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NSR database version of April 11, 2024.

Search: Author = W.Zuo

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2023LI03      Phys.Rev. C 107, 014302 (2023)

H.H.Li, Q.Yuan, J.G.Li, M.R.Xie, S.Zhang, Y.H.Zhang, X.X.Xu, N.Michel, F.R.Xu, W.Zuo

Investigation of isospin-symmetry breaking in mirror energy difference and nuclear mass with ab initio calculations

NUCLEAR STRUCTURE 21,23Al, 23Ne, 21,22O, 22,23Si, 23F, 27P, 27Mg, 46Ti, 46V, 46Cr; calculated levels, J, π. 18,19Ne, 19Na, 20,21Na, 22,23,24,25Al, 27Si, 29S, 33Ar; calculated mirror energy difference in the mirror nuclei states. A=17-75; calculated coefficient "b" of the isobaric multiplet mass equation. Ab initio valence-space in-medium similarity renormalization group (VS-IMSRG) method. Comparison to experimental data and AME2020.

doi: 10.1103/PhysRevC.107.014302
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2023LI55      Phys.Lett. B 846, 138197 (2023)

J.G.Li, H.H.Li, S.Zhang, Y.M.Xing, W.Zuo

Double-magicity of proton drip-line nucleus 22Si with ab initio calculation

NUCLEAR STRUCTURE 22O, 22Si, 26Si, 26Mg, 24Si, 24Ne; calculated energy levels, the mirror energy difference (MED). 22Si, 22O; deduced double magic nuclei using ab initio valence space in-medium similarity renormalization group.

doi: 10.1016/j.physletb.2023.138197
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2023LI61      Chin.Phys.C 47, 124101 (2023)

H.-H.Li, J.-G.Li, M.-R.Xie, W.Zuo

Ab initio calculations of mirror energy difference in sd-shell nuclei

NUCLEAR STRUCTURE 21,22,23,24Al, 21O, 22F, 23Ne, 24Na, 19Na, 19O, 20Mg, 20O; calculated energy levels, J, π using the ab initio VS-IMSRG method. Comparison with experimental data.

doi: 10.1088/1674-1137/acf035
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2023YI06      Phys.Rev. C 108, 034002 (2023)

P.Yin, X.L.Shang, J.N.Hu, J.Y.Fu, E.Epelbaum, W.Zuo

Pairing properties of semilocal coordinate- and momentum-space regularized chiral interactions

doi: 10.1103/PhysRevC.108.034002
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2022HA32      Phys.Rev. C 106, 064332 (2022)

S.C.Han, X.L.Shang, W.Zuo, G.C.Yong, Y.Gao

In-medium nucleon-nucleon cross section in nuclear matter

NUCLEAR REACTIONS 1H(p, X), (n, X), 1NN(n, X), E=40-420 MeV; calculated σ(E) and medium correction factors in nuclear matter with various densities and isospin asymmetries. 124Sn(132Sn, X), E=270 MeV/nucleon; calculated proton and neutron transverse and elliptic flows. Calculations in the framework of the Brueckner-Hartree-Fock approach.

doi: 10.1103/PhysRevC.106.064332
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2022LI37      Phys.Lett. B 832, 137225 (2022)

J.G.Li, N.Michel, H.H.Li, W.Zuo

One-neutron halo structure of 29Ne

NUCLEAR STRUCTURE 26,27,28,29,30,31Ne; calculated neutron rms radii, valence-nucleon densities. 29,31Ne; deduced one-neutron halo character. The multiconfigurational approach GSM.

doi: 10.1016/j.physletb.2022.137225
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2022MI10      Phys.Rev. C 106, L011301 (2022)

N.Michel, J.G.Li, L.H.Ru, W.Zuo

Calculation of the Thomas-Ehrman shift in 16F and 15O(p, p) cross sections within the Gamow shell model

NUCLEAR STRUCTURE 16F, 16N; calculated low-lying levels, J, π. Gamow shell model (GSM) and Gamow shell model with coupled-channels (GSM-CC) calculations. Observed Thomas-Ehrman shift caused by special role played by the proton s1/2 partial wave in 16F. Comparison to experimental data.

NUCLEAR REACTIONS 15O(p, p'), E=0.5-1.25 MeV; calculated σ(θ). Gamow shell model with coupled-channels (GSM-CC) calculations using effective Hamiltonian, consisting of a 12C core and valence nucleons interacting with an effective nuclear interaction.

doi: 10.1103/PhysRevC.106.L011301
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2022YI05      J.Phys.(London) G49, 125102 (2022)

P.Yin, W.Du, W.Zuo, X.Zhao, J.P.Vary

Sub Coulomb barrier d+208Pb scattering in the time-dependent basis function approach

NUCLEAR REACTIONS 208Pb(d, d), E=3-7 MeV; calculated σ using the non-perturbative time-dependent basis function (tBF) approach; deduced the higher-order inelastic scattering effects are noticeable for sub barrier scatterings with the tBF method.

doi: 10.1088/1361-6471/ac79c3
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2022ZE02      Phys.Rev. C 106, 034307 (2022)

Q.B.Zeng, S.Guo, Z.Liu, J.G.Li, H.H.Li, J.G.Wang, Z.Y.Zhang, L.Ma, Y.H.Qiang, M.H.Huang, G.S.Li, Y.D.Fang, M.L.Liu, B.Ding, Y.Zheng, J.H.Li, H.Y.Lu, W.Q.Zhang, K.L.Wang, X.Y.Liu, H.Huang, F.F.Zeng, X.H.Yu, A.Rohilla, J.F.Huang, H.L.Fan, C.Qi, C.X.Yuan, C.M.Petrache, E.A.Lawrie, W.Zuo, Z.G.Gan, X.H.Zhou

Configurations of the low-lying states in 146Eu

RADIOACTIVITY 146mEu(IT) [from 124Sn(27Al, 5n), E=127 MeV, followed by mass-separation of evaporation residues (ERs) using the SHANS separator at the Sector-Focusing Cyclotron (SFC) of HIRFL-Lanzhou]; measured Eγ, Iγ, γγ-coin, isomer and level T1/2 by γ(t) and γγ(t) fast-timing method using three LaBr3(Ce) detectors, one coaxial and one Clover HPGe detectors, and analyzed using mirror symmetric centroid difference (MSCD) method. 146Eu; deduced levels, J, π, T1/2 of 6- levels and a 9+ isomer, multipolarities, upper limits of multipole mixing ratios, B(M1), spherical configurations. 146Sm; measured level T1/2 of the first 2+ state as a test case for measurements of short half-lives for levels in 146Eu. Comparison with shell model calculations using several different effective interactions, and with previous experimental results. Systematics of levels and B(M1) values in N=83 isotones 142Pr, 144Pm, 146Eu.

doi: 10.1103/PhysRevC.106.034307
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2021CH17      Phys.Rev. C 103, L031302 (2021)

J.Chen, S.M.Wang, H.T.Fortune, J.L.Lou, Y.L.Ye, Z.H.Li, N.Michel, J.G.Li, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, D.Y.Pang, F.R.Xu, W.Zuo, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, N.Aoi, H.J.Ong, E.Ideguchi, Y.Ayyad, K.Hatanaka, D.T.Tran, D.Bazin, J.Lee, Y.N.Zhang, J.Wu, H.N.Liu, C.Wen, T.Yamamoto, M.Tanaka, T.Suzuki

Observation of the near-threshold intruder 0- resonance in 12Be

NUCLEAR REACTIONS 2H(11Be, p)12Be, E=26.9 MeV/nucleon; measured E(p), I(p), σ(θ) using two parallel-plate avalanche counters (PPACs), and a set of annular double-sided silicon detectors (ADSSDs) at the RCNP, Osaka University. 12Be; deduced missing-mass spectra of 12Be unbound states, levels, J, π, a 0- resonance just above S(n), decay width. DWBA analysis. Comparison with Gamow coupled-channel and Gamow shell-model calculations.

doi: 10.1103/PhysRevC.103.L031302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2690. Data from this article have been entered in the XUNDL database. For more information, click here.

2021DO01      Phys.Lett. B 813, 136063 (2021)

J.M.Dong, Q.Zhao, L.J.Wang, W.Zuo, J.Z.Gu

α-Cluster formation in heavy α-emitters within a multistep model

RADIOACTIVITY 202,204,206,208,210,212,214,216,218Po, 204,206,208,210,212,214,216,218,220Rn, 206,208,210,212,214,216,218,220,222Ra(α); calculated formation probability values, contour plots within a multistep model.

doi: 10.1016/j.physletb.2021.136063
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2021GA32      Phys.Rev. C 104, 044607 (2021)

Y.Gao, Y.L.Guo, L.Zhang, G.C.Yong, Z.Y.Liu, W.Zuo

Pion production and absorption in heavy-ion collisions

NUCLEAR REACTIONS 197Au(197Au, X), E=400 MeV/nucleon; calculated local density distributions and time evolutions of inelastic reactions in central collision, fraction of the different types of free pions, average density and time at which a pion gets produced, π-+ ratio versus different types of free pions, average scattering number in the history of the free pions as a function of the kinetic energy and polar angle, dependence of the ratios of the charged pions emitted on kinetic energy in a direction closed to the beam direction. Isospin-dependent Boltzmann-Uehling-Uhlenbeck (IBUU) transport model for pion production and absorption in inelastic collisions.

doi: 10.1103/PhysRevC.104.044607
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2021LI19      Phys.Rev. C 103, 034305 (2021)

J.G.Li, N.Michel, W.Zuo, F.R.Xu

Unbound spectra of neutron-rich oxygen isotopes predicted by the Gamow shell model

NUCLEAR STRUCTURE 24,25,26,27,28O; calculated energies of ground states. 18,19,20,21,22,23,24,25,26,27,28O; calculated densities. 23,24,25,26O; calculated levels, resonances, J, π with 22O used as core. 25,26,27O; deduced ground states as resonances, thus unbound character. Gamow shell model (GSM) with Hamiltonian from effective field theory (EFT) for nuclei at neutron dripline and beyond. Comparison with experimental data.

doi: 10.1103/PhysRevC.103.034305
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2021LI29      Phys.Rev. C 103, 064324 (2021)

J.G.Li, N.Michel, W.Zuo, F.R.Xu

Reexamining the variational two-particle reduced density matrix for nuclear systems

NUCLEAR STRUCTURE 6,8He, 8Be, 20,22,24,26O, 20Ne, 24Mg, 28Si, 32S; calculated binding energies and normalized occupations of neutrons and protons using nuclear variational two-particle reduced density matrix (2RDM) method; deduced higher binding energies for nuclear systems with active valence neutrons and protons; discussed possible reasons for discrepancies and solutions. Comparison with available experimental data.

doi: 10.1103/PhysRevC.103.064324
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2021LI42      Phys.Rev. C 104, 024319 (2021)

J.G.Li, N.Michel, W.Zuo, F.R.Xu

Resonances of A=4 T=1 isospin triplet states within the ab initio no-core Gamow shell model

NUCLEAR STRUCTURE 3,4H, 3,4He, 4Li; calculated levels, resonances, widths using ab-initio no-core Gamow shell model (NCGSM) with various modern realistic nuclear forces. Comparison with experimental data.

doi: 10.1103/PhysRevC.104.024319
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2021LI62      Phys.Rev. C 104, L061306 (2021)

H.H.Li, J.G.Li, N.Michel, W.Zuo

Investigation of unbound hydrogen isotopes with the Gamow shell model

NUCLEAR STRUCTURE 4,5,6,7H; calculated level energies, J, π, neutron-emission widths using Gamow shell model (GSM), with the FHT, MN1, and MN2 interactions. Comparison with experimental results for level energies and widths from various experiments.

doi: 10.1103/PhysRevC.104.L061306
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2021MI10      Phys.Rev. C 103, 044319 (2021)

N.Michel, J.G.Li, F.R.Xu, W.Zuo

Proton decays in 16Ne and 18Mg and isospin-symmetry breaking in carbon isotopes and isotones

NUCLEAR STRUCTURE 15,16,17,18C, 15F, 16Ne, 17Na, 18Mg; calculated levels, J, π, widths, binding energies of carbon isotopes and isotones. 16Ne, 18Mg; calculated one-proton and two-proton decay widths. Gamow shell model (GSM) for proton-rich nuclei. Comparison with available experimental data.

doi: 10.1103/PhysRevC.103.044319
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2021SH15      Phys.Rev. C 103, 034316 (2021)

X.-L.Shang, J.-M.Dong, W.Zuo, P.Yin, U.Lombardo

Exact solution of the Brueckner-Bethe-Goldstone equation with three-body forces in nuclear matter

doi: 10.1103/PhysRevC.103.034316
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2021YA07      Phys.Rev.Lett. 126, 082501 (2021)

Z.H.Yang, Y.Kubota, A.Corsi, K.Yoshida, X.-X.Sun, J.G.Li, M.Kimura, N.Michel, K.Ogata, C.X.Yuan, Q.Yuan, G.Authelet, H.Baba, C.Caesar, D.Calvet, A.Delbart, M.Dozono, J.Feng, F.Flavigny, J.-M.Gheller, J.Gibelin, A.Giganon, A.Gillibert, K.Hasegawa, T.Isobe, Y.Kanaya, S.Kawakami, D.Kim, Y.Kiyokawa, M.Kobayashi, N.Kobayashi, T.Kobayashi, Y.Kondo, Z.Korkulu, S.Koyama, V.Lapoux, Y.Maeda, F.M.Marques, T.Motobayashi, T.Miyazaki, T.Nakamura, N.Nakatsuka, Y.Nishio, A.Obertelli, A.Ohkura, N.A.Orr, S.Ota, H.Otsu, T.Ozaki, V.Panin, S.Paschalis, E.C.Pollacco, S.Reichert, J.-Y.Rousse, A.T.Saito, S.Sakaguchi, M.Sako, C.Santamaria, M.Sasano, H.Sato, M.Shikata, Y.Shimizu, Y.Shindo, L.Stuhl, T.Sumikama, Y.L.Sun, M.Tabata, Y.Togano, J.Tsubota, F.R.Xu, J.Yasuda, K.Yoneda, J.Zenihiro, S.-G.Zhou, W.Zuo, T.Uesaka

Quasifree Neutron Knockout Reaction Reveals a Small s-Orbital Component in the Borromean Nucleus 17B

NUCLEAR REACTIONS 1H(17B, np)16B, E ∼ 277 MeV/nucleon; measured reaction products, Eγ, Iγ. 17B; deduced energy levels, partial σ and spectroscopic parameters, resonance widths. Comparison with GSM, VS-IMSRG, AMD, SM calculations. MINOS target, RIKEN Nishina Center.

doi: 10.1103/PhysRevLett.126.082501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2689.

2020CH07      Phys.Rev. C 101, 024610 (2020)

P.-H.Chen, F.Niu, W.Zuo, Z.-Q.Feng

Approaching the neutron-rich heavy and superheavy nuclei by multinucleon transfer reactions with radioactive isotopes

NUCLEAR REACTIONS 238U(124Sn, X), E=6.0 MeV/nucleon; calculated mass distribution of total kinetic energy of the primary binary fragments, potential energy surface in (N, Z) plane. 238U, 248Cm(238U, X), E=7.0 MeV/nucleon; calculated production cross sections of transcurium isotopes (Z=97-101, A=240-260), and compared with experimental data from GSI. 238U(124Sn, X), E=5.6, 6.0, 6.5 MeV/nucleon; calculated differential σ(θ) of Sn-like and U-like products. 238U, 248Cm(124Sn, X), (132Sn, X), E=6 MeV/nucleon; calculated production cross sections as functions of neutron and proton numbers of primary fragments and secondary fragments, production cross sections of Z=88-91, A=210-250, Z=93-96, A=226-260, Z=101-104, A=250-270, N=82, Z=74-90, N=126, Z=74-90, N=160-164, Z=87-98, N=150-154, Z=87-98, and Z=60-104, A=162-269 and above. Dinuclear system (DNS) model for production of neutron-rich isotopes via the multi-nucleon transfer (MNT) reactions.

doi: 10.1103/PhysRevC.101.024610
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2020MI04      Phys.Rev. C 101, 031301 (2020)

N.Michel, J.G.Li, F.R.Xu, W.Zuo

Two-neutron halo structure of 31F

NUCLEAR STRUCTURE 25,26,27,28,29,30,31F; calculated binding energies of neutron drip-line fluorine isotopes using Gamow-shell model, Hartree-Fock many-body perturbation theory method (HF-MBPT), and valence-space in-medium similarity renormalization-group (VS-IMSRG) frameworks, with comparison to values in AME2016. 27,29,31F; calculated neutron densities, rms radii, and correlation densities using Gamow-shell model, Berggren basis, effective field theory, and effective Hamiltonians. Discussed two-neutron halo structure of 31F.

doi: 10.1103/PhysRevC.101.031301
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2020SU02      Phys.Lett. B 800, 135096 (2020)

M.D.Sun, Z.Liu, T.H.Huang, W.Q.Zhang, A.N.Andreyev, B.Ding, J.G.Wang, X.Y.Liu, H.Y.Lu, D.S.Hou, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, Z.H.Li, J.Li, X.Wang, A.H.Feng, C.J.Lin, L.J.Sun, N.R.Ma, W.Zuo, H.S.Xu, X.H.Zhou, G.Q.Xiao, C.Qi, F.S.Zhang

Fine structure in the α decay of 223U

RADIOACTIVITY 223U, 219Th, 215Ra(α) [from 187Re(40Ar, 3np), E=188 MeV]; measured reaction products, Eα, Iα; deduced α-decay branches, fine structure.

doi: 10.1016/j.physletb.2019.135096
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Data from this article have been entered in the XUNDL database. For more information, click here.

2019DO01      Phys.Rev. C 99, 014319 (2019)

J.M.Dong, J.Z.Gu, Y.H.Zhang, W.Zuo, L.J.Wang, Yu.A.Litvinov, Y.Sun

Beyond Wigner's isobaric multiplet mass equation: Effect of charge-symmetry-breaking interaction and Coulomb polarization

NUCLEAR STRUCTURE A=13, 15, 17, 19, 21, 23, 25, 27, 29, 31, 33, 35, 37, 39, 41, 43, 45, 47, 49, 51, 53, 55, 57, 59, 61; calculated coefficient of the added cubic term to the isobaric multiplet mass equation (IMME) for T=3/2 isobaric quartets, and density differences between neutron and proton for A=37 and 43 isobaric doublets. A=12, 16, 20, 24, 28, 32, 36; calculated coefficients of the added cubic and quartic terms to the isobaric multiplet mass equation (IMME) for T=2 isobaric quintets. Deduced general deviation from the original IMME, and the magnitude of the deviation exhibiting an oscillation-like behavior with mass number, modulated by the shell effect. Comparison with available experimental values.

doi: 10.1103/PhysRevC.99.014319
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2019DO03      Nucl.Phys. A983, 133 (2019)

J.M.Dong, X.L.Shang, W.Zuo, Y.F.Niu, Y.Sun

An effective Coulomb interaction in nuclear energy density functionals

doi: 10.1016/j.nuclphysa.2019.01.003
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2019FA02      Phys.Rev. C 99, 041601 (2019)

X.-H.Fan, G.-C.Yong, W.Zuo

Probing nuclear bubble configurations by proton-induced reactions

NUCLEAR REACTIONS 48Si(p, p'), E=0.8 GeV/nucleon; calculated proton and neutron densities in 48Si g.s., intensity of scattered protons as a function of kinetic energy and scattering angle, with and without a nuclear bubble configuration in 48Si using isospin-dependent Boltzmann-Uehling-Uhlenbeck (BUU) transport model. Relevance to probe potential bubble nuclei in future proton-induced nuclear reaction experiments.

doi: 10.1103/PhysRevC.99.041601
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2019FA03      Phys.Rev. C 99, 065804 (2019)

X.-H.Fan, X.-l.Shang, J.-M.Dong, W.Zuo

Neutron-proton pairing in nuclear matter

doi: 10.1103/PhysRevC.99.065804
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2019GU09      Nucl.Phys. A986, 18 (2019)

W.Guo, J.M.Dong, X.Shang, H.F.Zhang, W.Zuo, M.Colonna, U.Lombardo

Proton-proton 1S0 pairing in neutron stars

doi: 10.1016/j.nuclphysa.2019.02.008
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2019LI50      Phys.Rev. C 100, 054313 (2019)

J.G.Li, N.Michel, B.S.Hu, W.Zuo, F.R.Xu

Ab initio no-core Gamow shell-model calculations of multineutron systems

NUCLEAR STRUCTURE 3,4n; calculated resonances, energies and widths using the ab-initio no-core Gamow shell model based on nuclear chiral effective field theory interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.054313
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2019MI21      Phys.Rev. C 100, 064303 (2019)

N.Michel, J.G.Li, F.R.Xu, W.Zuo

Description of proton-rich nuclei in the A ≈ 20 region within the Gamow shell model

NUCLEAR STRUCTURE 17F, 18Ne, 19Na, 20Mg, 21Al, 22Si; calculated levels, J, π, proton-emission widths, binding energies, Hamiltonian Coulomb contributions of the ground and excited states of 16O isotones with respect to the 16O core using Gamow shell model (GSM) with the EFT and/or FHT interaction. Comparison with experimental data.

NUCLEAR REACTIONS 18Ne(p, p), E(cm)=0.5-2.5 MeV; calculated differential σ(E) using Gamow shell model and resonating group method (GSM-RGM) with the A-dependent EFT interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.064303
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2019YA23      Phys.Rev. C 100, 054325 (2019)

Z.X.Yang, X.L.Shang, G.C.Yong, W.Zuo, Y.Gao

Nucleon momentum distributions in asymmetric nuclear matter

doi: 10.1103/PhysRevC.100.054325
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2018DO02      Phys.Rev. C 97, 021301 (2018)

J.M.Dong, Y.H.Zhang, W.Zuo, J.Z.Gu, L.J.Wang, Y.Sun

Generalized isobaric multiplet mass equation and its application to the Nolen-Schiffer anomaly

ATOMIC MASSES 20O, 53Ni, 208Pb; calculated first-order symmetry energy coefficient for charge symmetry breaking (CSB) and second-order charge-independent breaking (CIB) components using SLy4, SLy5 and KBD interactions. Derived a generalized isobaric mass multiplet equation (GIMME), and applied to the study of Nolen-Schiffer anomaly (NSA) in the Coulomb displacement energy of mirror nuclei. A=10-60; calculated contributions of the CSB and CIB effects to coefficients of Tz and Tz2 using SLy4 interaction. 15O, 15N; 17F, 17O; 39Ca, 39K; 41Sc, 41Ca; calculated ΔNSA for T=1/2 mirror pairs due to CSB effects using SLy4, SLy5 and KBD interactions. A=18-42; calculated Coulomb displacement energy (CDE) of the T=1 mirror pairs using SLy4 interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.97.021301
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2018DO04      Phys.Rev. C 97, 034318 (2018)

J.M.Dong, L.J.Wang, W.Zuo, J.Z.Gu

Constraints on Coulomb energy, neutron skin thickness in 208Pb, and symmetry energy

NUCLEAR STRUCTURE 208Pb; calculated neutron skin thickness, density-dependent symmetry energy coefficient of nuclear matter by constraining the Coulomb energy with the mirror nuclei. A=17-65; calculated Coulomb displacement energies (CDEs) for T=1/2 mirror pairs, and compared with experimental data. 48Ca, 68Ni, 132Sn, 208Pb, 298Fl; calculated symmetry energy using self-consistent Skyrme-Hartree-Fock approach with SLy4 interaction. Discussed charge-symmetry-breaking (CSB) effect.

doi: 10.1103/PhysRevC.97.034318
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2018DO09      Phys.Atomic Nuclei 81, 283 (2018)

J.M.Dong, W.Zuo, J.Z.Gu

The Fourth-Order Symmetry Energy of Finite Nuclei

NUCLEAR STRUCTURE 208Pb; compiled published calculations of Fourth-Order Symmetry Energy using a large set of Skyrme interactions.

doi: 10.1134/S1063778818030109
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2018DU05      Phys.Rev. C 97, 064620 (2018)

W.Du, P.Yin, Y.Li, G.Chen, W.Zuo, X.Zhao, J.P.Vary

Coulomb excitation of the deuteron in peripheral collisions with a heavy ion

NUCLEAR REACTIONS U(d, d'), E=4.7, 19.4, 85.5 MeV/nucleon; calculated low and intermediate energy Coulomb excitations of uranium, internal charge distributions of 2H target before, during and after scattering, rms charge radii, rms momentum and rms orbital angular momentum, intrinsic energy of 2H during scattering using ab-initio nonperturbative, time-dependent basis function (tBF) method with JISP16 nucleon-nucleon interaction. Discussed excitation mechanism and dynamics.

doi: 10.1103/PhysRevC.97.064620
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2018FA03      Phys.Rev. C 97, 034604 (2018)

X.-H.Fan, G.-C.Yong, W.Zuo

Probing the density dependence of the symmetry energy by nucleon flow

NUCLEAR REACTIONS 124Sn(132Sn, X), E=0.3-0.6 GeV/nucleon; 197Au(197Au, X), E=0.6 GeV/nucleon; analyzed relative sensitivity of the symmetry-energy-sensitive observable free neutron to proton ratio n/p, relative sensitivity of neutron and proton elliptic flows as a function of transverse momentum, relative sensitivity of the difference between neutron transverse flow and proton transverse flow as a function of rapidity. Isospin-dependent BUU transport model for studies of nucleon observables sensitive to the nuclear symmetry energy.

doi: 10.1103/PhysRevC.97.034604
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2018GA03      Phys.Rev. C 97, 014609 (2018)

Y.Gao, G.-C.Yong, L.Zhang, W.Zuo

Influence of the nuclear symmetry energy on the collective flows of charged pions

doi: 10.1103/PhysRevC.97.014609
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2018HU13      Phys.Rev. C 98, 044302 (2018)

T.H.Huang, W.Q.Zhang, M.D.Sun, Z.Liu, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, Z.H.Li, J.Li, X.Wang, H.Y.Lu, A.H.Feng, C.J.Lin, L.J.Sun, N.R.Ma, D.X.Wang, F.S.Zhang, W.Zuo, X.H.Zhou, H.S.Xu, G.Q.Xiao

Identification of the new isotope 224Np

NUCLEAR REACTIONS 187Re(40Ar, 3n)224Np, E=188 MeV; measured evaporation residues (ERs), Eα, Iα of decaying ERs, production σ using SHANS separator and a double-sided silicon strip detector for α detection at SFC-HIRFL, Lanzhou; deduced evidence for the production of new isotope 224Np through the observation of six correlated α-decay chains, starting from 224Np to 212Fr.

RADIOACTIVITY 224Np, 220Pa, 220mPa, 216Ac(α)[from 187Re(40Ar, 3n)224Np, E=188 MeV, and successive α decays]; measured Eα, Iα, half-lives, αα-correlations. 220Pa, 216Ac, 212Fr; deduced levels, isomer in 220Pa.

doi: 10.1103/PhysRevC.98.044302
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2018WA23      J.Phys.(London) G45, 105102 (2018)

P.Wang, P.Yin, X.Shang, W.Zuo

Proton spectral functions in finite nuclei based on the extended Brueckner-Hartree-Fock approach

NUCLEAR STRUCTURE 12C, 27Al, 56Fe, 197Au; calculated radial density and asymmetry distributions, proton spectral function as a function of missing energy.

doi: 10.1088/1361-6471/aad8f5
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2018YA15      Phys.Rev. C 98, 014623 (2018)

Z.-X.Yang, X.-H.Fan, G.-C.Yong, W.Zuo

Effects of the initialization of nucleon momentum in heavy-ion collisions at medium energies

NUCLEAR REACTIONS 197Au(197Au, X), E=400 MeV/nucleon; calculated neutron and proton momentum distribution, free neutron to proton ratio, π- and π+ yields, nucleon transverse flow as function of rapidity, and nucleon elliptic flow as function of transverse momentum; deduced effects of effects of the difference of high momentum tails (HMTs) of nucleon momentum distribution. Isospin-dependent transport model Boltzmann-Uehling-Uhlenbeck (IBUU).

doi: 10.1103/PhysRevC.98.014623
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2018YI05      Chin.Phys.C 42, 114102 (2018)

P.Yin, J.Dong, W.Zuo

Effect of tensor correlations on the depletion of nuclear Fermi sea within the extended BHF approach

doi: 10.1088/1674-1137/41/11/114102
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2018ZH11      Appl.Radiat.Isot. 135, 92 (2018)

Q.Zhang, S.Li, L.Zhuang, Y.Huo, H.Lin, W.Zuo

Simulation study on neutron multiplicity of plutonium based on liquid scintillation detector

doi: 10.1016/j.apradiso.2018.01.022
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2017SU18      Phys.Lett. B 771, 303 (2017)

M.D.Sun, Z.Liu, T.H.Huang, W.Q.Zhang, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, Z.H.Li, J.Li, X.Wang, H.Y.Lu, C.J.Lin, L.J.Sun, N.R.Ma, C.X.Yuan, W.Zuo, H.S.Xu, X.H.Zhou, G.Q.Xiao, C.Qi, F.S.Zhang

New short-lived isotope 223Np and the absence of the Z = 92 subshell closure near N = 126

RADIOACTIVITY 223Np, 219Pa, 219Th, 218Ac, 216Ra, 215Ac(α) [from 187Re(40Ar, X)223Np, E=188 MeV]; measured decay products, Eα, Iα; deduced T1/2, Q-values, disprove the existence of a Z=92 subshell closure. Comparison with available data.

doi: 10.1016/j.physletb.2017.03.074
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2017YI01      Nucl.Phys. A961, 200 (2017)

P.Yin, X.Fan, J.Dong, W.Guo, W.Zuo

Model-dependence of neutrino emissivities and neutrino luminosities of neutron stars from the direct Urca processes and the modified Urca processes

doi: 10.1016/j.nuclphysa.2017.03.001
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2017YI06      Chin.Phys.C 41, 114102 (2017)

P.Yin, J.Dong, W.Zuo

Effect of tensor correlations on the depletion of nuclear Fermi sea within the extended BHF approach

doi: 10.1088/1674-1137/41/11/114102
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2016DO08      Chin.Phys.Lett. 33, 102101 (2016)

J.-M.Dong, W.Zuo, J.-Z.Gu

First-Order Symmetry Energy Induced by Neutron-Proton Mass Difference

NUCLEAR STRUCTURE 208Pb; calculated symmetry energy. Skyrme energy density functionals.

doi: 10.1088/0256-307X/33/10/102101
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2016LI06      Phys.Rev. C 93, 015803 (2016); Publisher's Note: Phys.Rev. C 102, 019907 (2020)

A.Li, J.N.Hu, X.L.Shang, W.Zuo

Nonrelativistic nucleon effective masses in nuclear matter: Brueckner-Hartree-Fock model versus relativistic Hartree-Fock model

doi: 10.1103/PhysRevC.93.015803
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2016YU04      Phys.Lett. B 762, 237 (2016)

C.Yuan, Z.Liu, F.Xu, P.M.Walker, Zs.Podolyak, C.Xu, Z.Z.Ren, B.Ding, M.L.Liu, X.Y.Liu, H.S.Xu, Y.H.Zhang, X.H.Zhou, W.Zuo

Isomerism in the "south-east" of 132Sn and a predicted neutron-decaying isomer in 129Pd

NUCLEAR STRUCTURE 134,136,138Sn, 130Cd, 128Pd, 135Sn, 131Cd, 129Pd, 132,134In, 130Ag; calculated energy levels, B(E2) values, one-neutron separation energies, J, π, T1/2. Comparison with available data.

doi: 10.1016/j.physletb.2016.09.030
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2015DO02      Phys.Rev. C 91, 034315 (2015)

J.Dong, W.Zuo, J.Gu

Constraints on neutron skin thickness in 208Pb and density-dependent symmetry energy

NUCLEAR STRUCTURE 208Pb; calculated neutron skin thickness and density dependence of symmetry energy based on a high linear correlation between skin thickness and the symmetry energy coefficient of nuclear matter at saturation density. Discussed measurement issues of skin thickness using novel Pb radius experiment (PREX).

doi: 10.1103/PhysRevC.91.034315
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2015GU08      Phys.Rev. C 91, 054616 (2015)

W.-M.Guo, G.-C.Yong, H.Liu, W.Zuo

Effects of pion potential and nuclear symmetry energy on the π-+ ratio in heavy-ion collisions at beam energies around the pion production threshold

NUCLEAR REACTIONS 197Au(197Au, X), E=200, 400 MeV/nucleon; calculated density- and momentum-dependent pion potentials, isoscalar and isovector potentials of pions, momentum distribution of π meson, effect of pion potential and symmetry energy on charged pion ratio π-+. Isospin-dependent Boltzmann-Uehling-Uhlenbeck (IBUU) transport model.

doi: 10.1103/PhysRevC.91.054616
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2015GU23      Phys.Rev. C 92, 054619 (2015)

W.-M.Guo, G.-C.Yong, W.Zuo

Effect of Δ potential on the π-+ ratio in heavy-ion collisions at intermediate energies

doi: 10.1103/PhysRevC.92.054619
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2015LI08      Phys.Rev. C 91, 035803 (2015)

A.Li, W.Zuo, G.X.Peng

Massive hybrid stars with a first-order phase transition

doi: 10.1103/PhysRevC.91.035803
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2014FA03      Phys.Rev. C 89, 017305 (2014)

X.Fan, J.Dong, W.Zuo

Density-dependent symmetry energy at subsaturation densities from nuclear mass differences

doi: 10.1103/PhysRevC.89.017305
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2014GU22      Phys.Rev. C 90, 044605 (2014)

W.-M.Guo, G.-C.Yong, W.Zuo

Effects of nuclear symmetry energy and in-medium NN cross section in heavy-ion collisions at beam energies below the pion production threshold

NUCLEAR REACTIONS 132Sn(124Sn, X), E=100, 150, 200, 250, 300 MeV/nucleon; 100Sn(100Sn, X), 128Pm(128Pm, X), E=100 MeV/nucleon; calculated maximal baryon densities, π-+ production ratios; deduced effects of in-medium NN cross section and the effects of symmetry energy on the π-+ ratio. Isospin-dependent Boltzmann-Uehling-Uhlenbeck (IBUU04) transport model.

doi: 10.1103/PhysRevC.90.044605
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2014HU03      Phys.Rev. C 89, 025802 (2014)

J.N.Hu, A.Li, H.Toki, W.Zuo

Extended quark mean-field model for neutron stars

doi: 10.1103/PhysRevC.89.025802
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2014WA18      Phys.Rev. C 89, 054319 (2014)

P.Wang, W.Zuo

Three-body force effect on the neutron and proton spectral functions in asymmetric nuclear matter

doi: 10.1103/PhysRevC.89.054319
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2014WA33      Chin.Phys.C 38, 084102 (2014)

P.Wang, W.Zuo

Three-body force effect on the properties of nuclear matter under the gap and continuous choices within the BHF approach

doi: 10.1088/1674-1137/38/8/084102
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2014ZU02      Eur.Phys.J. A 50, 12 (2014)

W.Zuo, I.Bombaci, U.Lombardo

Three-body force effect on nuclear symmetry energy and single-particle properties of asymmetric nuclear matter

doi: 10.1140/epja/i2014-14001-6
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2013DO01      Phys.Rev. C 87, 014303 (2013)

J.Dong, W.Zuo, J.Gu

Origin of symmetry energy in finite nuclei and density dependence of nuclear matter symmetry energy from measured α-decay energies

NUCLEAR STRUCTURE 208Pb; symmetry energy distribution, isospin asymmetry distribution function, polarizations of neutron and proton densities using the Skyrme-energy density functional and Hartree-Fock approach; deduced neutron skin thickness from experimental α-energies, and compared with other methods.

doi: 10.1103/PhysRevC.87.014303
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2013DO02      Nucl.Phys. A898, 32 (2013)

J.Dong, U.Lombardo, W.Zuo, H.Zhang

Dense nuclear matter and symmetry energy in strong magnetic fields

doi: 10.1016/j.nuclphysa.2012.11.011
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2013DO13      Phys.Rev. C 87, 062801 (2013)

J.M.Dong, U.Lombardo, W.Zuo

3PF2 pairing in high-density neutron matter

doi: 10.1103/PhysRevC.87.062801
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2013DO15      Phys.Rev. C 88, 014302 (2013)

J.Dong, H.Zhang, L.Wang, W.Zuo

Density dependence of the symmetry energy probed by β--decay energies of odd-A nuclei

NUCLEAR STRUCTURE 208Pb; analyzed symmetry energy coefficient from experimental Q(β-) values; deduced slope parameter of symmetry energy and compared with previous studies, density dependence of nuclear matter symmetry energy, neutron skin thickness.

doi: 10.1103/PhysRevC.88.014302
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2013GA46      Phys.Rev. C 88, 057601 (2013)

Y.Gao, G.C.Yong, Y.Wang, Q.Li, W.Zuo

Influence of the symmetry energy on the cone-azimuthal emission

doi: 10.1103/PhysRevC.88.057601
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2013LI54      Phys.Rev. C 88, 057303 (2013)

Z.Li, B.Sun, C.H.Shen, W.Zuo

Calculation of α-decay energies of superheavy nuclei in a hybrid method

RADIOACTIVITY 279Ds, 279,280,282Rg, 283,285Cn, 282,283,284,285,286Nh, 286,287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294Og(α); calculated α decay Q values using various mass models. Sinusoid-like periodic deviation when compared with experimental values. Prediction of unknown Q values by hybrid approach.

doi: 10.1103/PhysRevC.88.057303
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2013SH33      Phys.Rev. C 88, 025806 (2013)

X.-l.Shang, W.Zuo

Angle-dependent gap state in asymmetric nuclear matter

doi: 10.1103/PhysRevC.88.025806
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2013WA03      Phys.Rev. C 87, 014328 (2013)

P.Wang, S.-X.Gan, P.Yin, W.Zuo

Three-body force effect on off-shell mass operator and spectral functions in nuclear matter

doi: 10.1103/PhysRevC.87.014328
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2013YI01      Phys.Rev. C 87, 014314 (2013)

P.Yin, J.-Y.Li, P.Wang, W.Zuo

Three-body force effect on nucleon momentum distributions in asymmetric nuclear matter within the framework of the extended Brueckner-Hartree-Fock approach

doi: 10.1103/PhysRevC.87.014314
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2013YI04      Phys.Rev. C 88, 015804 (2013)

P.Yin, W.Zuo

Three-body force effect on neutrino emissivities of neutron stars within the framework of the Brueckner-Hartree-Fock approach

doi: 10.1103/PhysRevC.88.015804
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2012DO02      Phys.Rev. C 85, 034308 (2012)

J.Dong, W.Zuo, J.Gu, U.Lombardo

Density dependence of the nuclear symmetry energy constrained by mean-field calculations

NUCLEAR STRUCTURE 208Pb; calculated neutron skin thickness relation to saturation density, slope parameter, curvature parameter, properties of neutron stars, based on mean-field interactions. Comparison with previous studies.

doi: 10.1103/PhysRevC.85.034308
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2012GA13      Chin.Phys.Lett. 29, 042102 (2012)

S.-X.Gan, W.Zuo, U.Lombardo

Nucleon Effective Mass in Asymmetric Nuclear Matter within Extended Brueckner Approach

doi: 10.1088/0256-307X/29/4/042102
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2012GA23      Chin.Phys.C 36, 513 (2012)

S.-X.Gan, W.Zuo, U.Lombardo

Nucleon effective mass in symmetric nuclear matter from the extended Brueckner-Hartree-Fock approach

doi: 10.1088/1674-1137/36/6/006
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2012GA37      Phys.Rev. C 86, 034611 (2012)

Y.Gao, L.Zhang, W.Zuo, J.-Q.Li

Probing the nuclear symmetry energy using single and double π-+ ratios from mirror reaction systems

NUCLEAR REACTIONS 22O, 22Si(22Na, X), E=400 MeV/nucleon; calculated central baryon density, nuclear symmetry energy, π-+ ratios, kinetic energy distribution of the double π-+ ratio. Isospin and momentum-dependent hadronic transport model IBUU.

doi: 10.1103/PhysRevC.86.034611
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2012LI06      Chin.Phys.Lett. 29, 012101 (2012)

Z-H.Li, D.-P.Zhang, H.-J.Schulze, W.Zuo

Second-Order Contribution of the Incompressibility in Asymmetric Nuclear Matter

doi: 10.1088/0256-307X/29/1/012101
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2012LI07      Chin.Phys.Lett. 29, 012102 (2012)

Z.-H.Li, W.Zuo, W.-J.Guo

Single-Particle Properties of Isospin Asymmetric Nuclear Matter

doi: 10.1088/0256-307X/29/1/012102
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2012LI19      Phys.Rev. C 85, 037001 (2012)

Z.H.Li, W.Zuo

Isospin and temperature dependence of the rearrangement term in Brueckner theory

doi: 10.1103/PhysRevC.85.037001
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2012LI25      Chin.Phys.Lett. 29, 062104 (2012)

Z.-H.Li, W.Zuo

Symmetry Potential and Effective Mass with Consistent Three-Body Force

doi: 10.1088/0256-307X/29/6/062104
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2012YO02      Phys.Rev. C 85, 024911 (2012)

G.-C.Yong, X.Chen, H.-S.Xu, W.Zuo

Pion production by protons and 3He on a 197Au target at beam energies of 2.8, 5, 10, and 16.587 GeV/nucleon

doi: 10.1103/PhysRevC.85.024911
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2012ZH15      Chin.Phys.Lett. 29, 052501 (2012)

F.Zhang, B.-T.Hu, G.-C.Yong, W.Zuo

Effects of Symmetry Energy in the Reaction 40Ca+124Sn at 140 MeV/Nucleon

NUCLEAR REACTIONS 124Sn(40Ca, X), E=140 MeV/nucleon; calculated symmetry energy, baryon density, longitudinal momentum, σ(θ), neutron to proton ratios. Boltzmann-Uehling-Uhlenbeck transport model, comparison with available data.

doi: 10.1088/0256-307X/29/5/052501
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2012ZH16      Chin.Phys.Lett. 29, 052502 (2012)

F.Zhang, Y.Liu, G.-C.Yong, W.Zuo

Probing Nuclear Symmetry Energy with the Sub-threshold Pion Production

NUCLEAR REACTIONS 48Ca(48Ca, X)π+-, E=100, 150, 200, 250, 300 MeV/nucleon; calculated density dependence on nuclear symmetry energy, kinetic energy distribution. Boltzmann-Uehling-Uhlenbeck transport model, comparison with available data.

doi: 10.1088/0256-307X/29/5/052502
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2012ZU04      Chin.Phys.C 36, 967 (2012)

W.Zuo, S.-X.Gan, U.Lombardo

Single particle potentials of asymmetric nuclear matter in different spin-isospin channels

doi: 10.1088/1674-1137/36/10/009
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2011DO10      Nucl.Phys. A861, 1 (2011)

J.Dong, W.Zuo, W.Scheid

New approach for alpha decay half-lives of superheavy nuclei and applicability of WKB approximation

RADIOACTIVITY 270,272,274Bh, 274,275,276,278Mt, 278,279,280,282Rg, 283,285Cn, 282,283,284,286Nh, 287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 294Og(α); calculated T1/2, potential barrier, proton-, α- and cluster-penetrability. Comparison with available data.

doi: 10.1016/j.nuclphysa.2011.06.016
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2011DO11      Phys.Rev.Lett. 107, 012501 (2011)

J.Dong, W.Zuo, W.Scheid

Correlation between α-Decay Energies of Superheavy Nuclei Involving the Effects of Symmetry Energy

RADIOACTIVITY 280,282Rg, 283,285Cn, 282,283,284,285,286Nh, 286,297,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294Og(α); calculated Q-values; deduced symmetry dependent formula. Liquid-drop model.

doi: 10.1103/PhysRevLett.107.012501
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2011DO12      Phys.Rev. C 84, 014303 (2011)

J.M.Dong, W.Zuo, J.Z.Gu, Y.Z.Wang, L.G.Cao, X.Z.Zhang

Effects of tensor interaction on pseudospin energy splitting and shell correction

NUCLEAR STRUCTURE 106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn; calculated proton and neutron pseudospin orbit splittings. 132Sn, 298Fl; calculated neutron and proton shell correction energies, single particle spectra. Skyrme-Hartree-Fock approach with the SLy5+TF and T31+TF parameter sets combined with the BCS method.

doi: 10.1103/PhysRevC.84.014303
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2011GA37      Phys.Rev. C 84, 024301 (2011)

D.Gambacurta, L.Li, G.Colo, U.Lombardo, N.Van Giai, W.Zuo

Determination of local energy density functionals from Brueckner-Hartree-Fock calculations

NUCLEAR STRUCTURE 16O, 40Ca, 48Ca, 56Ni, 78Ni, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn, 208Pb; calculated binding energies, charge radii. 208Pb; calculated energies of giant monopole (ISGMR), dipole (IVGDR), quadrupole (ISGQR) and Gamow-Teller resonances. Brueckner-Hartree-Fock approximation, Skyrme parameterization and local energy density functionals. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.024301
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2011YO08      Phys.Rev. C 84, 034609 (2011)

G.-C.Yong, Y.Gao, W.Zuo, X.-C.Zhang

Initialization effect in heavy-ion collisions at intermediate energies

NUCLEAR REACTIONS 40Ca(40Ca, X), 48Ca(48Ca, X), E=400 MeV/nucleon; 197Au(197Au, X), E=200-800 MeV/nucleon; calculated neutron and proton density distributions, neutron to proton, and charged π-+ ratios of preequilibrium nucleon emissions, effect of initialization on different ratios. Boltzmann-Uehling-Uhlenbeck transport model plus the Skyrme force parameters.

doi: 10.1103/PhysRevC.84.034609
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2010DO08      Nucl.Phys. A832, 198 (2010)

J.Dong, H.Zhang, Y.Wang, W.Zuo, J.Li

Alpha-decay for heavy nuclei in the ground and isomeric states

RADIOACTIVITY 154Ho, 154Tm, 155Lu, 156Hf, 157,158,160,161Ta, 158W, 161,162,164Re, 166,167,169,174Ir, 173,176Au, 187Hg, 177,181Tl, 185,187Pb, 186,188,191,193,194,195Bi, 193,195,197,199,201Po, 195,197,198,202,212,214At, 195,197,199,201,203Rn, 200,202,204,206Fr, 205,207Ra, 206,208,216Ac, 216Th, 217Pa, 245Md, 253Lr, 257Db, 263Sg(α); calculated T1/2 using generalized liquid drop model (GLDM) for ground-state and isomers. Comparison with experimental data.

doi: 10.1016/j.nuclphysa.2009.10.082
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2010DO09      Chin.Phys.C 34, 182 (2010)

J.-M.Dong, H.-F.Zhang, W.Zuo, J.-Q.Li

Unified fission model for proton emission

NUCLEAR STRUCTURE 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,176Ir, 171Au, 177Tl, 185Bi; calculated proton radioactivity T1/2 for spherical emitters. Comparison with experimental data.

doi: 10.1088/1674-1137/34/2/005
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2010DO10      Phys.Rev. C 81, 064309 (2010)

J.Dong, W.Zuo, J.Gu, Y.Wang, B.Peng

α-decay half-lives and Qα values of superheavy nuclei

RADIOACTIVITY 271Sg, 270,272,274Bh, 275Hs, 274,275,276,278Mt, 279Ds, 278,279,280,282Rg, 281,283,284,285,287Cn, 281,282,283,284,286,288Nh, 285,286,287,288,289,291Fl, 286,287,288,289,290,292Mc, 289,290,291,292,293,295Lv, 293,294,295Ts, 294,295Og(α); calculated Q(α) and half-lives using Unified Fission Model (UFM). Comparison with experimental data.

doi: 10.1103/PhysRevC.81.064309
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2010WA14      Chin.Phys.Lett. 27, 062103 (2010)

Y.-J.Wang, H.-F.Zhang, W.Zuo, J.-Q.Li

Improvement of a Fission-Like Model for Nuclear α Decay

doi: 10.1088/0256-307X/27/6/062103
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2010XI06      Nucl.Phys. A848, 317 (2010)

Z.-T.Xia, W.Zuo

A mixing scheme for the structure of f0(600) and f0(1370)

doi: 10.1016/j.nuclphysa.2010.09.010
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2010ZH25      Phys.Rev. C 82, 015805 (2010)

H.F.Zhang, U.Lombardo, W.Zuo

Transport parameters in neutron stars from in-medium NN cross sections

doi: 10.1103/PhysRevC.82.015805
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2010ZU04      Nucl.Phys. A834, 574c (2010)


EOS and Single Particle Properties of Asymmetric Nuclear Matter

doi: 10.1016/j.nuclphysa.2010.01.095
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2009DO21      Chin.Phys.C 33, 633 (2009)

J.-M.Dong, H.-F.Zhang, Y-Z.Wang, W.Zuo, X.-N.Su, J.-Q.Li

α-decay half-lives of superheavy nuclei and general predictions

NUCLEAR STRUCTURE Z=105-118; calculated α-decay T1/2. Generalized liquid drop model (GLDM).

doi: 10.1088/1674-1137/33/8/007
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2009GA43      Chin.Phys.C 33, 848 (2009)

Y.Gao, J.-M.Dong, H.-F.Zhang, W.Zuo, J.-Q.Li

Properties and structure of N = Z nuclei within relativistic mean field theory

NUCLEAR STRUCTURE 84Mo; calculated proton and neutron density distributions, single-particle spectra, Fermi energy levels, binding energy, one and two nucleon separation energy, quadrupole deformation, rms radii. Axially deformed RMF.

doi: 10.1088/1674-1137/33/10/006
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2009LI14      Int.J.Mod.Phys. E18, 675 (2009)

J.Y.Liu, W.-J.Guo, W.Zuo, X.G.Lee

Studies for the equation of state in the isospin asymmetrical nuclear interactions

doi: 10.1142/S0218301309012793
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2009LI55      Phys.Rev. C 80, 064607 (2009)

L.L.Li, Z.H.Li, E.G.Zhao, S.G.Zhou, W.Zuo, A.Bonaccorso, U.Lombardo

Isospin splitting of the nucleon-nucleus optical potential

NUCLEAR REACTIONS 28Si, 90Zr, 208Pb(n, n)(p, p), (n, γ), (p, γ), E<100 MeV; calculated volume term of the optical model potential and isospin splitting using the Brueckner-Hartree-Fock approach with three-body force.

doi: 10.1103/PhysRevC.80.064607
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2009WA08      Chin.Phys.Lett. 26, 062101 (2009)

Y-Z.Wang, H.-F.Zhang, J.-M.Dong, X.-N.Su, W.Zuo, J.-Q.Li

Branching Ratios of α Decay for Nuclei near Deformed Shell Closures

RADIOACTIVITY 270Hs(α); Z=102-112; Calculated α-branching. Generalized Liquid Drop Model (GLDM).

doi: 10.1088/0256-307X/26/6/062101
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2009ZH18      Chin.Phys.Lett. 26, 072301 (2009)

H.-F.Zhang, J.-M.Dong, Y.-Z.Wang, X.-N.Su, Y.-J.Wang, L.-Z.Cai, T.-B.Zhu, B.-T.Hu, W.Zuo, J.-Q.Li

Theoretical Analysis and New Formulae for Half-Lives of Proton Emission

NUCLEAR STRUCTURE 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi; calculated proton radioactivity T1/2; deduced formulae for T1/2. comparison with experiment.

doi: 10.1088/0256-307X/26/7/072301
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2009ZH28      Phys.Rev. C 80, 037307 (2009)

H.F.Zhang, J.M.Dong, G.Royer, W.Zuo, J.Q.Li

Preformation of clusters in heavy nuclei and cluster radioactivity

RADIOACTIVITY 212,213,214Po, 215At, 238Pu(α), 221Fr, 221,222,223,224Ra, 225Ac, 226Ra(14C), 228Th(20O), 230U(22Ne), 230Th, 231Pa, 232,233,234U(24Ne), 233U(25Ne), 234U(26Ne), 234U, 236,238Pu(28Mg), 238Pu(30Mg), 238Pu(32Si), 242Cm(34Si); calculated preformation factor P0 of cluster decay. 223Ac, 224,226Th(14C), 223Ac(15N), 224Th(16O), 226Th(16O), 232Th, 236U(24Ne), 232Th(26Ne), 233U(28Mg), 237Np(30Mg), 240Pu, 241Am(34Si); calculated half-lives. 114,115,116,117,118,119Ba, 121La(12C), 114,115,116,117,118Ba, 119,120,121,122,124Ce, 125Pr(16O); calculated half-lives. Preformed cluster approach and generalized liquid drop model (GLDM). Comparison with experimental data.

doi: 10.1103/PhysRevC.80.037307
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2009ZH38      Phys.Rev. C 80, 057301 (2009)

H.F.Zhang, G.Royer, Y.J.Wang, J.M.Dong, W.Zuo, J.Q.Li

Analytic expressions for α particle preformation in heavy nuclei

RADIOACTIVITY N=82-178(α); analyzed α particle preformation factors from experimental Eα and half-lives; deduced analytical expressions for preformation factors.

doi: 10.1103/PhysRevC.80.057301
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2009ZH46      Chin.Phys.C 33, Supplement 1, 95 (2009)

H.-F.Zhang, Z.-K.Wang, X.-M.Cheng, W.Zuo, J.-Q.Li

Alpha decay half-lives of heavy nuclei within a generalized liquid drop model

RADIOACTIVITY 271Sg, 275Hs, 279Ds, 283,285Cn, 286,287,288,289Fl, 290,291,292,293Lv, 294Og, 275,276Mt, 279,280Rg, 283,284Nh, 287,288Mc, 272Bh(α); calculated T1/2 using experimental Q-values. Generalized liquid drop model. Comparison with experimental data.

doi: 10.1088/1674-1137/33/S1/031
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