NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = G.L.Zhang Found 69 matches. 2023HU10 Phys.Rev. C 107, 044309 (2023) Z.Huang, G.X.Zhang, C.X.Yuan, G.L.Zhang, D.Mengoni, B.S.Cai, S.P.Hu, H.Q.Zhang, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, D.Bazzacco, D.R.Napoli, F.Galtarossa, F.Recchia, G.de Angelis, M.Siciliano, R.Menegazzo, S.M.Lenzi Level scheme study of 91Mo: Weak-coupling approximation in the N=50 region NUCLEAR REACTIONS 89Y(6Li, X)91Mo, E=34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 91Mo; deduced levels, J, π, transition intensities, angular distribution from oriented nuclei (ADO) ratios, δ, T1/2 for two isomeric states, high-spin states, B(E2), configurations. Comparison with shell-model calculation employing the JUN45 interaction (KSHELL code). GALILEO ψ-ray spectrometer consisting of 25 Compton-suppressed HPGe tapered detectors at Tandem-XTU accelerator (INFN-LNL, Italy).
doi: 10.1103/PhysRevC.107.044309
2023RE11 Phys.Rev. C 108, 044301 (2023) Z.Ren, J.-B.Lu, G.-X.Dong, Y.Zheng, Y.-H.Wu, T.-J.Gao, P.-Y.Yang, Y.Hao, K.-Y.Ma, X.-G.Wu, C.-B.Li, Z.Huang, G.-X.Zhang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, D.Testov, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, D.Mengoni, D.Bazzacco, G.-L.Zhang Level scheme of 92Nb and observation of an oblate collective rotational band
doi: 10.1103/PhysRevC.108.044301
2022HU22 Phys.Rev. C 106, 064331 (2022) Z.Huang, G.X.Zhang, G.L.Zhang, S.P.Hu, S.M.Lenzi, D.Mengoni, J.L.Ferreira, Y.F.Lv, J.B.Lu, B.Paes, E.N.Cardozo, H.Q.Zhang, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, D.Bazzacco, P.R.John, D.R.Napoli, F.Galtarossa, F.Recchia, G.de.Angelis, M.Siciliano, R.Menegazzo, J.Lubian Level scheme study of 92Mo: Searching for evidence of core excitation NUCLEAR REACTIONS 89Y(6Li, 3n), E=34 MeV; measured Eγ, Iγ; γγ-coin, γγ(θ). 92Mo; deduced levels, J, π, δ, B(E1), T1/2 of excited states, high-spin states, angular distribution from the oriented nuclei (ADO) ratio, configurations. Comparison to JUN45 and JJGLEM shell-model calculation. GALILEO γ-array consisting of 25 Compton suppressed HPGe and 8 BGO crystals served as the anti-Compton shield of each HPGe at XTU Tandem accelerator (INFN Legnaro National Laboratory).
doi: 10.1103/PhysRevC.106.064331
2022RE11 Phys.Rev. C 106, 024323 (2022), Erratum Phys.Rev. C 107, 049902 (2023) Z.Ren, J.-B.Lu, G.-L.Zhang, Y.-H.Wu, T.-J.Gao, K.-Y.Ma, Z.Huang, G.-X.Zhang, M.-L.Wang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, D.Mengoni, D.Bazzacco Reinvestigation of the level structures of the N=49 isotones 89Zr and 91Mo NUCLEAR REACTIONS 89Y(6Li, 4n2p)89Zr, (6Li, 4n)91Mo, E=34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO), (particle)γ-coin using GALILEO array with 25 BGO-Compton-suppressed HPGe detectors for γ rays, and EUCLIDES 4π Si-ball array for charged particles at the Tandem-XTU accelerator of INFN-LNL, Legnaro. 89Zr, 91Mo; deduced high-spin levels, J, π, ADO ratios, multipolarities, configurations. 91Nb, 92Mo; deduced ADO ratios for certain γ-transitions. Comparison with spherical-basis shell-model calculations. NUCLEAR STRUCTURE 89Zr, 91Mo; calculated levels, J, π, components of the wave functions and their partitions for spherical configurations for protons and neutrons. Comparison with experimental data. Systematics of energies in N=49 isotones: 9/2+, 13/2+, 17/2+, 21/2+, 23/2+ and 25/2+ states in 89Zr, 91Mo, 93Ru, 95Pd, and those of 8+, 9+, 10+, 12+, 13+ and 14+ in 88Y, 90Nb, 92Tc, 94Rh.
doi: 10.1103/PhysRevC.106.024323
2021HU12 Eur.Phys.J. A 57, 137 (2021) Z.Huang, G.X.Zhang, S.P.Hu, B.Paes, E.N.Cardozo, J.L.Ferreira, M.J.Ermamatov, G.L.Zhang, J.B.Lu, M.Mazzocco, Y.F.Lv, H.Q.Zhang, H.B.Sun, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, F.Recchia, D.Mengoni, D.Bazzacco, J.Lubian, X.B.Qin, H.M.Zhao Angular distribution of γ rays emitted by oriented nuclei: the case of 92Mo formed in the reaction 6Li + 89Y NUCLEAR REACTIONS 89Y(6Li, X)92Mo, E=34 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, γ-ray angular distributions, E1, M2 transition strengths, mixing ratios and T1/2. Comparison with the NushellX calculation using the jjglem interaction.
doi: 10.1140/epja/s10050-021-00443-6
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
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
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
2020LI12 Phys.Rev. C 101, 044313 (2020) C.B.Li, G.L.Zhang, C.X.Yuan, G.X.Zhang, S.P.Hu, W.W.Qu, Y.Zheng, H.Q.Zhang, D.Mengoni, D.Testov, J.J.Valiente-Dobon, H.B.Sun, N.Wang, X.G.Wu, G.S.Li, M.Mazzocco, A.Gozzelino, C.Parascandolo, D.Pierroutsakou, M.La Commara, F.Recchia, A.I.Sison, S.Bakes, I.Zanon, S.Aydin, D.Bazzacco New level scheme and shell model description of 212Rn NUCLEAR REACTIONS 209Bi(6Li, 3n)212Rn, E=28, 30, 34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using GALILEO array at the Tandem-XTU accelerator of Legnaro National Laboratory. 212Rn; deduced levels, J, π, multipolarities, B(E2), B(E3), configurations. Comparison with large-scale shell-model calculations with multiparticle configurations. Systematics of low-, and medium-spin levels in N=126 isotones: 210Po, 212Rn, 214Ra and 216Th. Systematics of 3- to 0+ and 15/2- to 9/2+ excitation energies in N=126 and 127 isotones of Z=82-91. NUCLEAR STRUCTURE 212Rn; calculated levels, J, π, amplitudes of shell-model multiparticle configurations for different levels, B(M1), B(E2), B(E3) using large-scale shell-model calculations with multiparticle configurations. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.044313
2020RO16 Chin.Phys.C 44, 104003 (2020) C.-H.Rong, G.-L.Zhang, L.Gan, Z.-Ho.Li, L.C.Brandao, E.N.Cardozo, M.R.Cortes, Y.-J.Li, Ju.Su, S.-Q.Yan, S.Zeng, G.Lian, B.Guo, Y.-B.Wang, W.-P.Liu, J.Lubian The angular distributions of elastic scattering of 12, 13C+Zr NUCLEAR REACTIONS 90,91,92,94,96Zr(12C, 12C), (13C, 13C), E=66, 64 MeV; measured reaction products; deduced σ, the neutron spectroscopic amplitudes using the optical model and coupled channel calculations.
doi: 10.1088/1674-1137/abab8d
2020WA07 Eur.Phys.J. A 56, 31 (2020) M.Wang, W.J.Sun, B.H.Sun, J.Li, L.H.Zhu, Y.Zheng, G.L.Zhang, L.C.He, W.W.Qu, F.Wang, T.F.Wang, C.Xiong, C.Y.He, G.S.Li, J.L.Wang, X.G.Wu, S.H.Yao, C.B.Li, H.W.Li, S.P.Hu, J.J.Liu The ΔI = 2 bands in 109In: possible antimagnetic rotation NUCLEAR REACTIONS 100Mo(14N, 5n), E=78 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using two low-energy photon detectors and nine BGO-Compton-suppressed HPGe detectors at CIAE-Beijing. 109In; deduced levels, J, π, multipolarities, anti-magnetic rotational band, alignments, configurations. Comparison with calculations using titled axis cranking calculation in the framework of covariant density function theory (TAC-CDFT), and with previous experimental results. Systematics of bands based on πg7/2 orbital in 107,109,111,113In. See also 2018Wa15, a related experiment from the same laboratory.
doi: 10.1140/epja/s10050-020-00039-6
2019GH07 Nucl.Phys. A990, 294 (2019) Assessment of the quality of different pocket formulas in reproducing experimental sub-barrier fusion cross sections
doi: 10.1016/j.nuclphysa.2019.07.012
2019LA13 Astrophys.J. 879, 23 (2019) L.Lamia, M.Mazzocco, R.G.Pizzone, S.Hayakawa, M.La Cognata, C.Spitaleri, C.A.Bertulani, A.Boiano, C.Boiano, C.Broggini, A.Caciolli, S.Cherubini, G.D'Agata, H.da Silva, R.Depalo, F.Galtarossa, G.L.Guardo, M.Gulino, I.Indelicato, M.La Commara, G.La Rana, R.Menegazzo, J.Mrazek, A.Pakou, C.Parascandolo, D.Piatti, D.Pierroutsakou, S.M.R.Puglia, S.Romano, G.G.Rapisarda, A.M.Sanchez-Benitez, M.L.Sergi, O.Sgouros, F.Soramel, V.Soukeras, R.Sparta, E.Strano, D.Torresi, A.Tumino, H.Yamaguchi, G.L.Zhang Cross-section Measurement of the Cosmologically Relevant 7Be(n, α)4He Reaction over a Broad Energy Range in a Single Experiment NUCLEAR REACTIONS 2H(7Be, 2α), E<2 MeV; measured reaction products, Ep, Ip. 8Be; deduced σ, astrophysical reaction rates. Trojan Horse Method.
doi: 10.3847/1538-4357/ab2234
2019LV02 Chin.Phys.C 43, 104102 (2019) Y.-F.Lv, J.-B.Lu, G.-L.Zhang, Y.-H.Wu, C.-X.Yuan, G.-J.Fu, G.-X.Zhang, Z.Huang, M.-L.Wang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, C.-Q.Li, K.-Y.Ma, Y.-J.Ma, Yu.-Z.Liu, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, F.Recchia, D.Mengoni, D.Bazzacco Low-lying states of 92, 93Nb excited in the reactions induced by the weakly-bound nucleus 6Li near the Coulomb barrier NUCLEAR REACTIONS 89Y(6Li, X)92Nb/93Nb, E=34 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, level schemes.
doi: 10.1088/1674-1137/43/10/104102
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
2018CO08 Phys.Rev. C 97, 044613 (2018) G.Colucci, G.Montagnoli, A.M.Stefanini, H.Esbensen, D.Bourgin, P.Colovic, L.Corradi, M.Faggian, E.Fioretto, F.Galtarossa, A.Goasduff, J.Grebosz, F.Haas, M.Mazzocco, F.Scarlassara, C.Stefanini, E.Strano, S.Szilner, M.Urbani, G.L.Zhang Isotopic effects in sub-barrier fusion of Si + Si systems NUCLEAR REACTIONS 30Si(30Si, X), E=47-90 MeV; measured fusion evaporation residues (ERs), fusion σ(E) at the XTU tandem accelerator facility of LNL-INFN-Legnaro. Comparison with previous experimental results, 28Si+28Si data, and with theoretical calculations using coupled-channels method with aM3Y+repulsion potential, and including one- and two-phonon excitations and the mutual excitations of the low-lying 2+ and 3- states in projectiles and targets.
doi: 10.1103/PhysRevC.97.044613
2018QU04 Chin.Phys.C 42, 074001 (2018) W.-W.Qu, G.-L.Zhang, G.-Y.Tian, Z.-Q.Chen, S.-P.Xu, R.Wada Angular distribution measurement for 12C fragmentation via 12C + 12C scattering at 100 MeV/u NUCLEAR REACTIONS 12C(12C, X)9Be/10B/11B, E=100 MeV/nucleon; measured reaction products; deduced σ(θ). Comparison with theoretical calculations.
doi: 10.1088/1674-1137/42/7/074001
2018WA15 Phys.Rev. C 98, 014304 (2018), Erratum Phys.Rev. C 102, 069903 (2020) M.Wang, Y.Y.Wang, L.H.Zhu, B.H.Sun, G.L.Zhang, L.C.He, W.W.Qu, F.Wang, T.F.Wang, Y.Y.Chen, C.Xiong, J.Zhang, J.M.Zhang, Y.Zheng, C.Y.He, G.S.Li, J.L.Wang, X.G.Wu, S.H.Yao, C.B.Li, H.W.Li, S.P.Hu, J.J.Liu New high-spin structure and possible chirality in 109In NUCLEAR REACTIONS 100Mo(14N, 5n), E=78 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using two low-energy photon detectors and nine BGO-Compton-suppressed HPGe detectors at CIAE-Beijing. 109In; deduced levels, J, π, multipolarities, bands, alignments, configurations, and possible chiral partner bands. Comparison with calculations using titled axis cranking calculation in the framework of covariant density function theory (TAC-CDFT), and with previous experimental results. Systematics of yrast states in 103,105,107,109,111,113In.
doi: 10.1103/PhysRevC.98.014304
2018ZH06 Phys.Rev. C 97, 014611 (2018) G.L.Zhang, G.X.Zhang, S.P.Hu, Y.J.Yao, J.B.Xiang, H.Q.Zhang, J.Lubian, J.L.Ferreira, B.Paes, E.N.Cardozo, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, P.R.John, M.Siciliano, F.Galtarossa, R.Francesco, D.Mengoni, D.Bazzacco, E.T.Li, X.Hao, W.W.Qu One-neutron stripping processes to excited states of 90Y* in the 89Y(6Li, 5Li)90Y* reaction NUCLEAR REACTIONS 89Y(6Li, 5Li)90Y*, E=22, 34 MeV; measured in-beam and off-beam Eγ, Iγ, γγ- and pγ-coin, ΔE-E for protons, deuterons, tritons, and α particles, one-neutron stripping σ(E) using GALILEO array for γ rays and 4π Si-ball EUCLIDES for particles at the Tandem-XTU accelerator of Legnaro National Laboratory. 90Y, 93Mo; deduced level schemes. Comparisons of cross sections with parameter-free coupled reaction channel calculations.
doi: 10.1103/PhysRevC.97.014611
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
2017LI28 Nucl.Instrum.Methods Phys.Res. B410, 158 (2017) L.X.Liu, H.W.Wang, Y.G.Ma, X.G.Cao, X.Z.Cai, J.G.Chen, G.L.Zhang, J.L.Han, G.Q.Zhang, J.F.Hu, X.H.Wang, W.J.Li, Z.Yan, H.J.Fu Measurements of the total cross section of natBe with thermal neutrons from a photo-neutron source NUCLEAR REACTIONS 9Be(n, X), E=0.007-0.1 eV; measured reaction products, En, In, time-of-flight; deduced σ. Comparison with available data.
doi: 10.1016/j.nimb.2017.08.022
2017QU02 Phys.Rev. C 95, 044616 (2017) W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto Repulsive three-body force and channel-coupling effects via 12C+12C scattering at 100A MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=100 MeV/nucleon; measured scattered 12C using Grand Raiden high-resolution magnetic spectrometer, and 10B, 11C and other particles by the energy loss and time-of-flight (TOF) information, differential cross sections for the ground state, 4.44 MeV, 2+ state, and the sum of the 7.65 MeV, 0+ and the 9.64 MeV, 3- states in 12C using the Ring Cyclotron facility at RCNP-Osaka. Comparison with microscopic coupled-channel calculations, using the double folding method with three different complex G-matrix interactions, the ESC, CEG07b, and MPa.
doi: 10.1103/PhysRevC.95.044616
2016GU16 Phys.Rev. C 94, 044605 (2016) M.F.Guo, G.L.Zhang, P.R.S.Gomes, J.Lubian, E.Ferioli Negligible suppression of the complete fusion of 6, 7Li on light targets, at energies above the barrier NUCLEAR REACTIONS 12,13C, 16O, 24Mg(6Li, X), (7Li, X), E=2-12 MeV; calculated complete fusion σ(E) using coupled-channel (CC) approach. Comparison with from predictions of the statistical evaporation code CASCADE, and with experimental values. Discussed breakup process and breakup threshold anomaly (BTA).
doi: 10.1103/PhysRevC.94.044605
2016HU01 Phys.Rev. C 93, 014621 (2016) S.P.Hu, G.L.Zhang, J.C.Yang, H.Q.Zhang, P.R.S.Gomes, J.Lubian, J.L.Ferreira, X.G.Wu, J.Zhong, C.Y.He, Y.Zheng, C.B.Li, G.S.Li, W.W.Qu, F.Wang, L.Zheng, L.Yu, Q.M.Chen, P.W.Luo, H.W.Li, Y.H.Wu, W.K.Zhou, B.J.Zhu, H.B.Sun One-neutron stripping processes to excited states of the 6Li + 96Zr reaction at near-barrier energies NUCLEAR REACTIONS 96Zr(6Li, X)97Zr, E=14-28 MeV; measured particle spectra of α, protons and deuterons from break-up process, Eγ, Iγ, γγ-coin, fusion σ(E) for one-neutron stripping reaction at HI-13 Tandem Accelerator of CIAE-Beijing. Breakup of 6Li. 97Zr; deduced levels, J, π. No evidence of two-neutron transfer. Comparison of fusion σ(E) with coupled reaction channel (CRC) calculations for the one-neutron stripping of 6Li. NUCLEAR STRUCTURE 96,97Zr; calculated levels, J, π, spectroscopic amplitudes using shell-model with NUSHELLX code; deduced coupling scheme between 96Zr target and 97Zr final nucleus. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.014621
2016LI41 Phys.Rev. C 94, 024337 (2016) X.Q.Li, C.Xu, S.Q.Zhang, H.Hua, J.Meng, R.A.Bark, Q.B.Chen, C.Y.Niu, R.Han, S.M.Wyngaardt, S.Y.Wang, S.Wang, B.Qi, L.Liu, L.H.Zhu, Z.Shi, G.L.Zhang, B.H.Sun, X.Y.Le, C.Y.Song, Y.L.Ye, D.X.Jiang, F.R.Xu, Z.H.Li, J.J.Sun, Y.Shi, P.W.Zhao, W.Y.Liang, C.G.Li, C.G.Wang, X.C.Chen, Z.H.Li, D.P.Sun, C.Liu, Z.Q.Li, P.Jones, E.A.Lawrie, J.J.Lawrie, M.Wiedeking, T.D.Bucher, T.Dinoko, B.V.Kheswa, L.Makhathini, S.N.T.Majola, J.Ndayishimye, S.P.Noncolela, O.Shirinda, J.Gal, G.Kalinka, J.Molnar, B.M.Nyako, J.Timar, K.Juhasz, M.Arogunjo Spectroscopy of 155Yb: Structure evolution in the N=85 isotones NUCLEAR REACTIONS 144Sm(16O, 5n), E=118 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO ratios) at cyclotron facility of iThemba LABS. 155Yb; deduced high-spin levels, J, π, multipolarity, bands, configurations; calculated potential energy contour in (β, γ) plane. Comparison with semiempirical shell-model (SESM) calculations. Predicted coexistence of prolate and oblate shapes from adiabatic and configuration-fixed constrained triaxial covariant density functional theory (CDFT) calculations. Systematics of low-lying levels in N=84-87 isotones: 148,149,150,151Gd, 150,151,152,153Dy, 152,153,154,155Er, 154,155,156,157Yb, 156,157,158,159Hf.
doi: 10.1103/PhysRevC.94.024337
2016QU02 Eur.Phys.J. A 52, 327 (2016) A search for parameters of universal sub-barrier fusion excitation function COMPILATION 90,96Zr, 110Pd, 110Zr(32S, x), 90,96Zr, 124,132Sn(40Ca, x), (48Ca, x), 144,148,154Sm, 186W(16O, x), 144Sm(17O, x), E(cm)≈0.5-2 Coulomb barrier; compiled fusion σ; deduced simple estimates of fusion σ (one for symmetric and the other for asymmetric combination of nuclei), formula parameters.
doi: 10.1140/epja/i2016-16327-3
2016ZH04 Eur.Phys.J. A 52, 39 (2016) G.L.Zhang, W.W.Qu, M.F.Guo, H.Q.Zhang, R.Wolski, J.Q.Qian Comparative studies for different proximity potentials applied to sub-barrier fusion reactions NUCLEAR REACTIONS 58,60,62,64Ni, 76Ge(16O, x), 58,+60,64Ni, 74Ge, 118Sn(18O, x), 58,64Ni(58Ni, x), 64Ni(64Ni, x), 74Ge(18O, x), 90,96Zr, 110Pd(32S, x), (36S, x), (40Ca, x), (48Ca, x), 124,132Sn(40Ca, x), (48Ca, x), 118,124,132Sn(64Ni, x), 124,132Sn(58Ni, x), E(r)=0.8-1.3 [Er is the reduced E(cm)]; calculated Coulomb barrier height, fusion σ using different proximity potentials; deduced parameters using fusion σ data.
doi: 10.1140/epja/i2016-16039-8
2016ZH17 Nucl.Phys. A951, 86 (2016) G.L.Zhang, Y.J.Yao, M.F.Guo, M.Pan, G.X.Zhang, X.X.Liu Comparative studies for different proximity potentials applied to large cluster radioactivity of nuclei NUCLEAR STRUCTURE 222,224,226Ra, 228,230,232Th, 230,232,234,236U, 236,238,240Pu, 242Cm; calculated large cluster radioactivity T1/2 using more different proximity potentials, Compared with data and published calculations using different models.
doi: 10.1016/j.nuclphysa.2016.03.039
2015GU14 Int.J.Mod.Phys. E24, 1550040 (2015) Calculation of α half-lives for Z ≥ 94 nuclei by proximity potential with a new universal function RADIOACTIVITY 232,233,234,235,236,237,238,239,240Pu, 238,239,240,241,242,243Am, 240,241,242,243,244Cm, 245,247Bk, 242,244Cf, 250,251,252,253,254Cf, 251,252,253Es, 255Es, 251,252Fm, 254,256Fm, 254No, 261,263,265Sg, 266Sg, 271Sg, 264,265,266,267Bh, 272Bh, 264,265,266,267Hs, 269Hs, 275Hs, 270Ds, 284Cn, 286,288Fl, 290,292Lv, 294Og(α); calculated T1/2. Comparison with experimental data.
doi: 10.1142/S0218301315500408
2015GU16 Phys.Rev. C 92, 014615 (2015) C.L.Guo, G.L.Zhang, S.P.Hu, J.C.Yang, H.Q.Zhang, P.R.S.Gomes, J.Lubian, X.G.Wu, J.Zhong, C.Y.He, Y.Zheng, C.B.Li, G.S.Li, W.W.Qu, F.Wang, L.Zheng, L.Yu, Q.M.Chen, P.W.Luo, H.W.Li, Y.H.Wu, W.K.Zhou, B.J.Zhu, H.B.Sun Coupling effects on the fusion of 6Li + 154Sm at energies slightly above the Coulomb barrier NUCLEAR REACTIONS 154Sm(6Li, X)154Eu/156Gd/156Tb/157Tb, E=26-36 MeV; measured Eγ, Iγ from different evaporation residues formed via complete and incomplete fusion, complete and incomplete fusion σ(E), σ(E) for 3n+4n channels using on-line γ method at HI-13 Tandem Accelerator of CIAE-Beijing; deduced complete fusion suppression factor as a function of energy. Comparison with theoretical estimates using PACE2.
doi: 10.1103/PhysRevC.92.014615
2015HU03 Phys.Rev. C 91, 044619 (2015) S.P.Hu, G.L.Zhang, J.C.Yang, H.Q.Zhang, P.R.S.Gomes, J.Lubian, X.G.Wu, J.Zhong, C.Y.He, Y.Zheng, C.B.Li, G.S.Li, W.W.Qu, F.Wang, L.Zheng, L.Yu, Q.M.Chen, P.W.Luo, H.W.Li, Y.H.Wu, W.K.Zhou, B.J.Zhu, H.B.Sun Small suppression of the complete fusion of the 6Li+96Zr system at near-barrier energies NUCLEAR REACTIONS 96Zr(6Li, 2n), (6Li, 3n), (6Li, 4n), E=16-28 MeV; 96Zr(6Li, X)96Nb/98Mo/99Mo/100Mo, E=16-28 MeV; measured Eγ, Iγ, σ(E) for evaporation residues of 98,99,100Tc, complete, incomplete, and total fusion σ(E) for 96Nb and Mo isotopes using γ-activation method at Tandem Accelerator facility of CIAE-Beijing. Comparison with theoretical calculations using PACE2 code.
doi: 10.1103/PhysRevC.91.044619
2015LI23 Chin.Phys.C 39, 074101 (2015) X.-X.Liu, G.-L.Zhang, H.-Q.Zhang Study of fusion Q-value rule in sub-barrier fusion of heavy ions NUCLEAR REACTIONS Zr, Sn(Ca, X), Sm, Ni, Ge(O, X), Ni(Ni, X), Zr, Ni, Mg(S, X), Mg, Ni, Si(Si, X), E not given; analyzed available data; deduced fusion σ, Q-value.
doi: 10.1088/1674-1137/39/7/074101
2015QU02 Phys.Lett. B 751, 1 (2015) W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto Effects of repulsive three-body force in 12C + 12C scattering at 100A MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=100 MeV/nucleon; measured reaction products; deduced σ(θ). Three double-folding models with complex G-matrix interactions, the CEG07b, MPa, and ESC model calculations.
doi: 10.1016/j.physletb.2015.10.008
2015YA18 Eur.Phys.J. A 51, 122 (2015) Y.J.Yao, G.L.Zhang, W.W.Qu, J.Q.Qian Comparative studies for different proximity potentials applied to α decay RADIOACTIVITY 106,110Te, 110,112Xe, 144Nd, 146,148Sm, 148,152Gd, 152,154Dy, 152,154Er, 154,156Yb, 156,162Hf, 160,180W, 168,174Os, 176,188Pt, 178,188Hg, 178,190Pb, 188,212Po, 196,208Rn, 202,214Ra, 210,226Th, 218,230U, 228,242Pu, 238,248Cm, 240,252Cf, 246,256Fm, 252,256No, 254,258Rf, 264,270Hs, 286,288Fl, 292Lv, 294Og(α); calculated T1/2 using large set of different proximity potentials. Compared to data.
doi: 10.1140/epja/i2015-15122-0
2014GU28 Eur.Phys.J. A 50, 187 (2014) Analysis of proton radioactivity of nuclei by using proximity potential with a new universal function RADIOACTIVITY 105Sb, 109I, 112,113Cs, 145,146,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,166,167Ir, 171Au, 177Tl, 185Bi(p); calculated T1/2. Compared with other calculations and data.
doi: 10.1140/epja/i2014-14187-5
2014QU03 Phys.Rev. C 90, 064603 (2014) W.W.Qu, G.L.Zhang, H.Q.Zhang, R.Wolski Comparative studies of Coulomb barrier heights for nuclear models applied to sub-barrier fusion NUCLEAR REACTIONS 90,96Zr, 110Pd(32S, X), (36S, X), E not given; 90,96Zr, 124,132Sn(40Ca, X), (48Ca, X), E not given; 58,60,62,64Ni, 144,148,154Sm, (16O, X), (48Ca, X), E not given; 58,60,64Ni, 74,76Ge, 118Sn(18O, X), E not given; 58,64Ni, 124,132Sn(58Ni, X), E not given; 64Ni, 118,124,132Sn(64Ni, X), E not given; calculated reduced fusion σ as function of reduced energy parameter, and Coulomb barrier heights using Bass model, proximity potential models Prox00, Prox77 and Prox88, and double folding model (DFM) model.
doi: 10.1103/PhysRevC.90.064603
2014YA05 Chin.Phys.C 38, 034101 (2014) J.-C.Yang, G.-L.Zhang, D.-Y.Pang Systematic analysis of fusion barrier heights and positions for proton projectiles using the single folding model NUCLEAR REACTIONS 51V, 59Co, 63,65Cu, 92,94Zr, 93Nb, 95,98Mo, 103Rh, 110Pd, 107Ag, 109Mo, 111,116Cd, 115In, 117,118,119,120,122,124Sn, 130Te(p, X), E not given; analyzed available data; parametrized fusion barrier height.
doi: 10.1088/1674-1137/38/3/034101
2014YU01 Chin.Phys.C 38, 024001 (2014) L.Yu, G.-L.Zhang, I.Tanihata, X.-Y.Le Simulation of effects of incident beam condition in p-p elastic scattering
doi: 10.1088/1674-1137/38/2/024001
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
2013GU01 Nucl.Phys. A897, 54 (2013) Study of the universal function of nuclear proximity potential from density-dependent nucleon-nucleon interaction NUCLEAR REACTIONS 40Ca(16O, X), (40Ca, X), 48Ca(48Ca, X), 89Y(32S, X), (34S, X), 90,96Zr(36S, X), (40Ca, X), 92Zr(12C, X), (16O, X), (28Si, X), (35Cl, X), 124Sn(40Ca, X), 144Sm(16O, X), (17O, X), (28Si, X), 148Sm(16O, X), 197Au(19F, X), 204Pb(12C, X), 208Pb(9Be, X), (16O, X), (19F, X), (28Si, X), (64Ni, X), (70Zn, X), (86Kr, X), E not given; calculated proximity interaction barrier using double-folding model with density dependent NN interaction. Compared with other calculations and data.
doi: 10.1016/j.nuclphysa.2012.10.003
2013YA01 Phys.Rev. C 87, 014603 (2013) X.P.Yang, G.L.Zhang, H.Q.Zhang Systematic study of reaction functions of weakly bound nuclei NUCLEAR REACTIONS 12C(6He, X), (6Li, X), (7Li, X), (9Be, X), (16O, X), (17F, X), 27Al(6He, X), (6Li, X), (7Li, X), (7Be, X), (9Be, X), (12C, X), (14N, X), 58Ni(6He, X), (17F, X), (6Li, X), (7Be, X), (16O, X), (17F, X), 59Co(7Li, X), 64Zn(6He, X), (9Be, X), (16O, X), 64Ni(16O, X), 65Cu(6He, X), 197Au(6He, X), 208Pb(6He, X), (6Li, X), (7Li, X)(19F, X), (9Be, X), (17F, X), 209Bi(6He, X), (9Be, X), (11B, X), (16O, X), E not given; analyzed experimental elastic scattering data; deduced reaction cross sections, total reaction function. Calculated barrier parameters using Sao Paulo potential. Comparison with universal reaction function. Discusses breakup effects.
doi: 10.1103/PhysRevC.87.014603
2013ZH03 Eur.Phys.J. A 49, 10 (2013) Study of the universal function of nuclear proximity potential between α and nuclei from density-dependent nucleon-nucleon interaction NUCLEAR STRUCTURE Z=53-92; calculated α-nucleus proximity potential, α-decay Q-value, T1/2. Half life compared with double-folding model.
doi: 10.1140/epja/i2013-13010-3
2013ZH35 Nucl.Phys. A915, 70 (2013) L.Zheng, G.L.Zhang, J.C.Yang, W.W.Qu Calculation of half-lives of cluster decay by using proximity potential with a new universal function RADIOACTIVITY Z=56-102(8Be), (12C), (14C), (15N), (20O), (22O), (23F), (22Ne), (24Ne), (25Ne), (26Ne), (28Mg), (29Mg), (30Mg), (32Si), (34Si), (36S), (42S), (46Ar), (46Ca), (48Ca), (50Ca), (51Ti), (53Ti), (54Ti); calculated T1/2 using proximity potential with new universal function. Compared to data and other calculations.
doi: 10.1016/j.nuclphysa.2013.06.012
2012GU04 Chin.Phys.C 36, 205 (2012) C.-L.Guo, G.-L.Zhang, I.Tanihata, X.-Y.Le Simulation of 12C+12C elastic scattering at high energy by using the Monte Carlo method NUCLEAR REACTIONS 12C(12C, X), E=200-400 MeV/nucleon; calculated the relation between scattering angles and kinetic energy. Monte Carlo method.
doi: 10.1088/1674-1137/36/3/003
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
2011QU03 Nucl.Phys. A868-869, 1 (2011) The parametrization of Coulomb barrier heights and positions using the double folding model
doi: 10.1016/j.nuclphysa.2011.08.002
2010ZH51 Nucl.Phys. A848, 292 (2010) The preformation of cluster radioactivity for heavy nuclei RADIOACTIVITY 222,224,226Ra, 226Th(14C); 226Th(18O); 228Th(20O); 230U(22Ne); 230Th, 230,232,234,236U(24Ne); 234,236U(26Ne); 232,234U, 236,238Pu(28Mg); 236U, 238Pu(30Mg); 238Pu(32Si); analyzed cluster decay Q, T1/2 and related properties using preformed cluster model.
doi: 10.1016/j.nuclphysa.2010.09.017
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
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
2009ZH03 Chinese Physics B 18, 136 (2009) Nucleon-nucleon interactions in the double folding model for fusion reactions NUCLEAR REACTIONS 208Pb(16O, X), E(cm) < 110 MeV/nucleon; calculated fusion cross sections and barrier distributions.
doi: 10.1088/1674-1056/18/1/021
2009ZH09 Nucl.Phys. A823, 16 (2009) Determination of α preformation for heavy nuclei RADIOACTIVITY Z=84, 86, 88, 96, 98, 100, 102, 104, 106, 108, 110, 112, 114, 116, 118(α); analyzed T1/2, Q-values; calculated α penetration probability and preformation factors using a double folding model.
doi: 10.1016/j.nuclphysa.2009.03.005
2009ZH39 Phys.Rev. C 80, 064325 (2009) Calculation of α preformation for nuclei near N=162 and N=184 RADIOACTIVITY 242,243,244,245,246,247,248,249,250,251,252,253,254Cf, 260,266Sg, 264,266Hs, 270Ds, 284Cn, 286,288Fl, 290,292Lv, 294Og(α); Z=104-120, N=154-188(α); calculated Qα, penetration probabilities, and preformation factors for even-even nuclei using WKB approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.064325
2009ZH43 Chin.Phys.C 33, 354 (2009) Calculation of α decay half-lives for superheavy elements using the double folding model NUCLEAR STRUCTURE 270,271,272,273,274Hs, 271,272,273,274,275Mt, 274,275,276,277,278,279,280Ds, 275,276,277,278,279Rg, 279,280,281,282,283Nh, 287,288,289,290,291,292,293Ts; calculated α-decay T1/2; deduce predictions for superheavy elements. Comparison with theoretical models and experimental data.
doi: 10.1088/1674-1137/33/5/007
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
2008ZH09 Chin.Phys.Lett. 24, 1247 (2008) Coulomb Potentials between Spherical and Deformed Nuclei
doi: 10.1088/0256-307X/25/4/023
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
2007LO05 Phys.Rev. C 75, 057302 (2007) J.L.Lou, Z.H.Li, Y.L.Ye, H.Hua, D.X.Jiang, L.H.Lv, Z.Kong, Y.M.Zhang, F.R.Xu, T.Zheng, X.Q.Li, Y.C.Ge, C.Wu, G.L.Zhang, Z.Q.Chen, C.Li, D.Y.Pang, H.S.Xu, Z.Y.Sun, L.M.Duan, Z.G.Hu, R.J.Hu, H.G.Xu, R.S.Mao, Y.Wang, X.H.Yuan, H.Gao, L.J.Wu, H.R.Qi, T.H.Huang, F.Fu, F.Jia, Q.Gao, X.L.Ding, J.L.Han, X.Y.Zhang Observation of a new transition in the beta-delayed neutron decay of 18N RADIOACTIVITY 18N(β-); measured β-delayed neutron spectra. 18O; deduced level energies, J, π. Deduced B(GT), compared to shell model calculations.
doi: 10.1103/PhysRevC.75.057302
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
2006HU19 High Energy Phys. and Nucl.Phys. (China), Supplement 2, 30, 157 (2006) H.Hua, S.Wamg, J.Meng, Z.-H.Li, S.-Q.Zhang, F.-R.Xu, H.-L.Liu, S.-G.Zhou, Y.-L.Ye, D.-X.Jiang, T.Zheng, L.-H.Mu, X.-G.Wu, G.-S.Li, Q.-J.Wang, Z.-Q.Chen, C.-E.Wu, G.-L.Zhang, D.-Y.Pang, J.Wang, J.-L.Lou, B.Guo, G.Jin, S.-X.Wen, C.-Y.He, X.-Z.Chui, Y.Liu High-Spin States in 152Gd
2005LI60 Phys.Rev. C 72, 064327 (2005) Z.H.Li, Y.L.Ye, H.Hua, D.X.Jiang, Y.M.Zhang, F.R.Xu, Q.Y.Hu, G.L.Zhang, Z.Q.Chen, T.Zheng, C.E.Wu, J.L.Lou, X.Q.Li, D.Y.Pang, S.Wang, C.Li, H.S.Xu, Z.Y.Sun, L.M.Duan, Z.G.Hu, R.J.Hu, H.G.Xu, R.S.Mao, Y.Wang, X.H.Yuan, H.Gao, L.J.Wu, H.R.Qi, T.H.Huang, F.Fu, F.Jia, Q.Gao, X.L.Ding, J.L.Han, X.Y.Zhang β-decay of the neutron-rich nucleus 18N RADIOACTIVITY 18N(β-), (β-n) [from Be(22Ne, X)]; measured T1/2, β-delayed neutron spectra, Eγ, Iγ; deduced branching ratios, Gamow-Teller strengths. 18O deduced levels, J, π. Comparison with shell model calculations.
doi: 10.1103/PhysRevC.72.064327
2005WA14 Chin.Phys.Lett. 22, 1370 (2005) J.Wang, Y.-L.Ye, D.-X.Jiang, G.-L.Zhang, D.-Y.Pang, Z.-H.Li, T.Zheng, X.-Q.Li, Q.-J.Wang, Q.-Y.Hu, C.-E.Wu, A.Ozawa, Y.Yamaguchi, R.Kanungo, D.Fang, I.Tanihata Measurement of the Breakup Cross Sections in 6He + 9Be Reaction at 25 MeV/Nucleon NUCLEAR REACTIONS 9Be(6He, αX), E=25 MeV/nucleon; measured Eα, σ(θ). Comparison with Serber model predictions.
doi: 10.1088/0256-307X/22/6/020
2005WA23 Phys.Rev. C 72, 024317 (2005), Erratum Phys.Rev. C 105, 029903 (2022) S.Wang, H.Hua, J.Meng, Z.H.Li, S.Q.Zhang, F.R.Xu, H.L.Liu, Y.L.Ye, D.X.Jiang, T.Zheng, Q.J.Wang, Z.Q.Chen, C.E.Wu, G.L.Zhang, D.Y.Pang, J.Wang, J.L.Lou, B.Guo, G.Jin, S.G.Zhou, L.H.Zhu, X.G.Wu, G.S.Li, S.X.Wen, C.Y.He, X.Z.Cui, Y.Liu High-spin states in 152Gd NUCLEAR REACTIONS 148Nd(9Be, 5n), E=42, 45, 48, 52, 55 MeV; measured Eγ, Iγ; deduced excitation function. 148Nd(9Be, 5n), E=54 MeV; measured Eγ, Iγ, γγ-coin. 152Gd deduced high-spin levels, J, π, configuration, quadrupole deformation. Total Routhian surface calculations.
doi: 10.1103/PhysRevC.72.024317
2005YE01 Phys.Rev. C 71, 014604 (2005) Y.L.Ye, D.Y.Pang, D.X.Jiang, T.Zheng, Q.J.Wang, Z.H.Li, X.Q.Li, Y.C.Ge, C.Wu, G.L.Zhang, Q.Y.Hu, J.Wang, Z.Q.Chen, A.Ozawa, Y.Yamaguchi, R.Kanungo, I.Tanihata Quasielastic scattering of 6He on 9Be at 25 MeV/nucleon NUCLEAR REACTIONS 9Be(6He, 6He), E=25 MeV/nucleon; measured quasielastic σ(θ); deduced optical model parameters, inelastic channels contribution.
doi: 10.1103/PhysRevC.71.014604
2005YE05 J.Phys.(London) G31, S1647 (2005) Y.L.Ye, D.Y.Pang, G.L.Zhang, D.X.Jiang, T.Zheng, Z.H.Li, X.Q.Li, Q.J.Wang, Y.C.Ge, C.E.Wu, J.Wang, Z.Q.Chen, Y.Ai, A.Ozawa, Y.Yamaguchi, D.Q.Fang, I.Tanihata Study of the halo nucleus 6He through the direct nuclear reactions NUCLEAR REACTIONS 9Be(6He, 6He), (6He, 5He), (6He, α), (6He, αX), (6He, tX), E=25 MeV/nucleon; measured quasielastic, breakup, and transfer σ(θ). 6He deduced two-triton configuration.
doi: 10.1088/0954-3899/31/10/048
2004PA35 Chin.Phys.Lett. 21, 2151 (2004) D.-Y.Pang, Y.-L.Ye, D.-X.Jiang, T.Zheng, Q-J.Wang, Z.-H.Li, X.-Q.Li, Y.-C.Ge, C.-E.Wu, G.-L.Zhang, Q.-Y.Hu, J.Wang, A.Ozawa, Y.Yamaguchi, R.Kanungo, D.Fang, I.Tanihata Quasielastic Scattering of the Halo Nucleus 6He at 25 MeV/u from a 9Be Target NUCLEAR REACTIONS 9Be(6He, 6He), E=25 MeV/nucleon; measured σ(θ); deduced optical potential parameters. Double folding model.
doi: 10.1088/0256-307X/21/11/021
1997VE04 Europhys.Lett. 37, 25 (1997) J.Verheyden, S.Bukshpan, J.Dekoster, A.Vantomme, W.Deweerd, K.Milants, T.Barancira, G.L.Zhang, H.Pattyn Determination of Size and Interface Hyperfine Field of Co Nanosized Precipitates in Ag by Mossbauer Spectroscopy NUCLEAR REACTIONS 57,59Co(γ, γ), E not given; measured Mossbauer spectra; deduced hyperfine fields of Co nanoprecipitates in Ag.
doi: 10.1209/epl/i1997-00112-5
1990NI08 Hyperfine Interactions 59, 271 (1990) L.Niesen, G.L.Zhang, H.Andreasen, G.Weyer Hyperfine Interaction of Eu Impurities Implanted in Nickel NUCLEAR REACTIONS 151Eu(γ, γ), E=21.54 keV; measured Mossbauer spectra; deduced hyperfine, exchange fields temperature dependence. 151Gd source.
doi: 10.1007/BF02401227
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