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NSR database version of April 11, 2024.

Search: Author = Z.Z.Ren

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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
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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
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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
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2024YA04      Phys.Rev.Lett. 132, 072502 (2024)

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

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

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

RADIOACTIVITY 160Os(α), 156W(β+); measured decay products, Eα, Iα; deduced α-particles energies, Q-values, 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
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2024ZH04      Phys.Rev. C 109, 014608 (2024)

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

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

doi: 10.1103/PhysRevC.109.014608
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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
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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
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2022LU02      Nucl.Phys. A1021, 122408 (2022)

H.Lu, Z.z.Ren, D.Bai

Neutron-neutron short-range correlations and their impacts on neutron stars

doi: 10.1016/j.nuclphysa.2022.122408
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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-α1234 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
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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
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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
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2022ZH45      Phys.Rev. C 106, 024305 (2022)

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

Fine structure in the α decay of the 8+ isomer in 216, 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)α12-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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0273. Data from this article have been entered in the XUNDL database. For more information, click here.


2021QI03      Chin.Phys.C 45, 021002 (2021)

Y.-B.Qian, Z.-Z.Ren

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
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2021ZH22      Phys.Rev.Lett. 126, 152502 (2021)

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

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

RADIOACTIVITY 214,216,218U(α) [from 180,182W(36Ar, 4n), 184W(40Ca, 2nα), E<200 MeV]; measured decay products, Eα, Iα; deduced α-decay Q-values and reduced widths, 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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0279. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0220. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0209. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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2018BA43      Chin.Phys.C 42, 124102 (2018)

D.Bai, Z.-Z.Ren

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
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2018NI12      Chin.Phys.C 42, 114104 (2018)

D.-D.Ni, Z.-Z.Ren

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
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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
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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
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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
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2017LI46      Phys.Rev. C 96, 065503 (2017)

H.Li, Z.z.Ren

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
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2017NI16      Chin.Phys.C 41, 114104 (2017)

D.-D.Ni, Z.-Z.Ren

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
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2017TA10      Chin.Phys.C 41, 054103 (2017)

W.Tan, D.-d.Ni, Z.-z.Ren

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
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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
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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
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2016QI02      Eur.Phys.J. A 52, 68 (2016)

Y.Qian, Z.-z.Ren

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
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2016YU04      Phys.Lett. B 762, 237 (2016)

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

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

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

doi: 10.1016/j.physletb.2016.09.030
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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
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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
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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
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2015NI10      Phys.Rev. C 92, 034324 (2015)

D.d.Ni, Z.z.Ren

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


2013CA04      Chin.Phys.C 37, 034103 (2013)

D.-L.Cao, Z.-Z.Ren, T.-K.Dong

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
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2013NI01      Chin.Phys.Lett. 30, 022101 (2013)

D.-D.Ni, Z.-Z.Ren

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
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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
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2012CH48      J.Phys.(London) G39, 125105 (2012)

D.-D.Ni, Z.-Z.Ren

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
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2012DO14      J.Phys.:Conf.Ser. 381, 012135 (2012)

T.K.Dong, Y.Y.Chu, Z.Z.Ren

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
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2012NI02      Rom.J.Phys. 57, 407 (2012)

D.D.Ni, Z.Z.Ren

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)

Y.Ren, Z.-Z.Ren

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
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2012XU11      Chin.Phys.Lett. 29, 122102 (2012)

C.Xu, Z.-Z.Ren

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
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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
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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
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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
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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
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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
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2011SH13      J.Phys.(London) G38, 055103 (2011)

Z.-q.Sheng, D.-d.Ni, Z.-z.Ren

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
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2011WA16      Phys.Rev. C 84, 014609 (2011)

C.Wang, J.Zhang, Z.Z.Ren

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
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2010GU15      Chin.Phys.Lett. 27, 102102 (2010)

Y.-Q.Guo, Z.-Z.Ren

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
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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
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2010QI03      Chin.Phys.Lett. 27, 072301 (2010)

Y.-B.Qian, Z.-Z.Ren, D.-D.Ni

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
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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
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2010SH32      Eur.Phys.J. A 46, 241 (2010)

Z.-q.Sheng, Z.-z.Ren

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
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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
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2009CH69      Chin.Phys.C 33, 639 (2009)

S.Chen, Y.-Y.Chu, Z.-Z.Ren

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
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2009DO22      Chin.Phys.C 33, Supplement 1, 5 (2009)

T.-K.Dong, Z.-Z.Ren, C.Xu

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
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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
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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
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2008DO13      Chin.Phys.Lett. 25, 2425 (2008)

T.-K.Dong, Z.-Z.Ren

Parity Violating Electron Scattering in the Relativistic Eikonal Approximation

doi: 10.1088/0256-307X/25/7/026
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2008HE02      J.Phys.(London) G35, 035106 (2008)

X.-t.He, Z.-z.Ren

Enhanced sensitivity to variation of fundamental constants in the narrow nuclear transitions (II)

doi: 10.1088/0954-3899/35/3/035106
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2008HE09      Nucl.Phys. A806, 117 (2008)

X.-T.He, Z.-Z.Ren

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
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2008HE18      Int.J.Mod.Phys. E17, Supplement 1, 208 (2008)

X.T.He, Z.-Z.Ren

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0200.


2007FA11      Chin.Phys.Lett. 24, 2555 (2007)

Z.-Y.Fan, Z.-Z.Ren, C.Xu

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2047.


2007GU03      Chin.Phys.Lett. 24, 652 (2007)

Y.-Q.Guo, Z.-Z.Ren

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
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2007HE17      J.Phys.(London) G34, 1611 (2007)

X.T.He, Z.-Z.Ren

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2047.


2006JI02      Chin.Phys.Lett. 23, 812 (2006)

J.-G.Jiang, Z.-Z.Ren

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
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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
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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
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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
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2006ZH01      Chin.Phys.Lett. 23, 58 (2006)

Q.-J.Zhi, Z.-Z.Ren

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
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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
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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
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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
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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
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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
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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
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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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