Nuclear Science References (NSR)

doi: 10.1103/PhysRevC.109.034310
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2024WU05 Phys.Rev. C 109, 024326 (2024)

Y.-H.Wu, J.-B.Lu, Zh.Ren, G.-J.Fu, Ch.-Q.Li, P.-Y.Yang, Y.Hao, T.-J.Gao, L.-H.Zhu, X.-Zh.Cui, X.-G.Wu, Ch.-Y.He

Experimental study of the level structure in ⁹⁰Nb and systematics of level structure characteristics near A=90

doi: 10.1103/PhysRevC.109.024326
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2024XI03 Chin.Phys.C 48, 014104 (2024)

E.Xiao, X.Lei, Y.Huang, Y.Feng, L.Zhu, J.Su

Uncertainties of critical temperatures based on higher-order fluctuations of the largest fragment charge

NUCLEAR REACTIONS ⁴⁰Ca, ⁵⁶Fe, ⁹⁰Zr, ¹²⁰Sn, ¹³⁶Xe, ¹⁹⁷Au(¹²⁴Sn, X), E=400-1000 MeV/nucleon; analyzed available data; deduced parameters from the isotope thermometer utilizing the isospin-dependent quantum molecular dynamics model in conjunction with the statistical model GEMINI; deduced new signature of liquid-gas phase transition.

doi: 10.1088/1674-1137/ad021d
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2024YA04 Phys.Rev.Lett. 132, 072502 (2024)

H.B.Yang, Z.G.Gan, Y.J.Li, M.L.Liu, S.Y.Xu, C.Liu, M.M.Zhang, Z.Y.Zhang, M.H.Huang, C.X.Yuan, S.Y.Wang, L.Ma, J.G.Wang, X.C.Han, A.Rohilla, S.Q.Zuo, X.Xiao, X.B.Zhang, L.Zhu, Z.F.Yue, Y.L.Tian, Y.S.Wang, C.L.Yang, Z.Zhao, X.Y.Huang, Z.C.Li, L.C.Sun, J.Y.Wang, H.R.Yang, Z.W.Lu, W.Q.Yang, X.H.Zhou, W.X.Huang, N.Wang, S.G.Zhou, Z.Z.Ren, H.S.Xu

Discovery of New Isotopes ¹⁶⁰Os and ¹⁵⁶W: Revealing Enhanced Stability of the N=82 Shell Closure on the Neutron-Deficient Side

NUCLEAR REACTIONS ¹⁰⁶Cd(⁵⁸Ni, 4n)¹⁶⁰Os, E=335 MeV; measured reaction products; deduced new isotopes, σ. The Spectrometer for Heavy Atoms and Nuclear Structure (SHANS), the Sector Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL), China.

RADIOACTIVITY ¹⁶⁰Os(α), ¹⁵⁶W(β⁺); measured decay products, Eα, Iα; deduced α-particles energies, Q-values, T_1/2, α-decay reduced widths, N=82 shell closure toward the proton drip line. Comparison with theoretical calculations.

doi: 10.1103/PhysRevLett.132.072502
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2024ZH04 Phys.Rev. C 109, 014608 (2024)

M.M.Zhang, Z.Y.Zhang, Z.G.Gan, N.Wang, H.Yao, J.G.Wang, M.H.Huang, L.Ma, H.B.Yang, C.L.Yang, Y.L.Tian, Y.S.Wang, J.Y.Wang, Y.H.Qiang, X.L.Wu, S.Y.Xu, X.Y.Huang, Z.C.Li, Z.Zhao, L.C.Sun, H.Zhou, X.Zhang, G.Xie, L.Zhu, J.H.Zheng, Y.J.Li, F.Guan, Z.W.Lu, W.X.Huang, Y.He, H.S.Xu, Z.Z.Ren, S.G.Zhou

Experimental cross section study of ⁴⁰Ca + ¹⁷⁵Lu: Searching for new neutron-deficient Pa isotopes

doi: 10.1103/PhysRevC.109.014608
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2024ZH05 Phys.Rev. C 109, 014622 (2024)

M.-H.Zhang, Y.-H.Zhang, Y.Zou, Ch.Wang, L.Zhu, F.-Sh.Zhang

Predictions of synthesizing elements with Z=119 and 120 in fusion reactions

doi: 10.1103/PhysRevC.109.014622
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2024ZH08 Phys.Rev. C 109, 024606 (2024)

L.-L.Zhou, J.-J.Cai, L.-Q.Li, Z.-L.Wang, R.Zhu, X.-Y.Zhang, X.-R.Zhang, L.Zhu, G.Zhang, F.-Sh.Zhang

Fusion enhancement in the collisions with ⁴⁴Ca beams and the production of neutron-deficient ^245-250Lr isotopes

doi: 10.1103/PhysRevC.109.024606
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2023DU05 Eur.Phys.J. A 59, 93 (2023)

H.-X.Duan, F.Zhang, J.Su, L.Zhu, C.-C.Guo

Studying sub-saturation density symmetry energy with different nuclear thermometers

NUCLEAR REACTIONS U(¹⁵⁵Gd, X), E not given; ¹⁹⁷Au(¹⁹⁷Au, X), E=35 MeV/nucleon; analyzed available data; deduced the relation between nuclear temperatures and symmetry energy using the IQMD model.

doi: 10.1140/epja/s10050-023-01008-5
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2023FE04 Phys.Rev. C 107, 044606 (2023)

Y.Feng, Y.Huang, E.Xiao, X.Lei, L.Zhu, J.Su

Contributions of quasifission and fusion-fission in the ²⁴Mg + ¹⁷⁸Hf reaction at 145 MeV laboratory beam energy using the Boltzmann-Uehling-Uhlenbeck model

NUCLEAR REACTIONS ¹⁷⁸Hf(²⁴Mg, X), E=145 MV/nucleon; calculated time evolution of dinuclear systems of two fragments, mass numbers of fragment pairs, change of distance between fragments over time, σ of total capture, quasifission and fusion, contribution of quasi-inelastic, quasifission and fusion processes, mass-angular correlation of the fragments, dependence of the σ on the incompressibility parameter. Boltzmann-Uehling-Uhlenbeck model used with phase-space-density constraint (PSDC) method to describe heavy-ion collision near the Coulomb barrier. Comparison to experimental data.

doi: 10.1103/PhysRevC.107.044606
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2023LE01 Chin.Phys.C 47, 014102 (2023)

X.Lei, E.Xiao, Y.Feng, Y.Huang, L.Zhu, J.Su

Production of neutron-deficient nuclei around N = 126 by proton-induced spallation

NUCLEAR REACTIONS ²³⁷Np, ²³⁹Pu, ²⁴¹Am, ²⁴³Cm, ²⁴⁷Bk, ²⁵²Cf(p, X), E=1 GeV; analyzed available data. ^217,218,221Np, ^{222,223,224,225,226,227}Pu, ^{225,226,227,228,231}Am; deduced σ, yields. Comparison with the IQMD-GEMINI++ model calculations.

doi: 10.1088/1674-1137/ac9601
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2023LI08 Phys.Rev. C 107, 014614 (2023)

Z.Liao, L.Zhu, J.Su, C.Li

Dynamics of charge equilibration and effects on producing neutron-rich isotopes around N = 126 in multinucleon transfer reactions

NUCLEAR REACTIONS ¹⁹⁸Pt(¹²⁹Xe, X), E(cm)=470; ¹⁹⁸Pt(¹³⁶Xe, X), E(cm)=476 MeV; (¹⁴⁰Xe, X), E(cm)=466 MeV; calculated average N/Z values of projectile-like (PLF) and target-like (TLF) fragments as a function of the contact time, production σ for N=126 isotones. ¹⁹⁸Pt(¹⁴⁰Xe, X), (²⁰²Pt, X), (²³⁸U, X), E(cm)=466, 663, 741 MeV; calculated σ production of Ta, Re, W, and Os isotopes. Extended version of the dinuclear system model and the improved quantum molecular dynamics (ImQMD) model.

doi: 10.1103/PhysRevC.107.014614
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2023LI11 Phys.Rev. C 107, 024609 (2023)

G.-S.Li, J.Su, B.-H.Sun, S.Terashima, J.-W.Zhao, X.-D.Xu, J.-C.Zhang, G.Guo, L.-C.He, W.-P.Lin, W.-J.Lin, C.-Y.Liu, C.-G.Lu, B.Mei, Z.-Y.Sun, I.Tanihata, M.Wang, F.Wang, S.T.Wang, X.-L.Wei, J.Wang, J.-Y.Xu, J.-R.Liu, M.-X.Zhang, Y.Zheng, L.-H.Zhu, X.-H.Zhang

New measurement of the elemental fragmentation cross sections of 218 MeV/nucleon ²⁸Si on a carbon target

NUCLEAR REACTIONS ¹²C(²⁸Si, X), E=218 MeV/nucleon; measured reaction products, time-of-flight; deduced charge changing σ, elemental fragmentation σ (EFCSs) with charge changes 1-6. Comparison to the previous measurements and to the predictions from the models EPAX2, EPAX3, FRACS, ABRABLA07, NUCFRG2, and IQMD coupled with GEMINI (IQMD+GEMINI). Particle identification by means of MWPC and MUSIC detectors. Beam of ²⁸Si produced from ⁹Be(⁴⁰Ar, X), E=320 MeV/nucleon at Heavy Ion Research Facility (HIRFL-CSR, Lanzhou).

doi: 10.1103/PhysRevC.107.024609
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2023LI17 Int.J.Mod.Phys. E32, 2330002 (2023)

J.-J.Li, N.Tang, Y.-H.Zhang, M.-H.Zhang, C.Wang, X.-R.Zhang, L.Zhu, F.-S.Zhang

Progress on production cross-sections of unknown nuclei in fusion evaporation reactions and multinucleon transfer reactions

NUCLEAR REACTIONS ²³²Th(²⁰⁴Hg, X), E(cm)=678.1 MeV; ²⁴⁹Bk(²³⁸U, X), E(cm)=823.4 MeV; ²⁴⁸Cm(²³⁸U, X), E(cm)=824.9 MeV; calculated σ in fusion evaporation (FE) reactions and multinucleon transfer (MNT) reactions.

doi: 10.1142/S0218301323300023
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2023LI29 Phys. Rev. Res. 5, L022021 (2023)

Z.Liao, L.Zhu, Z.Gao, J.Su, C.Li

Optimal detection angles for producing N=126 neutron-rich isotones in multinucleon transfer reactions

NUCLEAR REACTIONS ²⁰⁸Pb(¹³⁶Xe, X)²⁰⁴Pt/²⁰³Ir/²⁰²Os/²⁰¹Re, E(cm)=526 MeV; calculated optimal angle ranges for detecting N=126 neutron-rich nuclides in the multinucleon transfer (MNT) process.

doi: 10.1103/PhysRevResearch.5.L022021
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2023SO06 Phys.Rev. C 107, 044609 (2023)

Q.Song, L.Zhu, B.Cai, C.Yuan, J.Su, H.Guo

Image processing of isotope yield in neutron-induced fission

NUCLEAR REACTIONS ²³⁵U, ²²⁹Th(n, F), E=2 MeV;²⁴³Am, ^236,238Np(n, F), E=0.0253 eV;²³⁹Pu(n, F), E=0.5 MeV; calculated fission yield mass distribution, fragments isomeric ratios for ¹²⁸Sb, ¹³⁰Sb, ¹³²Sb, ¹³¹Te, ¹³³Te, ¹³²I, ¹³⁴I, ¹³³Xe, ¹³⁵Xe. Predictions of machine-learning algorithm based on tensor decomposition method trained on 851 fission products from ENDF/ B-VIII.0 database. Comparison experimental data, TALYS and GEF calculations and JEFF-3.3, ENDF/B-VIII.0 evaluations.

doi: 10.1103/PhysRevC.107.044609
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2023WA22 Chin.Phys.C 47, 084001 (2023)

C.-J.Wang, G.Guo, H.J.Ong, Y.-N.Song, B.-H.Sun, I.Tanihata, S.Terashima, X.-L.Wei, J.-Y.Xu, X.-D.Xu, J.-C.Zhang, Yo.Zheng, L.-H.Zhu, Y.Cao, G.-W.Fan, B.-S.Gao, J.-X.Han, G.-S.Li, C.-G.Lu, H.-T.Qi, Y.Qin, Z.-Y.Sun, L.-P.Wan, K.-L.Wang, S.-T.Wang, X.-X.Wang, M.-X.Zhang, W.-W.Zhang, X.-B.Zhang, X.-H.Zhang, Z.-C.Zhou

Charge-changing cross section measurements of 300 MeV/nucleon ²⁸Si on carbon and data analysis

NUCLEAR REACTIONS C(²⁸Si, X), E=304 MeV/nucleon; measured reaction products; deduced σ. Comparison with available data. The second Radioactive Ion Beam Line in Lanzhou (RIBLL2).

doi: 10.1088/1674-1137/acd366
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2023ZH25 Phys.Rev. C 107, 064907 (2023)

L.Zhu, H.Zheng, K.Da, H.Gong, Z.Ye, G.Liu, R.C.Hwa

Universal energy dependence of measured temperatures for baryons produced in heavy-ion collisions

doi: 10.1103/PhysRevC.107.064907
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2023ZH28 Phys. Rev. Res. 5, L022030 (2023)

L.Zhu

Law of optimal incident energy for synthesizing superheavy elements in hot fusion reactions

NUCLEAR REACTIONS ²⁴³Am, ²⁵⁴Es, ²⁵⁷Fm(⁴⁸Ca, X), ²⁴⁹Cf, ²⁵⁴Es(⁴⁵Sc, X), ²⁴⁹Bk, ²⁴⁹Cm(⁵⁰Ti, X), ²⁴⁸Cm, ²⁴⁹Bk(⁵¹V, X), ²⁴³Am, ²⁴⁸Cm(⁵⁴Cr, X), ²⁴⁴Pu, ²⁴³Am(⁵⁵Mn, X), E not given; calculated optimal incident energies (OIE) for experiments; deduced correlations between results from the time-dependent Hartree-Fock theory and OIE for the superheavy elements (SHE).

doi: 10.1103/PhysRevResearch.5.L022030
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2022BA32 Int.J.Mod.Phys. E31, 2250065 (2022)

H.F.Bai, S.Y.Wang, W.Z.Xu, L.H.Zhu, X.G.Wu, D.P.Sun, C.Liu, Z.Q.Li, H.Jia, B.Qi, G.S.Li, S.Wang, R.J.Guo, X.C.Han, X.Xiao, L.Mu, C.Y.He, Y.Zheng, X.D.Wang, L.Zhu, Y.J.Li, L.Liu

Shape coexistence and possible isomers in ¹¹⁷Sn

NUCLEAR REACTIONS ¹¹⁴Cd(⁷Li, 3np)¹¹⁷Sn, E=48 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies, partial level scheme, J, π, DCO ratios, isomeric states. Comparison with systematics, the configuration-fixed constrained triaxial relativistic mean-field (RMF) calculations. The HI-13 tandem accelerator at China Institute of Atomic Energy in Beijing.

doi: 10.1142/S0218301322500653
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2022HU20 Phys.Rev. C 106, 054606 (2022)

Y.Huang, Y.Feng, E.Xiao, X.Lei, L.Zhu, J.Su

Influence of pre-scission neutron emission on high-energy ²³⁸U fission studied by the Langevin approach

NUCLEAR REACTIONS ²³⁸U(n, F), E=110, 325, 500 MeV; calculated potential energy surfaces, Langevin trajectory, pre-scission neutron multiplicity and kinetic energy, fragment mass distributions, average fragment mass, total kinetic energy of fission fragments, fragment deformation distribution. Three-dimensional Langevin approach considering nucleus elongation, deformation, and mass asymmetry coupled with Hauser-Feshbach statistical decay model to simulate the pre-scission neutron emission. Comparison with experimental data.

doi: 10.1103/PhysRevC.106.054606
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2022MU09 Phys.Lett. B 827, 137006 (2022)

L.Mu, S.Y.Wang, C.Liu, B.Qi, R.A.Bark, J.Meng, S.Q.Zhang, P.Jones, S.M.Wyngaardt, H.Jia, Q.B.Chen, Z.Q.Li, S.Wang, D.P.Sun, R.J.Guo, X.C.Han, W.Z.Xu, X.Xiao, P.Y.Zhu, H.W.Li, H.Hua, X.Q.Li, C.G.Li, R.Han, B.H.Sun, L.H.Zhu, T.D.Bucher, B.V.Kheswa, N.Khumalo, E.A.Lawrie, J.J.Lawrie, K.L.Malatji, L.Msebi, J.Ndayishimye, J.F.Sharpey-Schafer, O.Shirinda, M.Wiedeking, T.Dinoko, S.S.Ntshangase

First observation of the coexistence of multiple chiral doublet bands and pseudospin doublet bands in the A ≈ 80 mass region

NUCLEAR REACTIONS ⁸²Se(α, X)⁸¹Kr, E=65, 68 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, two nearly degenerate positive-parity bands. Comparison with the constrained covariant density functional theory and the multiparticle plus rotor model calculations.

doi: 10.1016/j.physletb.2022.137006
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2022SO09 Chin.Phys.C 46, 074108 (2022)

Q.-F.Song, L.Zhu, J.Su

Target dependence of isotopic cross sections in the spallation reactions ²³⁸U + p, d and ⁹Be at 1 AGeV

NUCLEAR REACTIONS ^1,2H, ⁹Be(²³⁸U, X), E=1 GeV/nucleon; calculated spallation σ using physical model dependent (Bayesian neural network) BNN, which includes the details of IQMD-GEMINI++ model and BNN.

doi: 10.1088/1674-1137/ac6249
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2022SU05 Phys.Rev. C 105, 024608 (2022)

J.Su, L.Zhu, E.Xiao

Fluctuations of the largest fragment charge in projectile fragmentation and its nonequilibrium effect

NUCLEAR REACTIONS ¹²⁰Sn(¹²⁴Sn, X), E=600 MeV/nucleon; calculated fluctuations of the largest fragment charge, mean multiplicity of intermediate-mass fragments for the equilibrium and nonequilibrium systems. Isospin-dependent quantum molecular dynamics (IQMD) model calculations. Comparison with available data.

doi: 10.1103/PhysRevC.105.024608
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2022XI03 J.Phys.(London) G49, 065102 (2022)

E.Xiao, Y.Feng, X.Lei, L.Zhu, J.Su

Dissipation of energy and higher-order fluctuations of the largest fragment charge in projectile fragmentation

NUCLEAR REACTIONS ¹²⁰Sn(¹⁰⁷Sn, X), E=60 MeV/nucleon; calculated density of the participant center, collective velocity, correlations between impact parameters, mean multiplicity of IMF. The isospin-dependent quantum molecular dynamics (IQMD) model is used to study the non-equilibrium thermalization and fragmentation.

doi: 10.1088/1361-6471/ac4f28
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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 T_1/2, 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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2022ZH45 Phys.Rev. C 106, 024305 (2022)

M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Zhang, Z.G.Gan, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, J.G.Wang, C.X.Yuan, C.Qi, A.N.Andreyev, X.Y.Huang, S.Y.Xu, Z.Zhao, L.X.Chen, J.Y.Wang, M.L.Liu, Y.H.Qiang, G.S.Li, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Y.F.Niu, L.Guo, Z.Z.Ren, S.G.Zhou

Fine structure in the α decay of the 8⁺ isomer in ^{216, 218}U

RADIOACTIVITY ^{216,216m,218,218m}U(α)[²¹⁸U from ¹⁸²W(⁴⁰Ar, 4n), E=190 MeV, ¹⁸⁴W(⁴⁰Ca, 2nα), E=206 MeV, ²¹⁶U from ¹⁸⁰W(⁴⁰Ar, 4n), E=191 MeV]; measured evaporation residues (EVRs), Eα, Iα, (EVR)α₁-α₂-correlations, T_1/2 using position-sensitive strip detectors (PSSDs) for α detection, and SHANS separator at HIRFL-Lanzhou. ^{216,216m,218,218m}U; deduced T_1/2, Q-values, α-branching ratio, α-decay hindrance factors. ²⁰⁴Rn, ^208,210Ra, ^212,214Th(α)[from ^216,218U α-decay chains]; measured Eα, T_1/2. ²¹²Th; deduced level, J, π, identification of the first 2+ state. ²¹⁵Ra, ^212,213,216Ac, ^{211,212,213,214,216,216m,217}Th, ^{216,217,217m,218}Pa, ^217,218,219U; observed Eα from their decays from (EVR)α-correlations. Comparison with previous experimental data.

doi: 10.1103/PhysRevC.106.024305
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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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2021HU19 Chin.Phys.C 45, 044003 (2021)

W.Hua, Z.Zhang, L.Ma, Z.Gan, H.Yang, M.Huang, C.Yang, M.Zhang, Y.Tian, X.Zhou, C.Yuan, C.Shen, L.Zhu

α-decay study of ²¹⁸Ac and ²²¹Th in ⁴⁰Ar+¹⁸⁶W reaction

RADIOACTIVITY ²¹⁸Ac, ²²¹Th, ²¹⁷Ra, ²¹³Rn(α) [from ¹⁸⁶W(⁴⁰Ar, X)²²¹Th/²¹⁸Ac, E=198.7 MeV]; measured decay products, Eα, Iα; deduced Q-values, T_1/2. Comparison with available data.

doi: 10.1088/1674-1137/abe0bd
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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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2021SU25 Nat.Phys. 17, 687 (2021), Erratum Nat.Phys. 18, 473 (2022)

V.Sulkosky, C.Peng, J.Chen, A.Deur, S.Abrahamyan, K.A.Aniol, D.S.Armstrong, T.Averett, S.L.Bailey, A.Beck, P.Bertin, F.Butaru, W.Boeglin, A.Camsonne, G.D.Cates, C.-C.Chang, S.Choi, E.Chudakov, L.Coman, J.C.Cornejo, B.Craver, F.Cusanno, R.De Leo, C.W.de Jager, J.D.Denton, S.Dhamija, R.Feuerbach, J.M.Finn, S.Frullani, K.Fuoti, H.Gao, F.Garibaldi, O.Gayou, R.Gilman, A.Glamazdin, C.Glashausser, J.Gomez, J.-O.Hansen, D.Hayes, F.W.Hersman, D.W.Higinbotham, T.Holmstrom, T.B.Humensky, C.E.Hyde, H.Ibrahim, M.Iodice, X.Jiang, L.J.Kaufman, A.Kelleher, K.E.Keister, W.Kim, A.Kolarkar, N.Kolb, W.Korsch, K.Kramer, G.Kumbartzki, L.Lagamba, V.Laine, G.Laveissiere, J.J.Lerose, D.Lhuillier, R.Lindgren, N.Liyanage, H.-J.Lu, B.Ma, D.J.Margaziotis, P.Markowitz, K.R.McCormick, M.Meziane, Z.-E.Meziani, R.Michaels, B.Moffit, P.Monaghan, S.Nanda, J.Niedziela, M.Niskin, R.Pandolfi, K.D.Paschke, M.Potokar, A.Puckett, V.A.Punjabi, Y.Qiang, R.D.Ransome, B.Reitz, R.Roche, A.Saha, A.Shabetai, S.Sirca, J.T.Singh, K.Slifer, R.Snyder, P.Solvignon, R.Stringer, R.Subedi, W.A.Tobias, N.Ton, P.E.Ulmer, G.M.Urciuoli, A.Vacheret, E.Voutier, K.Wang, L.Wan, B.Wojtsekhowski, S.Woo, H.Yao, J.Yuan, X.Zhan, X.Zheng, L.Zhu

Measurement of the generalized spin polarizabilities of the neutron in the low-Q² region

NUCLEAR REACTIONS ³He(polarized e^-, e^-), E=1.1-4.4 GeV; measured reaction products, Eβ, Iβ. ¹NN; deduced transverse-transverse and longitudinal-transverse interference σ, generalized neutron spin polarizabilities. Comparison with chiral effective field theory calculations.

doi: 10.1038/s41567-021-01245-9
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2021WA41 Phys.Rev. C 104, 034317 (2021)

X.Wang, L.Zhu, J.Su

Providing physics guidance in Bayesian neural networks from the input layer: The case of giant dipole resonance predictions

NUCLEAR STRUCTURE A=16-240; ^{124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160}Nd; analyzed giant-dipole resonance (GDR) data using Bayesian neural network (BNN) approach; evaluated and predicted nuclear data. Pearson's correlation coefficients applied for statistical dependence between nuclear properties in the ground state and the GDR energies. Relevance to discovering physics effects from complex nuclear data.

doi: 10.1103/PhysRevC.104.034317
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2021WA55 Chin.Phys.C 45, 124103 (2021)

X.Wang, L.Zhu, J.Su

Modeling complex networks of nuclear reaction data for probing their discovery processes

NUCLEAR REACTIONS ⁶³Cu(n, 2n), ⁶Li(γ, xn), E not given; analyzed available data; deduced model to build networks for discovery processes of nuclear reaction data based on a Bayesian statistics-based approach.

doi: 10.1088/1674-1137/ac23d5
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2021ZH22 Phys.Rev.Lett. 126, 152502 (2021)

Z.Y.Zhang, H.B.Yang, M.H.Huang, Z.G.Gan, C.X.Yuan, C.Qi, A.N.Andreyev, M.L.Liu, L.Ma, M.M.Zhang, Y.L.Tian, Y.S.Wang, J.G.Wang, C.L.Yang, G.S.Li, Y.H.Qiang, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Z.Z.Ren, S.G.Zhou

New α-Emitting Isotope ²¹⁴U and Abnormal Enhancement of α-Particle Clustering in Lightest Uranium Isotopes

RADIOACTIVITY ^214,216,218U(α) [from ^180,182W(³⁶Ar, 4n), ¹⁸⁴W(⁴⁰Ca, 2nα), E<200 MeV]; measured decay products, Eα, Iα; deduced α-decay Q-values and reduced widths, T_1/2, abnormal enhancement by the strong monopole interaction between the valence protons and neutrons. Comparison withavailable data, calculations.

doi: 10.1103/PhysRevLett.126.152502
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2021ZH37 Phys.Rev. C 104, 014902 (2021)

L.Zhu, H.Zheng, R.C.Hwa

Centrality and transverse-momentum dependence of hadrons in Pb + Pb collisions at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.104.014902
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2021ZH58 Phys.Rev. C 104, 044606 (2021)

L.Zhu, J.Su

Unified description of fusion and multinucleon transfer processes within the dinuclear system model

NUCLEAR REACTIONS ²³⁸U(⁴⁸Ca, X), (⁴⁸Ca, 3n), (⁴⁸Ca, 4n), E(cm)=182-204 MeV; calculated potential energy surface (PES) as a function of mass asymmetry and β₂, capture σ(E), fusion probability as function of incident energy and deformation parameter β₂, and evaporation residue (ER) σ(E) using DNS-SYSU code. ²⁴³Am(⁴⁸Ca, 2n), (⁴⁸Ca, 3n), (⁴⁸Ca, 4n), E^*=25-48 MeV; ²⁴⁴Pu, ²⁴⁸Cm(⁴⁸Ca, 3n), (⁴⁸Ca, 4n), E^*=30-58 MeV; ²⁴⁹Cf(⁴⁸Ca, 3n), E^*=28-42 MeV; calculated evaporation residue σ(E). ²³⁸U(⁴⁸Ca, X), E(cm)=180, 196, 204 MeV; calculated mass distribution of primary fragments, total kinetic energy (TKE)-mass distributions of multi-nucleon transfer (MNT) products. ²³⁸U(⁴⁸Ca, F), E(cm)=196 MeV; calculated Production cross sections of Ac (A=220-236), Th (A=223-238), Pa (A=227-240), U (A=229-242), and Np (A=232-240). ²³⁸U(⁴⁸Ca, X)⁶⁰Ca/²⁰⁰W/²⁴⁵U/²⁴⁶Np/²⁸¹Cn/²⁸²Cn/²⁸³Cn/²⁸⁴Cn/²⁸⁵Cn, E(cm)=180-270 MeV; calculated production σ(E). Dinuclear system (DNS) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.104.044606
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2020MA41 Eur.Phys.J. A 56, 209 (2020)

K.Y.Ma, J.B.Lu, J.Li, Y.J.Ma, D.Yang, W.J.Sun, Q.Y.Yang, X.Guan, J.Q.Wang, H.N.Pan, H.Wang, T.F.Cui, D.M.Zhang, L.H.Zhu, X.G.Wu, Y.Zheng, C.B.Li

Candidate magnetic rotational band in ¹⁰⁹Ag

NUCLEAR REACTIONS ¹¹⁰Pd(⁷Li, 4nα)¹⁰⁹Ag, E=46 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies and intensities, J, π, level scheme, bands, momenta, B(M1)/B(E2) ratios.

doi: 10.1140/epja/s10050-020-00213-w
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2020MA47 J.Phys.(London) G47, 085106 (2020)

K.Y.Ma, J.B.Lu, J.Li, D.Yang, Y.J.Ma, W.J.Sun, J.Q.Wang, Q.Y.Yang, H.Wang, H.N.Pan, D.M.Zhang, L.H.Zhu, X.G.Wu, Y.Zheng, C.B.Li

Possible 'stapler' band in ¹⁰⁹Ag nucleus

NUCLEAR REACTIONS ¹¹⁰Pd(⁷Li, X)¹⁰⁹Ag, E=46 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, multipolarities, J, π, negative-parity band. Comparison with theoretical calculations.

doi: 10.1088/1361-6471/ab920c
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2020SU12 Phys.Rev. C 101, 044606 (2020)

J.Su, L.Zhu, C.Guo

Constraints on the effective mass splitting by the isoscalar giant quadrupole resonance

NUCLEAR STRUCTURE ⁴⁰Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated correlation between the square of the excitation energies of isoscalar giant quadrupole resonances (ISGQRs) and the reciprocal of the weighted effective masses using the microscopic Langevin equation with particle density and kinetic-energy density from the Thomas-Fermi (TF) approach and the Hartree-Fock-Bogolyubov (SHFB) model. Comparison with experimental data. A=30-240; compiled experimental excitation energies of the ISGQRs as a function of mass number, and compared with several theoretical calculations.

doi: 10.1103/PhysRevC.101.044606
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2020SU18 Chin.Phys.C 44, 084106 (2020)

J.Su, L.Zhu, C.Guo, F.-S.Zhang

Isospin dependence of projectile fragmentation at hundreds of MeV/u

NUCLEAR REACTIONS ¹²⁰Sn(¹²⁴Sn, X), (¹⁰⁷Sn, X), E=600 MeV/nucleon; ²⁰⁸Pb(¹³⁶Xe, X), (¹²⁴Xe, X), E=1000 MeV/nucleon; analyzed available data; deduced isospin observables, neutron-to-proton ratios of the light particles emitted from the fragmenting. Isospin-dependent quantum molecular dynamics (IQMD) model and permitting only evaporation in the statistical model GEMINI, the IQMD+GEMINI model.

doi: 10.1088/1674-1137/44/8/084106
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2020WA07 Eur.Phys.J. A 56, 31 (2020)

M.Wang, W.J.Sun, B.H.Sun, J.Li, L.H.Zhu, Y.Zheng, G.L.Zhang, L.C.He, W.W.Qu, F.Wang, T.F.Wang, C.Xiong, C.Y.He, G.S.Li, J.L.Wang, X.G.Wu, S.H.Yao, C.B.Li, H.W.Li, S.P.Hu, J.J.Liu

The ΔI = 2 bands in ¹⁰⁹In: possible antimagnetic rotation

NUCLEAR REACTIONS ¹⁰⁰Mo(¹⁴N, 5n), E=78 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using two low-energy photon detectors and nine BGO-Compton-suppressed HPGe detectors at CIAE-Beijing. ¹⁰⁹In; deduced levels, J, π, multipolarities, anti-magnetic rotational band, alignments, configurations. Comparison with calculations using titled axis cranking calculation in the framework of covariant density function theory (TAC-CDFT), and with previous experimental results. Systematics of bands based on πg_7/2 orbital in ^{107,109,111,113}In. See also 2018Wa15, a related experiment from the same laboratory.

doi: 10.1140/epja/s10050-020-00039-6
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2020ZH22 Int.J.Mod.Phys. E29, 2030004 (2020)

L.Zhu, C.Li, C.-C.Guo, J.Su, P.W.Wen, G.Zhang, F.-S.Zhang

Theoretical progress on production of isotopes in the multinucleon transfer process

NUCLEAR REACTIONS ²³⁸U(⁶⁴Ni, X), E(cm)=307.5 MeV; ²⁰⁸Pb(¹²⁴Xe, X), E(cm)=50 MeV; ¹⁸⁶W(¹⁶⁰Gd, X), E=503 MeV; calculated transfer σ for production of neutron-rich transuranium nuclei.

doi: 10.1142/S0218301320300040
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2020ZH23 J.Phys.(London) G47, 065107 (2020)

L.Zhu

Selection of projectiles for producing trans-uranium nuclei in transfer reactions within the improved dinuclear system model

NUCLEAR REACTIONS ²³⁸U(¹³⁶Xe, X)Bk/Md, E(cm)=636 MeV; ²³⁸U(²³⁸U, X)Bk/Md, E(cm)=892 MeV; ²³⁸U(⁴⁸Ca, X)Bk/Md, E(cm)=201 MeV; analyzed available data. ^{235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260}Bk, ^{245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270}Md; calculated contour plots of the PES, production σ for Md and Bk.

doi: 10.1088/1361-6471/ab871f
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2019LI49 Phys.Rev. C 100, 054309 (2019)

C.Liu, S.Y.Wang, B.Qi, S.Wang, D.P.Sun, Z.Q.Li, R.A.Bark, P.Jones, J.J.Lawrie, L.Masebi, M.Wiedeking, J.Meng, S.Q.Zhang, H.Hua, X.Q.Li, C.G.Li, R.Han, S.M.Wyngaardt, B.H.Sun, L.H.Zhu, T.D.Bucher, B.V.Kheswa, K.L.Malatji, J.Ndayishimye, O.Shirinda, T.Dinoko, N.Khumalo, E.A.Lawrie, S.S.Ntshangase

New candidate chiral nucleus in the A ≈ 80 mass region: ⁸²₃₅Br₄₇

NUCLEAR REACTIONS ⁸²Se(α, 3np)⁸²Br, E=65, 68 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO), γγ(linear polarization) using the AFRODITE array at the separated-sector cyclotron (SSC) of iThemba LABS. ⁸²Br; deduced levels, J, π, multipolarities, band structures, configurations, B(M1)/B(E2) ratios, energy staggering parameter, degenerate positive-parity chiral doublet bands; calculated valence proton and valence neutron angular momenta as functions of spin for ^78,80,82Br, probability distributions for projection of total angular momentum for the chiral doublet bands in ⁸²Br using triaxial particle rotor model (TPRM).

doi: 10.1103/PhysRevC.100.054309
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2019MA48 Phys.Rev. C 100, 014326 (2019)

K.Y.Ma, J.B.Lu, J.Li, D.Yang, Y.J.Ma, W.J.Sun, X.Guan, D.M.Zhang, L.H.Zhu, X.G.Wu, Y.Zheng, C.B.Li, Y.Z.Liu

Possible antimagnetic rotational band and neutron alignment in ¹¹³In

NUCLEAR REACTIONS ¹¹⁰Pd(⁷Li, 4n), E=38, 50 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using HPGe detector array at CIAE-Beijing. ¹¹³In; deduced levels, J, π, multipolarities, configurations, alignments, magnetic dipole rotational (shears) bands, antimagnetic rotational bands. Comparison with self-consistent tilted axis cranking relativistic mean-field calculations, with the structure of ¹¹¹In, and with previous experimental results; predicted B(E2), deformation parameters β₂ and γ, and J²/B(E2).

doi: 10.1103/PhysRevC.100.014326
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2019SU17 Phys.Rev. C 100, 014602 (2019)

J.Su, L.Zhu, C.Guo, Z.Zhang

Uniform description of breakup mechanisms in central collision, projectile fragmentation, and proton-induced spallation

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=35 MeV/nucleon; ⁶³Cu(¹⁹⁷Au, X), E=600 MeV/nucleon; ¹²C(¹⁹⁷Au, X), E=1000 MeV/nucleon; ¹H(⁵⁶Fe, X), E=1000 MeV/nucleon; calculated charge distribution of fragments, multiplicity of intermediate mass fragments with Z=3-30, first and second fragment asymmetries versus the analogous bound charge. ⁴⁸Ti(⁴⁸Ti, X), E=30 MeV/nucleon; ¹²⁰Sn(¹²⁰Sn, X), E=600 MeV/nucleon; ¹H(⁹⁰Zr, X), E=2000 MeV/nucleon; calculated energy-density trajectories of the projectile centers, and fragment mass-excitation, correlations between the intermediate mass fragment (IMF) multiplicity and the total bound charge of the productions in the central collision, projectile fragmentation, and proton-induced spallation. Isospin-dependent quantum molecular dynamics (IQMD) model for breakup mechanisms in central collision, with the evaporations of light particles from the prefragments described by the statistical code GEMINI. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.014602
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2019WE04 Phys.Rev. C 99, 034606 (2019)

P.W.Wen, C.J.Lin, C.Li, L.Zhu, F.Zhang, F.S.Zhang, H.M.Jia, F.Yang, N.R.Ma, L.J.Sun, D.X.Wang, F.P.Zhong, H.H.Sun, L.Yang, X.X.Xu

Evaporation and fission of the primary fragments produced by multinucleon transfer reactions

NUCLEAR REACTIONS ²³⁸U(⁶⁴Ni, X), E(cm)=307.5 MeV; ²³⁸U(²³⁸U, X), E=1628, 1785, 2059 MeV; ²⁴⁸Cm(¹³⁶Xe, X), E=769 MeV; calculated isotopic production σ using GRAZING model with GEMINI++ statistical-decay model for multinucleon transfer (MNT) reactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.99.034606
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2019ZH13 Phys.Lett. B 791, 20 (2019)

L.Zhu, C.Li, J.Su, C.-C.Guo, W.Hua

Advantages of the multinucleon transfer reactions based on ²³⁸U target for producing neutron-rich isotopes around N=126

NUCLEAR REACTIONS ²³⁸U(¹⁸⁶W, X), (¹⁶⁰Gd, X), E(cm)=660, 475 MeV; analyzed available data; deduced mechanism of multinucleon transfer (MNT) reactions for producing neutron-rich heavy nuclei around N=126 using dinuclear system (DNS) model and isospin-dependent quantum molecular dynamics (IQMD) model.

doi: 10.1016/j.physletb.2019.02.015
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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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2019ZH44 J.Phys.(London) G46, 065102 (2019)

L.Zhu

Theoretical study on production of exotic nuclei near the neutron-drip line in multinucleon transfer reactions

NUCLEAR REACTIONS ⁴⁸Ca(⁴⁸Ca, X), E(cm)=65 MeV; ¹³⁶Xe(⁴⁸Ca, X), E(cm)=160 MeV; ²³⁸U(⁴⁸Ca, X), E(cm)=245 MeV; calculated mass distributions of primary fragments and final products in the DNS+GEMINI model.

doi: 10.1088/1361-6471/ab0bf1
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2019ZH48 Chin.Phys.C 43, 124103 (2019)

L.Zhu

Possibilities of producing superheavy nuclei in multinucleon transfer reactions based on radioactive targets

NUCLEAR REACTIONS ²⁴⁸Cm, ²³⁸U(²³⁸U, X)Cf/Es/Fm, E(cm)=800, 892 MeV; calculated yields of isotopes using DNS-sysu model. Comparison with experimental data.

doi: 10.1088/1674-1137/43/12/124103
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2019ZH52 Eur.Phys.J. A 55, 205 (2019)

L.Zhu, H.Zheng, R.Kong

Centrality and transverse momentum dependencies of hadrons in Pb+Pb collisions at √ s_NN = 5.02 TeV collisions at √ s_NN = 5.44 TeV from a multi-phase transport model

doi: 10.1140/epja/i2019-12903-3
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2018HW01 Phys.Rev. C 97, 054908 (2018)

R.C.Hwa, L.Zhu

Universal formula for baryon spectra in heavy-ion collisions and its implications

doi: 10.1103/PhysRevC.97.054908
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2018LI19 Phys.Rev. C 97, 044306 (2018)

L.Liu, S.Y.Wang, S.Wang, H.Hua, S.Q.Zhang, J.Meng, R.A.Bark, S.M.Wyngaardt, B.Qi, D.P.Sun, C.Liu, Z.Q.Li, H.Jia, X.Q.Li, C.Xu, Z.H.Li, J.J.Sun, L.H.Zhu, P.Jones, E.A.Lawrie, J.J.Lawrie, M.Wiedeking, T.D.Bucher, T.Dinoko, L.Makhathini, S.N.T.Majola, S.P.Noncolela, O.Shirinda, J.Gal, G.Kalinka, J.Molnar, B.M.Nyako, J.Timar, K.Juhasz, M.Arogunjo

Evolution from quasivibrational to quasirotational structure in ¹⁵⁵Tm and yrast 27/2^- to 25/2^- energy anomaly in the A ≈ 150 mass region

NUCLEAR REACTIONS ¹⁴⁴Sm(¹⁶O, 4np), E=118 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO) using the AFRODITE array for γ detection at iThemba LABS-SSC. ¹⁵⁵Tm; deduced high-spin levels, J, π, Eγ/spin ratio (E-GOS curves), side band, configuration, quasivibrational to quasirotational structure for the ground-state band; calculated potential energy surface (PES) in (ϵ₂, γ) plane. Systematics of E-GOS curves for ^{153,155,157,159}Tm, ¹⁵³Ho, ¹⁵⁷Lu, ¹⁵⁹Ta. Systematics of ground and side bands in ^{155,157,159,161}Tm, and energy differences between 25/2- and 27/2- yrast states in ^151,153Ho, ^153,155Tm, and ^155,157Lu.

doi: 10.1103/PhysRevC.97.044306
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2018LI33 Phys.Rev. C 98, 014618 (2018)

F.Li, L.Zhu, Z.-H.Wu, X.-B.Yu, J.Su, C.-C.Guo

Predictions for the synthesis of superheavy elements Z=119 and 120

NUCLEAR REACTIONS ²³⁸U, ^242,244Pu, ²⁴³Am, ^245,248Cm, ²⁴⁹Bk, ²⁴⁹Cf(⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n), E^*=25-60 MeV; calculated evaporation residue σ(E), and compared with available experimental data. ²⁵²Es(⁴⁰Ca, 3n), E(cm)=204.08 MeV; ²⁵²Es(⁴²Ca, 3n), E(cm)=203.00 MeV; ²⁴⁹Cf(⁴⁵Sc, 3n), E(cm)=211.09 MeV; ²⁵⁵Es(⁴⁰Ca, 4n), E(cm)=207.02 MeV; ²⁵⁴Es(⁴⁰Ca, 3n), E(cm)=203.60 MeV; ²⁴⁷Bk(⁴⁷Ti, 3n), E(cm)=219.19 MeV; ²⁴⁸Bk(⁴⁶Ti, 3n), E(cm)=217.76 MeV; ²⁴²Cm(⁵¹V, 2n), E(cm)=225.86 MeV; ²⁴⁸Cf(⁴⁵Sc, 2n), E(cm)=209.29 MeV; ²⁴¹Am(⁵²Cr, 2n), E(cm)=231.94 MeV; ²⁵²Es(⁴⁴Ca, 3n), E(cm)=204.27 MeV; ²⁵³Es(⁴³Ca, 3n), E(cm)=202.49 MeV; ²⁵⁴Es(⁴²Ca, 3n), E(cm)=201.65 MeV; ²⁵¹Cf(⁴⁵Sc, 3n), E(cm)=210.03 MeV; ²⁴⁹Bk(⁴⁷Ti, 3n), E(cm)=217.18 MeV; ²⁴⁸Bk(⁴⁸Ti, 3n), E(cm)=219.47 MeV; ²⁴⁵Cm(⁵¹V, 3n), E(cm)=229.29 MeV; ²⁴⁷Bk(⁴⁹Ti, 3n), E(cm)=222.17 MeV; ²⁴⁶Cm(⁵⁰V, 3n), E(cm)=225.70 MeV; ²⁴⁴Cm(⁵¹V, 2n), E(cm)=224.00 MeV; ²⁵⁵Es(⁴²Ca, 4n), E(cm)=205.95 MeV; ²⁴³Am(⁵³Cr, 3n), E(cm)=236.20 MeV; ²⁵⁴Es(⁴³Ca, 4n), E(cm)=206.90 MeV; ²⁵³Es(⁴⁴Ca, 4n), E(cm)=210.94 MeV; ²⁴³Am(⁵²Cr, 2n), E(cm)=229.49 MeV; ²⁵⁴Es(⁴⁴Ca, 3n), E(cm)=201.64 MeV; ²⁵⁵Es(⁴³Ca, 3n), E(cm)=201.49 MeV; ²⁵⁵Es(⁴⁴Ca, 4n), E(cm)=207.59 MeV; ²⁵²Es(⁴⁶Ca, 3n), E(cm)=206.00 MeV; ²⁴⁸Bk(⁵⁰Ti, 3n), E(cm)=222.48 MeV; ²⁴⁷Cm(⁵¹V, 3n), E(cm)=226.83 MeV; ²⁵⁴Cf(⁴⁵Sc, 4n), E(cm)=211.93 MeV; ²⁴⁹Bk(⁴⁹Ti, 3n), E(cm)=218.88 MeV; ²⁵⁴Es(⁴⁶Ca, 3n), E(cm)=203.64 MeV; ²⁵⁵Es(⁴⁶Ca, 4n), E(cm)=210.13 MeV; ²⁵²Es(⁴⁸Ca, 3n), E(cm)=208.42 MeV; ²⁵⁵Es(⁴⁶Ca, 3n), E(cm)=204.13; ²⁵⁴Es(⁴⁸Ca, 3n), E(cm)=205.96 MeV; ²⁵⁵Es(⁴⁸Ca, 4n), E(cm)=212.72 MeV; ²⁴²Cm(⁵⁰Cr, 2n), E(cm)=234.22 MeV; ²⁴⁹Cf(⁴⁶Ti, 3n), E(cm)=222.89 MeV; ²⁴⁸Cf(⁴⁶Ti, 2n), E(cm)=219.12 MeV; ²⁵⁷Fm(⁴⁰Ca, 5n), E(cm)=222.66 MeV; ²⁵⁷Fm(⁴⁰Ca, 4n), E(cm)=211.66 MeV; ²⁵⁷Fm(⁴⁰Ca, 3n), E(cm)=205.66 MeV; ²⁵¹Cf(⁴⁶Ti, 3n), E(cm)=220.39 MeV; ²⁵²Es(⁴⁵Sc, 3n), E(cm)=214.17 MeV; ²⁵⁰Cf(⁴⁶Sc, 2n), E(cm)=218.88 MeV; ²⁴⁷Bk(⁵⁰V, 3n), E(cm)=231.13 MeV; ²⁴⁴Cm(⁵²Cr, 2n), E(cm)=234.88 MeV; ²⁴⁵Cm(⁵²Cr, 3n), E(cm)=240.80 MeV; ²⁴³Cm(⁵³Cr, 2n), E(cm)=236.02 MeV; ²⁴⁷Cm(⁵⁰Cr, 3n), E(cm)=235.12 MeV; ²⁵⁷Fm(⁴²Ca, 3n), E(cm)=205.29 MeV; ²⁵⁴Es(⁴⁵Sc, 3n), E(cm)=213.40 MeV; ²⁵⁷Fm(⁴³Ca, 4n), E(cm)=210.97 MeV; ²⁵⁷Fm(⁴⁴Ca, 3n), E(cm)=205.27 MeV; ²⁵⁷Fm(⁴⁶Ca, 3n), E(cm)=207.84 MeV; ²⁵⁰Cm(⁵³Cr, 3n), E(cm)=234.59 MeV; ²⁵⁷Fm(⁴⁸Ca, 3n), E(cm)=211.07 MeV; calculated production σ for Z=119 and 120 superheavy isotopes. Dinuclear system (DNS) model.

doi: 10.1103/PhysRevC.98.014618
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2018SU08 Phys.Rev. C 97, 054604 (2018)

J.Su, L.Zhu, C.Guo

Influence of the nuclear level density on the odd-even staggering in ⁵⁶Fe + spallation at energies from 300 to 1500 MeV/nucleon

NUCLEAR REACTIONS ¹H(⁵⁶Fe, X), E=300-1500 MeV/nucleon; calculated level-density parameter, energy backshift, σ(E), differential σ(E), odd-even staggering (OES), and neutron- and proton-separation energies for Z=8-26, T_z=-1/2, 0, +1/2, +1 residual nuclei; deduced influence of level density on OES. ⁵⁴Fe, ⁵²Mn; calculated level densities as function of excitation energy. Calculations performed using isospin-dependent quantum molecular dynamics (IQMD) model using statistical model GEMINI code. Comparison with experimental values.

doi: 10.1103/PhysRevC.97.054604
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2018SU12 Phys.Rev. C 98, 014610 (2018)

J.Su, W.Trautmann, L.Zhu, W.-J.Xie, F.-S.Zhang

Dynamical properties and secondary decay effects of projectile fragmentations in ¹²⁴Sn, ¹⁰⁷Sn + ¹²⁰Sn collisions at 600 MeV/nucleon

NUCLEAR REACTIONS ¹²⁰Sn(¹²⁴Sn, X), (¹⁰⁷Sn, X), E=600 MeV/nucleon; calculated mass number and excitation energy of fragments, longitudinal momenta, mean multiplicity of intermediate mass fragments (IMFs), σ(Z) of fragments, mean neutron-to-proton ratios of light fragments. Isospin-dependent quantum molecular dynamics model (IQMD) with and without the GEMINI statistical code. Comparison with experimental data for fragment yields from ALADIN Collaboration.

doi: 10.1103/PhysRevC.98.014610
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2018SU17 Phys.Rev. C 98, 024315 (2018)

J.Su, L.Zhu, C.Guo

Isoscalar giant monopole resonance within the Bohr-Mottelson model

NUCLEAR STRUCTURE A=20-240; analyzed excitation energies and incompressibility parameters, widths, surface and symmetry parameters, Coulomb parameter of the incompressibility of the Isoscalar giant monopole resonance (ISGMR) as a function of the mass number in nuclei from ¹²C to ²³⁸U using Bohr-Mottelson model. Comparison with other theoretical predictions.

doi: 10.1103/PhysRevC.98.024315
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2018TE06 Phys.Rev.Lett. 121, 242501 (2018)

S.Terashima, L.Yu, H.J.Ong, I.Tanihata, S.Adachi, N.Aoi, P.Y.Chan, H.Fujioka, M.Fukuda, H.Geissel, G.Gey, J.Golak, E.Haettner, C.Iwamoto, T.Kawabata, H.Kamada, X.Y.Le, H.Sakaguchi, A.Sakaue, C.Scheidenberger, R.Skibinski, B.H.Sun, A.Tamii, T.L.Tang, D.T.Tran, K.Topolnicki, T.F.Wang, Y.N.Watanabe, H.Weick, H.Witala, G.X.Zhang, L.H.Zhu

Dominance of Tensor Correlations in High-Momentum Nucleon Pairs Studied by (p, pd) Reaction

NUCLEAR REACTIONS ¹⁶O(p, pd), E=392 MeV; measured reaction products; deduced σ, σ(θ, E), isospin character of p-n pairs at large relative momentum. Comparison with the DWIA calculations.

doi: 10.1103/PhysRevLett.121.242501
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2018WA15 Phys.Rev. C 98, 014304 (2018), Erratum Phys.Rev. C 102, 069903 (2020)

M.Wang, Y.Y.Wang, L.H.Zhu, B.H.Sun, G.L.Zhang, L.C.He, W.W.Qu, F.Wang, T.F.Wang, Y.Y.Chen, C.Xiong, J.Zhang, J.M.Zhang, Y.Zheng, C.Y.He, G.S.Li, J.L.Wang, X.G.Wu, S.H.Yao, C.B.Li, H.W.Li, S.P.Hu, J.J.Liu

New high-spin structure and possible chirality in ¹⁰⁹In

NUCLEAR REACTIONS ¹⁰⁰Mo(¹⁴N, 5n), E=78 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using two low-energy photon detectors and nine BGO-Compton-suppressed HPGe detectors at CIAE-Beijing. ¹⁰⁹In; deduced levels, J, π, multipolarities, bands, alignments, configurations, and possible chiral partner bands. Comparison with calculations using titled axis cranking calculation in the framework of covariant density function theory (TAC-CDFT), and with previous experimental results. Systematics of yrast states in ^{103,105,107,109,111,113}In.

doi: 10.1103/PhysRevC.98.014304
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2018WU06 Phys.Rev. C 97, 064609 (2018)

Z.-H.Wu, L.Zhu, F.Li, X.-B.Yu, J.Su, C.-C.Guo

Synthesis of neutron-rich superheavy nuclei with radioactive beams within the dinuclear system model

NUCLEAR REACTIONS ^242,244Pu, ²⁴³Am, ^245,248,250Cm, ²⁴⁹Bk, ^250,251Cf(⁴⁸Ca, 2n), (⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n), E^*=25-60 MeV; ²³⁴Th(⁴²S, 2n), (⁴²S, 3n), (⁴²S, 4n), (⁴²S, 5n), E^*=20-65 MeV; ²³⁴Th, ²⁴⁴Pu(⁴⁶Ar, 2n), (⁴⁶Ar, 3n), (⁴⁶Ar, 4n), (⁴⁶Ar, 5n), E^*=20-65 MeV; ²³⁴Th, ²³⁸U, ²⁴⁸Cm, ²⁵⁵Es(⁴⁴Cl, 2n), (⁴⁴Cl, 3n), (⁴⁴Cl, 4n), (⁴⁴Cl, 5n), E^*=20-65 MeV; ²²⁸Ra(⁴⁵Cl, 2n), (⁴⁵Cl, 3n), (⁴⁵Cl, 4n), (⁴⁵Cl, 5n), E^*=20-65 MeV; ²⁴⁴Pu, ²⁴⁸Cm(⁴³Cl, 2n), (⁴³Cl, 3n), (⁴³Cl, 4n), (⁴³Cl, 5n), E^*=20-65 MeV; ²⁴⁴Pu, ²⁵⁴Cf, ²⁵⁵Es(⁴¹S, 2n), (⁴¹S, 3n), (⁴¹S, 4n), (⁴¹S, 5n), E^*=20-65 MeV; ²⁵⁷Fm(⁴²Ar, 2n), (⁴²Ar, 3n), (⁴²Ar, 4n), (⁴²Ar, 5n), E^*=20-65 MeV; ²⁶⁰Md(³⁸Cl, 2n), (³⁸Cl, 3n), (³⁸Cl, 4n), (³⁸Cl, 5n), E^*=20-65 MeV; calculated evaporation residue σ. ²²⁸Ra(⁴⁵Cl, 2n), E^*=36.0 MeV; ²²⁸Ra(⁴⁶Cl, 3n), E^*=46.0 MeV; ²²⁶Ra(⁴⁷Cl, 2n), E^*=36.0 MeV; ²³⁴Th(⁴²S, 4n), E^*=43.0 MeV; ²²⁸Ra(⁴⁶Ar, 2n), E^*=34.0 MeV; ²³⁴Th(⁴³S, 5n), E^*=51.0 MeV; ²³⁴Th(⁴²S, 3n), E^*=41.0 MeV; ²³⁴Th(⁴³S, 4n), E^*=46.0 MeV; ²³⁴Th(⁴⁴S, 5n), E^*=59.0 MeV; ²³⁴Th(⁴⁴Cl, 2n), E^*=37.0 MeV; ²³⁴Th(⁴⁵Cl, 3n), E^*=44.0 MeV; ²²⁸Ra(⁵⁰K, 2n), E^*=36.0 MeV; ²³⁴Th(⁴⁶Ar, 2n), E^*=34.0 MeV; ²³⁸U(⁴³S, 3n), E^*=41.0 MeV; ²³⁸U(⁴²S, 2n), E^*=37.0 MeV; ²³⁸U(⁴⁴Cl, 3n), E^*=38.0 MeV; ²³⁸U(⁴³Cl, 2n), E^*=36.0 MeV; ²³⁸U(⁴³S, 3n), E^*=41.0 MeV; ²³⁴Th(⁴⁷K, 2n), E^*=33.0 MeV; ²⁴⁴Pu(⁴¹S, 3n), E^*=38.0 MeV; ²⁴⁴Pu(⁴²S, 4n), E^*=42.0 MeV; ²³⁸U(⁴⁶Ar, 2n), E^*=33.0 MeV; ²⁴⁴Pu(⁴³Cl, 4n), E^*=44.0 MeV; ²⁴²Pu(⁴⁴Cl, 3n), E^*=37.0 MeV; ²⁴⁴Pu(⁴²Cl, 3n), E^*=38.0 MeV; ²⁴⁴Pu(⁴⁶Ar, 4n), E^*=38.0 MeV; ²⁴⁴Pu(⁴⁵Ar, 3n), E^*=44.0 MeV; ²⁴²Pu(⁴⁶Ar, 2n), E^*=33.0 MeV; ²⁴⁸Cm(⁴³Cl, 4n), E^*=38.0 MeV; ²⁵⁰Cm(⁴²Cl, 5n), E^*=43.0 MeV; ²⁴⁸Cm(⁴⁴Cl, 5n), E^*=43.0 MeV; ²⁴⁸Cm(⁴⁴Cl, 4n), E^*=38.0 MeV; ²⁵⁰Cm(⁴²Cl, 4n), E^*=39.0 MeV; ²⁵⁰Cm(⁴³Cl, 5n), E^*=45.0 MeV; ²⁵⁴Cf(⁴¹S, 5n), E^*=40.0 MeV; ²⁵³Cf(⁴²S, 5n), E^*=40.0 MeV; ²⁵⁰Cm(⁴⁴Ar, 4n), E^*=37.0 MeV; ²⁵⁵Es(⁴¹S, 5n), E^*=40.0 MeV; ²⁵⁴Cf(⁴²Cl, 5n), E^*=40.0 MeV; ²⁵³Cf(⁴³Cl, 5n), E^*=39.0 MeV; ²⁵⁵Es(⁴¹S, 4n), E^*=37.0 MeV; ²⁵³Cf(⁴³Cl, 4n), E^*=36.0 MeV; ²⁵⁴Cf(⁴²Cl, 4n), E^*=37.0 MeV; ²⁵⁰Cm(⁴⁸Ca, 4n), E^*=35.0 MeV; ²⁴⁸Cm(⁴⁸Ca, 2n), E^*=31.0 MeV; ²⁵⁰Cm(⁴⁶Ca, 2n), E^*=35.0 MeV; ²⁵⁵Es(⁴⁴Cl, 5n), E^*=40.0 MeV; ²⁵⁴Cf(⁴⁴Ar, 4n), E^*=36.0 MeV; ²⁵⁷Fm(⁴¹S, 4n), E^*=37.0 MeV; ²⁵⁰Cm(⁴⁸Ca, 3n), E^*=31.0 MeV; ²⁵⁵Es(⁴⁴Cl, 4n), E^*=36.0 MeV; ²⁵³Cf(⁴⁶Ar, 4n), E^*=34.0 MeV; ²⁵⁴Cf(⁴⁶Ar, 5n), E^*=41.0 MeV; ²⁵⁰Cf(⁴⁸Ca, 3n), E^*=34.0 MeV; ²⁵⁰Cm(⁴⁹Ti, 4n), E^*=42.0 MeV; ²⁵²Cf(⁴⁶Ca, 3n), E^*=36.0 MeV; ²⁶⁰Md(³⁸Cl, 3n), E^*=41.0 MeV; ²⁶⁰Md(³⁹Cl, 4n), E^*=42.0 MeV; ²⁵⁷Fm(⁴²Ar, 4n), E^*=41.0 MeV; ²⁵¹Cf(⁴⁸Ca, 3n), E^*=30.0 MeV; ²⁵²Cf(⁴⁸Ca, 4n), E^*=38.0 MeV; ²⁵⁰Cm(⁴⁹Ti, 3n), E^*=34.0 MeV; ²⁵⁷Fm(⁴²Ar, 3n), E^*=33.0 MeV; ²⁵⁷Fm(⁴³Ar, 4n), E^*=38.0 MeV; ²⁶⁰Md(³⁹Cl, 3n), E^*=37.0 MeV; ²⁴⁴Pu(⁴³Cl, n), E^*=40.0 MeV; ²³⁸Cm(⁴⁸Ca, 2np), E^*=41.0 MeV; ²⁵⁴Cf(⁴¹S, 5n), E^*=40.0 MeV; ²⁴⁸Cm(⁴⁸Ca, 2nα), E^*=46.0 MeV; ²⁴⁸Cm(⁴³Cl, 4n), E^*=38.0 MeV; ²⁴²Pu(⁴⁸Ca, 2np), E^*=35.0 MeV; ²⁴⁸Cm(⁴⁴Cl, 4n), E^*=38.0 MeV; ²⁴²Pu(⁴⁸Ca, np), E^*=40.0 MeV; ²⁴⁴Pu(⁴⁸Ca, 3np), E^*=45.0 MeV; ²⁵⁵Es(⁴¹S, 5n), E^*=40.0 MeV; ²⁴⁵Cm(⁴⁸Ca, np), E^*=32.0 MeV; ²⁴⁹Bk(⁴⁸Ca, 2nα), E^*=37.0 MeV; ²⁵⁵Es(⁴¹S, 4n), E^*=37.0 MeV; ²⁴⁸Cm(⁴⁸Ca, 3np), E^*=44.0 MeV; ²⁴⁹Bk(⁴⁸Ca, nα), E^*=32.0 MeV; calculated evaporation residue σ, and optimal incident beam energies. ⁴⁸Ca(²³⁸U, 2n), (²³⁸U, 3n), (²³⁸U, 4n), E(cm)=184.13-214.13 MeV; calculated evaporation residue σ, potential energy surface, driving potential, survival and complete fusion probabilities, and capture σ. Dinuclear system model. ²⁷¹Db, ^272,273Sg, ²⁷⁶Bh, ²⁷⁸Hs, ²⁷⁹Mt, ²⁸²Ds, ²⁸³Rg, ²⁸⁶Cn, ^287,288Nh, ²⁹⁰Fl, ^291,292Mc, ^294,295Lv, ^295,296Og; calculated evaporation residue σ, and optimal incident beam energies for various reactions. Comparison with available experimental data. Relevance to synthesis of neutron-rich superheavy nuclei using radioactive ion beams, such as those at ATLAS-ANL.

doi: 10.1103/PhysRevC.97.064609
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2018XI05 Phys.Rev. C 97, 064608 (2018)

W.-J.Xie, J.Su, L.Zhu, F.-S.Zhang

Effects of the pion-nucleon potential in ¹⁹⁷Au + ¹⁹⁷Au collisions at 1.5 GeV/nucleon

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=1.5 GeV/nucleon; calculated pion multiplicity, excitation function of pion multiplicity, rapidity distributions of directed and elliptic flows, rapidity dependence of the and centrality dependence of midrapidity and elliptic flows, polar angle distributions of π⁺ and π^-, transverse momentum dependence of the strength function of the azimuthal anisotropy, using isospin-dependent quantum molecular dynamics (IQMD) model using various sets of the pion-nucleon (πN) potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.97.064608
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2018ZH17 Phys.Rev. C 97, 044614 (2018)

L.Zhu, P.-W.Wen, C.-J.Lin, X.-J.Bao, J.Su, C.Li, C.-C.Guo

Shell effects in a multinucleon transfer process

NUCLEAR REACTIONS ¹⁹⁸Pt(¹³⁶Xe, X), E(cm)=643, 420 MeV; ²⁰⁸Pb(¹³⁶Xe, X), E(cm)=450, 526 MeV; ¹⁸⁶W(¹³⁶Xe, X), E(cm)=408 MeV; ¹⁸⁶W(¹⁵⁰Nd, X), E(cm)=451 MeV; calculated potential energy surfaces, total kinetic energy losses (TKEL), and production σ with and without shell corrections using dinuclear system (DNS) model; deduced shell effects on producing trans-target nuclei. Comparison with experimental values.

doi: 10.1103/PhysRevC.97.044614
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2018ZH39 Phys.Rev. C 98, 034609 (2018)

L.Zhu, J.Su, P.-W.Wen, C.-C.Guo, C.Li

Multinucleon transfer process in the reaction ¹⁶⁰Gd + ¹⁸⁶W

NUCLEAR REACTIONS ¹⁸⁶W(¹⁶⁰Gd, X), E(cm)=430, 450, 503, 550 MeV; calculated potential energy surface as a function of mass asymmetry and β₂ deformation, σ(E) for production of primary products as function of mass number, TKEL and β₂, N/Z distribution of primary products, and production σ(E) of Os and Np isotopes, ²⁰²Os, ²⁰¹Re, ²⁴⁰Np, ²⁴¹U, and isotopes of Z=60-100, N=90-150. Dinuclear system (DNS) model with GEMINI code for multinucleon transfer (MNT) process.

doi: 10.1103/PhysRevC.98.034609
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2018ZH50 Eur.Phys.J. A 54, 175 (2018)

L.Zhu, H.Zheng, C.M.Ko, Y.Sun

Light nuclei production in Pb+Pb collisions at √ s_NN = 2.76 TeV

doi: 10.1140/epja/i2018-12610-7
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2018ZH55 Phys.Rev. C 98, 054905 (2018)

W.Zhao, L.Zhu, H.Zheng, C.M.Ko, H.Song

Spectra and flow of light nuclei in relativistic heavy ion collisions at energies available at the BNL Relativistic Heavy Ion Collider and at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.98.054905
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2017GA30 Eur.Phys.J. A 53, 197 (2017)

Y.Gao, H.Zheng, L.L.Zhu, A.Bonasera

Description of charged particle pseudorapidity distributions in Pb+Pb collisions with Tsallis thermodynamics

doi: 10.1140/epja/i2017-12397-y
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2017HE09 Chin.Phys.C 41, 044003 (2017)

L.-C.He, Y.Zheng, L.-H.Zhu, H.-L.Ma, X.-G.Wu, C.-Y.He, G.-S.Li, L.-L.Wang, X.Hao, Y.Liu, X.-Q.Li, B.Pan, Z.-Y.Li, H.-B.Ding

Collective states and shape competition in ¹²⁶Te

NUCLEAR REACTIONS ¹²⁴Sn(⁷Li, 4np)¹²⁶Te, E=48 MeV; measured reaction products, Eγ, Iγ; deduced energies, relative intensities, directional correlation of oriented states ratios, and initial and final state J, π of γ-rays. Comparison with theoretical calculations.

doi: 10.1088/1674-1137/41/4/044003
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2017LI16 Phys.Rev. C 95, 054612 (2017)

J.Li, C.Li, G.Zhang, L.Zhu, Z.Liu, F.-S.Zhang

Production cross sections of neutron-rich ^261-263No isotopes

NUCLEAR REACTIONS ²⁰⁸Pb(⁴⁸Ca, X), E*=10-45 MeV; ²⁴⁴Pu(¹⁸O, X), (²²O, 4n), E*=30-70 MeV; calculated capture σ(E*). Compared with experimental data for ²⁰⁸Pb+⁴⁸Ca. ²⁴⁴Pu(¹⁸O, 3n), (¹⁸O, 4n), (¹⁸O, 5n), ²⁴⁴Pu(²²O, 3n), (²²O, 4n), (²²O, 5n), E*(CN)=20-80 MeV; calculated survival probabilities. ²⁰⁸Pb(⁴⁸Ca, n), (⁴⁸Ca, 2n), (⁴⁸Ca, 3n), (⁴⁸Ca, 4n), E*(CN)=10-55 MeV; ^228,230Th(²⁶Mg, 3n), (²⁶Mg, 4n), (²⁶Mg, 5n), E*(CN)=35-75 MeV; ^242,244Pu(¹⁸O, 3n), (¹⁸O, 4n), (¹⁸O, 5n), (²²O, 3n), (²²O, 4n), (²²O, 5n), E*(CN)=30-80 MeV; calculated σ(E). ²²⁸Th(²⁶Mg, 5n)²⁴⁹No, E=164.9 MeV; ²⁰⁴Pb(⁴⁸Ca, 2n)²⁵⁰No, E=216.7 MeV; ²⁰⁶Pb(⁴⁸Ca, 4n)²⁵⁰No, E=242.2 MeV; ²²⁸Th(²⁶Mg, 4n)²⁵⁰No, E=140.4 MeV; ²⁰⁶Pb(⁴⁸Ca, 3n)²⁵¹No, E=226.2 MeV; ²⁴⁴Cm(¹²C, 5n)²⁵¹No, E=83.0 MeV; ²⁰⁶Pb(⁴⁸Ca, 2n)²⁵²No, E=217.1 MeV; ²³⁰Th(²⁶Mg, 4n)²⁵²No, E=135.8 MeV; ²⁴⁴Cm(¹²C, 4n)²⁵²No, E=73.3 MeV; ²⁰⁶Pb(⁴⁸Ca, n)²⁵³No, E=217.4 MeV; ²⁰⁷Pb(⁴⁸Ca, 2n)²⁵³No, E=216.7 MeV; ²³⁰Th(²⁶Mg, 3n)²⁵³No, E=133.6 MeV; ²⁴⁴Cm(¹³C, 4n)²⁵³No, E=72.8 MeV; ²⁴⁶Cm(¹²C, 5n)²⁵³No, E=83.0 MeV; ²⁰⁸Pb(⁴⁸Ca, 2n)²⁵⁴No, E=216.7 MeV; ²⁴⁴Cm(¹³C, 3n)²⁵⁴No, E=69.8 MeV; ²⁴⁶Cm(¹²C, 4n)²⁵⁴No, E=72.0 MeV; ²⁴⁶Cm(¹³C, 5n)²⁵⁴No, E=78.5 MeV; ²⁴²Pu(¹⁸O, 5n)²⁵⁵No, E=106.8 MeV; ²⁴⁶Cm(¹³C, 4n)²⁵⁵No, E=69.5 MeV; ²⁴⁸Cm(¹²C, 5n)²⁵⁵No, E=77.8 MeV; ²⁴²Pu(¹⁸O, 4n)²⁵⁶No, E=93.9 MeV; ²⁴⁶Cm(¹³C, 3n)²⁵⁶No, E=67.5 MeV; ²⁴⁸Cm(¹²C, 4n)²⁵⁶No, E=71.2 MeV; ²⁴⁸Cm(¹³C, 5n)²⁵⁶No, E=74.8 MeV; ²⁴²Pu(¹⁸O, 3n)²⁵⁷No, E=91.8 MeV; ²⁴⁴Pu(¹⁸O, 5n)²⁵⁷No, E=105.8 MeV; ²⁴⁸Cm(¹²C, 3n)²⁵⁷No, E=69.2 MeV; ²⁴⁸Cm(¹³C, 4n)²⁵⁷No, E=70.5 MeV; ²⁴⁴Pu(¹⁸O, 4n)²⁵⁸No, E=95.0 MeV; ²⁴⁸Cm(¹³C, 3n)²⁵⁸No, E=71.1 MeV; ²⁴²Pu(²²O, 5n)²⁵⁹No, E=106.9 MeV; ²⁴⁴Pu(¹⁸O, 3n)²⁵⁹No, E=90.7 MeV; ²⁴²Pu(²²O, 4n)²⁶⁰No, E=93.8 MeV; ²⁴²Pu(²²O, 3n)²⁶¹No, E=91.6 MeV; ²⁴⁴Pu(²²O, 5n)²⁶¹No, E=100.8 MeV; ²⁴⁴Pu(²²O, 4n)²⁶²No, E=92.1 MeV; ²⁴⁴Pu(²²O, 3n)²⁶³No, E=89.9 MeV; calculated production σ, and compared with experimental data. Dinuclear system (DNS) model for fusion-evaporation (FE) reaction.

doi: 10.1103/PhysRevC.95.054612
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2017PU05 Phys.Rev. C 96, 055203 (2017); Erratum Phys.Rev. C 98, 019907 (2018)

A.J.R.Puckett, E.J.Brash, M.K.Jones, W.Luo, M.Meziane, L.Pentchev, C.F.Perdrisat, V.Punjabi, F.R.Wesselmann, A.Afanasev, A.Ahmidouch, I.Albayrak, K.A.Aniol, J.Arrington, A.Asaturyan, H.Baghdasaryan, F.Benmokhtar, W.Bertozzi, L.Bimbot, P.Bosted, W.Boeglin, C.Butuceanu, P.Carter, S.Chernenko, M.E.Christy, M.Commisso, J.C.Cornejo, S.Covrig, S.Danagoulian, A.Daniel, A.Davidenko, D.Day, S.Dhamija, D.Dutta, R.Ent, S.Frullani, H.Fenker, E.Frlez, F.Garibaldi, D.Gaskell, S.Gilad, R.Gilman, Y.Goncharenko, K.Hafidi, D.Hamilton, D.W.Higinbotham, W.Hinton, T.Horn, B.Hu, J.Huang, G.M.Huber, E.Jensen, C.Keppel, M.Khandaker, P.King, D.Kirillov, M.Kohl, V.Kravtsov, G.Kumbartzki, Y.Li, V.Mamyan, D.J.Margaziotis, A.Marsh, Y.Matulenko, J.Maxwell, G.Mbianda, D.Meekins, Y.Melnik, J.Miller, A.Mkrtchyan, H.Mkrtchyan, B.Moffit, O.Moreno, J.Mulholland, A.Narayan, S.Nedev, Nuruzzaman, E.Piasetzky, W.Pierce, N.M.Piskunov, Y.Prok, R.D.Ransome, D.S.Razin, P.Reimer, J.Reinhold, O.Rondon, M.Shabestari, A.Shahinyan, K.Shestermanov, S.Sirca, I.Sitnik, L.Smykov, G.Smith, L.Solovyev, P.Solvignon, R.Subedi, E.Tomasi-Gustafsson, A.Vasiliev, M.Veilleux, B.B.Wojtsekhowski, S.Wood, Z.Ye, Y.Zanevsky, X.Zhang, Y.Zhang, X.Zheng, L.Zhu

Polarization transfer observables in elastic electron-proton scattering at Q² = 2.5, 5.2, 6.8, and 8.5 GeV²

NUCLEAR REACTIONS ¹H(polarized e, e)p, E<5.717 GeV; measured elastically scattered electrons by a large-solid-angle electromagnetic calorimeter (BigCal) in coincidence with the scattered protons, polarization of recoiling protons by focal plane polarimeter (FPP), proton angular distributions and azimuthal asymmetries, focal-plane helicity difference/sum ratio asymmetry, analyzing powers at JLab's Continuous Electron Beam Accelerator Facility (CEBAF); deduced ratio of the proton's electric and magnetic form factors μ_pG_p^E/G_p^M. Comparison with other experimental data, and with theoretical predictions.

doi: 10.1103/PhysRevC.96.055203
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2017SU23 Phys.Rev. C 96, 024601 (2017)

J.Su, L.Zhu, C.-Y.Huang, W.-J.Xie, F.-S.Zhang

Effects of symmetry energy and effective k-mass splitting on central ⁹⁶Ru(⁹⁶Zr) + ⁹⁶Zr(⁹⁶) collisions at 50 to 400 MeV/nucleon

NUCLEAR REACTIONS ⁹⁶Ru(⁹⁶Zr, X), ⁹⁶Zr(⁹⁶Ru, X), E=50-400 MeV/nucleon; calculated slope and quantum temperatures, np, nn, and pp collisions as a function of time, observable n/p ratio from the free neutrons and protons as a function of rapidity; investigated isospin mixing in central heavy-ion collisions (HICs). Isospin-dependent quantum molecular dynamics model in combination with the statistical decay code GEMINI. Comparison with experimental data from FOPI Collaboration.

doi: 10.1103/PhysRevC.96.024601
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2017WA18 Phys.Lett. B 770, 83 (2017)

F.Wang, B.H.Sun, Z.Liu, R.D.Page, C.Qi, C.Scholey, S.F.Ashley, L.Bianco, I.J.Cullen, I.G.Darby, S.Eeckhaudt, A.B.Garnsworthy, W.Gelletly, M.B.Gomez Hornillos, T.Grahn, P.T.Greenlees, D.G.Jenkins, G.A.Jones, P.Jones, D.T.Joss, R.Julin, S.Juutinen, S.Ketelhut, S.Khan, A.Kishada, M.Leino, M.Niikura, M.Nyman, J.Pakarinen, S.Pietri, Z.Podolyak, P.Rahkila, S.Rigby, J.Saren, T.Shizuma, J.Sorri, S.Steer, J.Thomson, N.J.Thompson, J.Uusitalo, P.M.Walker, S.Williams, H.F.Zhang, W.Q.Zhang, L.H.Zhu

Spectroscopic factor and proton formation probability for the d_3/2 proton emitter ^151mLu

RADIOACTIVITY ¹⁵¹Lu(p) [from ⁹⁶Ru(⁵⁸Ni, X)¹⁵¹Lu, E=266, 274 MeV]; measured decay products, Ep, Ip, Eγ, Iγ; deduced γ-ray energies and intensities, spectroscopic factors, proton-decay formation amplitudes, Q-value, T_1/2. Comparison with theoretical calculations.

doi: 10.1016/j.physletb.2017.04.034
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2017WA32 Phys.Rev. C 96, 034611 (2017)

T.Wang, G.Li, L.Zhu, O.Hen, G.Zhang, Q.Meng, L.Wang, H.Han, H.Xia

Aspects of charge distribution measurement for ²⁵²Cf(sf)

RADIOACTIVITY ²⁵²Cf(SF); measured charge distribution and yields of fission fragments of Z=33-43, charge dispersion of A=101 nuclei ¹⁰¹Y, ¹⁰¹Zr, ¹⁰¹Nb, ¹⁰¹Mo, and ¹⁰¹Tc using grid-ionization chamber (GIC) and a gas ΔE-E detector coupled with a surface-barrier detector; deduced kinetic energy averaged widths as function of atomic mass A, widths of charge distributions, Charge polarization as a function of the mass number of primary fission fragments, average most probable charge as a function of mass number of light fragments. Comparison with theoretical calculations.

doi: 10.1103/PhysRevC.96.034611
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2017WA49 Phys.Rev. C 96, 064307 (2017); Erratum Phys.Rev. C 97, 029902 (2018)

F.Wang, B.H.Sun, Z.Liu, C.Qi, L.H.Zhu, C.Scholey, S.F.Ashley, L.Bianco, I.J.Cullen, I.G.Darby, S.Eeckhaudt, A.B.Garnsworthy, W.Gelletly, M.B.Gomez Hornillos, T.Grahn, P.T.Greenlees, D.G.Jenkins, G.A.Jones, P.Jones, D.T.Joss, R.Julin, S.Juutinen, S.Ketelhut, S.Khan, A.Kishada, M.Leino, M.Niikura, M.Nyman, R.D.Page, J.Pakarinen, S.Pietri, Zs.Podolyak, P.Rahkila, S.Rigby, J.Saren, T.Shizuma, J.Sorri, S.Steer, J.Thomson, N.J.Thompson, J.Uusitalo, P.M.Walker, S.Williams

Reinvestigation of the excited states in the proton emitter ¹⁵¹Lu: Particle-hole excitations across the N=Z=64 subshell

NUCLEAR REACTIONS ⁹⁶Ru(⁵⁸Ni, 2np), E=266, 274 MeV; measured fusion-evaporation residues, Eγ, Iγ, γγ-coin, pγ-coin using RITU separator, GREAT spectrometer and JUROGAM array at the K130 cyclotron facility of the University of Jyvaskyla. Recoil-Decay Tagging (RDT) technique. ¹⁵¹Lu; deduced high-spin levels, J, π, sequences. Comparison with large-scale shell-model calculations.

doi: 10.1103/PhysRevC.96.064307
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2017WE14 J.Phys.(London) G44, 115101 (2017)

P.-w.Wen, C.Li, L.Zhu, C.Lin, F.-s.Zhang

Mechanism of multinucleon transfer reaction based on the GRAZING model and DNS model

NUCLEAR REACTIONS ²⁰⁸Pb(¹³⁶Xe, X), E(cm)=450 MeV; ²³⁸U(⁶⁴Ni, X), E(cm)=307 MeV; calculated isotopic production σ of transfer products using GRAZING model, DNS model and the summation of the GRAZING and DNS models.

doi: 10.1088/1361-6471/aa8b07
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2017YI02 Phys.Rev. C 95, 054913 (2017)

X.Yin, C.M.Ko, Y.Sun, L.Zhu

Elliptic flow of light nuclei

doi: 10.1103/PhysRevC.95.054913
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2017ZH19 Phys.Rev. C 95, 044608 (2017)

L.Zhu, J.Su, P.-W.Wen

Optimal incident energies for production of neutron-deficient actinide nuclei in the reaction ⁵⁸Ni + ²³⁸U

NUCLEAR REACTIONS ²³⁸U(⁵⁸Ni, X)²¹⁶Np/²¹⁷Np/²¹⁸Np/²¹⁹Np/²²²Np/²²⁴Np/²²⁶Np/²²⁸Np/²³⁰Np/²³²Np/²³⁴Np/²³⁶Np/²³⁸Np/²⁴⁰Np, E(cm)=260-400 MeV; calculated production σ(E) for A=216-240 Np isotopes. ^{222,223,224,225,226,227}Pu, ^{224,225,226,227,228,231}Am, ^{228,229,230,231,232}Cm, ^{230,231,232,235,236,237}Bk; predicted optimal incident energies (OPEs) for producing unknown neutron-deficient isotopes with Z=9497 in ⁵⁸Ni+²³⁸U transfer reaction. Dinuclear system model.

doi: 10.1103/PhysRevC.95.044608
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2017ZH21 Nucl.Phys. A964, 93 (2017)

L.Zhu, J.Su, F.-S.Zhang

Theoretical predictions on production of neutron-deficient nuclei with Z ≥ 93 in multinucleon transfer reactions

NUCLEAR REACTIONS ²³³U(⁵⁸Ni, x), E(cm)=1.2, 1.3, 1.4 Coulomb barrier;²³⁸U(⁵⁸Ni, x), (⁶⁴Ni, x), E(cm)=1.3 Coulomb barrier;²⁴⁵Cm(⁴⁰Ca, x), E(cm)=1.2, 1.3, 1.4 Coulomb barrier; calculated production σ of some neutron-deficient actinide isotopes; deduced feasible ways to produce neutron-deficient actinide nuclei in future.

doi: 10.1016/j.nuclphysa.2017.05.063
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2017ZH32 Phys.Rev. C 96, 024606 (2017)

L.Zhu, F.-S.Zhang, P.-W.Wen, J.Su, W.-J.Xie

Production of neutron-rich nuclei with Z=60-73 in reactions induced by Xe isotopes

NUCLEAR REACTIONS ²³⁸U(¹³⁶Xe, X), E(cm)=636 MeV; calculated production σ for A=122-150 Ba, Cs, Te and I isotopes, and compared with experimental data. ²³⁸U(¹²⁴Xe, X), (¹³⁶Xe, X), (¹⁴⁴Xe, X), E(cm)=473-493 MeV; calculated production σ for target-like fragments (TLFs) with A=206-250, Z=88-96 neutron-rich isotopes, PES as functions of Z and N in ¹⁴⁴Xe+²³⁸U reaction, yield distributions of total primary fragments as a function of their N/Z ratio for ¹²⁴Xe+²³⁸U and ¹⁴⁴Xe+²³⁸U reactions. ¹⁶⁰Gd, ¹⁷⁰Er, ¹⁸⁶W(¹³⁶Xe, X), (¹⁴⁴Xe, X), E(cm)=353-406 MeV; calculated production σ for A=140-190, Z=60-73 neutron-rich isotopes. Dinuclear system model.

doi: 10.1103/PhysRevC.96.024606
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2017ZH51 Chin.Phys.C 41, 124102 (2017)

L.Zhu

Theoretical study on production cross sections of exotic actinide nuclei in multinucleon transfer reactions

NUCLEAR REACTIONS ²³⁸U(¹¹²Sn, X), ²⁴⁸Cm(¹³⁶Xe, X), (¹⁴⁴Xe, X)²³⁰Am, E=496, 513 MeV; calculated production σ. Comparison with available data.

doi: 10.1088/1674-1137/41/12/124102
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2016LI05 Phys.Rev. C 93, 014618 (2016)

C.Li, F.Zhang, J.Li, L.Zhu, J.Tian, N.Wang, F.-S.Zhang

Multinucleon transfer in the ¹³⁶Xe + ²⁰⁸Pb reaction

NUCLEAR REACTIONS ²⁰⁸Pb(¹³⁶Xe, X), E(cm)=450 MeV; calculated density distribution contours as function of time, lifetime of the neck, total-kinetic-energy-mass distributions for different impact parameters, TKEL distributions of primary binary fragments, average excitation energy of projectile-like fragments (PLFs) and target-like fragments (TLFs) as a function of neck lifetime, mass distributions of primary binary fragments at different impact parameters, production cross sections for N=110-140, Pt, Au, Hg, Tl, Pb, Bi, Po and At isotopes. Improved quantum molecular dynamics model (ImQMD) for multinucleon transfer reaction using statistical decay code GEMINI. Comparison with prediction of the dinuclear system and GRAZING model, and with available experimental data.

doi: 10.1103/PhysRevC.93.014618
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2016LI12 Phys.Rev.Lett. 116, 112501 (2016)

C.Liu, S.Y.Wang, R.A.Bark, S.Q.Zhang, J.Meng, B.Qi, P.Jones, S.M.Wyngaardt, J.Zhao, C.Xu, S.-G.Zhou, S.Wang, D.P.Sun, L.Liu, Z.Q.Li, N.B.Zhang, H.Jia, X.Q.Li, H.Hua, Q.B.Chen, Z.G.Xiao, H.J.Li, L.H.Zhu, T.D.Bucher, T.Dinoko, J.Easton, K.Juhasz, A.Kamblawe, E.Khaleel, N.Khumalo, E.A.Lawrie, J.J.Lawrie, S.N.T.Majola, S.M.Mullins, S.Murray, J.Ndayishimye, D.Negi, S.P.Noncolela, S.S.Ntshangase, B.M.Nyako, J.N.Orce, P.Papka, J.F.Sharpey-Schafer, O.Shirinda, P.Sithole, M.A.Stankiewicz, M.Wiedeking

Evidence for Octupole Correlations in Multiple Chiral Doublet Bands

NUCLEAR REACTIONS ⁷⁰Zn(¹²C, 3np), E=60, 65 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced energy levels, J, π, medium- amd high-spin states, yrast positive- and negative-parity bands. Comparison with microscopic multidimensionally-constrained covariant density functional theory and triaxial particle rotor model calculations.

doi: 10.1103/PhysRevLett.116.112501
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2016LI41 Phys.Rev. C 94, 024337 (2016)

X.Q.Li, C.Xu, S.Q.Zhang, H.Hua, J.Meng, R.A.Bark, Q.B.Chen, C.Y.Niu, R.Han, S.M.Wyngaardt, S.Y.Wang, S.Wang, B.Qi, L.Liu, L.H.Zhu, Z.Shi, G.L.Zhang, B.H.Sun, X.Y.Le, C.Y.Song, Y.L.Ye, D.X.Jiang, F.R.Xu, Z.H.Li, J.J.Sun, Y.Shi, P.W.Zhao, W.Y.Liang, C.G.Li, C.G.Wang, X.C.Chen, Z.H.Li, D.P.Sun, C.Liu, Z.Q.Li, P.Jones, E.A.Lawrie, J.J.Lawrie, M.Wiedeking, T.D.Bucher, T.Dinoko, B.V.Kheswa, L.Makhathini, S.N.T.Majola, J.Ndayishimye, S.P.Noncolela, O.Shirinda, J.Gal, G.Kalinka, J.Molnar, B.M.Nyako, J.Timar, K.Juhasz, M.Arogunjo

Spectroscopy of ¹⁵⁵Yb: Structure evolution in the N=85 isotones

NUCLEAR REACTIONS ¹⁴⁴Sm(¹⁶O, 5n), E=118 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO ratios) at cyclotron facility of iThemba LABS. ¹⁵⁵Yb; deduced high-spin levels, J, π, multipolarity, bands, configurations; calculated potential energy contour in (β, γ) plane. Comparison with semiempirical shell-model (SESM) calculations. Predicted coexistence of prolate and oblate shapes from adiabatic and configuration-fixed constrained triaxial covariant density functional theory (CDFT) calculations. Systematics of low-lying levels in N=84-87 isotones: ^{148,149,150,151}Gd, ^{150,151,152,153}Dy, ^{152,153,154,155}Er, ^{154,155,156,157}Yb, ^{156,157,158,159}Hf.

doi: 10.1103/PhysRevC.94.024337
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2016SU21 Phys.Rev. C 94, 034619 (2016)

J.Su, L.Zhu, C.-Y.Huang, W.-J.Xie, F.-S.Zhang

Correlation between symmetry energy and effective k-mass splitting with an improved isospin- and momentum-dependent interaction

NUCLEAR REACTIONS ¹²⁴Sn(¹²⁴Sn, X), ¹¹²Sn(¹¹²Sn, X), E=50, 120 MeV/nucleon; analyzed double ratios of the coalescence invariant neutron and proton spectra in central collisions; extracted isospin transport ratios from the yield ratios of A=7 isotopes using IQMD+GEMINI model.

doi: 10.1103/PhysRevC.94.034619
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2016WA03 Phys.Rev. C 93, 014606 (2016)

T.Wang, G.Li, L.Zhu, Q.Meng, L.Wang, H.Han, W.Zhang, H.Xia, L.Hou, R.Vogt, J.Randrup

Correlations of neutron multiplicity and γ-ray multiplicity with fragment mass and total kinetic energy in spontaneous fission of ²⁵²Cf

RADIOACTIVITY ²⁵²Cf(SF); measured E(n), I(n), Eγ, Iγ; deduced total kinetic energy (TKE), neutron and γ-ray multiplicities, correlations of neutron and γ-ray multiplicities, ratio of average γ-ray yield to the average neutron multiplicity as function of fragment mass, γ-ray multiplicity as a function of the total fragment kinetic energy TKE.

doi: 10.1103/PhysRevC.93.014606
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2016ZH23 Phys.Rev. C 93, 064610 (2016)

L.Zhu, J.Su, F.-S.Zhang

Influence of the neutron numbers of projectile and target on the evaporation residue cross sections in hot fusion reactions

NUCLEAR REACTIONS ²³⁸U(³⁴S, 3n)²⁶⁹Hs, ²³⁸U(³⁴S, 4n)²⁶⁸Hs, ²³⁸U(³⁴S, 5n)²⁶⁷Hs, ²³⁸U(³⁶S, 3n)²⁷²Hs, ²³⁸U(³⁶S, 4n)²⁷¹Hs, ²³⁸U(³⁶S, 5n)²⁷⁰Hs, E(cm)=140-210 MeV; ²³⁸Pu(⁴⁸Ca, 3n)²⁸³Fl, ²³⁸Pu(⁴⁸Ca, 4n)²⁸²Fl, ²³⁸Pu(⁴⁸Ca, 5n)²⁸¹Fl, ²³⁹Pu(⁴⁸Ca, 3n)²⁸⁴Fl, ²³⁹Pu(⁴⁸Ca, 4n)²⁸³Fl, ²⁴⁰Pu(⁴⁸Ca, 3n)²⁸⁵Fl, ²⁴⁰Pu(⁴⁸Ca, 4n)²⁸⁴Fl, ²⁴²Pu(⁴⁸Ca, 2n)²⁸⁸Fl, ²⁴²Pu(⁴⁸Ca, 3n)²⁸⁷Fl, ²⁴²Pu(⁴⁸Ca, 4n)²⁸⁶Fl, ²⁴²Pu(⁴⁸Ca, 5n)²⁸⁵Fl, ²⁴⁴Pu(⁴⁸Ca, 3n)²⁸⁹Fl, ²⁴⁴Pu(⁴⁸Ca, 4n)²⁸⁸Fl, ²⁴⁴Pu(⁴⁸Ca, 5n)²⁸⁷Fl, ²⁴⁴Pu(⁴²Ca, 3n)²⁸³Fl, ²⁴⁴Pu(⁴²Ca, 4n)²⁸²Fl, ²⁴⁴Pu(⁴²Ca, 5n)²⁸¹Fl, ²⁴⁴Pu(⁴³Ca, 3n)²⁸⁴Fl, ²⁴⁴Pu(⁴³Ca, 4n)²⁸³Fl, ²⁴⁴Pu(⁴³Ca, 5n)²⁸²Fl, ²⁴⁴Pu(⁴⁴Ca, 3n)²⁸⁵Fl, ²⁴⁴Pu(⁴⁴Ca, 4n)²⁸⁴Fl, ²⁴⁴Pu(⁴⁴Ca, 5n)²⁸³Fl, ²⁴⁴Pu(⁴⁶Ca, 3n)²⁸⁷Fl, ²⁴⁴Pu(⁴⁶Ca, 4n)²⁸⁶Fl, ²⁴⁴Pu(⁴⁶Ca, 5n)²⁸⁵Fl, ²³⁸U(⁴⁴Ca, 3n)²⁷⁹Cn, ²³⁸U(⁴⁴Ca, 4n)²⁷⁸Cn, ²³⁸U(⁴⁴Ca, 5n)²⁷⁷Cn, ²⁴²Pu(⁴⁴Ca, 3n)²⁸³Fl, ²⁴²Pu(⁴⁴Ca, 4n)²⁸²Fl, ²⁴²Pu(⁴⁴Ca, 5n)²⁸¹Fl, ²⁴⁸Cm(⁴⁴Ca, 3n)²⁸⁹Lv, ²⁴⁸Cm(⁴⁴Ca, 4n)²⁸⁸Lv, ²⁴⁸Cm(⁴⁴Ca, 5n)²⁸⁷Lv, ²³⁸U(⁴⁶Ca, 3n)²⁸¹Cn, ²³⁸U(⁴⁶Ca, 4n)²⁸⁰Cn, ²³⁸U(⁴⁶Ca, 5n)²⁷⁹Cn, ²³⁷Np(⁴⁶Ca, 3n)²⁸⁰Nh, ²³⁷Np(⁴⁶Ca, 4n)²⁷⁹Nh, ²³⁷Np(⁴⁶Ca, 5n)²⁷⁸Nh, ²³⁹Pu(⁴⁶Ca, 3n)²⁸²Fl, ²³⁹Pu(⁴⁶Ca, 4n)²⁸¹Fl, ²³⁹Pu(⁴⁶Ca, 5n)²⁸⁰Fl, ²⁴⁰Pu(⁴⁶Ca, 3n)²⁸³Fl, ²⁴⁰Pu(⁴⁶Ca, 4n)²⁸²Fl, ²⁴⁰Pu(⁴⁶Ca, 5n)²⁸¹Fl, ²⁴¹Am(⁴⁶Ca, 3n)²⁸⁴Mc, ²⁴¹Am(⁴⁶Ca, 4n)²⁸³Mc, ²⁴¹Am(⁴⁶Ca, 5n)²⁸²Mc, ²⁴³Am(⁴⁶Ca, 3n)²⁸⁶Mc, ²⁴³Am(⁴⁶Ca, 4n)²⁸⁵Mc, ²⁴³Am(⁴⁶Ca, 5n)²⁸⁴Mc, ²⁴³Cm(⁴⁶Ca, 3n)²⁸⁶Lv, ²⁴³Cm(⁴⁶Ca, 4n)²⁸⁵Lv, ²⁴³Cm(⁴⁶Ca, 5n)²⁸⁴Lv, ²⁴⁵Cm(⁴⁶Ca, 3n)²⁸⁸Lv, ²⁴⁵Cm(⁴⁶Ca, 4n)²⁸⁷Lv, ²⁴⁵Cm(⁴⁶Ca, 5n)²⁸⁶Lv, ²³⁵U(⁴⁸Ca, 3n)²⁸⁰Cn, ²³⁵U(⁴⁸Ca, 4n)²⁷⁹Cn, ²³⁵U(⁴⁸Ca, 5n)²⁷⁸Cn, ²⁴¹Am(⁴⁸Ca, 3n)²⁸⁶Mc, ²⁴¹Am(⁴⁸Ca, 4n)²⁸⁵Mc, ²⁴¹Am(⁴⁸Ca, 5n)²⁸⁴Mc, ²⁴³Cm(⁴⁸Ca, 3n)²⁸⁹Lv, ²⁴³Cm(⁴⁸Ca, 4n)²⁸⁸Lv, ²⁴³Cm(⁴⁸Ca, 5n)²⁸⁷Lv; Calculated evaporation residues (ER) cross sections for superheavy elements, and compared with available experimental data. Maximum cross sections deduced for ²⁴³Cm(⁴⁶Ca, 3n)²⁸⁸Lv, E(cm)=200.7 MeV, ²⁴¹Am(⁴⁸Ca, 4n)²⁸⁵Mc, E(cm)=210.5 MeV, ²⁴⁸Cm(⁴⁴Ca, 4n)²⁸⁸Lv, E(cm)=201.7 MeV, and ²³⁸Pu(⁴⁸Ca, 4n)²⁸²Fl, E(cm)=208.7 MeV. Dinuclear system model.

doi: 10.1103/PhysRevC.93.064610
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2016ZH48 Phys.Rev. C 94, 054606 (2016)

L.Zhu, J.Su, W.-J.Xie, F.-S.Zhang

Production of neutron-rich transcalifornium nuclei in ²³⁸U-induced transfer reactions

NUCLEAR REACTIONS ²⁴⁸Cm(²³⁸U, X), E(cm)=800 MeV; calculated production σ for A=248-254 Es, Fm and Md isotopes, and compared with experimental data. ^248,250Cm, ²⁴⁹Cf, (²³⁸U, X), E(cm)=1.1(V_CN=interaction potential at the touching point); calculated production σ for A=245-270 Es, Fm, Md, No, Lr and Rf isotopes. Dinuclear system (DNS) model.

doi: 10.1103/PhysRevC.94.054606
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2016ZH50 Chin.Phys.C 40, 124105 (2016)

L.Zhu, J.Su, C.-Y.Huang, F.-S.Zhang

Effects of entrance channel on fusion probability in hot fusion reactions

NUCLEAR REACTIONS ²⁴⁸Cm(²⁶Mg, X)²⁷⁴Hs, ²³⁸U(³⁶S, X)²⁷⁴Hs, ²²⁶Ra(⁴⁸Ca, X)²⁷⁴Hs, E<60 MeV/nucleon; ²³⁸U(⁴⁸Ca, X)²⁸⁶Cn, ²³⁴U(⁵²Ca, X)²⁸⁶Cn, ²³¹Pa(⁵⁵Sc, X)²⁸⁶Cn, E<60 MeV/nucleon; analyzed available data; calculated fusion probability as a function of dinuclear system excitation energy. Comparison with available data.

doi: 10.1088/1674-1137/40/12/124105
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2015CH24 Phys.Rev. C 91, 044303 (2015)

Z.Q.Chen, S.Y.Wang, L.Liu, P.Zhang, H.Jia, B.Qi, S.Wang, D.P.Sun, C.Liu, Z.Q.Li, X.G.Wu, G.S.Li, C.Y.He, Y.Zheng, L.H.Zhu

High-spin states and possible "stapler'" band in ¹¹⁵In

NUCLEAR REACTIONS ¹¹⁴Cd(⁷Li, 2nα), E=48 MeV; measured Eγ, Iγ, γγ-coin, angular distribution (ADO) ratios of γ rays using HI-13 tandem accelerator at CIAE-Beijing facility. ¹¹⁵In; deduced levels, J, π, dipole bands, multipolarity, configuration, alignment plot, oblate band built on the stapler mechanism. Comparison with tilted axis cranking model based on covariant density functional theory (TAC-CDFT) calculations.

doi: 10.1103/PhysRevC.91.044303
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2015FA06 Hyperfine Interactions 230, 155 (2015)

P.Fan, H.Zhang, D.Yuan, Y.Zheng, Y.Zuo, Q.Zhang, X.Ma, X.Wu, G.Li, L.Zhu, Q.Fan, J.Liang, X.Zhang, S.Zhu

g-factor measurements of high spin states in ¹⁰⁸Cd

NUCLEAR REACTIONS ⁷⁶Ge(³⁷Cl, 4np), E=135 MeV; measured reaction products, Eγ, Iγ; deduced energy levels, J, π, g-factors. Comparison with theoretical calculations.

doi: 10.1007/s10751-015-1123-2
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2015XU09 Phys.Rev. C 91, 061303 (2015)

C.Xu, X.Q.Li, J.Meng, S.Q.Zhang, H.Hua, S.Y.Wang, B.Qi, C.Liu, Z.G.Xiao, H.J.Li, L.H.Zhu, Z.Shi, Z.H.Li, Y.L.Ye, D.X.Jiang, J.J.Sun, Z.H.Zhang, Y.Shi, P.W.Zhao, Q.B.Chen, W.Y.Liang, R.Han, C.Y.Niu, C.G.Li, C.G.Wang, Z.H.Li, S.M.Wyngaardt, R.A.Bark, P.Papka, T.D.Bucher, A.Kamblawe, E.Khaleel, N.Khumalo, E.A.Lawrie, J.J.Lawrie, P.Jones, S.M.Mullins, S.Murray, M.Wiedeking, J.F.Sharpey-Schafer, S.N.T.Majola, J.Ndayishimye, D.Negi, S.P.Noncolela, S.S.Ntshangase, O.Shirinda, P.Sithole, M.A.Stankiewicz, J.N.Orce, T.Dinoko, J.Easton, B.M.Nyako, K.Juhasz

Spectroscopy of ⁷⁶Se: Prolate-to-oblate shape transition

NUCLEAR REACTIONS ⁷⁰Zn(¹²C, 2nα), E=60, 65 MeV; measured Eγ, Iγ, γγ-, (particle)γγ-coin using AFRODITE array for γ rays and DIAMANT array for charged particles at iThemba LABS. ⁷⁶Se; deduced high-spin levels, J, π, bands, configuration, kinematic and dynamic moments of inertia, band crossing frequency, shape transition. Comparison with cranked shell-model calculations. systematics of band crossings in ^{70,72,74,76,78,80}Se, ^{72,74,76,78,80,82}Kr.

doi: 10.1103/PhysRevC.91.061303
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2015XU15 Sci. Rep. 5, 18350 (2015)

L.-Q.Xu, Y.-W.Liu, X.Kang, D.-D.Ni, K.Yang, No.Hiraoka, K.-D.Tsuei, L.-F.Zhu

The realization of the dipole (γ, γ) method and its application to determine the absolute optical oscillator strengths of helium

NUCLEAR REACTIONS He(γ, γ), E<100 eV; measured reaction products; deduced absolute dipole oscillator strengths, absolute optical oscillator strength (OOS). Comparison with available data. The Taiwan beamline BL12XU of SPring-8.

doi: 10.1038/srep18350
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2015ZH06 Phys.Rev. C 91, 034617 (2015)

F.Zhang, C.Li, L.Zhu, H.Liu, F.-S.Zhang

Effect of fragment emission time on the temperature of momentum quadrupole fluctuations

doi: 10.1103/PhysRevC.91.034617
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2015ZH17 J.Phys.(London) G42, 085102 (2015)

L.Zhu, Z.Q.Feng, F.-S.Zhang

Production of heavy neutron-rich nuclei in transfer reactions within the dinuclear system model

NUCLEAR REACTIONS ²⁰⁸Pb(¹³⁶Xe, X)²¹⁰Po/²²²Rn/²²⁴Ra, E(cm)=514 MeV; ²⁰⁸Pb(⁵⁸Ni, X), E(cm)=256.8 MeV; ²⁴⁸Cm(²³⁸U, X)Es/Fm/Md, E(cm)=800 MeV; ²³⁸U(¹⁷⁶Yb, X)Eu/Yb/Ho, E(cm)=600 MeV; calculated σ. Comparison with experimental data.

doi: 10.1088/0954-3899/42/8/085102
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2015ZH46 Phys.Rev. C 92, 064911 (2015)

L.Zhu, C.Ko, X.Yin

Light (anti-)nuclei production and flow in relativistic heavy-ion collisions

doi: 10.1103/PhysRevC.92.064911
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2014KA30 Phys.Rev.Lett. 113, 022502 (2014)

J.Katich, X.Qian, Y.X.Zhao, K.Allada, K.Aniol, J.R.M.Annand, T.Averett, F.Benmokhtar, W.Bertozzi, P.C.Bradshaw, P.Bosted, A.Camsonne, M.Canan, G.D.Cates, C.Chen, J.-P.Chen, W.Chen, K.Chirapatpimol, E.Chudakov, E.Cisbani, J.C.Cornejo, F.Cusanno, M.M.Dalton, W.Deconinck, C.W.de Jager, R.De Leo, X.Deng, A.Deur, H.Ding, P.A.M.Dolph, C.Dutta, D.Dutta, L.El Fassi, S.Frullani, H.Gao, F.Garibaldi, D.Gaskell, S.Gilad, R.Gilman, O.Glamazdin, S.Golge, L.Guo, D.Hamilton, O.Hansen, D.W.Higinbotham, T.Holmstrom, J.Huang, M.Huang, H.F.Ibrahim, M.Iodice, X.Jiang, G.Jin, M.K.Jones, A.Kelleher, W.Kim, A.Kolarkar, W.Korsch, J.J.LeRose, X.Li, Y.Li, R.Lindgren, N.Liyanage, E.Long, H.-J.Lu, D.J.Margaziotis, P.Markowitz, S.Marrone, D.McNulty, Z.-E.Meziani, R.Michaels, B.Moffit, C.Munoz Camacho, S.Nanda, A.Narayan, V.Nelyubin, B.Norum, Y.Oh, M.Osipenko, D.Parno, J.C.Peng, S.K.Phillips, M.Posik, A.J.R.Puckett, Y.Qiang, A.Rakhman, R.D.Ransome, S.Riordan, A.Saha, B.Sawatzky, E.Schulte, A.Shahinyan, M.H.Shabestari, S.Sirca, S.Stepanyan, R.Subedi, V.Sulkosky, L.-G.Tang, A.Tobias, G.M.Urciuoli, I.Vilardi, K.Wang, Y.Wang, B.Wojtsekhowski, X.Yan, H.Yao, Y.Ye, Z.Ye, L.Yuan, X.Zhan, Y.Zhang, Y.-W.Zhang, B.Zhao, X.Zheng, L.Zhu, X.Zhu, X.Zong

Measurement of the Target-Normal Single-Spin Asymmetry in Deep-Inelastic Scattering from the Reaction ³He ↑ (e, e')X

doi: 10.1103/PhysRevLett.113.022502
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2014MO25 J.Phys.(London) G41, 105109 (2014)

P.Monaghan, R.Shneor, R.Subedi, B.D.Anderson, K.Aniol, J.Annand, J.Arrington, H.B.Benaoum, F.Benmokhtar, P.Bertin, W.Bertozzi, W.Boeglin, J.P.Chen, S.Choi, E.Chudakov, C.Ciofi degli Atti, E.Cisbani, W.Cosyn, B.Craver, C.W.de Jager, R.J.Feuerbach, E.Folts, S.Frullani, F.Garibaldi, O.Gayou, S.Gilad, R.Gilman, O.Glamazdin, J.Gomez, O.Hansen, D.W.Higinbotham, T.Holmstrom, H.Ibrahim, R.Igarashi, E.Jans, X.Jiang, L.Kaufman, A.Kelleher, A.Kolarkar, E.Kuchina, G.Kumbartzki, J.J.LeRose, R.Lindgren, N.Liyanage, D.J.Margaziotis, P.Markowitz, S.Marrone, M.Mazouz, D.Meekins, R.Michaels, B.Moffit, H.Morita, S.Nanda, C.F.Perdrisat, E.Piasetzky, M.Potokar, V.Punjabi, Y.Qiang, J.Reinhold, B.Reitz, G.Ron, G.Rosner, J.Ryckebusch, A.Saha, B.Sawatzky, J.Segal, A.Shahinyan, S.Sirca, K.Slifer, P.Solvignon, V.Sulkosky, N.Thompson, P.E.Ulmer, G.M.Urciuoli, E.Voutier, K.Wang, J.W.Watson, L.B.Weinstein, B.Wojtsekhowski, S.Wood, H.Yao, X.Zheng, L.Zhu

Measurement of the ¹²C(e, e'p)¹¹B two-body breakup reaction at high missing momentum

NUCLEAR REACTIONS ¹²C(E, E'P), E200-400 MeV; measured reaction products, Ep, Ip; deduced σ(θ, E). Comparison with WS+Glauber calculations.

doi: 10.1088/0954-3899/41/10/105109
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2014YA02 Phys.Rev. C 89, 014327 (2014)

S.H.Yao, H.L.Ma, L.H.Zhu, X.G.Wu, C.Y.He, Y.Zheng, B.Zhang, G.S.Li, C.B.Li, S.P.Hu, X.P.Cao, B.B.Yu, C.Xu, Y.Y.Cheng

Lifetime measurements and magnetic rotation in ¹⁰⁷Ag

NUCLEAR REACTIONS ¹⁰⁰Mo(¹¹B, 4n)¹⁰⁷Ag, E=46 MeV; measured Eγ, Iγ, γγ-coin, level half-lives by DSAM at HI-13-CIAE tandem accelerator facility. ¹⁰⁷Ag; deduced high spin levels, J, π, magnetic dipole rotational bands, B(M1), B(E2), configuration. Systematics of angular momentum versus rotational frequency plots in ^103,105Rh, ^105,107,109Ag, ^111,113In. Comparison with predictions of particle rotor model. Discussed evolution of magnetic rotation mechanism in A AP 110 mass region.

doi: 10.1103/PhysRevC.89.014327
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Note: The following list of authors and aliases matches the search parameter L.Zhu: , L.C.ZHU, L.F.ZHU, L.H.ZHU, L.L.ZHU, L.P.ZHU, L.Q.ZHU, L.Y.ZHU