NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Z.Z.Ren Found 114 matches. Showing 1 to 100. [Next]2024GU03 Phys.Rev. C 109, 014304 (2024) S.T.Guo, Y.X.Yu, Z.Wang, G.J.Fu, Z.Z.Ren Atomic mass relations of mirror nuclei
doi: 10.1103/PhysRevC.109.014304
2024WA04 Phys.Rev. C 109, 014624 (2024) K.Wang, Y.Y.Yang, Jin Lei, A.M.Moro, V.Guimaraes, J.G.Li, F.F.Duan, Z.Y.Sun, G.Yang, D.Y.Pang, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Liu, J.L.Lou, H.J.Ong, B.F.Lv, S.Guo, M.Kumar Raju, X.H.Wang, R.H.Li, X.X.Xu, Z.Z.Ren, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu Elastic scattering and breakup reactions of the mirror nuclei 12B and 12N on 208Pb using ab initio structure inputs
doi: 10.1103/PhysRevC.109.014624
2024WA14 Phys.Lett. B 850, 138503 (2024) J.G.Wang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, H.B.Yang, C.L.Yang, Y.H.Qiang, X.Y.Huang, Z.Zhao, S.Y.Xu, Z.C.Li, L.X.Chen, L.C.Sun, H.Zhou, X.Zhang, X.L.Wu, Y.L.Tian, Y.S.Wang, J.Y.Wang, W.X.Huang, M.L.Liu, Z.W.Lu, Y.He, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov α-decay properties of new neutron-deficient isotope 203Ac RADIOACTIVITY 203Ac, 199Fr, 195At, 191Bi(α) [from 169Tm(40Ca, 6n)203Ac, E=226 MeV]; measured decay products, Eα, Iα; deduced α-particle energies, transitions T1/2, J, π, partial decay scheme, reduced α-decay widths, proton separation energies, the onset of deformation in neutron-deficient Ac isotopes. Comparison with systematics. The superconducting linear accelerator, China Accelerator Facility for superheavy Elements (CAFE2) at Institute of Modern Physics, Chinese Academy of Sciences.
doi: 10.1016/j.physletb.2024.138503
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, T1/2, α-decay reduced widths, N=82 shell closure toward the proton drip line. Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.132.072502
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
2022DU05 Phys.Rev. C 105, 034602 (2022) F.F.Duan, Y.Y.Yang, J.Lei, K.Wang, Z.Y.Sun, D.Y.Pang, J.S.Wang, X.Liu, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Hu, Z.H.Gao, X.X.Xu, C.J.Lin, H.M.Jia, N.R.Ma, L.J.Sun, D.X.Wang, G.Yang, S.Y.Jin, Z.Z.Ren, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu Elastic scattering and breakup reactions of neutron-rich nucleus 11Be on 208Pb at 210 MeV NUCLEAR REACTIONS 208Pb(11Be, 11Be), (11Be, 10Be), E=210 MeV; measured reaction products; deduced σ(θ), σ. Comparison with CDCC calculations and experimental results for other reaction systems including tightly- and weakly-bound projectiles impinging on medium to heavy mass targets. Beam by Heavy-Ion Research Facility in Lanzhou (HIRFL, China).
doi: 10.1103/PhysRevC.105.034602
2022HU12 Phys.Lett. B 834, 137484 (2022) M.H.Huang, Z.G.Gan, Z.Y.Zhang, L.Ma, J.G.Wang, M.M.Zhang, H.B.Yang, C.L.Yang, X.Y.Huang, Z.Zhao, S.Y.Xu, L.X.Chen, X.J.Wen, Y.F.Niu, C.X.Yuan, Y.L.Tian, Y.S.Wang, J.Y.Wang, M.L.Liu, Y.H.Qiang, W.Q.Yang, H.B.Zhang, Z.W.Lu, S.Guo, W.X.Huang, Y.He, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov α decay of the new isotope 204Ac RADIOACTIVITY 204,205Ac(α) [from 169Tm(40Ca, xn), E=202, 210, 212, 214 MeV using SHANS2 separator at CAFE2 and SHANS separator at HRIFL, Lanzhou accelerator facility]; 200Fr, 196At(α) [from 204Ac α-decay chain]; measured evaporation residues (ERs), Eα, (ER)α-α-α correlated events, production cross sections, T1/2 of decays using two multiwire proportional counters for implanted events, double-sided silicon strip detectors (DSSSDs) for α particles, and a segmented clover Ge detector for γ radiation. 204,205Ac, 200Fr, 196At; deduced T1/2 of decays of ground-state decays, and Eα values, reduced α-width in Rasmussen formalism, favored α decay for 204Ac decay. 204Ac(p); no proton decay events observed. 201,201m,202,202m,203,204,205Fr, 204,205,206Ra(α); observed α spectra, (ERs)-α-α-correlated events. Comparison with previous available experimental results. Systematics of experimental and theoretical T1/2 and Q(α) values for 196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211At, 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213Fr, 203,204,205,206,207,208,209,210,211,212,213,214,215Ac, 211,212,213,214,215,216,217Pa, using Hartree-Fock-BCS (HFBSC) method, and macroscopic-microscopic (MM) mass formula for theory.
doi: 10.1016/j.physletb.2022.137484
2022LU02 Nucl.Phys. A1021, 122408 (2022) Neutron-neutron short-range correlations and their impacts on neutron stars
doi: 10.1016/j.nuclphysa.2022.122408
2022YA15 Phys.Rev. C 105, L051302 (2022) H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, C.X.Yuan, Y.F.Niu, C.L.Yang, Y.L.Tian, L.Guo, Y.S.Wang, J.G.Wang, H.B.Zhou, X.J.Wen, H.R.Yang, X.H.Zhou, Y.H.Zhang, W.X.Huang, Z.Liu, S.G.Zhou, Z.Z.Ren, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, D.I.Solovyev New isotope 207Th and odd-even staggering in α-decay energies for nuclei with Z > 82 and N < 126 RADIOACTIVITY 207Th(α)[from 176Hf(36Ar, 5n), E=197-199 MeV]; 208Th(α)[from 176Hf(36Ar, 4n), E=197-199 MeV]; 203Ra, 199Rn, 195Po(α)[from 207Th α-decay chain]; 204Ra, 200Rn, 196Po(α)[from 208Th α-decay chain]; measured evaporation residues (ERs), Eα, and ER-α1-α2-α3-α4 correlated α-decay chain from the decays of 207Th and208Th. 207,208Th; deduced α-decay T1/2, production σ. Z=84-92, N=102-126; discussed systematics of experimental and theoretically calculated (by relativistic Hartree-Fock-Bogoliubov and large-scale shell-model approaches) odd-even staggering (OES) of Q(α), Q(proton) and Q(neutron). Position-sensitive silicon strip detectors (PSSDs), non-position sensitive Si detectors, and SHANS gas-filled recoil separator at the sector focusing cyclotron facility of HIRFL, Lanzhou.
doi: 10.1103/PhysRevC.105.L051302
2022YA27 Phys.Rev. C 106, 064311 (2022) H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, M.M.Zhang, C.L.Yang, Y.L.Tian, Y.S.Wang, H.B.Zhou, X.J.Wen, J.G.Wang, Z.Zhao, S.Y.Xu, L.X.Chen, X.Y.Huang, C.X.Yuan, Y.F.Niu, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, S.G.Zhou, Z.Z.Ren, H.S.Xu, V.K.Utyonkov, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, D.I.Solovyev Examining the impact of α-decay energies on the odd-even staggering in half-lives: α-decay spectroscopy of 207-209Ac RADIOACTIVITY 207,208,208m,209Ac(α)[from 176Hf(36Ar, X), E=197-199 MeV]; measured evaporation residues (ER), Eα, Iα, αα-coin, (ER)αα-coin; deduced T1/2, Q values, decay branches. 204mFr(IT) [from 208Ac(α)]; deduced T1/2, isomer level energy, tentative J and π for the newly found 80-keV isomer. 204Fr(α)[from 208,208mAc(α)]; deduced T1/2. Found new α-decay branching 208Ac and assigned to the transition from ground state to the excited (2+, 4+) state. Comparison to the calculations performed in the framework of Wentzel-Kramers-Brillouin approximation. Spectrometer for Heavy Atoms and Nuclear Structure (SHANS) at Sector Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL).
doi: 10.1103/PhysRevC.106.064311
2022YU04 Phys.Rev. C 106, 044309 (2022) Y.X.Yu, Y.Lu, G.J.Fu, C.W.Johnson, Z.Z.Ren Nucleon-pair truncation of the shell model for medium-heavy nuclei NUCLEAR STRUCTURE 44,46,48Ti, 48,50Cr, 52Fe, 60,62,64Zn, 66,68Ge, 68Se, 108,110Xe, 112,114Ba, 116,118,120Ce; calculated levels, J, π, yrast states, B(E2). Particle-number conserved Bardeen-Cooper-Schrieffer (NBCS) approximation developed for implementing efficient truncation scheme in the frame of shell-model. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.044309
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, 218U RADIOACTIVITY 216,216m,218,218mU(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, T1/2 using position-sensitive strip detectors (PSSDs) for α detection, and SHANS separator at HIRFL-Lanzhou. 216,216m,218,218mU; deduced T1/2, Q-values, α-branching ratio, α-decay hindrance factors. 204Rn, 208,210Ra, 212,214Th(α)[from 216,218U α-decay chains]; measured Eα, T1/2. 212Th; deduced level, J, π, identification of the first 2+ state. 215Ra, 212,213,216Ac, 211,212,213,214,216,216m,217Th, 216,217,217m,218Pa, 217,218,219U; observed Eα from their decays from (EVR)α-correlations. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.106.024305
2021MA39 Phys.Rev. C 103, L061302 (2021) W.H.Ma, D.Patel, Y.Y.Yang, J.S.Wang, Y.Kanada-En'yo, R.F.Chen, J.Lubian, Y.L.Ye, Z.H.Yang, Z.Z.Ren, S.Mukherjee, J.B.Ma, S.L.Jin, P.Ma, J.X.Li, Y.S.Song, Q.Hu, Z.Bai, M.R.Huang, X.Q.Liu, Y.J.Zhou, J.Chen, Z.H.Gao, F.F.Duan, S.Y.Jin, S.W.Xu, G.M.Yu, G.Z.Shi, Q.Wang, T.F.Wang, X.Y.Ju, Z.G.Hu, Y.H.Zhang, X.H.Zhou, H.S.Xu, G.Q.Xiao, W.L.Zhan Observation of 6He + t cluster states in 9Li NUCLEAR REACTIONS 208Pb(9Li, X), E=32.7 MeV/nucleon, [secondary 9Li beam from 9Be(12C, X), E=53.7 MeV/nucleon, followed by separation and purification of fragments using RIBLL1 at HIRFL-Lanzhou facility]; measured reaction products and outgoing charged particles, angular distributions of charged particles using Si telescope and CsI(Tl) scintillator array. 9Li; deduced resonant states, relative energy spectrum of 6He+t cluster states from the decay of 9Li resonances, differential breakup cross-section, isoscalar monopole transition matrix element M(IS0) and monopole strength B(IS0), energy-weighted sum rule (EWSR) for the transferred angular momentum. DWBA and CDCC analysis of angular distributions, and GCM calculations for the cluster states in 9Li. Relevance to differences between the triton and α clusters, and impact of these differences on the formation of nuclei containing triton clusters.
doi: 10.1103/PhysRevC.103.L061302
2021QI03 Chin.Phys.C 45, 021002 (2021) New look at Geiger-Nuttall law and α clustering of heavy nuclei RADIOACTIVITY Hf, W, Os, Pt, Hg, Pb, Po, Rn, Ra, Th(α); calculated T1/2 using Geiger-Nuttall (GN) law. Comparison with available data.
doi: 10.1088/1674-1137/abce14
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, T1/2, abnormal enhancement by the strong monopole interaction between the valence protons and neutrons. Comparison withavailable data, calculations.
doi: 10.1103/PhysRevLett.126.152502
2021ZH45 Chin.Phys.C 48, 084102 (2021) Q.-J.Zhi, X.-P.Zhang, J.-L.You, Q.Zheng, Z.-Z.Ren Calculation of double-β decay half-lives using an improved Primakoff-Rosen formula RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe, 150Nd, 238U(2β-); calculated two-neutrino mode T1/2. Comparison with available data.
doi: 10.1088/1674-1137/ac0097
2020HE05 Chin.Phys.C 44, 034106 (2020) X.-T.He, S.-Y.Zhao, Z.-H.Zhang, Z.-Z.Ren High-K multi-particle bands and pairing reduction in 254No NUCLEAR STRUCTURE 254No; calculated multi-particle states and rotational properties of the two-particle bands using the cranked shell model with pairing correlations treated by the particle number conserving method.
doi: 10.1088/1674-1137/44/3/034106
2020HE10 Chin.Phys.C 44, 034106 (2020) X.-T.He, S.-Y.Zhao, Z.-H.Zhang, Z.-Z.Ren High-K multi-particle bands and pairing reduction in 254No NUCLEAR STRUCTURE 254No; calculated Nilsson single-particle levels, J, π, energy levels, moments of inertia, bands using the cranked shell model with pairing correlations treated by the particle number conserving method.
doi: 10.1088/1674-1137/44/3/034106
2020MA27 Phys.Rev.Lett. 125, 032502 (2020) L.Ma, Z.Y.Zhang, Z.G.Gan, X.H.Zhou, H.B.Yang, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, H.B.Zhou, X.T.He, Y.C.Mao, W.Hua, L.M.Duan, W.X.Huang, Z.Liu, X.X.Xu, Z.Z.Ren, S.G.Zhou, H.S.Xu Short-Lived α-Emitting Isotope 222Np and the Stability of the N = 126 Magic Shell NUCLEAR REACTIONS 187Re(40Ar, 5N)222Np, E=198.7 MeV; measured reaction products, Eα, Iα. 220Pa, 219Th; deduced Q-values, T1/2. Comparison with systematics.
doi: 10.1103/PhysRevLett.125.032502
2020SH02 Phys.Lett. B 801, 135174 (2020) X.-X.Shi, Q.Liu, J.-Y.Guo, Z.-Z.Ren Pseudospin and spin symmetries in single particle resonant states in Pb isotopes NUCLEAR STRUCTURE 190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220Pb; calculated energies and widths, pseudospin and spin splittings. RMF-CMR theory.
doi: 10.1016/j.physletb.2019.135174
2020SH10 Chin.Phys.C 44, 054103 (2020) X.-X.Shi, Q.Liu, D.-D.Ni, J.-Y.Guo, Z.-Z.Ren The first excited single-proton resonance in 15F by complex-scaled Green's function method NUCLEAR STRUCTURE 15F; calculated eigenvalues of resonant states, resonance energies and widths, level densities, phase shifts, σ using the complex-scaled Green's function (CGF) method.
doi: 10.1088/1674-1137/44/5/054103
2020ZH01 Phys.Lett. B 800, 135102 (2020) M.M.Zhang, H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, C.L.Yang, C.X.Yuan, Y.S.Wang, Y.L.Tian, H.B.Zhou, S.Huang, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, X.X.Xu, J.G.Wang, H.R.Yang, L.M.Duan, W.Q.Yang, S.G.Zhou, Z.Z.Ren, X.H.Zhou, H.S.Xu, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, M.V.Shumeiko A new isomeric state in 218Pa RADIOACTIVITY 218Pa(α) [from 182W(40Ar, 3np)218Pa, E=190 MeV]; measured decay products, Eα, Iα, Eγ, Iγ; deduced ground and isomeric states T1/2, α and γ-ray energies and intensities, J, π.
doi: 10.1016/j.physletb.2019.135102
2019SH37 Phys.Lett. B 797, 134820 (2019) Y.P.Shen, B.Guo, T.L.Ma, D.Y.Pang, D.D.Ni, Z.Z.Ren, Y.J.Li, Z.D.An, J.Su, J.C.Liu, Q.W.Fan, Z.Y.Han, X.Y.Li, Z.H.Li, G.Lian, Y.Su, Y.B.Wang, S.Q.Yan, S.Zeng, W.P.Liu First experimental constraint of the spectroscopic amplitudes for the α-cluster in the 11B ground state NUCLEAR REACTIONS 7Li(6Li, d), E=24 MeV; measured reaction products; deduced spectroscopic amplitudes (SA) for the α-cluster in the 11B ground state. Comparison with available data.
doi: 10.1016/j.physletb.2019.134820
2019YO05 Chin.Phys.C 43, 114104 (2019) J.-L.You, X.-P.Zhang, Q.-J.Zhi, Z.-Z.Ren, Q.-D.Wu The contribution of the first forbiden transitions to the nuclear β--decay half-life RADIOACTIVITY 134Sb, 135Te, 137Xe, 137,138,139Cs, 139,140Ba, 140,141La, 141,143,144Ce, 142,143,144,145,146Pr, 147Nd, 147Pm, 165,166Dy, 166Ho, 169Er, 170,171,172,173Tm(β-); analyzed available data; deduced eight parameters using the least-squares fit of the experimental β--decay T1/2 that includes contribution of the first forbidden (FF) transitions.
doi: 10.1088/1674-1137/43/11/114104
2019ZH23 Phys.Rev.Lett. 122, 192503 (2019) Z.Y.Zhang, Z.G.Gan, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, M.D.Sun, H.Y.Lu, W.Q.Zhang, H.B.Zhou, X.Wang, C.G.Wu, L.M.Duan, W.X.Huang, Z.Liu, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, Yu.S.Tsyganov, A.A.Voinov, A.N.Polyakov New Isotope 220Np: Probing the Robustness of the N=126 Shell Closure in Neptunium RADIOACTIVITY 220Np, 216Pa, 212Ac, 208Fr(α) [from 185Re(40Ar, 5n)220Np/216Pa/212Ac/208Fr, E=201 MeV]; measured decay products, Eα, Iα; deduced T1/2, Q-values. Comparison with systematics.
doi: 10.1103/PhysRevLett.122.192503
2019ZH54 Phys.Rev. C 100, 064317 (2019) M.M.Zhang, Y.L.Tian, Y.S.Wang, X.H.Zhou, Z.Y.Zhang, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, Z.G.Gan, J.G.Wang, H.B.Zhou, S.Huang, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, X.X.Xu, L.M.Duan, Z.Z.Ren, S.G.Zhou, H.S.Xu Fine structure in the α decay of 219U RADIOACTIVITY 219U(α)[from 183W(40Ar, 4n), E=190 MeV]; measured Eα, Iα, αα-coin, (recoils)ααα-correlations, half-life of 219U decay, production σ of 219U using position-sensitive strip detectors (PSSDs) for α detection, and the SHANS separator at the Heavy Ion Research Facility (HIRFL) in Lanzhou. 215Th; deduced levels, J, π, α-branching ratios, α-decay reduced widths. 216,216m,217,219Th, 220Pa(α)[from 183W(40Ar, X), E=190 MeV]; 215Th, 211Ra[from 219U α decay]; measured Eα, half-lives of decays of the isotopes. Discussed α-decay systematics in neighboring nuclides. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.100.064317
2018BA43 Chin.Phys.C 42, 124102 (2018) Woods-Saxon-Gaussian potential and alpha-cluster structures of alpha + closed shell nuclei NUCLEAR STRUCTURE 212Po, 20Ne, 44Ti; calculated level scheme, B(E2), and alpha-decay T1/2 of the alpha-cluster structures in various alpha + closed shell nuclei.
doi: 10.1088/1674-1137/42/12/124102
2018NI12 Chin.Phys.C 42, 114104 (2018) Theoretical research on proton halos in exotic nuclei NUCLEAR STRUCTURE 17F, 25Al, 26,27,28P; calculated radial density probability distributions of all protons, all neutrons, the last valence proton, and nuclear matter in the Woods-Saxon potential.
doi: 10.1088/1674-1137/41/11/114104
2018YA01 Phys.Lett. B 777, 212 (2018) H.B.Yang, L.Ma, Z.Y.Zhang, C.L.Yang, Z.G.Gan, M.M.Zhang, M.H.Huang, L.Yu, J.Jiang, Y.L.Tian, Y.S.Wang, J.G.Wang, Z.Liu, M.L.Liu, L.M.Duan, S.G.Zhou, Z.Z.Ren, X.H.Zhou, H.S.Xu, G.Q.Xiao Alpha decay properties of the semi-magic nucleus 219Np RADIOACTIVITY 219Np(α) [from 187Re(36Ar, 4n), E=191.5 MeV]; 218,218U, 215Pa(α); measured decay products, Eα, Iα; deduced α-particle energy, T1/2, Q-value. Comparison with available data.
doi: 10.1016/j.physletb.2017.12.017
2017HU08 Phys.Rev. C 96, 014324 (2017) 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, C.J.Lin, L.J.Sun, N.R.Ma, Z.Z.Ren, F.S.Zhang, W.Zou, X.H.Zhou, H.S.Xu, G.Q.Xiao α-decay chain of the short-lived isotope 220Pa established using a digital pulse processing technique RADIOACTIVITY 220Pa(α)[from 187Re(40Ar, 3nα), E=188 MeV at HIRFL-Lanzhou facility]; 216Ac(α)[from 220Pa parent decay]; measured Eα, (evaporation residue)α-correlated events using the digital pulse processing technique, half-lives of decays of 220Pa and 216Ac; deduced J, π of the ground state of 220Pa, and reduced α-decay width. Comparison with previous experimental Eα and T1/2 for 220Pa.
doi: 10.1103/PhysRevC.96.014324
2017LI13 Chin.Phys.C 41, 054101 (2017) J.Liu, J.Zhang, C.Xu, Z.-Z.Ren Nuclear longitudinal form factors for axially deformed charge distributions expanded by nonorthogonal basis functions NUCLEAR STRUCTURE 12C; calculated charge form factors, charge density distributions. DWBA method.
doi: 10.1088/1674-1137/41/5/054101
2017LI46 Phys.Rev. C 96, 065503 (2017) Calculations of two-neutrino double-β decay for fpg shell nuclei RADIOACTIVITY 70Zn, 76Ge, 80,82Se, 86Kr(2β-); 64Zn, 74Se, 78Kr, 84Sr(2β+), (2EC); calculated half-lives for 2νββ decay mode, quenching factor T(GT) values, nuclear matrix elements (NMEs) for transitions to ground states, first excited 0+ and 2+ states using shell model with JUN45 effective interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.065503
2017NI16 Chin.Phys.C 41, 114104 (2017) Theoretical research on proton halos in exotic nuclei NUCLEAR STRUCTURE 65As, 17F, 26,27,28P, 56,57Cu; calculated nuclear radii, radial density probability distributions, single-particle energies; deduced halo. Comparison with available data.
doi: 10.1088/1674-1137/41/11/114104
2017TA10 Chin.Phys.C 41, 054103 (2017) Calculations of the β-decay half-lives of neutron-deficient nuclei RADIOACTIVITY 42,44,46Cr, 46,48,50Fe, 48,50,52,54Ni, 56,58,60,62Zn, 60,62,64,66Ge, 64,66,68,70Se(EC), (β+); calculated T1/2. Comparison with available data.
doi: 10.1088/1674-1137/41/5/054103
2017WA17 Chin.Phys.C 41, 064103 (2017) R.Wang, R.-Y.Wang, Y.-B.Qian, Z.-Z.Ren Signatures of shell evolution in alpha decay across the N = 126 shell closure RADIOACTIVITY 208,210,212,214Po, 209,211,213,215At, 210,212,214,216Rn, 211,213,215,217Fr, 212,214,216,218Ra, 213,215,217,219Ac, 214,216,218,220Th, 215,217,219,221Pa, 216,218,222U(α); calculated T1/2. Comparison with experimental data.
doi: 10.1088/1674-1137/41/6/064103
2016LI19 Chin.Phys.C 40, 034101 (2016) J.Liu, C.Zhang, Z.-Z.Ren, C.Xu Theoretical study on neutron distribution of 208Pb by parity-violating electron scattering NUCLEAR REACTIONS 208Pb(E, E), E=1.06 GeV; calculated form factors for skin and halo type. Comparison with experimental data.
doi: 10.1088/1674-1137/40/3/034101
2016QI02 Eur.Phys.J. A 52, 68 (2016) Calculations on decay rates of various proton emissions RADIOACTIVITY 105Sb, 109I, 112,113Cs, 117La, 121Pr, 130,131Eu, 135Tb, 140,141,141mHo, 145,146,146m,147,147m,150,150m,151,151mLu, 155,156,156m,157Ta, 159,160,161,161mRe, 164,165,165m,166,166m,167,167mIr, 171,171mAu, 177,177mTl, 185Bi(p); calculated T1/2. Compared with data and other calculations. 116La, 132Eu, 136Tb, 162,163Re, 169,170Au, 176,178Tl, 184Bi(p); calculated proton decay candidates T1/2. Deformed density-dependent model with spectroscopic factors from RMF combined with BCS.
doi: 10.1140/epja/i2016-16068-3
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
2015FA03 Phys.Rev. C 91, 014614 (2015) G.W.Fan, M.Fukuda, D.Nishimura, X.L.Cai, S.Fukuda, I.Hachiuma, C.Ichikawa, T.Izumikawa, M.Kanazawa, A.Kitagawa, T.Kuboki, M.Lantz, M.Mihara, M.Nagashima, K.Namihira, Y.Ohkuma, T.Ohtsubo, Z.z.Ren, S.Sato, Z.Q.Sheng, M.Sugiyama, S.Suzuki, T.Suzuki, M.Takechi, T.Yamaguchi, W.Xu Density distribution of 8Li and 8B and capture reaction at low energy NUCLEAR REACTIONS 9Be, 12C, 27Al(8Li, X), E=30-110 MeV, [8Li secondary beam produced in 9Be(13C, X), E=130 MeV/nucleon primary reaction]; measured reaction products, reaction σ(E) at HIMAC synchrotron and fragment-separator facility of NIRS, Japan; deduced density distributions of 8B and 8Li using modified Glauber model, halo structure of 8B. 7Li(n, γ)8Li, E=0.01 eV-1 MeV; 7Be(p, γ)8B, E=0-0.5 MeV; calculated capture σ(E) for (n, γ) and S(E) factor for (p, γ) reactions using density distributions determined in present work, comparison with experimental data.
doi: 10.1103/PhysRevC.91.014614
2015JI07 Phys.Rev. C 91, 054617 (2015) S.L.Jin, J.S.Wang, Y.Y.Yang, P.Ma, M.R.Huang, J.B.Ma, F.Fu, Q.Wang, M.Wang, Z.Y.Sun, Z.G.Hu, R.F.Chen, X.Y.Zhang, X.H.Yuan, X.L.Tu, Z.G.Xu, K.Yue, J.D.Chen, B.Tang, Y.D.Zang, D.P.Wu, Q.Hu, Z.Bai, Y.J.Zhou, W.H.Ma, J.Chen, C.J.Lin, X.X.Xu, Z.Z.Ren, C.Xu, D.D.Ni, Y.H.Zhang, H.S.Xu, G.Q.Xiao Reaction mechanism of 8B breakup at the Fermi energy NUCLEAR REACTIONS 12C(8B, 7Be), E=36 MeV/nucleon, [secondary 8B beam produced in 9Be(12C, X), E=80.1 MeV/nucleon primary reaction]; measured particle spectra, (7Be)p-coin in the breakup reactions from 8B at RIBLL-HIRFL-Lanzhou facility; deduced energy sum spectrum of the one-proton knockout residue, longitudinal momentum distributions of 7Be fragments for stripping and diffraction mechanisms. Comparison with CDCC calculations with Koning and Delaroche global parameterization.
doi: 10.1103/PhysRevC.91.054617
2015MA37 Phys.Rev. C 91, 051302 (2015) L.Ma, Z.Y.Zhang, Z.G.Gan, H.B.Yang, L.Yu, J.Jiang, J.G.Wang, Y.L.Tian, Y.S.Wang, S.Guo, B.Ding, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, G.Q.Xiao α-decay properties of the new isotope 216U RADIOACTIVITY 216,216m,218,218mU(α)[from 180W(40Ar, xn), E=189.5 MeV]; measured evaporation residues (ER), Eα, Iα, correlated ER-α1-α2 events, α-decay half-lives using SHANS spectrometer at HIRFL-Lanzhou facility; deduced 216U new isotope and its isomeric state, and α-reduced widths. 212,214Th, 208,210Ra(α); measured Eα, Iα, α-decay half-lives, α-reduced widths. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.051302
2015NI10 Phys.Rev. C 92, 034324 (2015) β-decay rates of odd-mass neutron-rich isotopes in the deformed quasiparticle random-phase approximation with realistic interactions RADIOACTIVITY 85,87,89,91,93,95,97,99,101Kr, 89,91,93,95,97,99,101,103,105,107Sr, 95,97,99,101,103,105,107,109,111,113Zr, 99,101,103,105,107,109,111,113,115,117Mo(β-); calculated half-lives. 91,93,101,105Sr(β-); calculated GT transition strength. Deformed quasiparticle random-phase approximation with realistic nucleon-nucleon interactions including both the GT and first-forbidden (FF) β transitions. Comparison with other theoretical calculations and with experimental values.
doi: 10.1103/PhysRevC.92.034324
2015XU06 Eur.Phys.J. A 51, 20 (2015) R.L.Xu, C.Wu, W.-L.Qian, Z.Z.Ren Dynamics of kaonic nuclei in an improved quark mass density-dependent model NUCLEAR STRUCTURE 24Ne, 32Ar, 34Si; calculated kaonic nuclei single-particle K- binding energy, Q, levels, J, nuclear density distribution, radius using different nucleon-nucleon forces within relativistic mean-field theory.
doi: 10.1140/epja/i2015-15020-5
2015YA13 Eur.Phys.J. A 51, 88 (2015) H.B.Yang, Z.Y.Zhang, J.G.Wang, Z.G.Gan, L.Ma, L.Yu, J.Jiang, Y.L.Tian, B.Ding, S.Guo, Y.S.Wang, T.H.Huang, M.D.Sun, K.L.Wang, S.G.Zhou, Z.Z.Ren, X.H.Zhou, H.S.Xu, G.Q.Xiao Alpha decay of the new isotope 215U RADIOACTIVITY 215U(α)[from 180W(40Ar, 5n)]; measured sequential α emission Eα, Iα(t), αα-coin; deduced α-decay energy, T1/2. NUCLEAR REACTIONS 180W(40Ar, 5n), E=205.5 MeV; measured reaction products; deduced σ. 180W(40Ar, xn), E=170-220 MeV; calculated σ for x=3-6 using HIVAP code. Compared with one other experimental point.
doi: 10.1140/epja/i2015-15088-9
2015ZH05 Phys.Rev. C 91, 024001 (2015) L.Zhang, Z.-z.Ren, M.Lyu, C.Ji Investigation of 23N in a three-body model NUCLEAR STRUCTURE 22,23N; calculated binding energies, single particle levels, S(2n), neutron, proton and matter rms radii, density distribution profiles, related features of the bound and excited states using Faddeev equations in a three-body model consisting of 21N core and two valence neutrons. Evidence of Efimov physics in the drip-line nucleus 23N.
doi: 10.1103/PhysRevC.91.024001
2014FA02 Chin.Phys.C 38, 014101 (2014) G.-W.Fan, X.-L.Cai, M.Fukuda, T.-F.Han, X.-C.Li, z.-Z.Ren, W.Xu Big deformation in 17C NUCLEAR REACTIONS 12C(17C, X), E=79 MeV/nucleon; analyzed available σ data. 17C; deduced one-neutron halo structure, dominant d-wave valence neutron. Woods-Saxon density potential.
doi: 10.1088/1674-1137/38/1/014101
2014FA06 Chin.Phys.C 38, 044101 (2014) G.-W.Fan, X.-L.Cai, M.Fukuda, T.-F.Han, X.-C.Li, Z.-Z.Ren, W.Xu Effect of nuclear deformation on direct capture reactions NUCLEAR REACTIONS 7Li(n, γ)8Li, E<0.6 MeV; calculated σ; deduced nuclear deformation effects. Spherical potential model.
doi: 10.1088/1674-1137/38/4/044101
2014WA03 Chin.Phys.C 38, 024102 (2014) Z.-J.Wang, Z.-Z.Ren, T.-K.Dong Probe the 2s1/2 and 1d3/2 state level inversion with electron-nucleus scattering NUCLEAR STRUCTURE 26,28,30,32,34,36,38,40Mg, 28,30,32,34,36,38,40,42,44,46Si, 30,32,34,36,38,40,42,44,46,48s, 32,34,36,38,40,42,44,46,48,50,52,54,56Ar; calculated proton state energy levels and occupation probabilities, charge density distributions, charge form factors. RMF model. NUCLEAR REACTIONS 24Mg, 28Si, 32S(E, X), E=250, 500 MeV; calculated σ(θ). Comparison with experimental data.
doi: 10.1088/1674-1137/38/2/024102
2014ZH03 Phys.Rev. C 89, 014308 (2014) Z.Y.Zhang, Z.G.Gan, L.Ma, L.Yu, H.B.Yang, T.H.Huang, G.S.Li, Y.L.Tian, Y.S.Wang, X.X.Xu, X.L.Wu, M.H.Huang, C.Luo, Z.Z.Ren, S.G.Zhou, X.H.Zhou, H.S.Xu, G.Q.Xiao α decay of the new neutron-deficient isotope 205Ac RADIOACTIVITY 205,206Ac(α)[from 169Tm(40Ca, 4n), (40Ca, 3n), E=196 MeV, and subsequent α decays]; measured Eα, Iα, (evaporation residues)αα-correlations, half-lives, production σ using gas-filled separator SHANS at HIRFL-Lanzhou facility; discussed J, π of parent states. 198At, 202Fr(α); measured Eα, half-lives. Comparison with previous measurements. 200Po, 201,202,202m,203At, 202,203,204,205,206Fr, 203,204,205Rn, 205Ra, 205mRa(α); observed Eα, (evaporation residues)α-correlations. 205,206,207,208,209,210,211,212,213,214,215Ac; systematics of Q(α) and half-lives.
doi: 10.1103/PhysRevC.89.014308
2013CA04 Chin.Phys.C 37, 034103 (2013) A theoretical study of halo structure using elastic proton-nucleus scattering NUCLEAR REACTIONS 10,12,14Be, 12,14,15C, 14,16,18,20,22,24,26,28O(p, p), E=200 MeV; calculated rms proton radii, neutron skin, binding energy, neutron density distribution; deduced neutron halo. Comparison with experimental data.
doi: 10.1088/1674-1137/37/3/034103
2013NI01 Chin.Phys.Lett. 30, 022101 (2013) Alpha-Decay Study of Unfavored Transitions in Bismuth Isotopes RADIOACTIVITY 187,188,189,190,191,192,193,194,195,197,199,201,203,209,210,211,212,213,214Bi(α); calculated T1/2. Generalized density-dependent cluster model (GDDCM), comparison with experimental data.
doi: 10.1088/0256-307X/30/2/022101
2013XU15 Eur.Phys.J. A 49, 141 (2013) R.L.Xu, C.Wu, W.-L.Qian, Z.Z.Ren, J.Liu Deformed even-even nuclei in a quark-meson coupling model with tensor coupling NUCLEAR STRUCTURE 89Y, 90Zr, 132Sn, 139La, 208Pb; calculated mass excess, charge radii, neutron skin thickness, single-particle states, J, spin-orbit splitting. 14,16,18,20,22,24O, 16,18,20,22,24,26Ne, 38,40,42,44,46,48Ar, 34,36,38,40,42,44,46,48,50Ca, 38,40,42,44,46,48,50,52Ti, 184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po; calculated mass excess, neutron radius, charge radius, quadrupole deformation. Gd, Dy, Er, Yb; calculated quadrupole deformation vs mass, 2n separation energy vs mass, charge radius vs mass. 118,120Te, 136Ce, 140,148Sm, 150Gd, 154Er, 156Yb, 158Hf, 162,168W, 188,190,192Os, 172,186,188Pt; calculated deformations, prolate minus oblate energy, shape coexistence. RMF models and IQMDD (improved quark mass density dependent model) with different parameters. Compared with available data.
doi: 10.1140/epja/i2013-13141-5
2012CH48 J.Phys.(London) G39, 125105 (2012) Calculations of the b-decay half-lives of neutron-rich nuclei RADIOACTIVITY 16,18,20,22C, 22,24,26,28O, 26,28,30,32,34Ne, 30,32,34,36,38,40Mg, 34,36,38,40,42,44Si, 40,42,44,46,48S, 46,48,50,52Ar, 52,54,56,58Ca, 54,56,58,60,62Ti, 58,60,62,64,66,68Cr, 64,66,68,70,72Fe, 70,72,74,76,78Ni, 76,78,80,82Zn, 82,84,86,88Ge, 88,90,92,94Se, 92,94,96,98,100Kr, 96,98,100,102,104Sr, 100,102,104,106,108,110Zr, 106,108,110,112,114Mo, 112,114,116,118,120Ru, 118,120,122,124Pd, 122,124,126,128,130,132Cd, 134,136Sn, 138,140,142Te, 142,144,146Xe, 146,148,150,152Ba, 150,152,154,156Ce(β-); calculated T1/2. pnQRPA with δ-form Gamow-Teller residual interaction, comparison with experimental data.
doi: 10.1088/0954-3899/39/12/125105
2012DO14 J.Phys.:Conf.Ser. 381, 012135 (2012) Nuclear neutron densities and parity violating electron scattering NUCLEAR REACTIONS 208Pb(e, e'), E=850 MeV; calculated parity-violating asymmetry factor vs momentum transfer using PWBA, relativistic eikonal approximation, partial-wave analysis.
doi: 10.1088/1742-6596/381/1/012135
2012NI02 Rom.J.Phys. 57, 407 (2012) New Formula of Half-Lives for Proton Emission from Spherical and Deformed Nuclei RADIOACTIVITY 105Sb, 109I, 112,113Cs, 117La, 121Pr, 130,131Eu, 135Tb, 140,141Ho, 145,146,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated T1/2; deduced new formula.
2012RE06 Phys.Rev. C 85, 044608 (2012) New Geiger-Nuttall law for α decay of heavy nuclei RADIOACTIVITY 190,191,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,212,213,214,215,216,217,218Po, 204,206,208,210,212,213,214,216,218,220,222Rn, 202,204,206,214,215,216,218,220,222,224,226Ra, 212,214,216,217,218,220,222,224,226,228,230,232Th, 218,219,222,224,226,228,230,232,234,236,238U, 158,160,162,164,166,168W, 156,158,160,162Hf, 154,156,158Yb, 152,154,156Er, 150,152,154Dy, 148,150,152Gd, 146,148Sm, 144Nd(α); calculated T1/2 by new Geiger-Nuttall law. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.044608
2012XU11 Chin.Phys.Lett. 29, 122102 (2012) Effect of Short-Range and Tensor Force Correlations on High-Density Behavior of Symmetry Energy NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated momentum distribution; deduced short-range and tensor correlations on nuclear symmetry energy.
doi: 10.1088/0256-307X/29/12/122102
2012ZH04 Chin.Phys.Lett. 29, 012502 (2012) Z.-Y.Zhang, Z.-G.Gan, L.Ma, M.-H.Huang, T.-H.Huang, X.-L.Wu, G.-B.Jia, G.-S.Li, L.Yu, Z.-Z.Ren, S.-G.Zhou, Y.-H.Zhang, X.-H.Zhou, H.-S.Xu, H.-Q.Zhang, G.-Q.Xiao, W.-L.Zhang Observation of the Superheavy Nuclide 271Ds RADIOACTIVITY 271Ds(α) [from 208Pb(64Ni, n), E=313.3 MeV]; measured decay products, Eα, Iα, α-α-coin.; deduced T1/2, α-decay chain. Comparison with experimental data.
doi: 10.1088/0256-307X/29/1/012502
2012ZH07 Chin.Phys.C 36, 210 (2012) X.-P.Zhang, G.-W.Li, Z.-Z.Ren, Q.Zheng, X.-L.Zhu, J.-P.Cheng Systematical law of (n, γ) reaction cross sections of even-even nuclei NUCLEAR REACTIONS Ge, Si, S, Sn, Te, Xe, Ba, Hf, W, Os(n, γ), E not given; analyzed experimental data; deduced systematics, σ formula.
doi: 10.1088/1674-1137/36/3/004
2012ZH29 Phys.Rev. C 86, 014301 (2012) B.Zhou, Z.-z.Ren, C.Xu, Y.Funaki, T.Yamada, A.Tohsaki, H.Horiuchi, P.Schuck, G.Ropke New concept for the ground-state band in 20Ne within a microscopic cluster model NUCLEAR STRUCTURE 20Ne; calculated energy surface contour maps of ground-state and first 2+ states, wave function overlaps, minimum energies and distances between α cluster and 16O cluster with respect to different spin-projected states for the ground-state band members up to 8+. Brink microscopic cluster model based on generalized Tohsaki, Horiuchi, Schuck, Ropke (THSR) wave functions. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.014301
2011CH38 Chin.Phys.C 35, 735 (2011) Y.Cheng, T.-K.Dong, W.-D.Dong, Z.-Z.Ren, A.-A.Xu Chemical composition of the lunar surface from neutron leakage fluxes
doi: 10.1088/1674-1137/35/8/007
2011LI23 Eur.Phys.J. A 47, 78 (2011) X.J.Liu, X.P.Zhang, D.D.Ni, Z.Z.Ren Benford's law and cross-sections of A(n, α)B reactions
doi: 10.1140/epja/i2011-11078-3
2011SH13 J.Phys.(London) G38, 055103 (2011) Systematic calculations on cluster radioactivity half-lives RADIOACTIVITY 112,113,114,115,116,117Cs, 114,115,116,117,118,119,120Ba, 117,118,119,120,121,122La, 120Ce, 219Fr, 219,220,227Ra, 219,220,221,222,228Ac, 220,221,221,222,223Th, 221,223,231,232,233,234Pa, 222,223,224,225,226U, 225,226,227,228Np, 228,229,230Pu(12C), 114,115,116,117,118,119Ba, 117,118,119,120,122La, 119,120,121,122,123,124Ce, 121,122,123,124,125,126Pr, 124,125,126Nd, 224,225Th, 224,225,226,227U, 225,226,227,228,229Np, 228,229,230Pu(16O), 126Pm(24Mg), 220Fr, 224Pa(13C), 227Th, 227,228Pa, 228U(18O), 227,228Ac(20O), 229,230Ac(22O), 232,233,234Pu, 233,234,235Am(26Mg), 236Am, 233,235Pu(27Mg), 237Pu(29Mg), 128,129,130,131,132Sm, 130,131,132,133,134,135Eu, 134,135Gd, 136,137Tb, 138Dy(28Si), 131Sm(29Si), 132Eu, 135Gd(29Si), 136Tb, 138Dy, 140,141Ho(32S), 143Er(36Ar), 239Pu, 239,241Cm(33Si), 225Ac, 221,222,223,224,226Ra, 226Th, 220,222,224,226,223,225Fr, 220,228Ra, 221,222,224,226,227Ac, 224,225,227,223Th, 225,226,227,228Pa, 227,228U(14C), 226Th(18O), 228,229Th(20O), 229,231Pa(23F), 229,230U, 230,231Np, 231,232Pu(22Ne), 231U(23Ne), 229Ac, 230,231,232,233Pa, 229,230,231,232Th, 230,231,232,233,234,235,236U, 231,232,233Np(24Ne), 234Pa, 235U(25Ne), 232Th, 236U(26Ne), 127Pm(24Mg), 232,233,234,235U, 234,235,236Np, 234,235,236,237,238Pu, 235Am(28Mg), 235U, 235Np(29Mg), 236,238Pu, 237Np(30Mg), 238Pu, 236,238Am(32Si), 238Np, 239,240,241,242Am, 238,239,240,241,242,243Cm, 240,241Bk(34Si); calculated T1/2.
doi: 10.1088/0954-3899/38/5/055103
2011WA16 Phys.Rev. C 84, 014609 (2011) Theoretical study of evaporation cross sections in the synthesis of very neutron-deficient nuclei NUCLEAR REACTIONS 92Mo(32S, X)124Ce*, E(cm)=112 MeV; 92Mo(36Ar, X)128Nd*, E(cm)=121 MeV; 96Ru(36Ar, X)132Sm*, E(cm)=120, 127 MeV; 97Mo(40Ca, X)137Sm*, E(cm)=142 MeV; 106Cd(32S, X)138Gd*, E(cm)=116 MeV; 106Cd(36Ar, X)142Dy*, E(cm)=131 MeV; 106Cd(40Ca, X)146Er*, E(cm)=147 MeV; 112Sn(40Ca, X)152Yb*, E(cm)=136 MeV; calculated fusion evaporation cross sections. Standard statistical (nuclear reaction video) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.014609
2010GU15 Chin.Phys.Lett. 27, 102102 (2010) Exploring Scaling Laws of Valence Neutron Distributions for Medium Nuclei NUCLEAR STRUCTURE 6,10He, 11,14Be, 14,17,19B, 15,19,22C, 17O, 47S; calculated rms radii of the valence neutron distributions; deduced neutron halo. Single-particle potential model.
doi: 10.1088/0256-307X/27/10/102102
2010JI15 Eur.Phys.J. A 44, 465 (2010) W.Z.Jiang, Z.Z.Ren, Z.Q.Sheng, Z.Y.Zhu Sensitivity of de-excitation energies of superdeformed secondary minima to the density dependence of symmetry energy with the relativistic mean-field theory NUCLEAR STRUCTURE 191,192,194Hg, 194,196,198,200Au; calculated ground state and superdeformed secondary minima properties, radii, deformation, neutron skin thickness using relativistic mean field model.
doi: 10.1140/epja/i2010-10962-6
2010QI03 Chin.Phys.Lett. 27, 072301 (2010) Theoretical Calculation for Half-Lives of Spherical Proton Emitters RADIOACTIVITY 105Sb, 145,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated proton radioactivity T1/2 for spherical emitters. Comparison with experimental data.
doi: 10.1088/0256-307X/27/7/072301
2010QI09 Chin.Phys.Lett. 27, 112301 (2010) Y.-B.Qian, Z.-Z.Ren, D.-D.Ni, Z.-Q.Sheng Half-Lives of Proton Emitters With a Deformed Density-Dependent Model RADIOACTIVITY 105Sb, 145,146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi, 109I, 112,113Cs, 117La, 121Pr, 130,131Eu, 135Tb, 140,141Ho(p); calculated T1/2 for semi-spherical and well-deformed proton emitters.
doi: 10.1088/0256-307X/27/11/112301
2010SH32 Eur.Phys.J. A 46, 241 (2010) Deformed relativistic mean-field calculations on nuclei near Z = 50 with FSUGold NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sn, 108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138Te, 110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,138,140,142Xe, 112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148Ba; calculated binding energies, quadrupole deformation parameters, hexadecupole moments, charge radii, two-neutron separation energies. Deformed relativistic mean-field theory, comparison with experimental data.
doi: 10.1140/epja/i2010-11038-5
2010WA39 Phys.Rev. C 82, 054605 (2010) C.Wang, J.Zhang, Z.Z.Ren, C.W.Shen How the projectile neutron number influences the evaporation cross section in complete fusion reactions with heavy ions NUCLEAR REACTIONS 208Pb(48Ti, n), (48Ti, 2n), (50Ti, n), (50Ti, 2n), (52Cr, n), (52Cr, 2n), (54Cr, n), (54Cr, 2n), E(cm)=180-230 MeV; calculated σ as function of excitation energy, capture σ, fusion probabilities as function of excitation energy using fusion-fission statistical model. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.054605
2009CH69 Chin.Phys.C 33, 639 (2009) Density-dependent potential for multi-neutron halo nuclei NUCLEAR STRUCTURE 6,8He; calculated density distributions, transparency function. Three-body calculation of the ground structures.
doi: 10.1088/1674-1137/33/8/008
2009DO22 Chin.Phys.C 33, Supplement 1, 5 (2009) Research on some superheavy nuclei RADIOACTIVITY 251,252,253,254,255,256,257No, 253,254,255,256,257,258,259Lr, 253,254,255,256,257,258,259Rf, 256,257,258,259,260,261Db, 258,259,260,261,262,263Sg, 260,261,262Bh, 264,265,266,267Hs, 264,265,266,267Mt(α); calculated α-decay energies, T1/2. Local-binding energy and Viola-Seaborg formulas.
doi: 10.1088/1674-1137/33/S1/002
2009HE02 Nucl.Phys. A817, 45 (2009) X.-t.He, Z.-z.Ren, S-x.Liu, E.-g.Zhao Influence of high-j intruder orbitals in odd mass transfermium nuclei 253No and 251Md NUCLEAR STRUCTURE 251Md, 253No; calculated rotational band properties, configurations using a cranked shell model and comparison with data.
doi: 10.1016/j.nuclphysa.2008.12.003
2008CH34 Int.J.Mod.Phys. E17, Supplement 1, 50 (2008) J.G.Chen, X.Z.Cai, Y.Shi, Y.G.Ma, Z.Z.Ren, D.Q.Fang, W.Guo, H.W.Wang, W.D.Tian, W.Q.Shen Nuclear halo and its scaling laws in the excited states of nuclei near the β-stability line NUCLEAR STRUCTURE 13,15N, 13C, 15O, 21Na; calculated binding energies, radii, excited states; deduced proton halo and proton skin. Nonlinear RMF model.
doi: 10.1142/S0218301308011756
2008DO13 Chin.Phys.Lett. 25, 2425 (2008) Parity Violating Electron Scattering in the Relativistic Eikonal Approximation
doi: 10.1088/0256-307X/25/7/026
2008HE02 J.Phys.(London) G35, 035106 (2008) Enhanced sensitivity to variation of fundamental constants in the narrow nuclear transitions (II)
doi: 10.1088/0954-3899/35/3/035106
2008HE09 Nucl.Phys. A806, 117 (2008) Temporal variation of the fine structure constant and the strong interaction parameter in the 229Th transition NUCLEAR STRUCTURE 209Pb, 209Bi, 229Th; calculated ground and excited state energies based on relative mean field theory.
doi: 10.1016/j.nuclphysa.2008.03.002
2008HE18 Int.J.Mod.Phys. E17, Supplement 1, 208 (2008) Particle-number conserving treatment for the ground state bands in even-even transfermium nuclei NUCLEAR STRUCTURE 250Fm, 252,254No; calculated ground state and high-spin bands, J, π. Cranked shell model.
doi: 10.1142/S0218301308011860
2007BA76 Chin.Phys.Lett. 24, 3384 (2007) Z.Bai, Q.Wang, J.-L.Han, ZG.Xiao, H.-S.Xu, Z.-Y.Sun, Z.-G.Hu, X.-Y.Zhang, H.-W.Wang, R.-S.Mao, X-H.Yuan, Z.-G.Xu, H.-B.Zhang, H.-G.Xu, H.-R.Qi, Y.Wang, F.Jia, L.-J.Wu, X.-L.Ding, Q.Gao, H.Gao, S.-L.Li, J.-Q.Li, Y.-P.Zhang, G.-Q.Xiao, G.-M.Jin, Z.-Z.Ren, S.-G.Zhou, W.Xu, G.-T.Fan, S.-Q.Zhang, D.-Y.Pang, Y.-K.Sergey Angular Dispersion and Deflection Function for Heavy Ion Elastic Scattering NUCLEAR REACTIONS 208Pb(17F, 17F), E=141 MeV; 208Pb(17O, 17O), E=128 MeV; measured differential cross sections, angular dispersion plots. 208Pb(16O, 16O), E=170.1 MeV; 208Pb(6He, 6He), E=27, 29.6 MeV; 208Pb(6Li, 6Li), E=73.7, 99 MeV; 208Pb(α, α), E=40 MeV; analyzed differential cross sections, angular dispersion plots.
doi: 10.1088/0256-307X/24/12/027
2007FA11 Chin.Phys.Lett. 24, 2555 (2007) A Simple Systematical Law of E2+1 Values for Heavy Nuclei in the NpNn Scheme and the Evolution of the Z = 64 Shell Gap NUCLEAR STRUCTURE Z ≥ 120; calculated excitation energy of the first 2+ state for even-even nuclei.
doi: 10.1088/0256-307X/24/9/025
2007FA16 Phys.Rev. C 76, 031601 (2007) D.Q.Fang, W.Guo, C.W.Ma, K.Wang, T.Z.Yan, Y.G.Ma, X.Z.Cai, W.Q.Shen, Z.Z.Ren, Z.Y.Sun, J.G.Chen, W.D.Tian, C.Zhong, M.Hosoi, T.Izumikawa, R.Kanungo, S.Nakajima, T.Ohnishi, T.Ohtsubo, A.Ozawa, T.Suda, K.Sugawara, T.Suzuki, A.Takisawa, K.Tanaka, T.Yamaguchi, I.Tanihata Examining the exotic structure of the proton-rich nucleus 23Al NUCLEAR REACTIONS 12C(23Al, p), E=74 MeV/nucleon; measured fragment longitudinal momentum distributions. 12C(23Al, X), (24Al, X), (24Al, X), E=74 MeV/nucleon; measured reaction cross sections. Compared results to model calculations.
doi: 10.1103/PhysRevC.76.031601
2007GU03 Chin.Phys.Lett. 24, 652 (2007) Structures of Light Neutron-Rich Nuclei with Orbit-Orbit Coupling NUCLEAR STRUCTURE 11,12,13Be, 12,13,14B, 13,14,15C, 14,15,16N, 15,16,17O; calculated radii, density distributions, single-particle energies. Single-particle shell model, orbit-orbit coupling.
doi: 10.1088/0256-307X/24/3/018
2007HE17 J.Phys.(London) G34, 1611 (2007) Enhanced sensitivity to variation of fundamental constants in the transitions of 229Th and 249Bk NUCLEAR STRUCTURE 229Th, 249Bk; calculated transition frequencies between the first excited and ground states, including their sensitivity to the temporal variation of the strong and fine structure constant.
doi: 10.1088/0954-3899/34/7/003
2007LI05 Chin.Phys.Lett. 24, 660 (2007) J.-Y.Liu, G.-Q.Xiao, W.-J.Guo, Z.-Z.Ren, W.Zuo, X.-G.Lee Sensitive Probe for Symmetry Potential NUCLEAR REACTIONS 9Be(6He, X), (8He, X), (6Li, X), (8Li, X), E=10-100 MeV/nucleon; calculated neutron/proton emission ratio, sensitivity to symmetry potential. NUCLEAR STRUCTURE 6,8He, 6,8Li; calculated binding energies, radii, density distributions.
doi: 10.1088/0256-307X/24/3/020
2007RE06 J.Radioanal.Nucl.Chem. 272, 209 (2007) Z.Z.Ren, Y.C.Mao, Q.J.Zhi, C.Xu, T.K.Dong Systematical calculations on the ground state properties of heavy and superheavy nuclei RADIOACTIVITY 260,262,264,266,268,270,272,274,276Sg, 262,264,266,268,270,272,274,276,278Hs(α); calculated Eα, T1/2. 260,261,262,263,264,265,266,267,268Sg(SF); calculated T1/2. Z=106-118; calculated α-decay T1/2.
doi: 10.1007/s10967-007-0501-x
2006GU28 Int.J.Mod.Phys. E15, 1523 (2006) W.Guo, D.Q.Fang, Y.G.Ma, C.W.Ma, K.Wang, T.Z.Yan, X.Z.Cai, W.Q.Shen, Z.Y.Sun, Z.Z.Ren, J.G.Chen, J.H.Chen, G.H.Liu, E.J.Ma, G.L.Ma, Y.Shi, Q.M.Su, W.D.Tian, H.W.Wang, C.Zhong, J.X.Zuo, M.Hosoi, T.Izumikawa, R.Kanungo, S.Nakajima, T.Ohnishi, T.Ohtsubo, A.Ozawa, T.Suda, K.Sugawara, T.Suzuki, A.Takisawa, K.Tanaka, T.Yamaguchi, I.Tanihata Measurements of reaction cross section and fragment momentum distribution for N=10 proton-rich isotones NUCLEAR REACTIONS 12C(23Al, 22MgX), (24Al, 23MgX), (22Mg, 21NaX), (21Na, 20NeX), E not given; measured fragment parallel momentum distribution following one-proton removal. 12C(23Al, X), (24Al, X), E not given; measured reaction σ.
doi: 10.1142/S0218301306005101
2006JI02 Chin.Phys.Lett. 23, 812 (2006) Half-Lives of Spherical Proton Emitters RADIOACTIVITY 105Sb, 145,146,146m,147,147mTm, 150,150m,151,151mLu, 155,156,156m,157Ta, 160,161,161mRe, 164,165,166,166m,167,167mIr, 171,171mAu, 177,177mTl, 185Bi(p); calculated proton decay T1/2, Q. DWBA method, comparison with data.
doi: 10.1088/0256-307X/23/4/014
2006LI31 Int.J.Mod.Phys. E15, 1069 (2006) J.-Ye.Liu, W.-J.Guo, Z.Z.Ren, W.Zuo, X.-G.Lee, Y.-Z.Xing Average property of fragmentation reaction and momentum dissipation induced by halo-nuclei in heavy ion collisions NUCLEAR REACTIONS 48Ca(11Li, X), (11B, X), (14Be, X), (14N, X), (19B, X), (19F, X), (23Al, X), (23Na, X), E ≈ 10-160 MeV/nucleon; calculated fragment multiplicities, time evolution features, nuclear stopping; deduced halo effects. Isospin-dependent quantum molecular dynamics.
doi: 10.1142/S0218301306004752
2006LI37 Chinese Physics 15, 1738 (2006) J.-Y.Liu, W.-J.Guo, Z.-Z.Ren, Y.-Z.Xing, W.Zuo, X.-G.Lee Isospin- and momentum-dependent interaction in isospin-dependent quantum molecular dynamics NUCLEAR REACTIONS 44Ar(44Ar, X), 89Kr(89Kr, X), 94Kr(94Kr, X), 94Zr(94Zr, X), 94Mo(94Mo, X), 94Ru(94Ru, X), 124Sn(124Sn, X), E=50 MeV/nucleon; calculated fragments isospin fractionation ratios, related features. Isospin-dependent quantum molecular dynamics, isospin- and momentum-dependent interaction.
doi: 10.1088/1009-1963/15/8/018
2006MA96 High Energy Phys. and Nucl.Phys. (China), Supplement 2, 30, 186 (2006) C.-W.Ma, D.-Q.Fang, W.Guo, K.Wang, T.-Z.Yan, Y.-G.Ma, X.-Z.Cai, W.-Q.Shen, Z.-Y.Sun, Z.-Z.Ren, J.-G.Chen, W.-D.Tian, H.-W.Wang, E.-J.Ma, G.-H.Liu, Y.Shi, Q.-M.Su, C.Zhong, M.Hosoi, T.Izumikawa, R.Kanungo, S.Nakajima, T.Ohnishi, T.Ohtsubo, T.Suda, K.Sugawara, T.Suzuki, A.Ozawa, A.Takisawa, K.Tanaka, T.Yamaguchi, I.Tanihata Study of Exoticness of Proton-Rich Nuclei 23Al and it's Neighboring Nuclei
2006WA17 Chin.Phys.Lett. 23, 1731 (2006) Q.Wang, J.-L.Han, Z.-G.Xiao, H.-S.Xu, Z.-Yu.Sun, Z.-G.Hu, X.-Y.Zhang, H.-W.Wang, R.-S.Mao, X.-H.Yuan, Z.-G.Xu, T.-C.Zhao, H.-B.Zhang, H.-G.Xu, H.-R.Qi, Y.Wang, F.Jia, L.-J.Wu, X.-L.Ding, Q.Gao, H.Gao, S.-L.Li, Z.Bai, G.-Q.Xiao, G.-M.Jin, Z.-Z.Ren, S.-G.Zhou, Yu.-K.Sergey Exotic Behaviour of Angular Dispersion of Weakly Bound Nucleus 17F at Small Angles NUCLEAR REACTIONS 208Pb(17F, 17F), E=141 MeV; 208Pb(17O, 17O), E=128 MeV; measured σ(θ); deduced possible halo effects.
doi: 10.1088/0256-307X/23/7/021
2006ZH01 Chin.Phys.Lett. 23, 58 (2006) Deformations and B(E2) Values of Ne and Mg Nuclei around N = 20 NUCLEAR STRUCTURE 26,28,30,32,34Ne, 28,30,32,34,36Mg; calculated binding energies, deformation parameters, B(E2). Macroscopic-microscopic model, isospin-dependent Nilsson potential, comparison with data.
doi: 10.1088/0256-307X/23/1/018
2005CH02 Eur.Phys.J. A 23, 11 (2005) J.G.Chen, X.Z.Cai, W.Q.Shen, Y.G.Ma, Z.Z.Ren, H.Y.Zhang, W.Z.Jiang, C.Zhong, Y.B.Wei, W.Guo, X.F.Zhou, K.Wang, G.L.Ma Halo or skin in the excited states of some light mirror nuclei NUCLEAR STRUCTURE 13C, 13,15N, 15O, 21Ne, 21Na; calculated binding energies, radii, density distributions; deduced halo features. Nonlinear relativistic mean-field approach, comparison with data.
doi: 10.1140/epja/i2004-10074-0
2005CH71 Chinese Physics 14, 2444 (2005) J.-G.Chen, X.-Z.Cai, T.-T.Wang, Yu.-G.Ma, Z.-Z.Ren, D.-Q.Fang, C.Zhong, Yi.-B.Wei, W.Guo, X.-F.Zhou, K.Wang, G.-L.Ma, W.-D.Tian, J.-H.Chen, T.-Z.Yan, J.-X.Zuo, C.-W.Ma, W.-Q.Shen Investigation on the deformation of Ne and Mg isotope chains within relativistic mean-field model NUCLEAR STRUCTURE 18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36Ne, 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44Mg; calculated deformations, binding energies, shape coexistence features. Relativistic mean-field model, comparison with data.
doi: 10.1088/1009-1963/14/12/013
2005JI06 Eur.Phys.J. A 25, 29 (2005) W.Z.Jiang, Z.Z.Ren, T.T.Wang, Y.L.Zhao, Z.Y.Zhu Relativistic mean-field study for Zn isotopes NUCLEAR STRUCTURE 52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75Zn; calculated binding energies, radii, deformation. Relativistic mean-field approach.
doi: 10.1140/epja/i2004-10235-1
2005LI22 Phys.Lett. B 617, 24 (2005) J.Y.Liu, W.J.Guo, Z.Z.Ren, Y.Z.Xing, W.Zuo, X.G.Lee Special roles of loose neutron-halo nucleus structure on the fragmentation and momentum dissipation in heavy ion collisions NUCLEAR STRUCTURE 19B, 19F; calculated neutron and proton density distributions, radii. NUCLEAR REACTIONS 48Ca(19B, X), (19F, X), E=30-150 MeV/nucleon; calculated fragmentation multiplicities, nuclear stopping, time evolution features; deduced halo effect. Isospin-dependent quantum molecular dynamics.
doi: 10.1016/j.physletb.2005.05.011
2005TA08 Chin.Phys.Lett. 22, 843 (2005) F.Tai, D.-H.Chen, C.Xu, Z.-Z.Ren Ground State Properties of New Element Z = 113 and Its Alpha Decay Chain RADIOACTIVITY 278Nh, 274Rg, 270Mt, 266Bh(α); calculated Qα, T1/2. NUCLEAR STRUCTURE 278Nh, 274Rg, 270Mt, 266Bh, 262Db; calculated binding energies, deformation parameters. Several models compared with data.
doi: 10.1088/0256-307X/22/4/018
2004CH60 Chin.Phys.Lett. 21, 2140 (2004) J.-G.Chen, X.-Z.Cai, T.-T.Wang, Y.-G.Ma, Z.-Z.Ren, D.-Q.Fang, C.Zhong, Y.-B.Wei, W.Guo, X.-F.Zhou, K.Wang, G.-L.Ma, W.-D.Tian, J.-X.Zuo, C.-W.Ma, J.-H.Chen, T.-Z.Yan, W.-Q.Shen Investigation of Exotic Structure of the Largely Deformed Nucleus 23Al in the Relativistic-Mean-Field Model NUCLEAR STRUCTURE 23Al; calculated ground-state binding energy, quadrupole deformation, radii, one- and two-proton separation energies, excited states energies, J, π, configurations. 20Ne, 21Na, 22Mg; calculated ground-state quadrupole deformations. Deformed relativistic mean field model.
doi: 10.1088/0256-307X/21/11/018
2004GA62 High Energy Phys. and Nucl.Phys. (China) 28, 332 (2004) Z.-G.Gan, H.-M.Fan, Z.Qin, X.-L.Wu, J.-S.Guo, X.-G.Lei, C.-F.Dong, H.-G.Xu, R.-F.Chen, F.-M.Zhang, B.Guo, H.-Y.Liu, H.-L.Wang, C.-Y.Xie, Z.-Q.Feng, Y.Zheng, L.-T.Song, P.Luo, H.-S.Xu, X.-H.Zhuo, G.-M.Jin, Z.-Z.Ren First Observation for Isotope 265Bh(Z=107)
2003CH33 Chin.Phys.Lett. 20, 1021 (2003) J.-G.Chen, X.-Z.Cai, H.-Y.Zhang, W.-Q.Shen, Z.-Z.Ren, W.-Z.Jiang, Y.-G.Ma, C.Zhong, Y.-B.Wei, W.Guo, X.-F.Zhou, G.-L.Ma, K.Wang Proton Halo or Skin in the Excited States of Light Nuclei NUCLEAR STRUCTURE 9B, 13,15N; calculated binding energies, excited states energies, density distributions. Relativistic mean-field approach.
doi: 10.1088/0256-307X/20/7/314
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