NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = C.J.Lin Found 119 matches. Showing 1 to 100. [Next]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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
2014ZH18 Phys.Rev. C 89, 054602 (2014) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
2006ZH12 Chin.Phys.Lett. 23, 1146 (2006) C.-L.Zhang, H.-Q.Zhang, C.-J.Lin, M.Ruan, Z.-H.Liu, F.Yang, X.-K.Wu, P.Zhou, G.-P.An, H.-M.Jia, Z.-D.Wu, X.-X.Xu.C.-L.Bai Unusual Threshold Anomaly in the 6Li+208Pb System NUCLEAR REACTIONS 208Pb(6Li, 6Li), E=25-46 MeV; measured elastic σ(θ); deduced optical potential parameters, effects of coupling to breakup channel.
doi: 10.1088/0256-307X/23/5/023
2005LI49 Eur.Phys.J. A 26, 73 (2005) Z.H.Liu, C.Signorini, M.Mazzocco, M.Ruan, H.Q.Zhang, T.Glodariu, Y.W.Wu, F.Soramel, C.J.Lin, F.Yang Partial fusion of a weakly bound projectile with heavy target at energies above the Coulomb barrier NUCLEAR REACTIONS 208Pb(6Li, X), E(cm)=27-39 MeV; 209Bi(9Be, X), E(cm)=34-50 MeV; analyzed complete and incomplete fusion σ; deduced reaction mechanism features.
doi: 10.1140/epja/i2004-10305-4
2005ZH34 Chin.Phys.Lett. 22, 3048 (2005) H.-Q.Zhang, Z.-H.Liu, F.Yang, C.-J.Lin, M.Ruan, Y.-W.Wu, Z.-X.Li, X.-Z.Wu, K.Zhao, N.Wang Dynamical Effects on Sub-barrier Fusion of 40, 48Ca+90, 96Zr NUCLEAR REACTIONS 96Zr(48Ca, X), E=139.75-176 MeV; 96Zr(48Ca, X), E=133.75-170 MeV; measured fusion σ; 90,96Zr(40Ca, X), E ≈ 120-160 MeV; analyzed fusion σ; deduced dynamical effects. Quantum molecular dynamics model calculation.
doi: 10.1088/0256-307X/22/12/017
2004IK03 Prog.Theor.Phys.(Kyoto), Suppl. 154, 45 (2004) H.Ikezoe, K.Satou, S.Mitsuoka, K.Nishio, K.Tsuruta, S.-C.Jeong, C.-J.Lin Effect of Closed Shell Structure on Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 134,138Ba(82Se, X), (86Kr, X), 204Pb(16O, X), Ce(82Se, X), E* ≈ 5-80 MeV; measured evaporation residue σ; deduced shell effects.
doi: 10.1143/PTPS.154.45
2004LI19 Phys.Rev. C 69, 034326 (2004) Z.H.Liu, M.Ruan, Y.L.Zhao, H.Q.Zhang, F.Yang, Z.Y.Ma, C.J.Lin, B.Q.Chen, Y.W.Wu, W.L.Zhan, Z.Y.Guo, G.Q.Xiao, H.S.Xu, Z.Y.Sun, J.X.Li, Z.J.Chen Evidence for enhancement of the total reaction cross sections for 27, 28P with a 28Si target and examination of possibly relevant mechanisms NUCLEAR REACTIONS Si(23Na, X), (24Mg, X), (25Mg, X), (25Al, X), (26Al, X), (26Si, X), (27Si, X), (27P, X), (28P, X), E ≈ 20-40 MeV/nucleon; measured reaction σ; deduced reaction mechanism features. Secondary beams from 36Ar fragmentation. Modified Glauber model analysis.
doi: 10.1103/PhysRevC.69.034326
2004LI56 Prog.Theor.Phys.(Kyoto), Suppl. 154, 184 (2004) Impacts of the Cutoff of Coupled-Channels Effects on Heavy-Ion Fusion Reactions at Extreme Sub-Barrier Energies NUCLEAR REACTIONS 58,64Ni(58Ni, X), (64Ni, X), E(cm) ≈ 90-120 MeV; analyzed fusion σ; deduced dynamic polarization potentials.
doi: 10.1143/PTPS.154.184
2004LI57 Chin.Phys.Lett. 21, 1711 (2004) Z.-H.Liu, M.Ruan, Y.-L.Zhao, H.-Q.Zhang, F.Yang, Z.-Y.Ma, C.-J.Lin, B.-Q.Chen, Y.-W.Wu, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao, H.-S.Xu, Z.-Y.Sun, J.-X.Li, Z.-Q.Chen Possible Experimental Evidence of a Moderate Proton Halo in 29S NUCLEAR REACTIONS 28Si(29Si, X), (27Si, X), (28P, X), (27P, X), E ≈ 40 MeV/nucleon; measured reaction σ. 29S deduced proton halo features. Modified Glauber theory analysis.
doi: 10.1088/0256-307X/21/9/009
2004MI38 Prog.Theor.Phys.(Kyoto), Suppl. 154, 53 (2004) S.Mitsuoka, H.Ikezoe, K.Nishio, K.Satou, K.Tsuruta, C.-J.Lin Dependence of Heavy-Ion Fusion Reaction on Nuclear Deformation NUCLEAR REACTIONS 154Sm(60Ni, X), (64Ni, X), 182W(32S, X), 150Nd(76Ge, X), 198Pt(28Si, X), E* ≈ 10-70 MeV; measured fusion excitation functions; deduced deformation effects.
doi: 10.1143/PTPS.154.53
2004NI10 Phys.Rev.Lett. 93, 162701 (2004) K.Nishio, H.Ikezoe, Y.Nagame, M.Asai, K.Tsukada, S.Mitsuoka, K.Tsuruta, K.Satou, C.J.Lin, T.Ohsawa Evidence of Complete Fusion in the Sub-Barrier 16O + 238U Reaction NUCLEAR REACTIONS 238U(16O, 4n), (16O, 5n), (16O, 6n), E(cm) ≈ 70-105 MeV; measured evaporation residue σ; deduced complete fusion at sub-barrier energies, role of orientation and deformation. Comparison with statistical model predictions.
doi: 10.1103/PhysRevLett.93.162701
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