NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.Q.Zhang Found 133 matches. Showing 1 to 100. [Next]2024ZH15 Nucl.Instrum.Methods Phys.Res. A1059, 168983 (2024) H.Q.Zhang, P.Kuang, X.T.Yu, P.Zhang, F.Y.Liu, R.S.Yu, X.Z.Cao, B.Y.Wang Development of novel positron lifetime measurement system for potential liquid material inspection
doi: 10.1016/j.nima.2023.168983
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
2023YA02 Phys.Rev. C 107, 014325 (2023) M.J.Yang, H.Sagawa, C.L.Bai, H.Q.Zhang Effects of two-particle--two-hole configurations and tensor force on β decay of magic nuclei RADIOACTIVITY 34Si, 68,78Ni, 132Sn(β-); calculated T1/2, Gamow-Teller strength distribution with respect to daughter nucleus. Self-consistent Hartree-Fock plus subtracted second random-phase approximation (HF+SSRPA) model with Skyrme EDFs (SGII, SAMi, SAMi-T).Comparison to experimental data.
doi: 10.1103/PhysRevC.107.014325
2023ZH08 Phys.Rev. C 107, 024305 (2023) J.Zhang, X.-T.He, Y.-C.Li, H.-Q.Zhang Parity-doublet bands in the odd-A isotones 237U and 239Pu investigated by a particle-number-conserving method based on the cranked shell model NUCLEAR STRUCTURE 237U, 239Pu; calculated cranked Nilsson levels near the Fermi surface for neutrons and protons, kinematic moments of inertia and alignments of the parity-doublet rotational bands, neutron and proton orbitals occupation probabilities, contributions of protons to the angular momentum alignments, contributions of neutrons to the moments of inertia. Particle-number-con serving method in the framework of the cranked shell model (PNC-CSM) calculations. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.024305
2022BA38 Chin.Phys.C 46, 114104 (2022) C.L.Bai, D.L.Fang, H.Q.Zhang, C.L.Bai, D.L.Fang, H.Q.Zhang Roles of tensor and isoscalar pairing interactions in β-Decay calculations for possible r-process waiting point nuclei with N ∼ 82 and 126 RADIOACTIVITY 120,122,124,126,128,130,132Cd(β-); calculated T1/2 with the self-consistent Hartree-Fock-Bogoliubov (HFB) theory with the proton-neutron quasi-particle random phase approximation (pnQRPA) based on the Skyrme force. Comparison with available data.
doi: 10.1088/1674-1137/ac80ee
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
2022YA20 Phys.Rev. C 106, 014319 (2022) M.J.Yang, C.L.Bai, H.Sagawa, H.Q.Zhang Gamow-Teller transitions in magic nuclei calculated by the charge-exchange subtracted second random-phase approximation NUCLEAR STRUCTURE 48Ca, 90Zr, 132Sn, 208Pb; calculated Gamow-Teller (GT) strength distributions as function of excitation energy and peak height; evaluated quenching factors of the Ikeda sum rule due to couplings to two-particle two-hole (2p-2h) configurations, effects of tensor interactions on the excitation energies and the quenching factors of GT strength distributions. Self-consistent Hartree-Fock (HF) plus charge-exchange subtracted second random-phase approximation (SSRPA) calculations with several different Skyrme energy density functions (EDFs). Comparison with experimental data.
doi: 10.1103/PhysRevC.106.014319
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
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
2021WU12 Phys.Rev. C 104, 054303 (2021) D.Wu, C.L.Bai, H.Sagawa, S.Nishimura, H.Q.Zhang β-delayed one-neutron emission probabilities within a neural network model RADIOACTIVITY Z=2-57(β-n); calculated β--delayed one-neutron emission probabilities P1n using machine learning (ML) technique and feed-forward neural network (FNN) with root mean squared Prop (RMSProp) method; analyzed correlations between P1n, half-lives, Q-values, neutron shell effects, distance from the first β--delayed neutron emitter, and competitions between β--delayed one- and two- neutron emissions P1n and P2n. 109,110,111,112,113,114,115,116Tc, 116,117,118,119,120,121Ru, 118,119,120,121,122,123,124Rh, 121,122,123,124,125,126,127,128Pd, 124,125,126,127,128,129Ag, 127,128,129,130Cd(β-n); 79Cu, 80Zn, 81Ga, 128Pd, 129Ag, 130Ag(β-n); calculated β--delayed one-neutron emission probabilities P1n using ML-FNN techniques, and compared with experimental and evaluated data in literature, and with theoretical calculations using FRDM12+(Q)RPA+HF and RHB+RQRPA approaches. Relevance to r-process nuclei in nucleosynthesis, and waiting-point nuclei at N=50 and N=82.
doi: 10.1103/PhysRevC.104.054303
2021YA14 Phys.Rev. C 103, 054308 (2021) M.J.Yang, C.L.Bai, H.Sagawa, H.Q.Zhang Effects of the Skyrme tensor force on 0+, 2+, and 3- states in 16O and 40C nuclei within the second random-phase approximation NUCLEAR STRUCTURE 16O, 40Ca; calculated isoscalar and isovector strength distributions and energy moments of the monopole (0+), quadrupole (2+) and octupole (3-) transitions B(E0), B(E2) and B(E3), major 1p-1h and 2p-2h configurations; deduced major impact of tensor force in SGII+Te1 on the coupling between 1p-1h and 2p-2h model spaces. Subtracted second random-phase approximation (SSRPA) method with Skyrme energy density functional. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.054308
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
2020WU09 Phys.Rev. C 102, 054323 (2020) D.Wu, C.L.Bai, H.Sagawa, H.Q.Zhang Calculation of nuclear charge radii with a trained feed-forward neural network NUCLEAR STRUCTURE 40,42,44,46,48,50,52Ca, 108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 138,140,142,144,146,148,150,152,154Sm, 182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212Pb; calculated nuclear charge radii, correlation between the symmetry energy and charge radii of Ca isotopes, and confirmed this correlation by Skyrme Hartree-Fock-Bogoliubov calculation. A multilayer feed-forward neural network model (ML-FNN).
doi: 10.1103/PhysRevC.102.054323
2019CA13 Phys.Rev. C 99, 054615 (2019) A.Gomez Camacho, A.Diaz-Torres, H.Q.Zhang Comparative study of the effect of resonances of the weakly bound nuclei 6, 7Li on total fusion with light to heavy mass targets NUCLEAR REACTIONS 27Al(7Li, X), E(cm)=8-24 MeV; 59Co(7Li, X), E(cm)=10-24 MeV; 144Sm(7Li, X), E(cm)=20-38 MeV; 209Bi(7Li, X), E(cm)=25-50 MeV; 28Si(6Li, X), E(cm)/VB=1-3.6 MeV; 59Co(6Li, X), E(cm)/VB=0.8-2.0 MeV; 96Zr(6Li, X), E(cm)/VB=0.8-1.7 MeV; 198Pt(6Li, X), E(cm)/VB=0.8-1.4 MeV; 209Bi(6Li, X), E(cm)/VB=0.9-1.2 MeV; calculated total fusion σ(E), effects of resonant and non-resonant breakup states in projectile nuclei on total fusion σ. Continuum-discretized coupled-channel (CDCC) calculations. Comparison with available experimental data.
doi: 10.1103/PhysRevC.99.054615
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
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
2018GO08 Phys.Rev. C 97, 054610 (2018) A.Gomez Camacho, B.Wang, H.Q.Zhang Systematic continuum-discretized coupled-channels calculations of total fusion for 6Li with targets 28Si, 59Co, 96Zr, 198Pt, and 209Bi: Effect of resonance states NUCLEAR REACTIONS 28Si, 59Co, 96Zr, 198Pt, 209Bi(6Li, 6Li), (6Li, dα), E(cm)=8-48 MeV; calculated total fusion σ(E) and fusion widths for elastic channel, resonance and non-resonance subspaces, net polarization potentials using continuum discretized coupled-channel calculations (CDCC); deduced effect of resonant break-up states on fusion σ. NUCLEAR STRUCTURE 6Li; calculated centroid energies and widths of 3+, 2+ and 1+ resonances, and compared with experimental values.
doi: 10.1103/PhysRevC.97.054610
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
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
2017GO20 Chin.Phys.C 41, 124103 (2017) A.Gomez Camacho, J.Lubian, H.Q.Zhang, S.-G.Zhou CDCC calculations of fusion of 6Li with targets 144Sm and 154Sm: effect of resonance states NUCLEAR REACTIONS 144,154Sm(6Li, X), E(cm)<40 MeV; calculated total fusion σ. Comparison with available data.
doi: 10.1088/1674-1137/41/12/124103
2017SA28 Phys.Rev. C 95, 054619 (2017) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Comparative analysis of the fusion reactions 48Ti + 58Fe and 58Ni + 54Fe NUCLEAR REACTIONS 48Ti(58Fe, X), E(cm)=65-90 MeV; 58Ni(54Fe, X), E(cm)=85-110 MeV; analyzed experimental reduced fusion excitation functions, capture probabilities, fusion (capture) σ(E), fusion barrier distributions by universal fusion function; deduced astrophysical S factor, enhancement of sub-barrier fusion cross section. Quantum diffusion approach and the universal fusion function representation.
doi: 10.1103/PhysRevC.95.054619
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
2017WU11 Eur.Phys.J. A 53, 183 (2017) F.Wu, C.L.Bai, J.M.Yao, H.Q.Zhang, X.Z.Zhang Existence problem of proton semi-bubble structure in the 21+ state of 34Si NUCLEAR STRUCTURE 34Si, 36S; calculated first proton orbitals, proton sp levels, J, B(E2), proton density distribution vs radius using HF (Hartree-Fock) plus RPA (Random Phase Approximation) based on Skyrme-type interaction; deduced possibility of lower proton density ("bubble") in the center of nucleus.
doi: 10.1140/epja/i2017-12375-5
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
2016CH30 Phys.Rev. C 94, 021301 (2016) X.C.Chen, J.Zhao, C.Xu, H.Hua, T.M.Shneidman, S.G.Zhou, X.G.Wu, X.Q.Li, S.Q.Zhang, Z.H.Li, W.Y.Liang, J.Meng, F.R.Xu, B.Qi, Y.L.Ye, D.X.Jiang, Y.Y.Cheng, C.He, J.J.Sun, R.Han, C.Y.Niu, C.G.Li, P.J.Li, C.G.Wang, H.Y.Wu, Z.H.Li, H.Zhou, S.P.Hu, H.Q.Zhang, G.S.Li, C.Y.He, Y.Zheng, C.B.Li, H.W.Li, Y.H.Wu, P.W.Luo, J.Zhong Evolution of octupole correlations in 123Ba NUCLEAR REACTIONS 108Cd(19F, 3np), E=90 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) at HI-13 tandem facility of the CIAE-Beijing. 123Ba; deduced high-spin levels, J, π, bands, multipolarity, B(E1)/B(E2) ratio. 123,125,145Ba; systematics of B(E1)/B(E2) ratios, theoretical and experimental energy displacements between the opposite-parity bands, octupole correlations, potential-energy surface contours in (β2, β3) plane. Comparison with predictions of multidimensionally-constrained relativistic mean-field (MDC-RMF) model, and cluster model based on dinuclear system.
doi: 10.1103/PhysRevC.94.021301
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
2016MA06 Phys.Rev. C 93, 014317 (2016) H.-L.Ma, B.-G.Dong, Y.-L.Yan, H.-Q.Zhang, D.-Q.Yuan, S.-Y.Zhu, X.-Z.Zhang Pygmy and giant dipole resonances in the nitrogen isotopes NUCLEAR STRUCTURE 17,18,19,20N; calculated S(p), S(n), mass radii, B(E1), transition densities and transition matrix elements, and energy-weighted sum rule (EWSR) for pygmy dipole resonances (PDR), GDR energies and splitting of isospin doublets, photoabsorption cross sections. Configuration-interaction shell model with the WBP10 effective interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.014317
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
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
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
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
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
2015SA02 Phys.Rev. C 91, 014613 (2015) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Examination of the different roles of neutron transfer in the sub-barrier fusion reactions 32S + 94, 96Zr and 40Ca + 94, 96Zr NUCLEAR REACTIONS 90,94,96Zr(40Ca, X), E(cm)=84-108 MeV; 90,96Zr(48Ca, X), E(cm)=88-109 MeV; 90,94,96Zr(32S, X), E(cm)=70-86 MeV; 90,96Zr(36S, X), E(cm)=71-186 MeV; calculated capture cross sections and compared with experimental data, analyzed experimental reduced fusion excitation functions; deduced s-wave capture probabilities as function of incident energy. Quantum diffusion approach and the universal fusion function representation.
doi: 10.1103/PhysRevC.91.014613
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
2015SU12 Phys.Rev. C 92, 054302 (2015) J.J.Sun, C.Xu, X.Q.Li, H.Hua, S.Q.Zhang, F.R.Xu, W.Y.Liang, C.F.Jiao, J.Meng, X.G.Wu, S.P.Hu, H.Q.Zhang, Z.H.Li, Y.L.Ye, D.X.Jiang, Y.Y.Cheng, C.He, R.Han, C.Y.Niu, C.G.Li, C.G.Wang, Z.H.Li, G.S.Li, C.Y.He, Y.Zheng, C.B.Li, H.W.Li, J.L.Wang, J.J.Liu, Y.H.Wu, P.W.Luo, S.H.Yao, B.B.Yu, X.P.Cao, H.B.Sun Band crossing and shape evolution in 73Ge NUCLEAR REACTIONS 70Zn(7Li, 3np), E=30, 35 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) at HI-13 tandem facility of CIAE-Beijing. 73Ge; deduced high-spin levels, J, π, multipolarity, γ-branching ratios, bands, kinematic moments of inertia, configurations, signature splitting. Comparison with cranked Woods-Saxon-Strutinsky calculations using total-Routhian-surface (TRS) methods, and with band features in 75Se and 77Kr.
doi: 10.1103/PhysRevC.92.054302
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
2014BA55 Phys.Rev. C 90, 054335 (2014) C.L.Bai, H.Sagawa, G.Colo, Y.Fujita, H.Q.Zhang, X.Z.Zhang, F.R.Xu Low-energy collective Gamow-Teller states and isoscalar pairing interaction NUCLEAR STRUCTURE 42Ca, 46Ti, 50Cr, 54Fe, 58Ni; calculate neutron pairing gaps, Gamow-Teller (GT) strength distributions and sum rule values for IAR states, energy differences between the lowest GT and IAR states in N=Z+2 nuclei. HFB+QRPA calculations with the Skyrme forces SGII, SGII+Te3, and SAMi. Comparison with experimental values.
doi: 10.1103/PhysRevC.90.054335
2014HU09 Phys.Lett. B 732, 59 (2014) S.-P.Hu, H.-L.Ma, X.-P.Cao, X.-G.Wu, H.-Q.Zhang, H.Hua, J.-J.Sun, H.-B.Sun, C.-Y.He, Y.Zheng, G.-S.Li, C.-B.Li, S.-H.Yao, B.-B.Yu, J.-L.Wang, H.-W.Li, Y.-H.Wu, J.-J.Liu, P.-W.Luo, C.Xu, Y.-Y.Cheng Multiple triaxial bands and abnormal signature inversion in 7433As NUCLEAR REACTIONS 70Zn(7Li, 3n), E=30 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced energies, relative intensities, positive- and negative-parity bands. Comparison with Cranked Nilsson-Strutinsky (CNS) model calculations.
doi: 10.1016/j.physletb.2014.03.014
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
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
2014SA24 Eur.Phys.J. A 50, 71 (2014) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Derivation of breakup probabilities from experimental elastic backscattering data NUCLEAR STRUCTURE 6,8He, 8Li, 7,9,11Be, 8,9B, 15C, 17F; calculated breakup probability near and above Coulomb barrier.
doi: 10.1140/epja/i2014-14071-4
2014SU09 Phys.Lett. B 734, 308 (2014) J.J.Sun, Z.Shi, X.Q.Li, H.Hua, C.Xu, Q.B.Chen, S.Q.Zhang, C.Y.Song, J.Meng, X.G.Wu, S.P.Hu, H.Q.Zhang, W.Y.Liang, F.R.Xu, Z.H.Li, G.S.Li, C.Y.He, Y.Zheng, Y.L.Ye, D.X.Jiang, Y.Y.Cheng, C.He, R.Han, Z.H.Li, C.B.Li, H.W.Li, J.L.Wang, J.J.Liu, Y.H.Wu, P.W.Luo, S.H.Yao, B.B.Yu, X.P.Cao, H.B.Sun Spectroscopy of 74Ge: From soft to rigid triaxiality NUCLEAR REACTIONS 70Zn(7Li, 2np), E=30, 35 MeV; measured reaction products, Eγ, Iγ; deduced level energies, J, π, yrast bands, energy staggering, triaxiality. Comparison with five-dimensional collective Hamiltonian model calculations. NUCLEAR STRUCTURE 72,74,76,78Ge; calculated energy levels, J, π, potential energy surfaces. Five-dimensional collective Hamiltonian (5DCH) model.
doi: 10.1016/j.physletb.2014.05.069
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
2013MA64 Phys.Rev. C 88, 034322 (2013) H.L.Ma, S.-H.Yao, B.-G.Dong, X.-G.Wu, H.-Q.Zhang, X.-Z.Zhang Risk of misinterpreting nearly degenerate doublet bands as chiral partners in odd-even 103, 105, 107Ag and odd-odd 106Ag NUCLEAR STRUCTURE 103,105,106,107Ag; calculated single particle Routhians as function of rotational frequencies, energies of nearly degenerate negative-parity doublet bands, deformation trajectories, B(E2); comparison with experimental data suggests consistency with planar cranking model interpretation. Existence of chiral structure of such degenerate bands questioned. Configuration-dependent cranked Nilsson-Strutinsky (CNS) calculations.
doi: 10.1103/PhysRevC.88.034322
2013SA03 Eur.Phys.J. A 49, 19 (2013) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Threshold energy for sub-barrier fusion hindrance phenomenon NUCLEAR REACTIONS 120Sn(16O, X), E(cm)=38-64 MeV; calculated quasielastic barrier, sub-barrier fusion threshold energy, barrier distribution, σ. 208Pb(16O, X), E(cm)=65-87 MeV;208Pb(α, X), E(cm)=17-27 MeV; calculated quasielastic barrier, sub-barrier fusion threshold energy, barrier distribution, σ. Quantum diffusion approach; compared with available data.
doi: 10.1140/epja/i2013-13019-6
2013SA31 Eur.Phys.J. A 49, 54 (2013) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Sub-barrier capture reactions with 16, 18O and 40, 48Ca beams NUCLEAR REACTIONS 50Cr(18O, X), 52Cr(16O, X), E(cm)=14-58 MeV;74Ge(18O, X), 76Ge(16O, X), E(cm)=27-42 MeV;92Mo(16O, X), 92Mo(18O, X), E(cm)=35-59 MeV;112,118,124Sn(18O, X), E(cm)=42-81 MeV;124,132Sn(40Ca, X), (48Ca, X), E(cm)=105-135 MeV; calculated σ. 74Ge(18O, X), 76Ge(16O, X), E(cm)=30-50 MeV;144,154Sm(16O, X), E(cm)≈50-70 MeV; calculated quasielastic σ. Quantum diffusion approach, compared to data.
doi: 10.1140/epja/i2013-13054-3
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
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
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
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
2012MA12 Phys.Rev. C 85, 044307 (2012) H.-L.Ma, B.-G.Dong, Y.-L.Yan, H.-Q.Zhang, X.-Z.Zhang Proton pygmy dipole resonances in 17, 18Ne: Collective versus noncollective excitations NUCLEAR STRUCTURE 17,18Ne; calculated nucleon and matter density distributions, mass and charge radii, E1 response functions from excited states, EWSR, E1 transition densities, contribution to total matrix elements for deexcitation from proton pygmy dipole resonances (PDRs). Interacting shell model with self-consistent Skyrme-Hartree-Fock wave functions. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.044307
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
2012SA09 Phys.Rev. C 85, 024616 (2012); Erratum Phys.Rev. C 85, 069903 (2012) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Role of neutron transfer in capture processes at sub-barrier energies NUCLEAR REACTIONS 124Sn(40Ca, X), E(cm)=106-127 MeV; 90,96Zr(40Ca, X), E(cm)=85-113 MeV; 130Te, 132Sn(58Ni, X), (64Ni, X), E(cm)=140-200 MeV; 208Pb(58Ni, X), (64Ni, X), E(cm)=220-245 MeV; 132Sn(40Ca, X), (48Ca, X), E(cm)=98-144 MeV; 100Mo(60Ni, X), (64Ni, X), E(cm)=118-162 MeV; 150Nd(60Ni, X), (64Ni, X), E(cm)=160-210 MeV; calculated capture cross sections and reduced capture cross sections with and without 2-neutron transfer. Quantum diffusion approach for transfer of neutrons. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.024616
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
2012SA30 Phys.Rev. C 86, 014602 (2012) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Influence of neutron transfer in reactions with weakly and strongly bound nuclei on the sub-barrier capture process NUCLEAR REACTIONS 232Th(12C, X), (13C, X), (14C, X), (15C, X), E(cm)=49-79 MeV; 237Np(12C, X), E(cm)=50-78 MeV; 206Pb(6He, X), 208Pb(α, X), E(cm)=12-26 MeV; 208Pb(12C, X), (13C, X), (14C, X), (15C, X), E(cm)=48-79 MeV; 208Pb(18O, X), E(cm)=66-86 MeV; 126Sn(40Ca, X), (48Ca, X), E(cm)-V(b)=-13-23 MeV; 112,116,120Sn(32S, X), E(cm)=84-113 MeV; 92,94,96,98,100Mo, 100,102,104Ru, 104,106,108,110Pd (32S, X), (36S, X), E(cm)=70-96 MeV; 132Sn(32S, X), (36S, X), E(cm)-V(b)=-11-21 MeV; 112,118,124Sn(18O, X), E(cm)=41-81 MeV; 68Zn(9Li, X), 70Zn(7Li, X), E(cm)=6-22 MeV; 70Zn(9Li, X), E(cm)=8-16 MeV; calculated capture σ. Quantum diffusion approach. Comparison with experimental data. Predictions of capture σ for (13,14,15C)+208Pb, (32,36S)+132Sn, and (40,48)Ca+126Sn reactions. Discussed influence of neutron transfer on capture cross sections.
doi: 10.1103/PhysRevC.86.014602
2012SA40 Phys.Rev. C 86, 034614 (2012) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Astrophysical s factor, logarithmic slope of the excitation function, and barrier distribution NUCLEAR REACTIONS 54Fe, 58,60,64Ni(58Ni, X), E=82-114 MeV; 40Ca(40Ca, X), E=46-67 MeV; 89Y(60Ni, X), E=119-139 MeV; 90,96Zr(48Ca, X), (40Ca, x), (32S, X), E=85-114 MeV; calculated capture σ(E), mean square angular momentum, astrophysical S factor, logarithmic slope of the excitation function, fusion barrier distributions. Quantum diffusion approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.034614
2012SA52 Phys.Rev. C 86, 054610 (2012) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Search for a systematic behavior of the breakup probability in reactions with weakly bound projectiles at energies around the Coulomb barrier NUCLEAR REACTIONS 27Al, 64Zn, 89Y, 124Sn, 144Sm, 208Pb, 209Bi(9Be, X), 64Zn, 144Sm, 198Pt, 208Pb, 209Bi(6Li, X), 27Al, 64Zn, 159Tb, 165Ho, 197Au, 209Bi(7Li, X), 70Zn, 208Pb, 209Bi(9Li, X), 208Pb(11Li, X), 64Zn, 197Au(α, X), 64Zn, 197Au, 209Bi(6He, X), 197Au(8He, X), 159Tb, 209Bi(10B, X), (11BE, X), 208Pb(11Li, X), E(cm)=5-50 MeV; calculated capture cross sections; analyzed breakup probabilities for weakly bound projectiles using experimental complete fusion σ. Quantum diffusion approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.054610
2012SA59 Eur.Phys.J. A 48, 188 (2012) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Quasifission at extreme sub-barrier energies NUCLEAR REACTIONS 92Mo(92Mo, X), E(cm)=178-208 MeV;94Mo(94Mo, X), E(cm)=172-207 MeV;100Ru(100Ru, X), E(cm)=185-218 MeV;104Pd(104Pd, X), E(cm)=201-240 MeV;112Sn(78Kr, X), E(cm)=170-218 MeV; calculated capture σ using quantum diffusion approach.
doi: 10.1140/epja/i2012-12188-0
2012YU08 J.Phys.(London) G39, 105105 (2012) Vorticity of threshold strength in neutron drip-line nuclei
doi: 10.1088/0954-3899/39/10/105105
2012ZH04 Chin.Phys.Lett. 29, 012502 (2012) Z.-Y.Zhang, Z.-G.Gan, L.Ma, M.-H.Huang, T.-H.Huang, X.-L.Wu, G.-B.Jia, G.-S.Li, L.Yu, Z.-Z.Ren, S.-G.Zhou, Y.-H.Zhang, X.-H.Zhou, H.-S.Xu, H.-Q.Zhang, G.-Q.Xiao, W.-L.Zhang Observation of the Superheavy Nuclide 271Ds RADIOACTIVITY 271Ds(α) [from 208Pb(64Ni, n), E=313.3 MeV]; measured decay products, Eα, Iα, α-α-coin.; deduced T1/2, α-decay chain. Comparison with experimental data.
doi: 10.1088/0256-307X/29/1/012502
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
2012ZH36 Chin.Phys.Lett. 29, 092102 (2012) Q.-L.Zhang, D.-Q.Yuan, H.-Q.Zhang, P.Fan, Y.Zuo, Y.-N.Zheng, K.Masuta, M.Fukuda, M.Mihara, T.Minamisono, A.Kitagawa, S.-Y.Zhu The ab initio Calculation of Electric Field Gradient at the Site of P Impurity in α-Al3O2 NUCLEAR MOMENTS 28P; analyzed quadrupole coupling frequency; deduced quadrupole moment. Comparison with nuclear shell model.
doi: 10.1088/0256-307X/29/9/092102
2011BA18 Phys.Rev. C 83, 054316 (2011) C.L.Bai, H.Q.Zhang, H.Sagawa, X.Z.Zhang, G.Colo, F.R.Xu Spin-isospin excitations as quantitative constraints for the tensor force NUCLEAR STRUCTURE 90Zr, 208Pb; calculated Gamow-Teller (GT) and charge-exchange spin-dipole (SD) excitation energies, centroid energies. HF+RPA model with Skyrme interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.054316
2011BA38 Phys.Rev. C 84, 044329 (2011) C.L.Bai, H.Sagawa, G.Colo, H.Q.Zhang, X.Z.Zhang Spin-dipole excitations in 16O and tensor correlations NUCLEAR STRUCTURE 16F, 208Bi; calculated charge-exchange spin-dipole (SD) strength distributions and energies using different interactions. Hartree-Fock (HF) plus self-consistent random-phase approximation (RPA) using Skyrme-type interactions. 16O; investigated effect of tensor force on the charge-exchange SD transition. Role of triplet-even and triplet-odd tensor interactions.
doi: 10.1103/PhysRevC.84.044329
2011SA11 Eur.Phys.J. A 47, 38 (2011) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Sub-barrier capture with quantum diffusion approach: Actinide-based reactions NUCLEAR REACTIONS 232Th(16O, X), E(cm)=63-112 MeV;232Th(19F, X), E(cm)=66-98 MeV;232Th(32S, X), E(cm)=128-174 MeV;238U(α, X), E(cm)=14-42 MeV;238U(16O, X), E(cm)=65-105 MeV;238U(20Ne, X), E(cm)=88-128 MeV;238U(30Si, X), E(cm)=112-152 MeV;238U(32S, X), E(cm)=128-174 MeV;238U(36S, X), E(cm)=134-186 MeV;238U(48Ca, X), E(cm)=168-218 MeV;244Pu(36S, X), E(cm)=142-182 MeV;244Pu(48Ca, X), E(cm)=178-220 MeV;244Pu(50Ti, X), E(cm)=197-232 MeV;246Cm(48Ca, X), E(cm)=182-220 MeV;248Cm(36S, X), E(cm)=142-172 MeV;248Cm(48Ca, X), E(cm)=182-220 MeV; calculated σ. 232Th(16O, X), E(cm)=68-90 MeV;232Th(19F, X), E(cm)=68-98 MeV;232Th(48Ca, X), E(cm)=161-198 MeV;238U(16O, X), E(cm)=70-89 MeV; calculated mean-square angular momentum. 232Th(16O, X), E(cm)=67.5-75.5 MeV;238U(α, X), E(cm)=14.5-26.5 MeV;238U(16O, X), E(cm)=67-92 MeV; calculated S-factor. Diffusion approach to capture σ below Coulomb barrier with deformation taken into account. Comparison with available data.
doi: 10.1140/epja/i2011-11038-y
2011SA65 Phys.Rev. C 84, 064614 (2011) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, W.Scheid, H.Q.Zhang Effects of nuclear deformation and neutron transfer in capture processes, and fusion hindrance at deep sub-barrier energies NUCLEAR REACTIONS 154Sm(48Ca, X), E(cm)=125-150 MeV; 144,154Sm(40Ar, X), E(cm)=105-145 MeV; 144,154Sm(16O, X), E(cm)=50-90 MeV; 74Ge(74Ge, X), E(cm)=105-140 MeV; 90,94Zr(28Si, X), E(cm)=60-95 MeV; 112,116,122Sn(40Ar, X), 144,154Sm(28Si, X), E(cm)=90-125 MeV; 90,96Zr(32S, X), (36S, X), E(cm)=65-95 MeV; 168Er(34S, X), E(cm)=105-140 MeV; 132Sn(64Ni, X), E(cm)=145-200 MeV; 100Mo(60Ni, X), (64Ni, X), E(cm)=120-160 MeV; 58,64Ni(58Ni, X), E(cm)=88-110 MeV; 150Nd(60Ni, X), (64Ni, X), E(cm)=160-210 MeV; 74Ge(58Ni, X), (64Ni, X), E(cm)=95-120 MeV; 208Pb(40Ca, X), (48Ca, X), E(cm)=160-195 MeV; 90,96Zr(40Ca, X), E(cm)=85-115 MeV; 94Zr(40Ca, X), E(cm)=85-105 MeV; 192Os(40Ca, X), E(cm)=150-185 MeV; 48Ca(40Ca, X), E(cm)=44-68 MeV; 194Pt(40Ca, X), E(cm)=160-200 MeV; 116,124Sn(40Ca, X), E(cm)=105-130 MeV; 110Pd(32S, X), (36S, X), E(cm)=75-95 MeV; 142Ce(28Si, X), E(cm)=85-125 MeV; 198Pt, 208Pb(28Si, X), E(cm)=110-150 MeV; 154Sm(32S, X), E(cm)=95-130 MeV; 208Pb(32S, X), E(cm)=130-160 MeV; 207Pb(58Ni, X), (64Ni, X), E(cm)=220-250 MeV; 154Sm(40Ca, X), (48Ca, X), E(cm)=120-150 MeV; 64Ni, (64Ni, X), E(cm)=85-105 MeV; 238U(40Ca, X), (48Ca, X), E(cm)=170-215 MeV; 48Ca(36S, X), E(cm)=35-55 MeV; 64Ni(36S, X), E(cm)=50-60 MeV; calculated capture cross sections. Quantum diffusion approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064614
2010BA22 Phys.Rev.Lett. 105, 072501 (2010) C.L.Bai, H.Q.Zhang, H.Sagawa, X.Z.Zhang, G.Colo, F.R.Xu Effect of the Tensor Force on the Charge Exchange Spin-Dipole Excitations of 208Pb NUCLEAR STRUCTURE 208Pb; calculated charge exchange spin-dipole excitations; deduced tensor correlations, tensor strength parameters, strength distributions. Self-consistent Skyrme hartree-Fock formalism.
doi: 10.1103/PhysRevLett.105.072501
2010BA26 Nucl.Phys. A834, 65c (2010) Tensor Effects on Spin-Dependent Charge-Exchange transitions NUCLEAR STRUCTURE 208Pb; calculated GT (Gamow-Teller) and SD (Spin-Dipole) transition strength functions.
doi: 10.1016/j.nuclphysa.2010.01.019
2010BA34 Chin.Phys.Lett. 27, 102101 (2010) C.-L.Bai, H.-Q.Zhang, X.-Z.Zhang, F.-R.Xu, H.Sagawa, G.Colo Effect of the Tensor Force on Charge-Exchange Spin-Dependent Multipole Excitations NUCLEAR STRUCTURE 90Zr; calculated charge-exchange spin-dipole and spin-quadrupole strength functions; deduced RPA tensor correlation shift.
doi: 10.1088/0256-307X/27/10/102101
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
2010YU02 J.Phys.(London) G37, 075108 (2010) N.Yu, H.Q.Zhang, H.M.Jia, S.T.Zhang, M.Ruan, F.Yang, Z.D.Wu, X.X.Xu, C.L.Bai Unusual potential behavior for the weakly bound nucleus 9Be in elastic scattering from 208Pb and 209Bi near the threshold NUCLEAR REACTIONS 208Pb, 209Bi(9Be, 9Be), E=37-50 MeV; measured reaction products; deduced σ(θ), optical potential parameters.
doi: 10.1088/0954-3899/37/7/075108
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
2009BA17 Phys.Lett. B 675, 28 (2009) C.L.Bai, H.Sagawa, H.Q.Zhang, X.Z.Zhang, G.Colo, F.R.Xu Effect of tensor correlations on Gamow-Teller states in 90Zr and 208Pb NUCLEAR STRUCTURE 90Zr, 208Pb; calculated Gamow-Teller strength distributions including tensor correlation in HF and RPA model. Comparison with data.
doi: 10.1016/j.physletb.2009.03.077
2009BA19 Phys.Rev. C 79, 041301 (2009) C.L.Bai, H.Q.Zhang, X.Z.Zhang, F.R.Xu, H.Sagawa, G.Colo Quenching of Gamow-Teller strength due to tensor correlations in 90Zr and 208Pb NUCLEAR STRUCTURE 90Zr, 208Pb; calculated Gamow-Teller (GT) and spin-quadrupole (SQ) strength distributions. Random-phase approximation (RPA) and Hartree-Fock (HF) calculations.
doi: 10.1103/PhysRevC.79.041301
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
2009YU04 Chin.Phys.Lett. 26, 112101 (2009) Three-Body Faddeev Approach to Two-Proton Emissions from 18Ne Excited State NUCLEAR STRUCTURE 18Ne; calculated excitation energy spectrum and relative momentum distribution of the two protons using Faddeev approach. Comparison with experiment.
doi: 10.1088/0256-307X/26/11/112101
2009ZH06 Chinese Physics B 18, 531 (2009) D.-H.Zhang, J.-X.Cheng, B.Cheng, F.Wang, Q.Wang, H.-Q.Zhang, R.Xu, H.-M.Jia, X.-Q.Li Helium production from 84Kr - and 197Au - emulsion interactions at high energies
doi: 10.1088/1674-1056/18/2/024
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
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