NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = W.Zuo Found 174 matches. Showing 1 to 100. [Next]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
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
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
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
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
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
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
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
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
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
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
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-/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
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
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
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
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
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
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
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
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
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
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
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
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
2019FA02 Phys.Rev. C 99, 041601 (2019) 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
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
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
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
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
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
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
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
2018DO09 Phys.Atomic Nuclei 81, 283 (2018) 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
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
2018FA03 Phys.Rev. C 97, 034604 (2018) 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
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
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
2018WA23 J.Phys.(London) G45, 105102 (2018) 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
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
2018YI05 Chin.Phys.C 42, 114102 (2018) Effect of tensor correlations on the depletion of nuclear Fermi sea within the extended BHF approach
doi: 10.1088/1674-1137/41/11/114102
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
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
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
2017YI06 Chin.Phys.C 41, 114102 (2017) Effect of tensor correlations on the depletion of nuclear Fermi sea within the extended BHF approach
doi: 10.1088/1674-1137/41/11/114102
2016DO08 Chin.Phys.Lett. 33, 102101 (2016) 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
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
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
2015DO02 Phys.Rev. C 91, 034315 (2015) 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
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-/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-/π+. Isospin-dependent Boltzmann-Uehling-Uhlenbeck (IBUU) transport model.
doi: 10.1103/PhysRevC.91.054616
2015GU23 Phys.Rev. C 92, 054619 (2015) Effect of Δ potential on the π-/π+ ratio in heavy-ion collisions at intermediate energies
doi: 10.1103/PhysRevC.92.054619
2015LI08 Phys.Rev. C 91, 035803 (2015) Massive hybrid stars with a first-order phase transition
doi: 10.1103/PhysRevC.91.035803
2014FA03 Phys.Rev. C 89, 017305 (2014) Density-dependent symmetry energy at subsaturation densities from nuclear mass differences
doi: 10.1103/PhysRevC.89.017305
2014GU22 Phys.Rev. C 90, 044605 (2014) 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-/π+ production ratios; deduced effects of in-medium NN cross section and the effects of symmetry energy on the π-/π+ ratio. Isospin-dependent Boltzmann-Uehling-Uhlenbeck (IBUU04) transport model.
doi: 10.1103/PhysRevC.90.044605
2014HU03 Phys.Rev. C 89, 025802 (2014) Extended quark mean-field model for neutron stars
doi: 10.1103/PhysRevC.89.025802
2014WA18 Phys.Rev. C 89, 054319 (2014) Three-body force effect on the neutron and proton spectral functions in asymmetric nuclear matter
doi: 10.1103/PhysRevC.89.054319
2014WA33 Chin.Phys.C 38, 084102 (2014) 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
2014ZU02 Eur.Phys.J. A 50, 12 (2014) Three-body force effect on nuclear symmetry energy and single-particle properties of asymmetric nuclear matter
doi: 10.1140/epja/i2014-14001-6
2013DO01 Phys.Rev. C 87, 014303 (2013) 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
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
2013DO13 Phys.Rev. C 87, 062801 (2013) 3PF2 pairing in high-density neutron matter
doi: 10.1103/PhysRevC.87.062801
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
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
2013LI54 Phys.Rev. C 88, 057303 (2013) 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
2013SH33 Phys.Rev. C 88, 025806 (2013) Angle-dependent gap state in asymmetric nuclear matter
doi: 10.1103/PhysRevC.88.025806
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
2013YI01 Phys.Rev. C 87, 014314 (2013) 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
2013YI04 Phys.Rev. C 88, 015804 (2013) 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
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
2012GA13 Chin.Phys.Lett. 29, 042102 (2012) Nucleon Effective Mass in Asymmetric Nuclear Matter within Extended Brueckner Approach
doi: 10.1088/0256-307X/29/4/042102
2012GA23 Chin.Phys.C 36, 513 (2012) Nucleon effective mass in symmetric nuclear matter from the extended Brueckner-Hartree-Fock approach
doi: 10.1088/1674-1137/36/6/006
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-/π+ ratios from mirror reaction systems NUCLEAR REACTIONS 22O, 22Si(22Na, X), E=400 MeV/nucleon; calculated central baryon density, nuclear symmetry energy, π-/π+ ratios, kinetic energy distribution of the double π-/π+ ratio. Isospin and momentum-dependent hadronic transport model IBUU.
doi: 10.1103/PhysRevC.86.034611
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
2012LI07 Chin.Phys.Lett. 29, 012102 (2012) Single-Particle Properties of Isospin Asymmetric Nuclear Matter
doi: 10.1088/0256-307X/29/1/012102
2012LI19 Phys.Rev. C 85, 037001 (2012) Isospin and temperature dependence of the rearrangement term in Brueckner theory
doi: 10.1103/PhysRevC.85.037001
2012LI25 Chin.Phys.Lett. 29, 062104 (2012) Symmetry Potential and Effective Mass with Consistent Three-Body Force
doi: 10.1088/0256-307X/29/6/062104
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
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
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+/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
2012ZU04 Chin.Phys.C 36, 967 (2012) Single particle potentials of asymmetric nuclear matter in different spin-isospin channels
doi: 10.1088/1674-1137/36/10/009
2011DO10 Nucl.Phys. A861, 1 (2011) 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
2011DO11 Phys.Rev.Lett. 107, 012501 (2011) 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
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
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
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-/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
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
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
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
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
2010XI06 Nucl.Phys. A848, 317 (2010) A mixing scheme for the structure of f0(600) and f0(1370)
doi: 10.1016/j.nuclphysa.2010.09.010
2010ZH25 Phys.Rev. C 82, 015805 (2010) Transport parameters in neutron stars from in-medium NN cross sections
doi: 10.1103/PhysRevC.82.015805
2010ZU04 Nucl.Phys. A834, 574c (2010) EOS and Single Particle Properties of Asymmetric Nuclear Matter
doi: 10.1016/j.nuclphysa.2010.01.095
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
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
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
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
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
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
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
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
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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