (1991) W.K.Wilson, D.Cebra, S.Howden, J.Karn, D.Krofcheck, R.Lacey, T.Li, A.Nadasen, T.Reposeur, A.Vander Molen, C.A.Ogilvie, G.D.Westfall, J.S.Winfield Mean Field Deflection in Peripheral Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(12C, pX), E=50 MeV/nucleon; measured p(frament)-coin, proton transverse momentum spectra; deduced proton deflection direction.
doi: 10.1103/PhysRevC.43.2696
1990WI03 Phys.Rev. C41, R1881 (1990) W.K.Wilson, W.Benenson, D.A.Cebra, J.Clayton, S.Howden, J.Karn, T.Li, C.A.Ogilvie, A.Vander Molen, G.D.Westfall, J.S.Winfield, B.Young, A.Nadasen Azimuthal Asymmetry in Ar + V Collisions from E/A = 35 to 85 MeV NUCLEAR REACTIONS 51V(40Ar, X), E=35-85 MeV/nucleon; measured σ(fragment θ); deduced asymmetry mechanism.
doi: 10.1103/PhysRevC.41.R1881
1989PE12 Phys.Rev.Lett. 63, 2353 (1989) J.C.Peng, M.J.Leitch, J.D.Bowman, F.Irom, J.Kapustinsky, T.K.Li, L.C.Liu, C.S.Mishra, J.E.Simmons, Z.F.Wong, C.Smith, R.R.Whitney Coherent Eta-Meson Production in the Reaction π- + 3He → Eta + t NUCLEAR REACTIONS 3He(π-, t), (π+, t), E at 650, 620 MeV/c; measured eta production σ(θ); deduced eta production mechanism.
doi: 10.1103/PhysRevLett.63.2353
1987PE05 Phys.Rev.Lett. 58, 2027 (1987) J.C.Peng, J.Kapustinsky, C.Lee, M.J.Leitch, T.K.Li, C.Liu, J.M.Moss, J.E.Simmons, S.M.Tang, C.Smith, R.R.Whitney Observation of Eta-Meson Production in the Reaction π- + 3He → Eta + t NUCLEAR REACTIONS 3He(π-, t), E at 680 MeV/c; measured triton spectra; deduced eta-meson production σ. Large acceptance spectrometer.
doi: 10.1103/PhysRevLett.58.2027
1979KU01 Nucl.Phys. A313, 434 (1979) S.Kubono, T.K.Li, D.Dehnhard, D.A.Lewis, J.F.Petersen, J.L.Artz The 18O(18O, 16O)20O Reaction at 52 MeV NUCLEAR REACTIONS 18O(18O, 16O), 18O(18O, 18O), E(lab)=52 MeV; measured σ(θ). Enriched target. Microscopic analysis, exact finite-range DWBA.
doi: 10.1016/0375-9474(79)90511-6
1977IA01 J.Inorg.Nucl.Chem. 39, 7 (1977) R.Iafigliola, H.Huang, J.K.P.Lee, T.Y.Li The Decay of 85gZr RADIOACTIVITY 85Zr; measured Eγ, Iγ, γγ-coin, T1/2, γ(t); deduced branching, log ft. 85Y deduced levels, T1/2.
doi: 10.1016/0022-1902(77)80422-3
1977KU04 Phys.Rev.Lett. 38, 817 (1977) S.Kubono, D.Dehnhard, D.A.Lewis, T.K.Li, J.L.Artz, D.J.Weber, P.J.Ellis, A.Dudek-Ellis j Dependence of the (19F, 16O) Reaction and Spin-Orbit Forces in the Heavy-Ion Optical Potential NUCLEAR REACTIONS 28,30Si(19F, 16O), E=60 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.38.817
1976LI01 Phys.Rev. C13, 55 (1976) T.K.Li, D.Dehnhard, R.E.Brown, P.J.Ellis Investigation of the (d, 5/2)2 and (d5/2s1/2) Two-Particle Configurations in 18O Using the 17O(d, p)18O Reaction at 18 MeV NUCLEAR REACTIONS 17O(d, d), E=18.0 MeV; measured σ(θ); deduced optical model parameters. 17O(d, p), E=18.0 MeV; measured σ(Ep, θ). 18O levels deduced L, S. Enriched target.
doi: 10.1103/PhysRevC.13.55
1975MO09 Phys.Rev.Lett. 34, 1527 (1975); Erratum Phys.Rev.Lett. 35, 192 (1975) H.P.Morsch, D.Dehnhard, T.K.Li Strong Polarization of the 1p-Shell Core in the Lowest 0+ States of 24Mg and 28Si NUCLEAR REACTIONS 24Mg, 28Si(α, α'), E=23.5 MeV; measured σ(Eα', θ). 24Mg, 28Si levels deduced E0 matrix elements, S.
doi: 10.1103/PhysRevLett.34.1527
1974HO35 Nuovo Cim. 23A, 669 (1974) Decay of 75Kr RADIOACTIVITY 75Kr; measured Eγ, Iγ, T1/2, γγ-coin, γce-coin; deduced log ft. 75Br deduced levels, J, π.
doi: 10.1007/BF02821983
1972CH33 Nucl.Phys. A193, 225 (1972) H.C.Cheung, J.K.P.Lee, J.E.Kitching, S.K.Mark, T.Y.Li Low-Lying States of 80,82Br from (d, p) Reactions NUCLEAR REACTIONS 79,81Br(d, p), Ed=12.0 MeV; measured (Ep, θ), Q. 80,82Br deduced levels, J, L, π, transition strengths. Enriched targets.
doi: 10.1016/0375-9474(72)90248-5
1972MA61 Nucl.Phys. A195, 609 (1972) I.A.Mackenzie, S.K.Mark, T.Y.Li The 6Li(p, 2p)5He Reaction at 100 MeV NUCLEAR REACTIONS 6Li(p, 2p)5He, E=100 MeV; measured σ(E1, E2;θ(1)=θ(2)=30°-54°). ΔE-E telescope systems, plastic scintillation detectors. Enriched target.
doi: 10.1016/0375-9474(72)91082-2
1971MA61 Nucl.Phys. A178, 225 (1971) I.A.Mackenzie, S.K.Mark, T.Y.Li 6Li(p, pd)4He Reaction at 100 MeV NUCLEAR REACTIONS 6Li(p, pd), E=100 MeV; measured σ(Ep, Ed;θ(p)=θ(d)=45.5 to 57°). 14° analyzing magnet, Δe-E telescope system, plastic scintillation detectors. Enriched target. PWIA calculations.
doi: 10.1016/0375-9474(71)90200-4
1971SC26 Nucl.Phys. A176, 567 (1971) J.L.Schoonover, T.Y.Li, S.K.Mark The 9Be(p, d)8Be Reaction NUCLEAR REACTIONS 9Be(p, d), E=46, 100 MeV; analyzed σ(θ). 8Be levels deduced S. DWBA, local-energy approximation.
doi: 10.1016/0375-9474(71)90938-9
1971WA28 Nucl.Phys. A178, 201 (1971) Energies and Intensities of Cm L X-Rays Emitted in Coincidence with the α-Decay of 252Cf RADIOACTIVITY 252Cf, 241Am; measured E(L X-ray), I(L X-ray). 252Cf; measured Eγ, Iγ. 248Cm transition deduced ICC. Np; measured I(L X-ray). Cm; measured E(L X-ray) , I(L X-ray); deduced l2, l3 fluorescence yields.
doi: 10.1016/0375-9474(71)90198-9
1970HO07 Can.J.Phys. 48, 765 (1970) A.J.Houdayer, T.Y.Li, S.K.Mark Scattering of 100-MeV Protons by 11B and 16O NUCLEAR REACTIONS 11B, 16O(p, p), (p, p'), E=100 MeV; measured σ(Ep', θ); deduced optical model parameters. 11B levels deduced excitation strengths.
doi: 10.1139/p70-097
1969LI01 Can.J.Phys. 47, 257(1969) Distorted-Wave Born Approximation Analysis for the Reaction 12C(p, d)11C at 100 MeV NUCLEAR REACTIONS 12C(p, d), E=100 MeV. 11C deduced levels, L(n), S. DWBA analysis.
doi: 10.1139/p69-034
1969LI02 Nucl.Phys. A123, 147(1969) DWBA Analysis of 6Li(p, d)5Li and 7Li(p, d)6Li Reactions at 100 MeV NUCLEAR REACTIONS 6,7Li(p, d), E=100 MeV; measured σ(Ed, θ); deduced optical-model parameters. 5,6Li levels deduced S.
doi: 10.1016/0375-9474(69)90895-1
1968HI08 Can.J.Phys. 46, 1273 (1968) Analysis of the 19F(p, α)16O Reaction NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p68-448
1967CR05 Nucl.Phys. A96, 367(1967) R.M.Craig, B.Hird, C.J.Kost, T.Y.Li The 19F(p, α)16O, 12C(p, α)9B and 7Li(p, α)4He Reactions Near 45 MeV NUCLEAR REACTIONS 19F(p, α), 12C(p, α), 7Li(p, α), E = 30.5-45.1 MeV; measured σ(E; θ). Natural targets.
doi: 10.1016/0375-9474(67)90718-X
1966CR05 Phys.Letters 21, 177 (1966) R.M.Craig, B.Hird, C.J.Kost, T.Y.Li The (p, α) Reaction Mechanism at 45 MeV NUCLEAR STRUCTURE 12C, 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90305-2
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