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NSR database version of April 11, 2024.

Search: Author = C.Lin

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2024DA03      Phys.Rev. C 109, 024617 (2024)

F.C.Dai, P.W.Wen, C.J.Lin, J.J.Liu, X.X.Xu, K.L.Wang, H.M.Jia, L.Yang, N.R.Ma, F.Yang

Theoretical study of multinucleon transfer reactions by coupling the Langevin dynamics iteratively with the master equation

doi: 10.1103/PhysRevC.109.024617
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2023LI06      Phys.Rev. C 107, 014320 (2023)

Z.Li, J.Zhu, T.Wang, M.Liu, J.Wang, Y.Yang, C.Lin, J.Ma, P.Ma, Z.Bai, Y.Yu, X.Zhang, X.Liu, F.Duan, C.G.Lu, H.Yang, X.Wei, J.Zhang, S.Jin, Z.Gao, Y.Hu, Y.Yao, J.Wang, S.Guo, W.Jiang, B.Yang, J.He

Cluster structure of 11C investigated with a breakup reaction

NUCLEAR REACTIONS 12C(11C, α)7Be, E=25 MeV/nucleon; measured reaction products, Eα, Iα, Eγ, Iγ, αγ-coin, (particle)α-coin; deduced invariant-mass spectra, exclusive σ, excitation functions. 11C; deduced resonances, J, π, rotational bands, rotational parameter. Provided evidence for 2α+3He structure. DSSD-CsI(Tl) telescopes and scintillator detectors (LaBr:Ce3 and NaI(Tl)) at heavy ion research facility in Lanzhou (HIRFL-RIBLL1).

doi: 10.1103/PhysRevC.107.014320
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2023LU04      Phys.Rev. C 108, 014302 (2023)

H.Y.Lu, Z.Liu, Z.H.Li, X.Wang, J.Li, H.Hua, H.Huang, W.Q.Zhang, Q.B.Zeng, X.H.Yu, T.H.Huang, M.D.Sun, 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, C.J.Lin, L.J.Sun, N.R.Ma, H.S.Xu, X.H.Zhou, G.Q.Xiao, F.S.Zhang

Reinvestigation of 222U in high-precision digital α-decay spectroscopy: Solution to the reduced decay-width anomaly

RADIOACTIVITY 222U(α) [from 186W(40Ar, 4n), E=80 MeV, followed by separation of fragments using SHANS separator at HRIFL-Lanzhou]; 218Th, 214Ra(α)[from 222U α decay chain]; measured Eα, Iα, evaporation residues (ER)-α correlations, T1/2 using DSSD detectors; deduced reduced α-decay width, and analyzed using NpNn scheme. 218Ac, 219Th, 220Pa(α); measured Eα, and T1/2. Systematics of reduced α-decay widths for g.s. to g.s. α transitions in even-even Z=84-92, N≥126 isotopes as function of NpNn. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.108.014302
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Data from this article have been entered in the XUNDL database. For more information, click here.


2023MA57      Chin.Phys.C 47, 114001 (2023)

K.Ma, Y.-L.Ye, Ch.-J.Lin, J.-H.Chen, D.-X.Wang, J.-X.Han, H.-M.Jia, L.Yang, L.-Sh.Yang, Z.-Y.Hu, Y.Chen, W.-L.Pu, G.Li, Zh.-W.Tan, D.-H.Huang, T.-P.Luo, Sh.-H.Zhong, J.-L.Lou, X.-F.Yang, Zh.-H.Li, Q.-T.Li, J.-Y.Xu, Z.-H.Yang, K.Wei

New measurement of 4He and proton decays from resonant states in 19Ne

RADIOACTIVITY 19N(p), (α) [from 6Li(16O, X)19Ne, E=96 MeV]; measured decay products, Ep, Ip, Eα, Iα; deduced excitation-energy spectra, level energies, resonance parameters for astrophysical applications. The HI-13 tandem accelerator facility at the China Institute of Atomic Energy, Beijing.

doi: 10.1088/1674-1137/acc16f
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Data from this article have been entered in the XUNDL database. For more information, click here.


2023WA01      Chin.Phys.C 47, 014001 (2023)

D.-X.Wang, Y.-L.Ye, C.-J.Lin, J.-H.Chen, K.Ma, J.-X.Han, H.-M.Jia, L.Yang, L.-S.Yang, Z.-Y.Hu, Y.Chen, W.-L.Pu, G.Li, Z.-W.Tan, H.-Y.Zhu, T.-P.Luo, S.-H.Zhong, D.-H.Huang, J.-L.Lou, X.-F.Yang, Q.-T.Li, J.-Y.Xu, Z.-H.Yang, K.Wei

α-cluster decay from 24Mg resonances produced in the 12C(16O, 24Mg)α reaction

RADIOACTIVITY 24Mg(α) [from 12C(16O, 24Mg), E=96 MeV]; measured decay products, Eα, Iα; deduced resonant states, the energy-momentum of a 20Ne fragment, resonance parameters. Comparison with available data, theoretical calculations. The HI-13 tandem accelerator at the China Institute of Atomic Energy (CIAE) in Beijing.

doi: 10.1088/1674-1137/ac9e9a
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2023YA32      Chin.Phys.C 47, 124104 (2023)

Y.Yang, P.-W.Wen, Ch.-J.Lin, H.-M.Jia, L.Yang, N.-Ru.Ma, F.Yang, T.-P.Luo, T.-H.Mo, Ch.Chang, H.-R.Duan, M.-H.Zhang, Zh.-J.Huang, Ch.Yin

Systematic extraction of the strong absorption distance and Coulomb barrier from elastic scattering

NUCLEAR REACTIONS 58Ni(16O, 16O), (8B, 8B), 64Ni(6Li, 6Li), E=10-40 MeV; analyzed available data. 11Be, 8B, 8He, 11Li; deduced σ, reduced strong absorption distance, Coulomb barrier radius.

doi: 10.1088/1674-1137/acf7b8
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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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2022HI12      Phys.Rev. C 106, 064614 (2022)

D.J.Hinde, R.du Rietz, D.Y.Jeung, K.J.Cook, M.Dasgupta, E.C.Simpson, R.G.Thomas, M.Evers, C.J.Lin, D.H.Luong, L.R.Gasques, R.Rafiei, A.Wakhle, C.Simenel

Experimental investigation of the role of shell structure in quasifission mass distributions

NUCLEAR REACTIONS 154Sm, 162Dy, 170Er, 174Yb, 186W, 192Os, 196Pt, 200Hg(48Ti, F), E=198-245 MeV; measured reaction products; deduced fission fragment mass-angle distributions, ratio of the fusion-fission yield to the total fission yield, mass-ratio spectra, compound nuclei forming probability. Pointed that with increasing target (or equivalently compound nucleus)atomic number, a rapid transition occurs from dominant fusion-fission to dominantly quasifission. Comparison to GEF calculations. Position-sensitive multiwire proportional counters (MWPCs) at 14UD tandem electrostatic accelerator (Australian National University).

doi: 10.1103/PhysRevC.106.064614
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2022WE02      Phys.Rev. C 105, 034606 (2022)

P.W.Wen, C.J.Lin, H.M.Jia, L.Yang, F.Yang, D.H.Huang, T.P.Luo, C.Chang, M.H.Zhang, N.R.Ma

New Coulomb barrier scaling law with reference to the synthesis of superheavy elements

NUCLEAR REACTIONS 198Pt, 208Pb, 209Bi, 249Cm(136Xe, X), 198Pt(204Hg, X), 208Pb, 238U, 248Cm, 249Cf(238U, X), E not given; deduced Coulomb barrier height. Barrier information is extracted from the experimental fusion excitation functions by the empirical cross section formula, which is based on a single-Gaussian distribution of fusion barrier heights.

doi: 10.1103/PhysRevC.105.034606
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2021JI16      Symmetry 13, 2278 (2021)

H.Jian, Y.Gao, F.Dai, J.Liu, X.Xu, C.Yuan, K.Kaneko, Y.Sun, P.Liang, G.Shi, L.Sun, L.Xayavong, C.Lin, J.Lee, Z.Li, Y.Yang, P.Li, R.Fan, S.Zha, H.Zhu, J.Li, Q.Gao, Z.Zhang, R.Chen, J.Wang, D.Wang, H.Wu, K.Wang, Y.Lam, F.Duan, P.Ma, Z.Gao, Q.Hu, Z.Bai, J.Ma, J.Wang, F.Zhong, C.Wu, D.Luo, Y.Jiang, Y.Liu, D.Hou, R.Li, N.Ma, W.Ma, G.Yu, D.Patel, S.Jin, Y.Wang, Y.Yu, Q.Zhou, P.Wang, L.Hu, X.Wang, H.L.Zang, Q.Zhao, L.Yang, P.Wen, F.Yang, H.Jia, G.Zhang, M.Pan, X.Wang, H.Sun, M.Wang, Z.Hu, X.Zhou, Y.Zhang, H.Xu, M.Liu, H.-J.Ong, W.Yang

β-Delayed γ Emissions of 26P and Its Mirror Asymmetry

RADIOACTIVITY 26P(β+), (EC) [from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation using RIBBL1 at HRIBF, Lanzhou facility]; measured Eγ, Iγ, βγ-coin, T1/2 of 26P decay. 26Si; deduced levels, J, π, β++ϵ feedings, logft, mirror asymmetry parameter from comparison with the ϵ decay of mirror nucleus 26Na to 26Mg, mirror-energy differences (MEDs), and halo structure in 26P. Comparison with shell-model calculations.

NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P/27S, E=80.6 MeV/nucleon; measured reaction products, particle-identification (PID) plot of ΔE vs TOF for the ions separated using RIBBL1 separator at HRIBF, Lanzhou facility.

doi: 10.3390/sym13122278
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2021RO14      Eur.Phys.J. A 57, 143 (2021)

C.H.Rong, J.Rangel, Y.S.Wu, G.L.Zhang, G.X.Zhang, C.J.Lin, E.N.Cardozo, X.Y.Wang, L.Yang, N.R.Ma, D.X.Wang, L.J.Sun, H.M.Jia, F.Yang, J.S.Wang, Y.Y.Yang, J.B.Ma, P.Ma, Z.Bai, S.W.Xu, F.F.Duan, X.B.Qin, H.M.Zhao, J.Lubian

Study of quasi-elastic scattering of 17F+208Pb at energies around Coulomb barrier

NUCLEAR REACTIONS 208Pb(17F, 17F), E=94.5 MeV; measured reaction products. 17F; deduced σ(θ), σ. Comparison with continuum discretized coupled channel method (CDCC) calculations.

doi: 10.1140/epja/s10050-021-00454-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0269.


2021SH23      Phys.Rev. C 103, L061301 (2021)

G.Z.Shi, J.J.Liu, Z.Y.Lin, H.F.Zhu, X.X.Xu, L.J.Sun, P.F.Liang, C.J.Lin, J.Lee, C.X.Yuan, S.M.Wang, Z.H.Li, H.S.Xu, Z.G.Hu, Y.Y.Yang, R.F.Chen, J.S.Wang, D.X.Wang, H.Y.Wu, K.Wang, F.F.Duan, Y.H.Lam, P.Ma, Z.H.Gao, Q.Hu, Z.Bai, J.B.Ma, J.G.Wang, F.P.Zhong, C.G.Wu, D.W.Luo, Y.Jiang, Y.Liu, D.S.Hou, R.Li, N.R.Ma, W.H.Ma, G.M.Yu, D.Patel, S.Y.Jin, Y.F.Wang, Y.C.Yu, Q.W.Zhou, P.Wang, L.Y.Hu, X.Wang, H.L.Zang, P.J.Li, Q.R.Gao, H.Jian, S.X.Zha, F.C.Dai, R.Fan, Q.Q.Zhao, L.Yang, P.W.Wen, F.Yang, H.M.Jia, G.L.Zhang, M.Pan, X.Y.Wang, H.H.Sun, X.H.Zhou, Y.H.Zhang, M.Wang, M.L.Liu, H.J.Ong, W.Q.Yang

β-delayed two-proton decay of 27S at the proton-drip line

RADIOACTIVITY 27S(β+2p)[from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation and purification of fragments using RIBLL1 at HIRFL-Lanzhou facility, and implanted into three W1-type double-sided silicon strip detectors (DSSDs)]; measured reaction products, E(p), I(p), pp-coin, p(θ), half-life of 27S decay using Si detectors surrounded by HPGe detectors; deduced branching ratio of β+2p decay, identified as a two-proton transition, dominantly sequential, via the isobaric-analog state (IAS) in 27P to the ground state of 25Al.

doi: 10.1103/PhysRevC.103.L061301
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021ST19      Eur.Phys.J. A 57, 334 (2021)

V.Starastsin, A.Demyanova, A.Danilov, A.Ogloblin, S.Dmitriev, S.Goncharov, Ch.-J.Lin, L.Yang, D.-X.Wang, H.-M.Jia, F.-P.Zhong, F.Yang, Y.-J.Yao, Sh.-H.Zhong, P.-W.Wen, N.R.Ma, H.-Q.Zhang, D.Janseitov, N.Burtebayev, S.Khlebnikov, G.Adamian, N.Antonenko

Structures of the excited states in 9Be studied by scattering of 23 MeV deuterons

NUCLEAR REACTIONS 9Be(d, d), E=23 MeV; measured reaction products; deduced σ(θ), excited state energies, J, π, resonance widths, B(Eλ), form factors. The distorted wave Born approximation (DWBA) and modified diffraction model (MDM).

doi: 10.1140/epja/s10050-021-00643-0
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2021WE07      Phys.Rev. C 103, 054601 (2021)

P.W.Wen, C.J.Lin, R.G.Nazmitdinov, S.I.Vinitsky, O.Chuluunbaatar, A.A.Gusev, A.K.Nasirov, H.M.Jia, A.Gozdz

Potential roots of the deep subbarrier heavy-ion fusion hindrance phenomenon within the sudden approximation approach

NUCLEAR REACTIONS 100Mo(64Ni, X), E=120-160 MeV; 64Ni(64Ni, X), E=85-110 MeV; 64Ni(28Si, X), E=120-160 MeV; 12C(12C, X), E=1-6 MeV; calculated fusion cross sections σ(E) and astrophysical S(E) factors using improved coupled-channels (CC) by finite element method and incoming wave boundary conditions (IWBCs), with the Woods-Saxon potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.103.054601
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2021YA01      Phys.Lett. B 813, 136045 (2021)

L.Yang, C.J.Lin, H.Yamaguchi, J.Lei, P.W.Wen, M.Mazzocco, N.R.Ma, L.J.Sun, D.X.Wang, G.X.Zhang, K.Abe, S.M.Cha, K.Y.Chae, A.Diaz-Torres, J.L.Ferreira, S.Hayakawa, H.M.Jia, D.Kahl, A.Kim, M.S.Kwag, M.La Commara, R.Navarro-Perez, C.Parascandolo, D.Pierroutsakou, J.Rangel, Y.Sakaguchi, C.Signorini, E.Strano, X.X.Xu, F.Yang, Y.Y.Yang, G.L.Zhang, F.P.Zhong, J.Lubian

Insight into the reaction dynamics of proton drip-line nuclear system 17F+58Ni at near-barrier energies

NUCLEAR REACTIONS 58Ni(17F, 17F), (17F, X), E=43.6, 47.5, 55.7, 63.1 MeV; measured reaction products, Eα, Iα, Ep, Ip. 16O, 17F; deduced σ, σ(θ) quasielastic scattering and fusion.

doi: 10.1016/j.physletb.2020.136045
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2687.


2021YA16      Chin.Phys.C 45, 054104 (2021)

Y.-J.Yao, C.-J.Lin, L.Yang, N.-R.Ma, D.-X.Wang, G.-l.Zhang, G.-X.Zhang, H.-M.Jia, F.Yang, F.-P.Zhong, P.i-W.Wen, X.-B.Qin, H.-M.Zhao

Relative probabilities of breakup channels in reactions of 6, 7Li with 209Bi at energies around and above the Coulomb barrier

NUCLEAR REACTIONS 209Bi(6Li, X), (7Li, X), E=30, 40, 47 MeV; measured reaction products, Eα, Iα, Ep, Ip, α-p coin., α-α-coin.; deduced σ(E), relative probabilities of the breakup channels.

doi: 10.1088/1674-1137/abe3ee
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2021YU04      Chin.Phys.C 45, 084002 (2021)

H.-z.Yu, J.Li, Y.-L.Ye, B.Yang, C.-J.Lin, H.-M.Jia, J.-L.Lou, X.-F.Yang, T.Baba, Q.-T.Li, Y.-C.Ge, Z.-H.Li, H.Hua, J.-Y.Xu, Z.-H.Yang, J.Feng, H.-L.Zang, Q.Liu, W.Jiang, Y.Liu, J.-J.Li, W.Liu, S.-W.Bai, J.Chen, J.-X.Han, J.-H.Chen, K.Ma, D.-X.Wang, L.Yang, N.-R.Ma, L.-J.Sun

Novel evidence for the σ-bond linear-chain molecular structure in 14C

NUCLEAR REACTIONS 7Li(11B, α)14C, E=55 MeV; measured reaction products, Eα, Iα. 4He, 10Be; deduced Q-values, energy levels, J, π. Comparison with theoretically predicted band head of the positive-parity σ-bond linear-chain molecular band.

doi: 10.1088/1674-1137/ac04a0
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Data from this article have been entered in the XUNDL database. For more information, click here.


2020DU18      Phys.Lett. B 811, 135942 (2020)

F.F.Duan, Y.Y.Yang, K.Wang, A.M.Moro, V.Guimaraes, D.Y.Pang, J.S.Wang, Z.Y.Sun, J.Lei, A.Di Pietro, X.Liu, G.Yang, J.B.Ma, P.Ma, S.W.Xu, Z.Bai, X.X.Sun, Q.Hu, J.L.Lou, X.X.Xu, H.X.Li, S.Y.Jin, H.J.Ong, Q.Liu, J.S.Yao, H.K.Qi, C.J.Lin, H.M.Jia, N.R.Ma, L.J.Sun, D.X.Wang, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu

Scattering of the halo nucleus 11Be from a lead target at 3.5 times the Coulomb barrier energy

NUCLEAR REACTIONS 208Pb(11Be, 11Be), (11Be, X), E=140 MeV; 208Pb(10Be, X), (10Be, X), E=127 MeV; 208Pb(9Be, 9Be), (9Be, X), E=88 MeV; measured reaction products. 9,10,11Be; deduced σ(θ), σ(E), σ. Comparison with continuum discretized coupled channel (CDCC) as well as by the XCDCC calculations.

doi: 10.1016/j.physletb.2020.135942
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0235.


2020JI04      Phys.Rev. C 101, 031304 (2020)

W.Jiang, Y.L.Ye, C.J.Lin, Z.H.Li, J.L.Lou, X.F.Yang, Q.T.Li, Y.C.Ge, H.Hua, D.X.Jiang, D.Y.Pang, J.Li, J.Chen, Z.H.Yang, X.H.Sun, Z.Y.Tian, J.Feng, B.Yang, H.L.Zang, Q.Liu, P.J.Li, Z.Q.Chen, Y.Liu, Y.Zhang, J.Ma, H.M.Jia, X.X.Xu, L.Yang, N.R.Ma, L.J.Sun

Determination of the cluster-decay branching ratio from a near-threshold molecular state in 10Be

NUCLEAR REACTIONS 9Be(9Be, 10Be)8Be, E=45 MeV; measured Eα, Iα, E(6He), I(6He), E(9Be), I(9Be), α(6He)-coin, and σ of 10Be population channel from the decay of 10Be* to α+6He using ΔE-E telescope detectors at CIAE HI-13 tandem accelerator facility. 10Be; deduced Q-value spectra, resonances, α-decay branching ratio, and α-cluster spectroscopic factor, σ-bond molecular rotational band. Comparison with previous experimental data.

doi: 10.1103/PhysRevC.101.031304
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Data from this article have been entered in the XUNDL database. For more information, click here.


2020LI06      Phys.Rev. C 101, 024305 (2020)

P.F.Liang, L.J.Sun, J.Lee, S.Q.Hou, X.X.Xu, C.J.Lin, C.X.Yuan, J.J.He, Z.H.Li, J.S.Wang, D.X.Wang, H.Y.Wu, Y.Y.Yang, Y.H.Lam, P.Ma, F.F.Duan, Z.H.Gao, Q.Hu, Z.Bai, J.B.Ma, J.G.Wang, F.P.Zhong, C.G.Wu, D.W.Luo, Y.Jiang, Y.Liu, D.S.Hou, R.Li, N.R.Ma, W.H.Ma, G.Z.Shi, G.M.Yu, D.Patel, S.Y.Jin, Y.F.Wang, Y.C.Yu, Q.W.Zhou, P.Wang, L.Y.Hu, X.Wang, H.L.Zang, P.J.Li, Q.Q.Zhao, H.M.Jia, L.Yang, P.W.Wen, F.Yang, G.L.Zhang, M.Pan, X.Y.Wang, H.H.Sun, Z.G.Hu, R.F.Chen, M.L.Liu, W.Q.Yang, Y.M.Zhao

Simultaneous measurement of β-delayed proton and γ emission of 26P for the 25Al(p, γ)26Si reaction rate

RADIOACTIVITY 26P(β+), (β+p)[from 9Be(32S, X), E=806 MeV/nucleon, followed by in-flight separation by the RIBLL1 fragment separator at HIRFL-Lanzhou]; measured E(p), I(p), Eγ, Iγ, βp- and βγ-coin, half-life of the decay of 26P from correlated events of 26P implants and successive decays using three double-sided silicon strip detectors (DSSDs), five Clover-type HPGe detectors, and five quadrant silicon detectors (Q SDs). 26Si; deduced levels, J, π, Γp and Γγ of 5929, 3+ state. Comparison with previous experimental data, and with shell-model calculations.

NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P, E=806 MeV/nucleon; measured reaction products and TOF-ΔE spectrum using in-flight separation by the RIBLL1 fragment separator at HIRFL-Lanzhou. 25Al(p, γ)26Si, T=0.03-1.1 GK; deduced energies and strengths of resonances, corresponding astrophysical reaction rates, and compared with data in JINA REACLIB database.

doi: 10.1103/PhysRevC.101.024305
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Data from this article have been entered in the XUNDL database. For more information, click here.


2020SU02      Phys.Lett. B 800, 135096 (2020)

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

Fine structure in the α decay of 223U

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

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


2020WA16      Nucl.Instrum.Methods Phys.Res. A971, 164068 (2020)

X.Wang, Z.H.Li, Z.Liu, J.Li, H.Hua, H.Y.Lu, W.Q.Zhang, T.H.Huang, M.D.Sun, 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, C.J.Lin, L.J.Sun, N.R.Ma, H.S.Xu, X.H.Zhou, G.Q.Xiao, H.Y.Wu, C.Xu, S.Q.Zhang, X.Q.Li, R.Han, Z.Q.Chen, C.G.Wu, D.W.Luo, Y.Jin, J.Lin, D.X.Jiang, Y.L.Ye, F.S.Zhang

An effective digital pulse processing method for pile-up pulses in decay studies of short-lived nuclei

RADIOACTIVITY 219Th(α), 210,211Ra(IT) [from 175Lu, 186W, 187Re(40Ar, X), E=188 MeV]; measured decay products, Eα, Iα; deduced α spectra, proper baseline correction, standard pulse construction and plateau-region fitting, spectroscopic information of overlapping signals.

doi: 10.1016/j.nima.2020.164068
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2020WE03      Phys.Rev. C 101, 014618 (2020)

P.W.Wen, O.Chuluunbaatar, A.A.Gusev, R.G.Nazmitdinov, A.K.Nasirov, S.I.Vinitsky, C.J.Lin, H.M.Jia

Near-barrier heavy-ion fusion: Role of boundary conditions in coupling of channels

NUCLEAR REACTIONS 144Sm(16O, X), E=55-75 MeV; 100Mo(64Ni, X), E=120-160 MeV; 48Ca(36S, X), E=36-65 MeV; calculated tunneling probability and fusion σ(E) using finite element method for numerically solving the coupled Schrodinger equations with boundary conditions corresponding to total absorption. Comparison with coupled-channels calculations with CCFULL and KANTBP codes, and with experimental data.

doi: 10.1103/PhysRevC.101.014618
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2020YA14      Phys.Rev. C 101, 054603 (2020)

L.Yang, C.J.Lin, H.M.Jia, D.X.Wang, N.R.Ma, P.W.Wen, F.Yang, F.P.Zhong, S.H.Zhong, T.P.Luo

Insight into the radial sensitivity of phenomenological nucleus-nucleus interaction potentials

NUCLEAR REACTIONS 208Pb(9Be, X), E(cm)=34-44 MeV; 208Pb(16O, X), 209Bi(6He, X), E/VB=0.6-2.0; calculated radial sensitivities, volume integrals of potential volume and surface interaction, energy dependence of the sensitive regions (SRs) using the notch technique with optical model potential using FRESCO code. Comparison with experimental data.

doi: 10.1103/PhysRevC.101.054603
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2020ZH02      Phys.Lett. B 801, 135170 (2020), Corrigendum Phys.Lett. B 803, 135278 (2020)

N.T.Zhang, X.Y.Wang, D.Tudor, B.Bucher, I.Burducea, H.Chen, Z.J.Chen, D.Chesneanu, A.I.Chilug, L.R.Gasques, D.G.Ghita, C.Gomoiu, K.Hagino, S.Kubono, Y.J.Li, C.J.Lin, W.P.Lin, R.Margineanu, A.Pantelica, I.C.Stefanescu, M.Straticiuc, X.D.Tang, L.Trache, A.S.Umar, W.Y.Xin, S.W.Xu, Y.Xu

Constraining the 12C+12C astrophysical S-factors with the 12C+13C measurements at very low energies

NUCLEAR REACTIONS 12C(13C, p)24Na, E=4.640-10.995 MeV; measured reaction products, Eγ, Iγ; deduced σ, branching ratio, S-factor.

doi: 10.1016/j.physletb.2019.135170
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2019MA46      Eur.Phys.J. A 55, 87 (2019)

N.R.Ma, L.Yang, C.J.Lin, H.Yamaguchi, D.X.Wang, L.J.Sun, M.Mazzocco, H.M.Jia, S.Hayakawa, D.Kahl, S.M.Cha, G.X.Zhang, F.Yang, Y.Y.Yang, C.Signorini, Y.Sakaguchi, K.Abe, M.La Commara, D.Pierroutsakou, C.Parascandolo, E.Strano, A.Kim, K.Y.Chae, M.S.Kwag, G.L.Zhang, M.Pan, X.X.Xu, P.W.Wen, F.P.Zhong, H.H.Sun, G.Guo

MITA: A Multilayer Ionization-chamber Telescope Array for low-energy reactions with exotic nuclei

NUCLEAR REACTIONS 58Ni(17F, 17F'), E=55.7 MeV; measured ToF of different isotopes recorded by MITA, reaction products; deduced protons and α counts vs E, σ(θ) vs θ.

doi: 10.1140/epja/i2019-12765-7
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2019MA58      Phys.Rev. C 100, 024602 (2019)

M.Mazzocco, N.Keeley, A.Boiano, C.Boiano, M.La Commara, C.Manea, C.Parascandolo, D.Pierroutsakou, C.Signorini, E.Strano, D.Torresi, H.Yamaguchi, D.Kahl, L.Acosta, P.Di Meo, J.P.Fernandez-Garcia, T.Glodariu, J.Grebosz, A.Guglielmetti, Y.Hirayama, N.Imai, H.Ishiyama, N.Iwasa, S.C.Jeong, H.M.Jia, Y.H.Kim, S.Kimura, S.Kubono, G.La Rana, C.J.Lin, P.Lotti, G.Marquinez-Duran, I.Martel, H.Miyatake, M.Mukai, T.Nakao, M.Nicoletto, A.Pakou, K.Rusek, Y.Sakaguchi, A.M.Sanchez-Benitez, T.Sava, O.Sgouros, V.Soukeras, F.Soramel, E.Stiliaris, L.Stroe, T.Teranishi, N.Toniolo, Y.Wakabayashi, Y.X.Watanabe, L.Yang, Y.Y.Yang, H.Q.Zhang

Elastic scattering for the 8B and 7Be + 208Pb systems at near-Coulomb barrier energies

NUCLEAR REACTIONS 208Pb(8B, 8B), E=50 MeV, [8B secondary beam from 3He(6Li, 8B), E=11.2 MeV/nucleon primary reaction at RIKEN]; 208Pb(7Be, 7Be), E=37.4, 40.5, 42.2 MeV, [7Be secondary beam from 1H(7Li, 7Be), E=48.8 MeV primary reaction at LNL-Legnaro]; measured charged particles, σ(θ, E) using the EXPADES detector array, and angular distribution; analyzed by optical model and the continuum discretized coupled channels (CDCC) formalisms. Experiments performed at the CNS Radioactive Ion Beams (CRIB) facility at RIKEN, and EXOTIC facility at the Laboratori Nazionali di Legnaro (LNL).

doi: 10.1103/PhysRevC.100.024602
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2019WE04      Phys.Rev. C 99, 034606 (2019)

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

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

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

doi: 10.1103/PhysRevC.99.034606
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2019YA07      Phys.Rev. C 99, 064315 (2019)

B.Yang, Y.L.Ye, J.Feng, C.J.Lin, H.M.Jia, Z.H.Li, J.L.Lou, Q.T.Li, Y.C.Ge, X.F.Yang, H.Hua, J.Li, H.L.Zang, Q.Liu, W.Jiang, C.G.Li, Y.Liu, Z.Q.Chen, H.Y.Wu, C.G.Wang, W.Liu, X.Wang, J.J.Li, D.W.Luo, Y.Jiang, S.W.Bai, J.Y.Xu, N.R.Ma, L.J.Sun, D.X.Wang, Z.H.Yang, J.Chen

Investigation of the 14C+ α molecular configuration in 18O by means of transfer and sequential decay reaction

NUCLEAR REACTIONS 9Be(13C, α)18O*, E=65 MeV; measured recoil α particles and the two decay fragments 14C+α using an array of six charged-particle telescopes, Eα, Iα, (recoil)α-coin, αα-coin, invariant- and missing-mass spectrum, and angular correlation for the 10.3-MeV (4+) state at the HI-13 tandem accelerator of CIAE-Beijing. 18O; deduced levels, 14C+α resonant states, total widths, J, π, α-decay branching ratios, bands. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.99.064315
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2018HU13      Phys.Rev. C 98, 044302 (2018)

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

Identification of the new isotope 224Np

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

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

doi: 10.1103/PhysRevC.98.044302
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2018WA05      Int.J.Mod.Phys. E27, 1850014 (2018)

K.Wang, D.Q.Fang, Y.T.Wang, X.X.Xu, L.J.Sun, Z.Bai, M.R.Huang, S.L.Jin, C.Li, H.Li, J.Li, X.F.Li, C.J.Lin, J.B.Ma, P.Ma, W.H.Ma, M.W.Nie, C.Z.Shi, H.W.Wang, J.G.Wang, J.S.Wang, L.Yang, Y.Y.Yang, H.Q.Zhang, Y.J.Zhou, Y.G.Ma, W.Q.Shen

Spectroscopic study of β-delayed particle emission from proton-rich nucleus 23Si

RADIOACTIVITY 23Si(β+), (β+p), (β+2p) [from 9Be(28Si, X)23Si, E=75.8 MeV/nucleon]; measured decay products, Eγ, Iγ, Ep, Ip, p-γ and 2p-γ-coin.; deduced β-delayed charge-particle energy spectrum, decay energies and branching ratios for β-delayed protons, γ-ray energies, J, π, β-delayed proton branch and two proton emissions. Comparison with available data.

doi: 10.1142/S0218301318500143
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2018WA20      Eur.Phys.J. A 54, 107 (2018)

Y.-T.Wang, D.-Q.Fang, K.Wang, X.-X.Xu, L.-J.Sun, Z.Bai, P.-F.Bao, X.-G.Cao, Z.-T.Dai, B.Ding, W.-B.He, M.-R.Huang, S.-L.Jin, Y.Li, C.-J.Lin, L.-X.Liu, M.Lv, J.-B.Ma, P.Ma, H.-W.Wang, J.-G.Wang, J.-S.Wang, S.-T.Wang, Y.-Y.Yang, S.-Q.Ye, H.-Q.Zhang, M.-H.Zhao, C.-L.Zhou, Y.-G.Ma, W.-Q.Shen

β-delayed particle emission from 21Mg

RADIOACTIVITY 21Mg(EC), (β+), (ECp), (ECα), (β+p), (β+α); measured Eg, Ig, E(particle), I(particle), pγ-coin, charged particles using RIBBL1 (Radioactive Ion Beam Line) at Lanzhou, 21Mg decay-time spectrum, γ-ray energy spectrum correlated with β-delayed charged particles; deduced β-delayed charged particles energy spectrum, new partial decay scheme, levels, J, π, T1/2, log ft, branching ratios of individual states.

doi: 10.1140/epja/i2018-12543-1
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2018WA24      Phys.Lett. B 784, 12 (2018)

Y.T.Wang, D.Q.Fang, K.Wang, X.X.Xu, L.J.Sun, P.F.Bao, Z.Bai, X.G.Cao, Z.T.Dai, B.Ding, W.B.He, M.R.Huang, S.L.Jin, C.J.Lin, M.Lv, L.X.Liu, Y.Li, P.Ma, J.B.Ma, J.S.Wang, S.T.Wang, J.G.Wang, H.W.Wang, S.Q.Ye, Y.Y.Yang, C.L.Zhou, M.H.Zhao, H.Q.Zhang, Y.G.Ma, W.Q.Shen

Observation of β-delayed 2He emission from the proton-rich nucleus 22Al

RADIOACTIVITY 22Al(β+2p) [from Be(28Si, X), E=76 MeV/nucleon]; measured decay products, Eγ, Iγ. 22Mg; deduced the momentum and emission angle of the two protons, Ep, Ip. Comparison with Monte Carlo simulations.

doi: 10.1016/j.physletb.2018.07.034
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2018WO01      Acta Phys.Pol. B49, 387 (2018)

D.Wojcik, A.Trzcinska, E.Piasecki, M.Kisielinski, M.Kowalczyk, M.Wolinska-Cichocka, C.Bordeanu, B.Gnoffo, H.Jia, C.Lin, N.S.Martorana, M.Mutterer, E.V.Pagano, K.Piasecki, P.Russotto, L.Quatrocchi, W.H.Trzaska, G.Tiurin, R.Wolski, H.Zhang

Transfer Cross Sections at Near-barrier Energy for the 24Mg + 90, 92Zr Systems

NUCLEAR REACTIONS 90,92Zr(24Mg, x), E=76 MeV; measured using multidetector system ICARE with start signal bz the Microchannel Plate (MCP) and stop signal by one of Si detectors placed at polar angle 142, used also to measure the energy of reaction products, and beam energy monitored by Si detectors at 30; deduced E-ToF spectra of backscattered ions; measured stripping reactions involving up up to 4 nucleons and reaction channels up to 2 nucleons picked up (i.e. the product mass from A-6 to A+2, A is the target mass); deduced transfer σtr(θ) and lacking structure of distribution of barrier heights, the cross sections are considerably smaller than those for 20Ne projectile. Preliminary.

doi: 10.5506/aphyspolb.49.387
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2018ZH17      Phys.Rev. C 97, 044614 (2018)

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

Shell effects in a multinucleon transfer process

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

doi: 10.1103/PhysRevC.97.044614
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2018ZH18      Phys.Rev. C 97, 044618 (2018)

G.L.Zhang, G.X.Zhang, C.J.Lin, J.Lubian, J.Rangel, B.Paes, J.L.Ferreira, H.Q.Zhang, W.W.Qu, H.M.Jia, L.Yang, N.R.Ma, L.J.Sun, D.X.Wang, L.Zheng, X.X.Liu, X.T.Chu, J.C.Yang, J.S.Wang, S.W.Xu, P.Ma, J.B.Ma, S.L.Jin, Z.Bai, M.R.Huang, H.L.Zang, B.Yang, Y.Liu

Angular distribution of elastic scattering induced by 17F on medium-mass target nuclei at energies near the Coulomb barrier

NUCLEAR REACTIONS 89Y(17F, 17F), E=50, 59 MeV, [17F secondary beam from 1H(17O, n), E=7.6 MeV/nucleon primary reaction]; measured reaction products, 17F scattered particles, differential σ(θ, E) using DSSD and SSD detector telescopes at RIBLL facility in Lanzhou. 16F, 90Zr; calculated spectroscopic amplitudes for excited levels in the coupled reaction channels (CRC) formalism for one-proton transfer reactions using the Sao Paulo double-folding potential. Comparison with Continuum-discretized coupled-Channels (CDCC) calculations.

doi: 10.1103/PhysRevC.97.044618
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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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2017LI04      Phys.Rev. C 95, 021303 (2017)

J.Li, Y.L.Ye, Z.H.Li, C.J.Lin, Q.T.Li, Y.C.Ge, J.L.Lou, Z.Y.Tian, W.Jiang, Z.H.Yang, J.Feng, P.J.Li, J.Chen, Q.Liu, H.L.Zang, B.Yang, Y.Zhang, Z.Q.Chen, Y.Liu, X.H.Sun, J.Ma, H.M.Jia, X.X.Xu, L.Yang, N.R.Ma, L.J.Sun

Selective decay from a candidate of the σ-bond linear-chain state in 14C

NUCLEAR REACTIONS 9Be(9Be, α10Be)He, E=45 MeV; measured particle spectra at HI-13 tandem accelerator of CIAE-Beijing facility. 14C; deduced level energies from reconstruction of forward moving 10Be+α fragments, resonances, decays to α cluster and 10Be in its ground state, first 2+, and about 6-MeV state, relative decay strength, indication of a σ-bond linear chain structure in 14C. Comparison with predictions of improved antisymmetrized molecular dynamics (AMD) theory.

doi: 10.1103/PhysRevC.95.021303
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2017SU05      Phys.Rev. C 95, 014314 (2017)

L.J.Sun, X.X.Xu, D.Q.Fang, C.J.Lin, J.S.Wang, Z.H.Li, Y.T.Wang, J.Li, L.Yang, N.R.Ma, K.Wang, H.L.Zang, H.W.Wang, C.Li, C.Z.Shi, M.W.Nie, X.F.Li, H.Li, J.B.Ma, P.Ma, S.L.Jin, M.R.Huang, Z.Bai, J.G.Wang, F.Yang, H.M.Jia, H.Q.Zhang, Z.H.Liu, P.F.Bao, D.X.Wang, Y.Y.Yang, Y.J.Zhou, W.H.Ma, J.Chen, Y.G.Ma, Y.H.Zhang, X.H.Zhou, H.S.Xu, G.Q.Xiao, W.L.Zhan

β-decay study of the Tz = -2 proton-rich nucleus 20Mg

RADIOACTIVITY 20Mg(β+), (β+p)[from 9Be(28Si, X), E=75.8 MeV/nucleon at RIBLL-HIRFL-Lanzhou facility]; measured reaction products, Ep, Ip, Eγ, Iγ, γγ-, γβ- and pβ-coin, (20Mg)γ-coin, half-life of 20Mg decay. 20Na, 19Ne; deduced levels, branching ratios, logft values. Comparison with previous experimental results, and with β transitions in 20O mirror nucleus.

doi: 10.1103/PhysRevC.95.014314
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2017SU18      Phys.Lett. B 771, 303 (2017)

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

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

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

doi: 10.1016/j.physletb.2017.03.074
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2017WE04      Chin.Phys.C 41, 064102 (2017)

P.-W.Wen, Z.-Q.Feng, F.Zhang, C.Li, C.-J.Lin, F.-S.Zhang

Effect of positive Q-value neutron transfers on sub-barrier fusion reactions

NUCLEAR REACTIONS 90,94,96Zr(40Ca, X), E<100 MeV/nucleon; calculated fusion σ, Q-values of ground state to ground state neutron transfers. Modified quantum coupled channels model with all order couplings (CCFULL).

doi: 10.1088/1674-1137/41/6/064102
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2017WE14      J.Phys.(London) G44, 115101 (2017)

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

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

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

doi: 10.1088/1361-6471/aa8b07
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2017XU01      Phys.Lett. B 766, 312 (2017)

X.X.Xu, C.J.Lin, L.J.Sun, J.S.Wang, Y.H.Lam, J.Lee, D.Q.Fang, Z.H.Li, N.A.Smirnova, C.X.Yuan, L.Yang, Y.T.Wang, J.Li, N.R.Ma, K.Wang, H.L.Zang, H.W.Wang, C.Li, M.L.Liu, J.G.Wang, C.Z.Shi, M.W.Nie, X.F.Li, H.Li, J.B.Ma, P.Ma, S.L.Jin, M.R.Huang, Z.Bai, F.Yang, H.M.Jia, Z.H.Liu, D.X.Wang, Y.Y.Yang, Y.J.Zhou, W.H.Ma, J.Chen, Z.G.Hu, M.Wang, Y.H.Zhang, X.W.Ma, X.H.Zhou, Y.G.Ma, H.S.Xu, G.Q.Xiao, H.Q.Zhang

Observation of β-delayed two-proton emission in the decay of 22Si

RADIOACTIVITY 22Si(β+2p) [from 9Be(28Si, X), E=75.8 MeV/nucleon]; measured decay products, Ep, Ip; deduced Q-value, ground-state mass, two-proton separation energy. Comparison with large-scale shell-model calculations.

doi: 10.1016/j.physletb.2017.01.028
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2017YA06      Phys.Rev. C 95, 034616 (2017)

L.Yang, C.J.Lin, H.M.Jia, D.X.Wang, L.J.Sun, N.R.Ma, F.Yang, Z.D.Wu, X.X.Xu, H.Q.Zhang, Z.H.Liu, P.F.Bao

Optical model potentials for 6He + 64Zn from 63Cu (7Li, 6He) 64Zn reactions

NUCLEAR REACTIONS 63Cu(7Li, 7Li), (7Li, 6He), E=12.67, 15.21, 16.33, 23.30, 27.30, 30.96 MeV; measured particle spectra, σ(θ, E) for elastic scattering and transfer reaction using Q3D magnetic spectrometer and multilayer position sensitive focal plane gas detector at HI-13 accelerator facility of CIAE; deduced optical model potential parameters of 7Li+63Cu and 6He+64Zn using optical model. Coupled-reaction-channels (CRC) and distorted-wave-Born-approximation (DWBA) analysis.

doi: 10.1103/PhysRevC.95.034616
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2017YA20      Phys.Rev.Lett. 119, 042503 (2017)

L.Yang, C.J.Lin, H.M.Jia, D.X.Wang, N.R.Ma, L.J.Sun, F.Yang, X.X.Xu, Z.D.Wu, H.Q.Zhang, Z.H.Liu

Is the Dispersion Relation Applicable for Exotic Nuclear Systems? The Abnormal Threshold Anomaly in the 6He+209Bi System

NUCLEAR REACTIONS 208Pb(7Li, 6He), E=21.20, 24.30, 25.67, 28.55 MeV; measured reaction products; deduced σ(θ), precise optical potentials.

doi: 10.1103/PhysRevLett.119.042503
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2017YA26      Phys.Rev. C 96, 044615 (2017)

L.Yang, C.J.Lin, H.M.Jia, D.X.Wang, N.R.Ma, L.J.Sun, F.Yang, X.X.Xu, Z.D.Wu, H.Q.Zhang, Z.H.Liu

Abnormal behavior of the optical potential for the halo nuclear system 6He + 209Bi

NUCLEAR REACTIONS 208Pb(7Li, 6He), (7Li, 7Li), E=21.20, 24.30, 25.67, 28.55 MeV; measured transfer reaction products, particle spectra, σ(θ, E) for elastic channel and for (7Li, 6He) at the China Institute of Atomic Energy, Beijing, , data analyzed by optical model, distorted-wave Born approximation (DWBA), and coupled reaction channel (CRC) calculations; deduced S factors, configurations, real and imaginary potentials by CRC and DWBA calculations. 209Bi(6He, 6He), E=14.3, 17.3, 18.6, 21.4 MeV; analyzed previous σ(θ, E) data; deduced OMP parameters from CRC and DWBA calculations. Discussed dispersion relation for halo nuclear system.

doi: 10.1103/PhysRevC.96.044615
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2016LI45      Yuan.Wul.Ping. 33, 160 (2016); Nucl.Phys.Rev. 33, 160 (2016)

C.Lin, X.Xu, J.Wang, L.Sun, H.Jia, L.Yang, P.Ma, J.Ma, Y.Yang, S.Jin, M.Huang, Z.Bai, Z.Wu, F.Yang, Z.Hu, M.Wang, X.Lei, H.Zhang, H.Xu, G.Xiao

Proton and Two-proton Emissions from Proton-rich Nuclei with 10 ≤ Z ≤ 20

RADIOACTIVITY 28,29S, 26,27P, 17,18Ne(2p), 27S, 26P, 22,25Si, 20Mg, 23Si, 22Al, 21Mg, 24Si, 23Al, 36,37Ca(β+p), (β+2p); measured decay products, Ep, Ip; deduced energy, T1/2, branching-ratios.

doi: 10.11804/NuclPhysRev.33.02.160#
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2016MA70      Chin.Phys.C 40, 114001 (2016)

N.-R.Ma, H.-M.Jia, C.-J.Lin, L.Yang, X.-X.Xu, L.-J.Sun, F.Yang, Z.-D.Wu, H.-Q.Zhang, Z.-H.Liu, D.-X.Wang

Self-consistent analysis of sub-barrier fusion enhancement effect in Ca + Ca and Ni + N

NUCLEAR REACTIONS 40Ca(40Ca, X), (48Ca, X), 48Ca(48Ca, X), 58Ni(58Ni, X), 58Ni(64Ni, X), 64Ni(64Ni, X), E(cm)<110 MeV; calculated σ. Self-consistent method based on the CCFULL calculations.

doi: 10.1088/1674-1137/40/11/114001
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2016RA19      Phys.Rev. C 93, 054622 (2016)

T.Rajbongshi, K.Kalita, S.Nath, J.Gehlot, T.Banerjee, I.Mukul, R.Dubey, N.Madhavan, C.J.Lin, A.Shamlath, P.V.Laveen, M.Shareef, N.Kumar, P.Jisha, P.Sharma

Deformation effects on sub-barrier fusion cross sections in 16O + 174, 176Yb

NUCLEAR REACTIONS 174,176Yb(16O, X), E=64.6-103.6 MeV; measured evaporation residues (ER), scatter plots between ΔE and TOF of the events, fusion σ(E) using HIRA recoil mass spectrometer at IUAC-New Delhi; deduced barrier distribution, hexadecapole deformation parameter (β4). Comparison with coupled-Channel calculations using CCFULL code.

doi: 10.1103/PhysRevC.93.054622
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2016SU22      Yuan.Wul.Ping. 33, 230 (2016); Nucl.Phys.Rev. 33, 230 (2016)

L.Sun, X.Xu, C.Lin, J.Wang, D.Fang, Z.Li, Y.Wang, J.Li, L.Yang, N.Ma, K.Wang, H.Zhang, H.Wang, C.Li, C.Shi, M.Nie, X.Li, H.Li, J.Ma, P.Ma, S.Jin, M.Huang, Z.Bai, J.Wang, F.Yang, H.Jia, H.Zhang, Z.Liu, P.Bao, S.Wang, Z.Wu, Y.Yang, Z.Chen, J.Su, Y.Shen, Y.Zhou, W.Ma, J.Chen

An implantation and detection system for spectroscopy of 22, 24Si

RADIOACTIVITY 22,24Si(β+p); measured decay products, Ep, Ip; deduced energy levels, J, π, T1/2, branchning ratios.

doi: 10.11804/NuclPhysRev.33.02.230
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2016TI10      Chin.Phys.C 40, 111001 (2016)

Z.Y.Tian, Y.L.Ye, Z.H.Li, C.J.Lin, Q.T.Li, Y.C.Ge, J.L.Lou, W.Jiang, J.Li, Z.H.Yang, J.Feng, P.J.Li, J.Chen, Q.Liu, H.L.Zang, B.Yang, Y.Zhang, Z.Q.Chen, Y.Liu, X.H.Sun, J.Ma, H.M.Jia, X.X.Xu, L.Yang, N.R.Ma, L.J.Sun

Cluster decay of the high-lying excited states in 14C

NUCLEAR REACTIONS 9Be(9Be, 14C), E=45 MeV; measured reaction products, Eα, Iα. 14C, 10Be; deduced low-lying resonance states, cluster structures.

doi: 10.1088/1674-1137/40/11/111001
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2015GO05      Phys.Rev. C 91, 044610 (2015)

A.Gomez Camacho, N.Yu, H.Q.Zhang, P.R.S.Gomes, H.M.Jia, J.Lubian, C.J.Lin

Energy dependence of the optical potentials for the 9Be+208Pb and 9Be+209Bi systems at near-Coulomb-barrier energies

NUCLEAR REACTIONS 208Pb(9Be, 9Be), (9Be, X), E=37, 37.8.38, 38.2, 38.5, 38.7, 39, 39.5, 40, 41, 42, 44, 47.2, 50 MeV; 209Pb(9Be, 9Be), (9Be, X), E=37, 37.8.38, 38.2, 38.5, 38.7, 39, 39.5, 40, 41, 42, 44 MeV; analyzed elastic scattering σ(θ), fusion σ(E), fusion and direct reaction polarization potentials, no conclusive for the presence of threshold anomaly (TA) or the breakup threshold anomaly (BTA). Optical potential model.

doi: 10.1103/PhysRevC.91.044610
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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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2015OG06      Phys.Atomic Nuclei 78, 985 (2015); Yad.Fiz. 78, 1047 (2015)

A.A.Ogloblin, H.Q.Zhang, C.J.Lin, H.M.Jia, S.V.Khlebnikov, E.A.Kuzmin, A.N.Danilov, A.S.Demyanova, W.H.Trzaska, X.X.Xu, F.Yang, V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid

Analysis of the role of neutron transfer in asymmetric fusion reactions at subbarrier energies

NUCLEAR REACTIONS 208Pb(28Si, X), E=130-140 MeV; measured reaction products; deduced capture σ. Comparison with calculated values.

doi: 10.1134/S1063778815080116
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2015SU01      Chin.Phys.Lett. 32, 012301 (2015)

L.-J.Sun, C.-J.Lin, X.-X.Xu, J.-S.Wang, H.-M.Jia, F.Yang, Y.-Y.Yang, L.Yang, P.-F.Bao, H.-Q.Zhang, s.-L.Jin, Z.-D.Wu, N.-T.Zhang, S.-Z.Chen, J.-B.Ma, P.Ma, N.-R.Ma, Z.-H.Liu

Experimental Study of Beta-Delayed Proton Emission of 36, 37Ca

RADIOACTIVITY 36,37Ca(β+p) [from 9Be(20Ca, X), E=69.42 MeV/nucleon]; measured decay products, Eβ, Iβ, Ep, Ip; deduced T1/2 and their uncertainties, branching ratios. Comparison with available data.

doi: 10.1088/0256-307X/32/1/012301
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2015SU15      Nucl.Instrum.Methods Phys.Res. A804, 1 (2015)

L.J.Sun, X.X.Xu, C.J.Lin, J.S.Wang, D.Q.Fang, Z.H.Li, Y.T.Wang, J.Li, L.Yang, N.R.Ma, K.Wang, H.L.Zang, H.W.Wang, C.Li, C.Z.Shi, M.W.Nie, X.F.Li, H.Li, J.B.Ma, P.Ma, S.L.Jin, M.R.Huang, Z.Bai, J.G.Wang, F.Yang, H.M.Jia, H.Q.Zhang, Z.H.Liu, P.F.Bao, D.X.Wang, Y.Y.Yang, Y.J.Zhou, W.H.Ma, J.Chen

A detection system for charged-particle decay studies with a continuous-implantation method

doi: 10.1016/j.nima.2015.09.039
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2014JI03      Phys.Rev. C 89, 064605 (2014)

H.M.Jia, C.J.Lin, F.Yang, X.X.Xu, H.Q.Zhang, Z.H.Liu, Z.D.Wu, L.Yang, N.R.Ma, P.F.Bao, L.J.Sun

Fusion of 32S + 94Zr: Further exploration of the effect of the positive Qxn value neutron transfer channels

NUCLEAR REACTIONS 94Zr(32S, X), E=95-130 MeV; measured reaction products, fusion σ(E), fusion barrier distribution as function of incident energy at HI-13 accelerator facility of CIAE. Comparison with previous σ(E) results from 90,96Zr(32S, X), E(cm)=70-90 MeV and 90,94,96Zr(40Ca, X) reactions, and with couple channel (CC) calculations.

doi: 10.1103/PhysRevC.89.064605
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2014JI08      Phys.Rev. C 90, 031601 (2014)

H.M.Jia, C.J.Lin, F.Yang, X.X.Xu, H.Q.Zhang, Z.H.Liu, Z.D.Wu, L.Yang, N.R.Ma, P.F.Bao, L.J.Sun

Extracting the hexadecapole deformation from backward quasi-elastic scattering

NUCLEAR REACTIONS 152Sm, 170Er, 174Yb(16O, 16O), E=40-80 MeV; measured particle spectra, quasielastic (QEL) σ(E) at backward angles using HI-13 tandem accelerator facility at CIAE; deduced β4 deformation parameter. Coupled-channel calculations using CCFULL computer code.

doi: 10.1103/PhysRevC.90.031601
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2014OG01      Eur.Phys.J. A 50, 157 (2014)

A.A.Ogloblin, H.Q.Zhang, C.J.Lin, H.M.Jia, S.V.Khlebnikov, E.A.Kuzmin, W.H.Trzaska, X.X.Xu, F.Yan, V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid

Role of neutron transfer in asymmetric fusion reactions at sub-barrier energies

NUCLEAR REACTIONS 208Pb(28Si, x), (30Si, x), E(cm)≈115-150 MeV; measured reaction products using SSTD array; deduced fusion σ. 208Pb(20Ne, x), E(cm)=85-109 MeV;208Pb(28Si, x), (30Si, x), E(cm)≈115-150 MeV; calculated fusion σ using quantum diffusion approach. Compared with other available data. 7

doi: 10.1140/epja/i2014-14157-y
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2014WU08      Chin.Phys.Lett. 31, 092401 (2014)

Z.-D.Wu, L.Yang, C.-J.Lin, H.-M.Jia, F.Yang, X.-X.Xu, H.-Q.Zhang, Z.-H.Liu, P.-F.Bao, L.-J.Sun, N.-R.Ma, L.Zheng

A Sensitivity Test of Extracting the Optical Potential Parameters for 6He+209Bi from the Transfer Reaction 208Pb(7Li, 6He)209Bi

NUCLEAR REACTIONS 208Pb(7Li, 6He), E=25.67 MeV; analyzed available data; calculated σ(θ); deduced optical model potential parameters.

doi: 10.1088/0256-307X/31/9/092401
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2014YA09      Phys.Rev. C 89, 044615 (2014)

L.Yang, C.J.Lin, H.M.Jia, F.Yang, Z.D.Wu, X.X.Xu, H.Q.Zhang, Z.H.Liu, P.F.Bao, L.J.Sun, N.R.Ma

Optical model potentials for the 6He + 209Bi reaction from a 208Pb(7Li, 6He)209Bi reaction analysis

NUCLEAR REACTIONS 208Pb(7Li, 7Li), (7Li, 6He), E=25.67, 28.55, 32.55, 37.55, 42.55 MeV; measured ΔE-E and ΔE-Position spectra for 6,7He, σ(θ, E) for elastic scattering and for first three levels in 209Bi using Q3D magnetic spectrometer at CIAE accelerator facility. 209Bi; deduced levels, J, π, spectroscopic factors. Optical model potential (OMP), coupled reaction channel (CRC) and DWBA calculations and analysis of 7Li+208Pb and 6He+209Bi systems.

doi: 10.1103/PhysRevC.89.044615
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2014ZH18      Phys.Rev. C 89, 054602 (2014)

G.L.Zhang, X.X.Liu, C.J.Lin

Systematic analysis of the effect of a positive Q-value neutron transfer in fusion reactions

NUCLEAR REACTIONS 90,96Zr, 110Pd(32S, X), (36S, X); 90,96Zr, 124,132Sn(40Ca, X), (48Ca, X); 58,60,62,64Ni, 76Ge, 144,148,154Sm, 186W(16O, X); 144Sm(17O, X); 58,60,64Ni, 74Ge, 118Sn(18O, X); 58,64Ni, 124,132Sn(58Ni, X); 64Ni, 118,124,132Sn(64Ni, X), E near Coulomb barrier; analyzed experimental fusion σ(E) data in terms of fusion functions F(x) as a function of x; investigated systematic behavior of positive Q-value neutron transfer (PQNT), 2-neutron transfers.

doi: 10.1103/PhysRevC.89.054602
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2013DU17      Phys.Rev. C 88, 054618 (2013)

R.du Rietz, E.Williams, D.J.Hinde, M.Dasgupta, M.Evers, C.J.Lin, D.H.Luong, C.Simenel, A.Wakhle

Mapping quasifission characteristics and timescales in heavy element formation reactions

NUCLEAR REACTIONS 186W(16O, X)202Pb*, E(cm)=102.1 MeV; 192Os(16O, X)208Po*, E(cm)=102.3 MeV; 178Hf(24Mg, X)202Po*, E(cm)=102.1 MeV; 168Er(34S, X)202Po*, E(cm)=128.4 MeV; 144Sm(48Ti, X)192Po*, E(cm)=164.2 MeV; 196Pt(16O, X)212Rn*, E(cm)=102.0 MeV; 208Pb(12C, X)220Ra*, E(cm)=59.9 MeV; 200Hg(16O, X)216Ra*, E(cm)=102.8 MeV; 178Hf(32S, X)210Ra*, E(cm)=138.3 MeV; 162Dy(48Ti, X)210Ra*, E(cm)=168.9 MeV; 208Pb(16O, X)224Th*, E(cm)=103.0 MeV; 186W(34S, X)220Th*, E(cm)=144.5 MeV; 170Er(48Ti, X)218Th*, E(cm)=174.8 MeV; 154Sm(64Ni, X)218Th*, E(cm)=200.6 MeV; 174Yb(48Ti, X)222U*, E(cm)=178.1 MeV; 194Pt(32S, X)226Pu*, E(cm)=144.4 MeV; 178Hf(48Ti, X)226Pu*, E(cm)=180.8 MeV; 208Pb(30Si, X)238Cm*, E(cm)=134.7 MeV; 202Hg(32S, X)234Cm*, E(cm)=149.6 MeV; 186W(48Ti, X)234Cm*, E(cm)=186.3 MeV; 170Er(64Ni, X)234Cm*, E(cm)=216.2 MeV; 238U(12C, X)250Cf*, E(cm)=66.3 MeV; 232Th(18O, X)250Cf*, E(cm)=84.9 MeV; 208Pb(32S, X)240Cf*, E(cm)=149.9 MeV; 198Pt(40Ca, X)238Cf*, E(cm)=188.7 MeV; 192Os(48Ti, X)240Cf*, E(cm)=195.0 MeV; 238U(16O, X)254Fm*, E(cm)=103.5 MeV; 196Pt(48Ti, X)244Fm*, E(cm)=193.3 MeV; 208Pb(40Ca, X)248No*, E(cm)=190.2 MeV; 200Hg(48Ti, X)248No*, E(cm)=197.5 MeV; 184W(64Ni, X)248No*, E(cm)=252.3 MeV; 238U(24Mg, X)262Rf*, E(cm)=129.3 MeV; 232Th(30Si, X)262Rf*, E(cm)=144.0 MeV; 208Pb(48Ti, X)256Rf*, E(cm)=210.6 MeV; 192Os(64Ni, X)256Rf*, E(cm)=239.2 MeV; 238U(28Si, X)266Sg*, E(cm)=150.7 MeV; 232Th(34S, X)266Sg*, E(cm)=166.7 MeV; 198Pt(64Ni, X)262Sg*, E(cm)=241.7 MeV; 232Th(40Ca, X)272Ds*, E(cm)=211.5 MeV; 208Pb(64Ni, X)272Ds*, E(cm)=259.5 MeV; 238U(40Ca, X)278Cn*, E(cm)=210.7 MeV; 238U(48Ti, X)286Fl*, E(cm)=214.6 MeV; measured reaction products using CUBE spectrometer of multiwire proportional counters (MWPCs), mass-angle distributions (MAD) at ANU's Heavy Ion accelerator facility; deduced systematic dependence of quasifission characteristics as a function of identity of colliding nuclei, entrance channel and compound nucleus fissilities, effects of nuclear structure at lower beam energies. Relevance to formation of superheavy elements.

doi: 10.1103/PhysRevC.88.054618
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2013LU13      Phys.Rev. C 88, 034609 (2013)

D.H.Luong, M.Dasgupta, D.J.Hinde, R.du Rietz, R.Rafiei, C.J.Lin, M.Evers, A.Diaz-Torres

Predominance of transfer in triggering breakup in sub-barrier reactions of 6, 7Li with 144Sm, 207, 208Pb, and 209Bi

NUCLEAR REACTIONS 207,208Pb, 209Bi(6Li, X), E=26.5, 29.0 MeV; 144Sm(7Li, X), E=21.5, 24.0 MeV; 208Pb, 209Bi(7Li, X), E=24.0, 29.0 MeV; 207Pb(7Li, X), E=24.0, 29.0, 26.5 MeV; measured spectra of charged breakup fragments in binary coincidence mode using BALIN detector array at ANU Heavy Ion Accelerator Facility; deduced Q-value spectra of α+p, α+d, α+t, α+α modes of breakup of 6,7Li, relative time scales and relative energy spectra of breakup fragments, relative probabilities of major breakup modes. Dominance of nucleon transfer-initiated breakup.

doi: 10.1103/PhysRevC.88.034609
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2013XU13      Phys.Lett. B 727, 126 (2013)

X.X.Xu, C.J.Lin, H.M.Jia, F.Yang, H.Q.Zhang, Z.H.Liu, Z.D.Wu, L.Yang, P.F.Bao, L.J.Sun, H.S.Xu, J.S.Wang, Y.Y.Yang, Z.Y.Sun, Z.G.Hu, M.Wang, S.L.Jin, J.L.Han, N.T.Zhang, S.Z.Chen, X.G.Lei, M.R.Huang, P.Ma, J.B.Ma, Y.H.Zhang, X.H.Zhou, X.W.Ma, G.Q.Xiao

Correlations of two protons emitted from excited states of 28S and 27P

RADIOACTIVITY 28S, 27P(2p) [from 9Be(32S, X), E=80.4 MeV/nucleon]; measured decay products, Ep, Ip; deduced excitation spectra, Si-p-p and Al-p-p coincidences, σ(θ), distributions of the opening angle and the relative momentum of two protons emitted from excited levels, diproton branching ratio. Comparison with available data.

doi: 10.1016/j.physletb.2013.10.029
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2013YA07      Phys.Rev. C 87, 047601 (2013)

L.Yang, C.J.Lin, H.M.Jia, X.X.Xu, F.Yang, H.Q.Zhang, Z.H.Liu, P.F.Bao, L.J.Sun

Energy dependence of phenomenological optical model potentials for the 7Li+11B reaction

NUCLEAR REACTIONS 11B(7Li, 7Li), E=9.85, 13.3, 18.3, 23.3, 28.3 MeV; measured particle spectra, σ(θ, E); deduced best fit optical model potential parameters.

doi: 10.1103/PhysRevC.87.047601
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2012JI07      Phys.Rev. C 85, 054303 (2012)

H.Jiang, G.J.Fu, B.Sun, M.Liu, N.Wang, M.Wang, Y.G.Ma, C.J.Lin, Y.M.Zhao, Y.H.Zhang, Z.Ren, A.Arima

Predictions of unknown masses and their applications

ATOMIC MASSES Z=1-184, N=1-184; analyzed masses for 1566 nuclei using extrapolation approach and shell correction term, S(n), S(2n), S(p), and S(2p); one-neutron and one-proton drip nuclei, R-process nucleosynthesis and astrophysical implications. Comparison with AME-2011 interim mass evaluation, and with Duflo-Zuker model. 85Mo, 87,88,89Tc, 123Ag, 140I, 222Po, 226,227,228Rn, 233,234Ra, 235Ac; compared predicted masses with measured values.

RADIOACTIVITY 248,249,250,251,252,253,254,255,256,257No, 251,252,253,254,255,256,257,258,259Lr, 253,254,255,256,257,258,259,260,261Rf, 255,256,257,258,259,260,261,262Db, 256,257,258,259,260,261,262,263Sg(α); calculated Q(α), half-life. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.054303
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2012JI11      Phys.Rev. C 86, 044621 (2012)

H.M.Jia, C.J.Lin, F.Yang, X.X.Xu, H.Q.Zhang, Z.H.Liu, L.Yang, S.T.Zhang, P.F.Bao, L.J.Sun

Fusion of the 16O+76Ge and 18O+74Ge systems and the role of positive Q-value neutron transfers

NUCLEAR REACTIONS 76Ge(16O, X), 74Ge(18O, X), E=38-61 MeV; measured particle spectra, time of flight, evaporation residue σ(E, θ), fusion σ(E) at CIAE facility; deduced barrier distributions. Comparisons with coupled-channel and single-channel calculations.

doi: 10.1103/PhysRevC.86.044621
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2012LI03      Phys.Rev. C 85, 014611 (2012); Erratum Phys.Rev. C 96, 029901 (2017)

C.J.Lin, R.du Rietz, D.J.Hinde, M.Dasgupta, R.G.Thomas, M.L.Brown, M.Evers, L.R.Gasques, M.D.Rodriguez

Systematic behavior of mass distributions in 48Ti-induced fission at near-barrier energies

NUCLEAR REACTIONS 144,154Sm, 162Dy, 174Yb, 186W, 192Os, 196Pt, 200Hg, 208Pb(48Ti, F), E=206-296 MeV; measured fission fragment spectra (fragment)(fragment)-coin, fission yields; deduced mass-ratio distributions, mass widths as functions of excitation energy of compound nucleus, and excitation energies at saddle and scission points, mass-width enhancement factors. Comparison with saddle-point and scission-point model calculations.

doi: 10.1103/PhysRevC.85.014611
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2012NO01      Phys.Rev. C 85, 014607 (2012)

M.Notani, H.Esbensen, X.Fang, B.Bucher, P.Davies, C.L.Jiang, L.Lamm, C.J.Lin, C.Ma, E.Martin, K.E.Rehm, W.P.Tan, S.Thomas, X.D.Tang, E.Brown

Correlation between the 12C+12C, 12C+13C, and 13C+13C fusion cross sections

NUCLEAR REACTIONS 12C(13C, p)24Na, 13C(13C, np)24Na, E(cm)=2.6-4.8 MeV; measured Eγ, Iγ, βγ-coin from 24Na decay; deduced thick target yield by activation method, GEANT4 simulation, fusion cross section, S factors. 12C(12C, X), (13C, X), 13C(13C, X), E(cm)=2.5-6.5 MeV; analyzed fusion cross sections, fusion barrier parameters, spectroscopic factors by fitting with Wong formula. Comparison of experimental data with two coupled-channels calculations using ingoing wave boundary condition (IWBC).

doi: 10.1103/PhysRevC.85.014607
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2012SA04      Phys.Rev. C 85, 017603 (2012)

V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, C.J.Lin, H.Q.Zhang

Oblate-prolate deformation effect in capture reactions at sub-barrier energies

NUCLEAR REACTIONS 144Sm(16O, X), E(cm)=50-90 MeV; 144Sm(48Ca, X), E(cm)=125-160 MeV; 74Ge(74Ge, X), E(cm)=105-140 MeV; 170Er, 174Yb(36S, X), E(cm)=105-150 MeV; calculated capture cross section, mean angular momentum. Oblate and prolate deformation effects. Quantum-diffusion approach applied for the capture process in the reactions with deformed nuclei. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.017603
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2012SA13      Phys.Rev. C 85, 037602 (2012)

V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, C.J.Lin, H.Q.Zhang

Deformation effect in the sub-barrier capture process

NUCLEAR REACTIONS 198Pt(28Si, X), E(cm)=105-142 MeV; 194Pt(40Ca, X), E(cm)=153-200 MeV; 194Pt, 190Os(48Ca, X), E(cm)=150-175 MeV; 194Pt, 190Os(36S, X), E(cm)=115-141 MeV; calculated capture cross sections, mean angular momenta; deduced oblate and prolate deformation effects. Quantum-diffusion approach applied for capture process in reactions with deformed nuclei. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.037602
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2012TA13      J.Phys.:Conf.Ser. 337, 012016 (2012)

X.D.Tang, X.Fang, B.Bucher, H.Esbensen, C.L.Jiang, K.E.Rehm, C.J.Lin

Upper Limit on the molecular resonance strengths in the 12C+ 12C fusion reaction

NUCLEAR REACTIONS 12,13C(12C, X), (13C, X), E(cm)=2-6.5 MeV; analyzed published data on fusion reaction S-factor; deduced average S-factor, resonances, upper limit for molecular resonance strengths, empirical relationship using CRC-AW and EWS (equivalent square well).

doi: 10.1088/1742-6596/337/1/012016
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2012TA24      J.Phys.:Conf.Ser. 381, 012120 (2012)

X.D.Tang, H.Esbensen, X.Fang, B.Bucher, C.L.Jiang, K.E.Rehm, C.J.Lin, E.Brown

Does the 12C+12C fusion reaction trigger superburst?

NUCLEAR REACTIONS 12C(12C, X), (13C, X), E(cm)≈2.0-6.5 MeV;13C(13C, X), E(cm)≈2.9-6.5 MeV; calculated fusion reaction rate, modified S-factor using CC with IWBC (incoming wave boundary condition) and different interactions. Discussed role of possible resonance near E(cm)≈1.5 MeV.

doi: 10.1088/1742-6596/381/1/012120
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2012ZH21      Eur.Phys.J. A 48, 65 (2012)

G.L.Zhang, C.L.Zhang, H.Q.Zhang, C.J.Lin, D.Y.Pang, X.K.Wu, H.M.Jia, G.P.An, Z.D.Wu, X.X.Xu, F.Yang, Z.H.Liu, S.Kubono, H.Yamaguchi, S.Hayakawa, D.N.Binh, Y.K.Kwon, N.Iwasa, M.Mazzocco, M.La Commara, M.Romoli, C.Signorini

Quasi-elastic scattering of the proton drip line nucleus 17F on 12C at 60 MeV

NUCLEAR REACTIONS 12C(17F, 17F'), E=60 MeV; measured E(17F), I(17F, θ); deduced σ(θ), σ; calculated σ(θ) using optical model and CDCC; deduced parameters. Compared with data, also for nearby projectiles.

doi: 10.1140/epja/i2012-12065-x
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2010DA15      Nucl.Phys. A834, 147c (2010)

M.Dasgupta, L.R.Gasques, D.H.Luong, R.du Rietz, R.Rafiei, D.J.Hinde, C.J.Lin, M.Evers, A.Diaz-Torres

Reaction dynamics of weakly bound nuclei at near-barrier energies

NUCLEAR REACTIONS 208Pb, 209Bi(6Li, X), (7Li, X), (9Be, X), (10B, X), (11B, X), E not given; analyzed fusion suppression factor, systematics. Found simple dependency and relation to break-up.

doi: 10.1016/j.nuclphysa.2009.12.025
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2010FA10      Nucl.Phys. A834, 183c (2010)

G.T.Fan, W.Xu, C.J.Lin, B.J.Xu, F.Jia, G.W.Fan, H.M.Jia, L.F.Yang, Y.J.Li, Q.Y.Pan, W.Luo, X.X.Xu, Z.D.Wu

Systematic uncertainty studies for precision measurement on electric polarizabilities of 3He and 4He

doi: 10.1016/j.nuclphysa.2009.12.034
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2010JI07      Nucl.Phys. A834, 189c (2010)

H.M.Jia, C.J.Lin, H.Q.Zhang, F.Yang, Z.H.Liu, F.Jia, X.X.Xu, S.T.Zhang, K.Hagino

Systematic study of the surface diffuseness of nuclear potential with high precision large-angle quasi-elastic scattering

NUCLEAR REACTIONS 152,154Sm, 184W, 196Pt, 208Pb(16O, 16O'), E(cm)=35-70 MeV; measured σ(θ=175°); calculated σ using CC and single-channel formalisms; deduced nuclear potential diffuseness parameters.

doi: 10.1016/j.nuclphysa.2009.12.036
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2010JI11      Phys.Rev. C 82, 027602 (2010)

H.M.Jia, C.J.Lin, H.Q.Zhang, Z.H.Liu, N.Yu, F.Yang, F.Jia, X.X.Xu, Z.D.Wu, S.T.Zhang, C.L.Bai

Barrier distribution from 9Be+208Pb quasielastic scattering: Breakup effects in the interaction processes

NUCLEAR REACTIONS 208Pb(9Be, 9Be), E=23.9-44.0 MeV; measured particle-spectra, σ(E) for quasielastic scattering; deduced barrier distribution. Comparison with coupled-channel model calculations.

doi: 10.1103/PhysRevC.82.027602
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2010LI33      Nucl.Phys. A834, 450c (2010)

C.J.Lin, X.X.Xu, H.M.Jia, F.Yang, F.Jia, Z.D.Wu, S.T.Zhang, Z.H.Liu, H.Q.Zhang, H.S.Xu, Z.Y.Sun, J.S.Wang, Z.G.Hu, M.Wang, R.F.Chen, X.Y.Zhang, C.Li, X.G.Lei, Z.G.Xu, G.Q.Xiao, W.L.Zhan

Experimental study of the two-proton correlated emission from the excited states of 17, 18Ne and 28, 29S

NUCLEAR REACTIONS 197Au(17Ne, 17Ne'), (18Ne, 18Ne'), (28S, 28S'), (29S, 29S'), E not given; measured Coulomb excitation Ep, Ip(θ), pp-coin, E(particle), I(particle), relative energy spectra, angular distributions; deduced 2p halo states. Kinematically complete experiment, secondary radioactive beams.

RADIOACTIVITY 17,18Ne, 29S(2p); deduced possible 2p-decay or 2He-decay branching ratios.

doi: 10.1016/j.nuclphysa.2010.01.061
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2010XU03      Phys.Rev. C 81, 054317 (2010)

X.X.Xu, C.J.Lin, H.M.Jia, F.Yang, F.Jia, Z.D.Wu, S.T.Zhang, Z.H.Liu, H.Q.Zhang, H.S.Xu, Z.Y.Sun, J.S.Wang, Z.G.Hu, M.Wang, R.F.Chen, X.Y.Zhang, C.Li, X.G.Lei, Z.G.Xu, G.Q.Xiao, W.L.Zhan

Investigation of two-proton emission from excited states of the odd-Z nucleus 28P by complete-kinematics measurements

NUCLEAR REACTIONS 197Au(28P, 28P'), E=46.5 MeV/nucleon [28P secondary beam from 9Be(32S, X), E=80.4 MeV/nucleon primary reaction]; measured Ep, Ip, time of flight, (26Al)(p)(p)-coin. 28P; deduced levels, two-proton emission from excited states.9Be(32S, X)22Ne/23Na/24Mg/25Al/26Al/27Si/28P/29S, E=80.4 MeV/nucleon; measured yields.

doi: 10.1103/PhysRevC.81.054317
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2010XU11      Phys.Rev. C 82, 064316 (2010)

X.X.Xu, C.J.Lin, H.M.Jia, F.Yang, F.Jia, Z.D.Wu, S.T.Zhang, Z.H.Liu, H.Q.Zhang, H.S.Xu, Z.Y.Sun, J.S.Wang, Z.G.Hu, M.Wang, R.F.Chen, X.Y.Zhang, C.Li, X.G.Lei, Z.G.Xu, G.Q.Xiao, W.L.Zhan

Observation of two-α emission from high-lying excited states of 18Ne by complete-kinematics measurements

NUCLEAR REACTIONS 197Au(18Ne, 18Ne'), E=51.8 MeV, [18Ne secondary beam from 9Be(20Ne, X), E=78.2 MeV/nucleon primary reaction]; measured Eα, time-of-flight, (10C)αα-coin. 18Ne; deduced levels, αα(θ), relative momentum, sequential two-alpha emission via 14O excited states. Monte-Carlo simulations.

doi: 10.1103/PhysRevC.82.064316
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2010ZH06      Phys.Rev. C 81, 034611 (2010)

H.Q.Zhang, C.L.Zhang, C.J.Lin, Z.H.Liu, F.Yang, A.K.Nasirov, G.Mandaglio, M.Manganaro, G.Giardina

Competition between fusion-fission and quasifission processes in the 32S+184W reaction

NUCLEAR REACTIONS 184W(32S, X), E=140, 145, 150, 155, 160, 165, 170 MeV; measured capture σ, σ(θ) of fission fragments, fission excitation functions. 182,184(32S, X), E(cm)=120-220 MeV; analyzed fission excitation functions, comparison with previous experimental data and theoretical cross sections using dinuclear system (DNS) model for capture, complete fusion, quasifission, fast fission, and total evaporation residues.

doi: 10.1103/PhysRevC.81.034611
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2010ZH29      Nucl.Phys. A834, 201c (2010)

C.L.Zhang, H.Q.Zhang, C.J.Lin, A.K.Nasirov, G.Mandaglio, M.Manganaro, G.Giardina

Competition between fusion-fission and quasifission processes in 32S+184W reaction

NUCLEAR REACTIONS 184W(32S, F), E(cm)=118.8, 123.1, 127.3, 131.5, 135.8, 141.4, 144.4 MeV; measured fission fragment angular distributions; deduced fission, fusion σ, σ(θ), reaction mechanism features. Comparison with dinuclear system model.

doi: 10.1016/j.nuclphysa.2009.12.040
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2010ZH46      Phys.Rev. C 82, 054609 (2010)

H.Q.Zhang, C.J.Lin, F.Yang, H.M.Jia, X.X.Xu, Z.D.Wu, F.Jia, S.T.Zhang, Z.H.Liu, A.Richard, C.Beck

Near-barrier fusion of 32S+90, 96Zr: The effect of multi-neutron transfers in sub-barrier fusion reactions

NUCLEAR REACTIONS 90Zr(32S, X), E=100-130 MeV: 96Zr(32S, X), E=95-130 MeV; measured particle spectra of fusion evaporation residues (ER), E-TOF plot of ER and beam-like particles (BLP), fusion σ(E, θ); deduced barrier distributions. Comparison with coupled-channel (CC) calculations and with data for 96Zr(40Ca, X) reaction. Effects of multi-neutron transfers.

doi: 10.1103/PhysRevC.82.054609
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2009JI02      Chin.Phys.Lett. 26, 032301 (2009)

F.Jia, C.-J.Lin, H.-Q.Zhang, F.Yang, H.-M.Jia, X.-X.Xu, Z.-D.Wu, Z.-H.Liu, G.-L.Zhang, C.-L.Zhang

Experimental Evidence of Two-Proton Emissions from 18Ne Excited State

NUCLEAR REACTIONS 197Au(18Ne, 18Ne'), E not given; measured Ep, Ip. 18Ne; deduced level energies. Two proton decay.

doi: 10.1088/0256-307X/26/3/032301
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2009LI23      Phys.Rev. C 79, 064603 (2009)

C.J.Lin, H.M.Jia, H.Q.Zhang, F.Yang, X.X.Xu, F.Jia, Z.H.Liu, K.Hagino

Systematic study of the surface properties of the nuclear potential with high precision large-angle quasi-elastic scatterings

NUCLEAR REACTIONS 152,154Sm, 184W, 196Pt, 208Pb(16O, 16O), E=36-80 MeV; measured particle spectra, σ as a function of beam energy; deduced diffuseness parameters using single-channel and coupled-channels calculations.

doi: 10.1103/PhysRevC.79.064603
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2009LI29      Phys.Rev. C 80, 014310 (2009)

C.J.Lin, X.X.Xu, H.M.Jia, F.Yang, F.Jia, S.T.Zhang, Z.H.Liu, H.Q.Zhang, H.S.Xu, Z.Y.Sun, J.S.Wang, Z.G.Hu, M.Wang, R.F.Chen, X.Y.Zhang, C.Li, X.G.Lei, Z.G.Xu, G.Q.Xiao, W.L.Zhan

Experimental study of two-proton correlated emission from 29S excited states

NUCLEAR REACTIONS 197Au(29S, 29S'), E=49.2 MeV/nucleon; measured particle spectra by ΔE-tof, (29S)(p)(p)-coin. 29S; deduced excitation spectrum, two proton and 2He cluster decay branching ratios.

RADIOACTIVITY 29S(2p); measured (29S)(p)(p)-coin; deduced branching ratios of two proton and 2He cluster decay modes from excited states.

doi: 10.1103/PhysRevC.80.014310
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2009WU01      Chin.Phys.Lett. 26, 022503 (2009)

Z.-D.Wu, C.-J.Lin, H.-Q.Zhang, Z.-H.Liu, F.Yang, G.-P.An, C.-L.Zhang, G.-L.Zhang, H.-M.Jia, X.-X.Xu, C.-L.Bai, N.Yu, F.Jia

Optical Potential Parameters for Halo Nucleus System 6He+12C from Transfer Reaction 11B(7Li, 6He)12C

NUCLEAR REACTIONS 11B(7Li, 6He), E=18.3, 28.3 MeV; analyzed σ(θ). 12C(6He, 7Li); deduced optical potential parameters.

doi: 10.1088/0256-307X/26/2/022503
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2008AN17      Chin.Phys.Lett. 25, 4237 (2008)

G.-P.An, C.-J.Lin, H.-Q.Zhang, Z.-H.Liu, F.Yang, G.-L.Zhang, C.-L.Zhang, Z.-D.Wu, F.Jia, H.-M.Jia, X.-X.Xu, C.-L.Bai, N.Yu

Optical Potential Parameters of Weakly Bound Nuclear System 17F+13C

NUCLEAR REACTIONS 16O(14N, 14N), (14N, 13C), E=76.2, 57.0 MeV; measured σ(θ). Compared results to model calculations.

doi: 10.1088/0256-307X/25/12/014
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2008JI03      Chin.Phys.Lett. 25, 2834 (2008)

H.-M.Jia, C.-J.Lin, H.-Q.Zhang, Z.-H.Liu, F.Yang, F.Jia, C.-L.Zhang, G.-P.An, Z.-D.Wu, X.-X.Xu, C.-L.Bai, N.Yu

Surface Diffuseness Anomaly in 16O+208Pb Quasi-elastic Scattering at Backward Angle

NUCLEAR REACTIONS 208Pb(16O, 16O'), E=40.50-80.25 MeV; measured quasi=elastic scattering excitation function at backward angles.

doi: 10.1088/0256-307X/25/8/028
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2008LI25      J.Phys.(London) G35, 077001 (2008)

H.Y.Liao, H.M.Chang, M.H.Chou, M.Deniz, H.X.Huang, F.S.Lee, H.B.Li, J.Li, C.W.Lin, F.K.Lin, S.K.Lin, S.T.Lin, V.Singh, H.T.Wong, S.C.Wu, and the TEXONO Collaboration

Production and decay of the 73Ge*(1/2-) metastable state in a low-background germanium detector

RADIOACTIVITY 73Ga(β-), 73As(EC); measured Eγ, Iγ. 73Ge deduced neutrino-induced production close to a power reactor.

doi: 10.1088/0954-3899/35/7/077001
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2008YA03      Phys.Rev. C 77, 014601 (2008)

F.Yang, C.J.Lin, X.K.Wu, H.Q.Zhang, C.L.Zhang, P.Zhou, Z.H.Liu

Barrier distributions from 32S+90,96Zr quasi-elastic scattering: Investigation of the role of neutron transfer in sub-barrier fusion reactions

NUCLEAR REACTIONS 90,96Zr(32S, X), E=60-90 MeV; measured cross sections, barrier distributions.

doi: 10.1103/PhysRevC.77.014601
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2007BO39      At.Data Nucl.Data Tables 93, 831 (2007)

J.B.Boffard, B.Chiaro, T.Weber, C.C.Lin

Electron-impact excitation of argon: Optical emission cross sections in the range of 300-2500 nm

ATOMIC PHYSICS Ar(e, e'), E=25, 50, 100 eV; measured cross sections and excitation functions.

doi: 10.1016/j.adt.2007.06.004
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2007LI43      Nucl.Phys. A787, 281c (2007)

C.J.Lin, H.Q.Zhang, F.Yang, M.Ruan, Z.H.Liu, Y.W.Wu, X.K.Wu, P.Zhou, C.L.Zhang, G.L.Zhang, G.P.An, H.M.Jia, X.X.Xu

Effects of breakup of weakly bound projectile and neutron transfer on fusion reactions around Coulomb barrier

NUCLEAR REACTIONS 152Sm(16O, 16O), (16O, 16O'), (16O, X), E(cm)=45-70 MeV; measured σ(θ=156, θ=160, θ=164), evaporation residue σ for boron, carbon, nitrogen and oxygen isotopes; deduced reaction mechanism features. 208Pb(6Li, 6Li), (6Li, 6Li'), (6Li, X), (7Li, 7Li), (7Li, 7Li'), (7Li, X), E(cm)=18-42 MeV; 90,96Zr(32S, X), E(cm)=60-95 MeV; measured σ; deduced reaction mechanism features. 208Pb(6Li, 6Li), E(cm)=26-40 MeV; measured fusion σ; deduced reaction mechanism features. Comparison with coupled-channels model.

doi: 10.1016/j.nuclphysa.2006.12.044
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2007LI65      Phys.Rev. C 76, 044321 (2007)

C.J.Lin, X.Z.Zhang, R.Zhang, Z.H.Liu, H.Q.Zhang

Low-lying E1 strength in light drip-line nuclei

NUCLEAR STRUCTURE 11Be; calculated E1 strengths as function of excitation energy, DWA approximation, comparisons with experimental data, deduced spectroscopic factors.

doi: 10.1103/PhysRevC.76.044321
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2007SA44      Nucl.Phys. A790, 780c (2007)

A.N.Salgueiro, C.-Y.Lin, A.F.R.de Toledo Piza, M.Weidemuller

Doorway states and the Bose-Hubbard model

doi: 10.1016/j.nuclphysa.2007.03.118
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2007ZH02      Chin.Phys.Lett. 24, 397 (2007)

G.-L.Zhang, H.-Q.Zhang, Z-H.Liu, C.-L.Zhang, C.-J.Lin, F.Yang, G.-P.An, H.-M.Jia, Z.-D.Wu, X.-X.Xu, C.-L.Bai, N.Yu

Calculation of Interaction Potentials between Spherical and Deformed Nuclei

NUCLEAR REACTIONS 154Sm(32S, X), E(cm)=100-130 MeV; calculated interaction potentials, fusion σ, dependence on deformation and orientation. Double folding model.

doi: 10.1088/0256-307X/24/2/026
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2006NI09      Phys.Atomic Nuclei 69, 1399 (2006)

K.Nishio, H.Ikezoe, M.Asai, K.Tsukada, S.Mitsuoka, K.Tsuruta, K.Satou, C.J.Lin, T.Ohsawa

Evidence of Complete Fusion in the Subbarrier 16O + 238U Reaction

NUCLEAR REACTIONS 238U(16O, 4n), (16O, 5n), (16O, 6n), E(cm)=70-95 MeV; measured evaporation residue σ; deduced reaction mechanism features. Comparison with statistical model predictions.

RADIOACTIVITY 248,249,250Fm(α) [from 238U(16O, xn)]; measured Eα, T1/2.

doi: 10.1134/S1063778806080187
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2006SA09      Phys.Rev. C 73, 034609 (2006)

K.Satou, H.Ikezoe, S.Mitsuoka, K.Nishio, C.J.Lin, S.C.Jeong

Measurements of evaporation residue cross sections for the fusion reactions 86Kr + 134Ba and 86Kr + 138Ba

NUCLEAR REACTIONS 138Ba(86Kr, xnypzα), E(cm) ≈ 206-241 MeV; 134Ba(86Kr, xnypzα), E(cm) ≈ 220-227 MeV; measured evaporation residue σ; deduced shell structure effects.

doi: 10.1103/PhysRevC.73.034609
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Note: The following list of authors and aliases matches the search parameter C.Lin: , C.C.LIN, C.D.LIN, C.J.LIN, C.K.LIN, C.L.LIN, C.S.LIN, C.W.LIN, C.Y.LIN, C.Z.LIN