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NSR database version of April 11, 2024.

Search: Author = T.Li

Found 93 matches.

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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
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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
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2023LI49      Phys.Rev. C 108, L041602 (2023)

T.Li, H.Zhang, X.Wang

Theory of Coulomb excitation of the 229Th nucleus by protons

doi: 10.1103/PhysRevC.108.L041602
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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2022LI28      Few-Body Systems 63, 43 (2022)

W.P.Liu, Z.H.Li, J.J.He, X.D.Tang, G.Lian, J.Su, Y.P.Shen, Z.An, F.Q.Chao, J.J.Chang, L.H.Chen, H.Chen, X.J.Chen, Y.H.Chen, Z.J.Chen, B.Q.Cui, X.C.Du, X.Fang, C.B.Fu, L.Gan, B.Guo, Z.Y.Han, X.Y.Guo, G.Z.He, J.R.He, A.Heger, S.Q.Hou, H.X.Huang, N.Huang, B.L.Jia, L.Y.Jiang, S.Kubono, J.M.Li, M.C.Li, K.A.Li, E.T.Li, T.Li, Y.J.Li, M.Lugaro, X.B.Luo, H.Y.Ma, S.B.Ma, D.M.Mei, W.Nan, W.K.Nan, N.C.Qi, Y.Z.Qian, J.C.Qin, J.Ren, C.S.Shang, L.T.Sun, W.L.Sun, W.P.Tan, I.Tanihata, S.Wang, P.Wang, Y.B.Wang, Q.Wu, S.W.Xu, S.Q.Yan, L.T.Yang, Y.Yang, X.Q.Yu, Q.Yue, S.Zeng, L.Zhang, H.Zhang, H.Y.Zhang, L.Y.Zhang, N.T.Zhang, P.Zhang, Q.W.Zhang, T.Zhang, X.P.Zhang, X.Z.Zhang, W.Zhao, J.F.Zhou, Y.Zho

Progress of Underground Nuclear Astrophysics Experiment JUNA in China

NUCLEAR REACTIONS 12C(α, γ), 13C(α, n), 25Mg(p, γ), 19F(p, α), E(cm)<600 keV; measured reaction products; deduced yields near the Gamow window. Comparison with available data.

doi: 10.1007/s00601-022-01735-3
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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
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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
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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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021JI07      Chin.Phys.C 45, 063101 (2021)

L.-B.Jia, T.Li

Interpretation of the Galactic gamma-ray excess with the dark matter indicated by 8Be and 4He anomalous transitions

doi: 10.1088/1674-1137/abeda6
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2021LI25      At.Data Nucl.Data Tables 140, 101440 (2021)

T.Li, Y.Luo, N.Wang

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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021LI39      J.Phys.(London) G48, 095105 (2021)

T.Li, X.Wang

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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0231.


2019GU11      Int.J.Mod.Phys. E28, 1950015 (2019)

S.Guo, Z.Wang, T.Li, J.Liu

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
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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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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2013WA18      Phys.Rev. C 88, 011301 (2013)

N.Wang, T.Li

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
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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
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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
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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
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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
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2009LI32      Nucl.Phys. A828, 125 (2009)

T.Li, S.-M.Zhao, X.-Q.Li

Comprehensive calculations on the OZI-forbidden nonleptonic decays of orthoquarkonia J/ψ (Υ) ππ, ρπ

doi: 10.1016/j.nuclphysa.2009.06.021
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2009LI43      Phys.Rev. C 80, 044329 (2009)

S.X.Liu, T.Li, B.R.Chen

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2000LI19      J.Phys.(London) G26, L111 (2000)

Z.-T.Liang, T.-S.Li

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
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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
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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
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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
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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
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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
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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
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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
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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
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1995WE15      Chin.J.Nucl.Phys. 17, No 2, 106 (1995)

B.-F.Wei, B.Zhou, T.-Z.Li

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
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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
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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
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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0251.


1974HO35      Nuovo Cim. 23A, 669 (1974)

A.Houdayer, S.K.Mark, T.Y.Li

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
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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
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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
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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
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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
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1971WA28      Nucl.Phys. A178, 201 (1971)

R.L.Watson, T.K.Li

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
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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
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1969LI01      Can.J.Phys. 47, 257(1969)

T.Y.Li, S.K.Mark

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
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1969LI02      Nucl.Phys. A123, 147(1969)

T.Y.Li, S.K.Mark

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
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1968HI08      Can.J.Phys. 46, 1273 (1968)

B.Hird, T.Y.Li

Analysis of the 19F(p, α)16O Reaction

NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p68-448
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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
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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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Note: The following list of authors and aliases matches the search parameter T.Li: , T.C.LI, T.H.LI, T.K.LI, T.S.LI, T.X.LI, T.Y.LI, T.Z.LI