NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Z.Wu Found 79 matches. 2024HU03 Eur.Phys.J. A 60, (2024) Y.Hu, Yu.M.Gledenov, Z.Cui, J.Liu, H.Bai, C.Xia, Zh.Chen, Z.Wu, W.Ren, W.Cao, T.Fan, G.Zhang, E.Sansarbayar, G.Khuukhenkhuu, L.Krupa, I.Chuprakov, Q.Fan, X.Ruan, H.Huang, J.Ren, Y.Gao, X.Yang Cross section measurement for the 14N(n, α0, 1)11B reactions in the 4.5–11.5 MeV neutron energy region NUCLEAR REACTIONS 14N(n, α), E=4.5 -11.5 MeV; measured reaction products, En, In, Eα, Iα; deduced σ and uncertainties. Comparison with EXFOR, ENDF/B-VIII.0, ENDF/B-VII.1, JEFF-3.3, CENDL-3.2, ROSFOND-2010, ADS-2.0, JENDL-5, BROND-3.1, BROND-2.2, FENDL-3.2b, and TENDL-2021 libraries. The 4.5 MV Van de Graaff accelerator at Peking University and the HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE).
doi: 10.1140/epja/s10050-024-01268-9
2024WU07 Chin.Phys.C 48, 024101 (2024) From masses and radii of neutron stars to EOS of nuclear matter through neural network
doi: 10.1088/1674-1137/ad0e04
2024ZH02 Phys.Rev. C 109, 014303 (2024) Exotic nonaxial-octupole shapes in N=184 isotones from covariant density functional theories
doi: 10.1103/PhysRevC.109.014303
2023WU03 Phys.Rev. C 107, 034902 (2023) Probing the incompressibility of dense hadronic matter near the QCD phase transition in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.107.034902
2023WU05 Nucl.Phys. A1036, 122671 (2023) Z.-H.Wu, H.-B.Fu, T.Zhong, D.Huang, D.-D.Hu, X.-G.Wu α0(980)-meson twist-2 distribution amplitude within the QCD sum rules and investigation of D → α0(980)(→ ηπ)e+ ve
doi: 10.1016/j.nuclphysa.2023.122671
2023WU08 New Journal of Physics 25, 093039 (2023) Z.W.Wu, Z.Q.Tian, C.Z.Dong, A.Surzhykov, S.Fritzsche Hyperfine-induced effects on Kα1 linear polarization following electron-impact excitation of heliumlike Tl79+ ions with nuclear spin I=1/2 NUCLEAR MOMENTS 207Tl; calculated linear polarization of characteristic lines following electron-impact excitation of atoms or ions with arbitrary nuclear spin using the multi-configurational Dirac-Fock method and relativistic distorted-wave theory.
doi: 10.1088/1367-2630/acf8e9
2023XI04 Appl.Radiat.Isot. 197, 110817 (2023) Y.Xie, C.Cheng, W.Zhang, X.Wang, W.Qin, W.Liu, S.Lin, P.Xiao, Z.Wu, W.Jia Feasibility study of on-line monitoring gadolinium based on neutron induced gamma activation
doi: 10.1016/j.apradiso.2023.110817
2022WU05 Phys.Lett. B 825, 136886 (2022) Production of proton-rich nuclei in the vicinity of 100Sn via multinucleon transfer reactions NUCLEAR REACTIONS 112Sn(58Ni, X)Pd/Ag/Cd/In/Sn/Xe/I/Te/Sb, E(cm)=221.77 MeV; analyzed available data; calculated σ using TDHF+GEMINI approach.
doi: 10.1016/j.physletb.2022.136886
2021ZH44 Chin.Phys.C 48, 084001 (2021) J.Zhong, L.-T.Deng, S.-P.Hu, X.-G.Wu, P.C.Srivastava, A.Saxena, G.-S.Li, Y.Zheng, C.-B.Li, Q.-M.Chen, C.-Y.He, W.-K.Zhou, B.-J.Zhu, Q.-W.Fang, H.Hua, J.-J.Sun, H.-B.Sun, L.Gan, H.-G.Zhao, Q.Luo, Z.-X.Wu High spin states in 71Ga NUCLEAR REACTIONS 70Zn(7Li, 2nα)71Ga, E=30, 35 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, level scheme, positive and negative parity bands. Comparison with calculations in the framework of nuclear shell models with JUN45 and jj44b interactions.
doi: 10.1088/1674-1137/ac0098
2021ZH66 Nucl. Sci. Tech. 32, 107 (2021) J.Zhong, X.-G.Wu, S.-P.Hu, Y.-J.Ma, Y.Zheng, C.-B.Li, G.-S.Li, B.-J.Zhu, T.-X.Li, Y.-J.Jin, Y.-X.Gao, Q.-W.Fan, K.-Y.Ma, D.Yang, H.-B.Sun, H.-G.Zhao, L.Gan, Q.Luo, Z.X.Wu Lifetime measurements in 138Nd NUCLEAR REACTIONS 123Sb(19F, 4n), E=87 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and relative intensities, J, π, partial level scheme, level T1/2, B(E2). Comparison with Grodzins systematics and available data. The recoil distance Doppler shift technique in combination with the differential decay curve method. The HI-13 tandem accelerator of the China Institute of Atomic Energy (CIAE) in Beijing.
doi: 10.1007/s41365-021-00953-4
2020XU03 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 12C, 27Al, 28Si, 58Ni, 208Pb(8B, 8B), 9Be, 12C, 16O, 28Si, 58Ni, 120Sn, 208Pb(10B, 10B), 12C, 28Si, 58Ni, 208Pb, 209Bi(11B, 11B), E<50 MeV; analyzed available data. 8,10,11B; calculated σ; deduced global phenomenological optical model potentials.
doi: 10.1088/1674-1137/44/3/034101
2020XU04 Chin.Phys.C 44, 034101 (2020) Y.-L.Xu, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Applicability of 9Be global optical potential to description of 8, 10, 11B elastic scattering NUCLEAR REACTIONS 27Al, 58Ni, 208Pb, 12C, 28Si(8B, 8B), E<100 MeV; 27Al, 28Si, 58Ni, 120Sn, 16O, 9Be, 208Pb(10B, 10B), E<100 MeV; 28Si, 58Ni, 209Bi, 12C, 209Bi(11B, 11B), E<100 MeV; analyzed available data. 9Be; deduced optical model potential parameters, σ, σ(θ).
doi: 10.1088/1674-1137/44/3/034101
2020ZH26 Chin.Phys.C 44, 094001 (2020) J.Zhong, Y.-J.Ma, X.-G.Wu, B.-J.Zhu, C.-B.Li, G.-S.Li, Y.Zheng, Q.-M.Chen, C.-Y.He, L.-T.Deng, W.-K.Zhou, K.-Y.Ma, D.Yang, H.Guo, J.-Q.Wang, X.Guang, J.Sun, H.-B.Sun, S.-P.Hu, L.Gan, H.-G.Zhao, Q.Luo, Z.-X.Wu Lifetime measurement for the 21+ state in 106Cd NUCLEAR REACTIONS 94Zr(16O, 4n)106Cd, E=87 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, lifetime, B(E2). The Recoil Distance Doppler Shift technique in combination with the Differential Decay Curve Method.
doi: 10.1088/1674-1137/44/9/094001
2019CH53 J.Radioanal.Nucl.Chem. 322, 1605 (2019) Y.Chen, S.-H.Huang, R.i-X.Hu, Y.-G.Zhao, L.-L.Li, J.-J.Zhou, C.Li, J.-L.Zhang, Z.-H.Wu Age determination for uranium standard samples by 231Pa/235U radiochronometer
doi: 10.1007/s10967-019-06922-x
2019HU06 Nucl.Phys. A982, 927c (2019) H.Huang, B.Xiao, H.Xiong, Z.Wu, Y.Mu, H.Song Applications of deep learning to relativistic hydrodynamics
doi: 10.1016/j.nuclphysa.2018.11.004
2019WU07 Phys.Rev. C 99, 064902 (2019) Universal scaling of the σ field and net-protons from Langevin dynamics of model A
doi: 10.1103/PhysRevC.99.064902
2019WU09 Phys.Rev. C 100, 014612 (2019) Microscopic studies of production cross sections in multinucleon transfer reaction 58Ni 124Sn NUCLEAR REACTIONS 124Sn(58Ni, X), E(cm)=150, 153, 157, 160.6 MeV; calculated multinucleon transfer and production σ(E) for secondary fragments as function of number of transferred neutrons, energy dependence of the total cross sections integrated over all the neutron transfer channels, total kinetic energy loss, neutron to proton ratio of projectile-like and target-like fragments, transferred nucleon number, and neutron pickup and proton removal transfer probabilities using combined microscopic time-dependent Hartree-Fock (TDHF) and GEMINI++ statistical model approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.014612
2019XU05 Phys.Rev. C 99, 034618 (2019) Y.Xu, Y.Han, H.Liang, Z.Wu, H.Guo, C.Cai Global optical model potential for the weakly bound projectile 9Be NUCLEAR REACTIONS Mg(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 27Al(9Be, 9Be), E=12.0, 14.0, 18.0, 20.0, 22.0, 25.0, 28.0, 32.0, 33.0, 35.0.40.0, 47.5 MeV; 28Si(9Be, 9Be), E=12.0, 13.0, 14.0, 17.0, 20.0, 23.0, 26.0, 30.0, 45.0, 50.0, 60.0 MeV; 40Ca(9Be, 9Be), E=14.0, 20.0, 26.0, 45.0.50.0, 60.0 MeV; 58Ni(9Be, 9Be), E=20.0, 26.0 MeV; 64Zn(9Be, 9Be), E=17.0, 19.0, 21.0, 23.0, 26.0, 28.0, 28.4, 28.97 MeV; 89Y(9Be, 9Be), E=18.6, 20.6, 22.7, 24.7, 26.7, 28.7, 33.2 MeV; Ag(9Be, 9Be), E=26.0 MeV; 144Sm(9Be, 9Be), E=30.0, 31.5, 33.0, 34.0, 35.0, 37.0, 39.0, 41.0, 44.0, 48.0 MeV; 208Pb(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 9.5, 40.0, 41.0, 42.0, 44.0, 46.0, 47.2, 48.0, 50.0, 60.0, 68.0, 75.0 MeV; 209Bi(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 39.5, 40.0, 41.0, 42.0, 44.0, 46.0, 48.0 MeV; analyzed elastic σ(θ, E) data for global phenomenological energy-dependent optical model potential parameters for 9Be. 9Be, 12,13C, 27Al, 64Zn, 89Y, 144Sm(9Be, X), E=10-300 MeV; 28Si, Cu(9Be, X), E=10-500 MeV; 89Y(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (9Be, X), (11B, X); calculated reaction σ(E) using optical model and compared with experimental data. 9Be(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 12C(9Be, 9Be), E=13.0, 14.0, 14.5, 17.3, 19.0, 20.0, 21.0, 26.0, 153.8 MeV; 13C(9Be, 9Be), E=19.46, 25.05 MeV; 16O(9Be, 9Be), E=20.0, 25.94 MeV; calculated elastic σ(θ, E) using optical model parameters and compared with experimental data.
doi: 10.1103/PhysRevC.99.034618
2018GU21 Phys.Rev. C 98, 064609 (2018) Isotopic trends of quasifission and fusion-fission in the reactions 48Ca + 239, 244Pu NUCLEAR REACTIONS 239,244Pu(48Ca, X), E=204.02, 216.76 MeV; calculated time evolution of the mass density of 48Ca+239Pu, contact time, mass and charge of heavy fragments as a function of impact parameter for the tip and side collisions, mass-angle and total kinetic energy-mass distributions of quasi-fission (QF) fragments. Microscopic time-dependent Hartree-Fock (TDHF) method for the fusion and quasifission dynamics with the statistical evaporation model HIVAP for fusion-fission dynamics.
doi: 10.1103/PhysRevC.98.064609
2018LI33 Phys.Rev. C 98, 014618 (2018) F.Li, L.Zhu, Z.-H.Wu, X.-B.Yu, J.Su, C.-C.Guo Predictions for the synthesis of superheavy elements Z=119 and 120 NUCLEAR REACTIONS 238U, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-60 MeV; calculated evaporation residue σ(E), and compared with available experimental data. 252Es(40Ca, 3n), E(cm)=204.08 MeV; 252Es(42Ca, 3n), E(cm)=203.00 MeV; 249Cf(45Sc, 3n), E(cm)=211.09 MeV; 255Es(40Ca, 4n), E(cm)=207.02 MeV; 254Es(40Ca, 3n), E(cm)=203.60 MeV; 247Bk(47Ti, 3n), E(cm)=219.19 MeV; 248Bk(46Ti, 3n), E(cm)=217.76 MeV; 242Cm(51V, 2n), E(cm)=225.86 MeV; 248Cf(45Sc, 2n), E(cm)=209.29 MeV; 241Am(52Cr, 2n), E(cm)=231.94 MeV; 252Es(44Ca, 3n), E(cm)=204.27 MeV; 253Es(43Ca, 3n), E(cm)=202.49 MeV; 254Es(42Ca, 3n), E(cm)=201.65 MeV; 251Cf(45Sc, 3n), E(cm)=210.03 MeV; 249Bk(47Ti, 3n), E(cm)=217.18 MeV; 248Bk(48Ti, 3n), E(cm)=219.47 MeV; 245Cm(51V, 3n), E(cm)=229.29 MeV; 247Bk(49Ti, 3n), E(cm)=222.17 MeV; 246Cm(50V, 3n), E(cm)=225.70 MeV; 244Cm(51V, 2n), E(cm)=224.00 MeV; 255Es(42Ca, 4n), E(cm)=205.95 MeV; 243Am(53Cr, 3n), E(cm)=236.20 MeV; 254Es(43Ca, 4n), E(cm)=206.90 MeV; 253Es(44Ca, 4n), E(cm)=210.94 MeV; 243Am(52Cr, 2n), E(cm)=229.49 MeV; 254Es(44Ca, 3n), E(cm)=201.64 MeV; 255Es(43Ca, 3n), E(cm)=201.49 MeV; 255Es(44Ca, 4n), E(cm)=207.59 MeV; 252Es(46Ca, 3n), E(cm)=206.00 MeV; 248Bk(50Ti, 3n), E(cm)=222.48 MeV; 247Cm(51V, 3n), E(cm)=226.83 MeV; 254Cf(45Sc, 4n), E(cm)=211.93 MeV; 249Bk(49Ti, 3n), E(cm)=218.88 MeV; 254Es(46Ca, 3n), E(cm)=203.64 MeV; 255Es(46Ca, 4n), E(cm)=210.13 MeV; 252Es(48Ca, 3n), E(cm)=208.42 MeV; 255Es(46Ca, 3n), E(cm)=204.13; 254Es(48Ca, 3n), E(cm)=205.96 MeV; 255Es(48Ca, 4n), E(cm)=212.72 MeV; 242Cm(50Cr, 2n), E(cm)=234.22 MeV; 249Cf(46Ti, 3n), E(cm)=222.89 MeV; 248Cf(46Ti, 2n), E(cm)=219.12 MeV; 257Fm(40Ca, 5n), E(cm)=222.66 MeV; 257Fm(40Ca, 4n), E(cm)=211.66 MeV; 257Fm(40Ca, 3n), E(cm)=205.66 MeV; 251Cf(46Ti, 3n), E(cm)=220.39 MeV; 252Es(45Sc, 3n), E(cm)=214.17 MeV; 250Cf(46Sc, 2n), E(cm)=218.88 MeV; 247Bk(50V, 3n), E(cm)=231.13 MeV; 244Cm(52Cr, 2n), E(cm)=234.88 MeV; 245Cm(52Cr, 3n), E(cm)=240.80 MeV; 243Cm(53Cr, 2n), E(cm)=236.02 MeV; 247Cm(50Cr, 3n), E(cm)=235.12 MeV; 257Fm(42Ca, 3n), E(cm)=205.29 MeV; 254Es(45Sc, 3n), E(cm)=213.40 MeV; 257Fm(43Ca, 4n), E(cm)=210.97 MeV; 257Fm(44Ca, 3n), E(cm)=205.27 MeV; 257Fm(46Ca, 3n), E(cm)=207.84 MeV; 250Cm(53Cr, 3n), E(cm)=234.59 MeV; 257Fm(48Ca, 3n), E(cm)=211.07 MeV; calculated production σ for Z=119 and 120 superheavy isotopes. Dinuclear system (DNS) model.
doi: 10.1103/PhysRevC.98.014618
2018WU06 Phys.Rev. C 97, 064609 (2018) Z.-H.Wu, L.Zhu, F.Li, X.-B.Yu, J.Su, C.-C.Guo Synthesis of neutron-rich superheavy nuclei with radioactive beams within the dinuclear system model NUCLEAR REACTIONS 242,244Pu, 243Am, 245,248,250Cm, 249Bk, 250,251Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-60 MeV; 234Th(42S, 2n), (42S, 3n), (42S, 4n), (42S, 5n), E*=20-65 MeV; 234Th, 244Pu(46Ar, 2n), (46Ar, 3n), (46Ar, 4n), (46Ar, 5n), E*=20-65 MeV; 234Th, 238U, 248Cm, 255Es(44Cl, 2n), (44Cl, 3n), (44Cl, 4n), (44Cl, 5n), E*=20-65 MeV; 228Ra(45Cl, 2n), (45Cl, 3n), (45Cl, 4n), (45Cl, 5n), E*=20-65 MeV; 244Pu, 248Cm(43Cl, 2n), (43Cl, 3n), (43Cl, 4n), (43Cl, 5n), E*=20-65 MeV; 244Pu, 254Cf, 255Es(41S, 2n), (41S, 3n), (41S, 4n), (41S, 5n), E*=20-65 MeV; 257Fm(42Ar, 2n), (42Ar, 3n), (42Ar, 4n), (42Ar, 5n), E*=20-65 MeV; 260Md(38Cl, 2n), (38Cl, 3n), (38Cl, 4n), (38Cl, 5n), E*=20-65 MeV; calculated evaporation residue σ. 228Ra(45Cl, 2n), E*=36.0 MeV; 228Ra(46Cl, 3n), E*=46.0 MeV; 226Ra(47Cl, 2n), E*=36.0 MeV; 234Th(42S, 4n), E*=43.0 MeV; 228Ra(46Ar, 2n), E*=34.0 MeV; 234Th(43S, 5n), E*=51.0 MeV; 234Th(42S, 3n), E*=41.0 MeV; 234Th(43S, 4n), E*=46.0 MeV; 234Th(44S, 5n), E*=59.0 MeV; 234Th(44Cl, 2n), E*=37.0 MeV; 234Th(45Cl, 3n), E*=44.0 MeV; 228Ra(50K, 2n), E*=36.0 MeV; 234Th(46Ar, 2n), E*=34.0 MeV; 238U(43S, 3n), E*=41.0 MeV; 238U(42S, 2n), E*=37.0 MeV; 238U(44Cl, 3n), E*=38.0 MeV; 238U(43Cl, 2n), E*=36.0 MeV; 238U(43S, 3n), E*=41.0 MeV; 234Th(47K, 2n), E*=33.0 MeV; 244Pu(41S, 3n), E*=38.0 MeV; 244Pu(42S, 4n), E*=42.0 MeV; 238U(46Ar, 2n), E*=33.0 MeV; 244Pu(43Cl, 4n), E*=44.0 MeV; 242Pu(44Cl, 3n), E*=37.0 MeV; 244Pu(42Cl, 3n), E*=38.0 MeV; 244Pu(46Ar, 4n), E*=38.0 MeV; 244Pu(45Ar, 3n), E*=44.0 MeV; 242Pu(46Ar, 2n), E*=33.0 MeV; 248Cm(43Cl, 4n), E*=38.0 MeV; 250Cm(42Cl, 5n), E*=43.0 MeV; 248Cm(44Cl, 5n), E*=43.0 MeV; 248Cm(44Cl, 4n), E*=38.0 MeV; 250Cm(42Cl, 4n), E*=39.0 MeV; 250Cm(43Cl, 5n), E*=45.0 MeV; 254Cf(41S, 5n), E*=40.0 MeV; 253Cf(42S, 5n), E*=40.0 MeV; 250Cm(44Ar, 4n), E*=37.0 MeV; 255Es(41S, 5n), E*=40.0 MeV; 254Cf(42Cl, 5n), E*=40.0 MeV; 253Cf(43Cl, 5n), E*=39.0 MeV; 255Es(41S, 4n), E*=37.0 MeV; 253Cf(43Cl, 4n), E*=36.0 MeV; 254Cf(42Cl, 4n), E*=37.0 MeV; 250Cm(48Ca, 4n), E*=35.0 MeV; 248Cm(48Ca, 2n), E*=31.0 MeV; 250Cm(46Ca, 2n), E*=35.0 MeV; 255Es(44Cl, 5n), E*=40.0 MeV; 254Cf(44Ar, 4n), E*=36.0 MeV; 257Fm(41S, 4n), E*=37.0 MeV; 250Cm(48Ca, 3n), E*=31.0 MeV; 255Es(44Cl, 4n), E*=36.0 MeV; 253Cf(46Ar, 4n), E*=34.0 MeV; 254Cf(46Ar, 5n), E*=41.0 MeV; 250Cf(48Ca, 3n), E*=34.0 MeV; 250Cm(49Ti, 4n), E*=42.0 MeV; 252Cf(46Ca, 3n), E*=36.0 MeV; 260Md(38Cl, 3n), E*=41.0 MeV; 260Md(39Cl, 4n), E*=42.0 MeV; 257Fm(42Ar, 4n), E*=41.0 MeV; 251Cf(48Ca, 3n), E*=30.0 MeV; 252Cf(48Ca, 4n), E*=38.0 MeV; 250Cm(49Ti, 3n), E*=34.0 MeV; 257Fm(42Ar, 3n), E*=33.0 MeV; 257Fm(43Ar, 4n), E*=38.0 MeV; 260Md(39Cl, 3n), E*=37.0 MeV; 244Pu(43Cl, n), E*=40.0 MeV; 238Cm(48Ca, 2np), E*=41.0 MeV; 254Cf(41S, 5n), E*=40.0 MeV; 248Cm(48Ca, 2nα), E*=46.0 MeV; 248Cm(43Cl, 4n), E*=38.0 MeV; 242Pu(48Ca, 2np), E*=35.0 MeV; 248Cm(44Cl, 4n), E*=38.0 MeV; 242Pu(48Ca, np), E*=40.0 MeV; 244Pu(48Ca, 3np), E*=45.0 MeV; 255Es(41S, 5n), E*=40.0 MeV; 245Cm(48Ca, np), E*=32.0 MeV; 249Bk(48Ca, 2nα), E*=37.0 MeV; 255Es(41S, 4n), E*=37.0 MeV; 248Cm(48Ca, 3np), E*=44.0 MeV; 249Bk(48Ca, nα), E*=32.0 MeV; calculated evaporation residue σ, and optimal incident beam energies. 48Ca(238U, 2n), (238U, 3n), (238U, 4n), E(cm)=184.13-214.13 MeV; calculated evaporation residue σ, potential energy surface, driving potential, survival and complete fusion probabilities, and capture σ. Dinuclear system model. 271Db, 272,273Sg, 276Bh, 278Hs, 279Mt, 282Ds, 283Rg, 286Cn, 287,288Nh, 290Fl, 291,292Mc, 294,295Lv, 295,296Og; calculated evaporation residue σ, and optimal incident beam energies for various reactions. Comparison with available experimental data. Relevance to synthesis of neutron-rich superheavy nuclei using radioactive ion beams, such as those at ATLAS-ANL.
doi: 10.1103/PhysRevC.97.064609
2018XU01 Phys.Rev. C 97, 014615 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai Global phenomenological optical model potential for the 7Li projectile nucleus NUCLEAR REACTIONS 9Be(7Li, 7Li), E=15.75, 24.0, 30.0, 63.0, 130.0 MeV; 12C(7Li, 7Li), E=7.5, 9.0, 12.0, 15.0, 36.0, 131.8 MeV; 16O(7Li, 7Li), E=26.0, 36.0, 42.0, 50.0 MeV; 11B, 12,13C, 24Mg(7Li, 7Li), E=34.0 MeV; 24,26Mg(7Li, 7Li), E=88.7 MeV; 27Al(7Li, 7Li), E=6.0, 7.0, 8.0, 9.0, 10.0, 11.0, 12.0, 13.0, 14.0, 16.0, 18.0, 19.0, 24.0 MeV; 28Si(7Li, 7Li), E=8.0, 8.5, 9.0, 10.0, 11.0, 11.5, 13.0, 15.0, 16.0, 21.0, 26.0, 36.0, 177.8 MeV; 40,44,48Ca(7Li, 7Li), E=34.0; 40Ca(7Li, 7Li), E=88.7 MeV; 46,48Ti(7Li, 7Li), E=17.0 MeV; 54Fe(7Li, 7Li), E=36.0, 42.0, 48.0 MeV; 56Fe, 65Cu, 90Zr(7Li, 7Li), E=34.0 MeV; 58Ni(7Li, 7Li), E=14.22, 16.25.18.28, 19.0, 20.31.34.0, 42.0 MeV; 60,62Ni, 64,68Zn(7Li, 7Li), E=34.0 MeV; 80Se(7Li, 7Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 23.0, 26.0 MeV; 89Y(7Li, 7Li), E=60.0 MeV; 116Sn(7Li, 7Li), E=18.0, 19.0, 20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0 MeV; 120Sn(7Li, 7Li), E=19.5, 20.0, 20.5, 22.0, 24.0, 25.0, 26.0, 28.0, 30.044.0 MeV; 138Ba(7Li, 7Li), E=21.0, 22.0, 23.0, 24.0, 28.0, 30.0, 32.0, 52.0 MeV; 140Ce, 142Nd(7Li, 7Li), E=52.0 MeV; 144Sm(7Li, 7Li), E=21.6, 22.1, 22.6.23.0, 25.0, 27.0, 29.0, 30.0, 32.0, 35.0, 40.8, 52.0 MeV; 208Pb(7Li, 7Li), E=27.0, 29.0, 33.0, 39.0, 42.0, 52.0 MeV; 232Th(7Li, 7Li), E=24.0, 26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed σ(θ, E) experimental data by global phenomenological optical model potential. 13C, 27Al, 64Zn, 116Sn, 138Ba, (7Li, X), E<300 MeV; 28Si, Cu, 208Pb(7Li, X), E<400 MeV; calculated reaction σ(E) using optical model, and compared with experimental data.
doi: 10.1103/PhysRevC.97.014615
2018XU10 Phys.Rev. C 98, 024619 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai 6Li global phenomenological optical model potential NUCLEAR REACTIONS 24Mg, 48Ca(6Li, 6Li), E=240.0 MeV; 25,26Mg, 39K, 91Zr(6Li, 6Li), E=34.0 MeV; 27Al(6Li, 6Li), E=7.0, 8.0, 10.0, 12.0, 18.0, 34.0 MeV; 28Si(6Li, 6Li), E=7.5, 9.0, 11.0, 13.0, 16.0, 20.0, 21.0, 25.0, 27.0, 34.0, 46.0, 99.0, 135.0, 154.0, 210.0, 240.0, 318.0, 350.0 MeV; 40Ca(6Li, 6Li), E=50.6, 99.0, 156.0, 210.0, 240.0 MeV; 54Fe(6Li, 6Li), E=38.0, 44.0, 50.0 MeV; 59Co(6Li, 6Li), E=12.0, 18.0, 26.0, 30.0 MeV; 58Ni(6Li, 6Li), E=9.85, 11.21, 12.13, 13.04, 14.04, 34.0, 50.6, 73.7, 90.0, 99.0, 210.0, 240.0 MeV; 65Cu(6Li, 6Li), E=25.0 MeV; 64Zn(6Li, 6Li), E=10.77, 11.69, 12.0, 12.43, 13.0, 13.54, 13.8, 14.92, 15.0, 16.30, 16.5, 18.0, 18.14, 19.98, 22.0 MeV; 72,74,76Ge(6Li, 6Li), E=28.0 MeV; 80Se(6Li, 6Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 22.19, 23.0, 26.0 MeV; 89Y(6Li, 6Li), E=60.0 MeV; 90Zr(6Li, 6Li), E=11.0, 12.0, 13.0, 15.0, 17.0, 19.0, 21.0, 25.0, 30.0, 34.0, 60.0, 70.0, 73.7, 99.0, 156.0, 210.0, 240.0 MeV; 92,94,96Zr(6Li, 6Li), E=70.0 MeV; 112Sn(6Li, 6Li), E=21.0, 22.0, 23.0, 25.0, 30.0, 35.0 MeV; 116Sn(6Li, 6Li), E=20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0, 40.0 MeV; 118Sn(6Li, 6Li), E=42.0 MeV; 120Sn(6Li, 6Li), E=30.0, 44.0, 90.0 MeV; 124Sn(6Li, 6Li), E=73.7 MeV; 138Ba(6Li, 6Li), E=21.0, 22.0, 23.0, 24.0, 26.0, 28.0 MeV; 144Sm(6Li, 6Li), E=21.0, 22.1, 22.6, 24.1, 26.0, 28.0, 30.1, 32.2, 35.1, 42.3 MeV; 208Pb(6Li, 6Li), E=25.0, 29.0, 31.0, 33.0, 35.0, 36.0, 37.0, 39.0, 42.0, 43.0, 46.0, 48.0, 50.6, 73.7, 88.0, 90.0, 99.0, 156.0, 210.0 MeV; 209Bi(6Li, 6Li), E=24.0, 26.0, 28.0, 29.9, 30.0, 32.0, 32.8, 34.0, 36.0, 40.0, 44.0, 50.0 MeV; 232Th(6Li, 6Li), E=26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed differential σ(θ, E) data; deduced a new set of 6Li global phenomenological energy-dependent optical potential parameters based on the form of the Woods-Saxon potential within the optical model. 63,65Cu, 64Zn, 112,116Sn, 138Ba, 208Pb(6Li, X), E<400 MeV; calculated reaction σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.98.024619
2017LI21 Nucl.Sci.Eng. 187, 107 (2017) H.Liang, Z.Wu, Z.Zhang, Y.Han, X.Jiao Calculations and Analysis of n+93Nb Reaction NUCLEAR REACTIONS 93Nb(n, X), E<200 MeV; calculated σ, σ(E), σ(θ), σ(θ, E) using theoretical models. Comparison with ENDF/B-VII, JENDL-4, TENDL-2015 libraries, experimental data.
doi: 10.1080/00295639.2017.1295699
2017SU16 Phys.Rev. C 95, 054606 (2017) X.W.Su, Y.L.Han, H.Y.Liang, Z.D.Wu, H.R.Guo, C.H.Cai Global phenomenological optical model potential for 8Li projectile NUCLEAR REACTIONS 9Be(8Li, 8Li), E=14, 19.6, 27 MeV; 12C(8Li, 8Li), E=14, 23.9 MeV; 13C, 14N, 27Al, 197Au(8Li, 8Li), E=14 MeV; 51V(8Li, 8Li), E=18.5, 26 MeV; 58Ni(8Li, 8Li), E=14, 19.6, 20.2, 22 MeV; 208Pb(8Li, 8Li), E=24.4, 27.9, 28.9, 30.6, 33.1 MeV; calculated σ(θ, E) by optical potential model, and compared with experimental data; deduced global phenomenological optical model parameters (OMPs) for 8Li. 9Be(8Li, X), E=19.6 MeV; 12C(8Li, X), E=14 MeV; 51V(8Li, X), E=18.5, 26.0 MeV; 208Pb(8Li, X), E=24.4, 27.6, 28.89, 30.57, 33.13 MeV; calculated total σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.95.054606
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
2016LI45 Yuan.Wul.Ping. 33, 160 (2016); Nucl.Phys.Rev. 33, 160 (2016) C.Lin, X.Xu, J.Wang, L.Sun, H.Jia, L.Yang, P.Ma, J.Ma, Y.Yang, S.Jin, M.Huang, Z.Bai, Z.Wu, F.Yang, Z.Hu, M.Wang, X.Lei, H.Zhang, H.Xu, G.Xiao Proton and Two-proton Emissions from Proton-rich Nuclei with 10 ≤ Z ≤ 20 RADIOACTIVITY 28,29S, 26,27P, 17,18Ne(2p), 27S, 26P, 22,25Si, 20Mg, 23Si, 22Al, 21Mg, 24Si, 23Al, 36,37Ca(β+p), (β+2p); measured decay products, Ep, Ip; deduced energy, T1/2, branching-ratios.
doi: 10.11804/NuclPhysRev.33.02.160#
2016LI51 Chin.Phys.C 40, 114104 (2016) E.T.Li, B.Guo, Z.H.Li, Y.B.Wang, Y.J.Li, Z.D.Wu, J.Su, D.Y.Pang, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, Z.Y.Han, X.Hao, S.P.Hu, J.J.He, L.Jing, S.J.Jin, L.Li, X.Y.Li, Z.C.Li, G.Lian, J.C.Liu, Q.Luo, L.H.Qiao, Y.P.Shen, H.B.Sun, S.Q.Yan, X.Q.Yu, S.Zeng, D.H.Zhang, L.Y.Zhang, W.J.Zhang, Y.Zhou, W.P.Liu Radii of the bound states in 16N from the asymptotic normalization coefficients RADIOACTIVITY 16N(n) [from 15N(7Li, 6Li)16N, E=44 MeV]; analyzed available data; deduced asymptotic normalization coefficients (ANCs), rms radii of the valence neutron, probabilities of the valence neutron staying out of the core potentials.
doi: 10.1088/1674-1137/40/11/114104
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
2016SU13 Int.J.Mod.Phys. E25, 1650033 (2016) X.-W.Su, Y.-L.Han, H.-Y.Liang, Z.-D.Wu, H.-R.Guo, C.-H.Cai Global 6He optical model potential NUCLEAR REACTIONS 6,7Li, 9Be, 12C, 27Al, 28Si, 51V, 48Ti, 58Ni, 63,65Cu, 64Zn, 120Sn, 197Au, 206,208Pb, 209Bi(6He, X), (6He, 6He), E<300 MeV; analyzed available data; deduced optical potential; calculated σ, σ(θ).
doi: 10.1142/S0218301316500336
2016SU22 Yuan.Wul.Ping. 33, 230 (2016); Nucl.Phys.Rev. 33, 230 (2016) L.Sun, X.Xu, C.Lin, J.Wang, D.Fang, Z.Li, Y.Wang, J.Li, L.Yang, N.Ma, K.Wang, H.Zhang, H.Wang, C.Li, C.Shi, M.Nie, X.Li, H.Li, J.Ma, P.Ma, S.Jin, M.Huang, Z.Bai, J.Wang, F.Yang, H.Jia, H.Zhang, Z.Liu, P.Bao, S.Wang, Z.Wu, Y.Yang, Z.Chen, J.Su, Y.Shen, Y.Zhou, W.Ma, J.Chen An implantation and detection system for spectroscopy of 22, 24Si RADIOACTIVITY 22,24Si(β+p); measured decay products, Ep, Ip; deduced energy levels, J, π, T1/2, branchning ratios.
doi: 10.11804/NuclPhysRev.33.02.230
2016WU01 Phys.Rev. C 93, 034334 (2016) Empirical residual neutron-proton interaction in odd-odd nuclei ATOMIC MASSES A=10-260; analyzed np interactions from experimental binding energies for odd-A, even-even, odd-odd, and for all known (except N=Z) nuclei; calculated δnp interaction using mac-mic mass formula, shell model mass formulas with parameters taken from literature, and the HFB mass formula. Z=9-131, N=7-219; deduced δnp interaction for all the predicted 2564 odd-odd nuclei from mass formulas. Z=5-103, N=5-153; deduced δnp interaction for all the known 486 odd-odd nuclei from experimental binding energies and nuclear mass formula calculations. Numerical results for individual nuclei are given in two supplementary files.
doi: 10.1103/PhysRevC.93.034334
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
2015WU04 Phys.Rev. C 92, 024306 (2015) Z.-Y.Wu, C.Qi, R.Wyss, H.-L.Liu Global calculations of microscopic energies and nuclear deformations: Isospin dependence of the spin-orbit coupling NUCLEAR STRUCTURE A=16-375, N=8-270; 24,26,28,30,32,34,36,38,40,42,44Si, 44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76Cr, 48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82Fe, 62,64,66,68,70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104Ge, 66,68,70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116Se, 70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118Kr, 78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124Zr, 82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Mo, 86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138Ru, 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264Hg, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266Pb; calculated microscopic binding energies and ground-state nuclear deformations β2, γ and β4 for 1850 even-even nuclei. Macroscopic-microscopic framework using three Woods-Saxon parametrizations with different isospin dependencies. Comparison with results of other macroscopic-microscopic mass models. Discussed isospin dependence of spin-orbital force.
doi: 10.1103/PhysRevC.92.024306
2014GU02 Phys.Rev. C 89, 012801 (2014) B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, S.Q.Yan, Z.D.Wu, E.T.Li, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, J.J.He, S.J.Jin, L.Jing, L.Li, Z.C.Li, G.Lian, J.C.Liu, Y.P.Shen, Y.B.Wang, X.Q.Yu, S.Zeng, L.Y.Zhang, W.J.Zhang, W.P.Liu Spectroscopic factors for low-lying 16N levels and the astrophysical 15N(n, γ)16N NUCLEAR REACTIONS 15N(7Li, 6Li)16N, E=44 MeV; measured 6Li spectrum, σ(θ) using Q3D magnetic spectrograph at CIAE's HI-13 tandem accelerator facility. 16N; deduced levels, J, π, configurations, spectroscopic factors for ground and first three excited states. DWBA analysis. Comparison with shell model calculations. 15N(n, γ)16N, at T=0.01-3 GK; deduced astrophysical reaction rates. Comparison with previous experimental and theoretical results.
doi: 10.1103/PhysRevC.89.012801
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
2014LI10 Ann.Nucl.Energy 69, 301 (2014) The energy spectra and double-differential cross-sections for p+92, 94, 95, 96, 97, 98, 100Mo reactions at the incident energies from threshold to 200 MeV NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(p, xn), (p, xp), (p, xd), (p, xα), (p, xt), E<160 MeV; calculated σ(E), σ(E, θ). Exciton model including the improved Iwamoto-Harada model, comparison with experimental data.
doi: 10.1016/j.anucene.2014.02.008
2014LI49 Phys.Rev. C 90, 067601 (2014) E.T.Li, Z.H.Li, Y.J.Li, B.Guo, Y.B.Wang, D.Y.Pang, J.Su, S.Q.Yan, S.Zeng, L.Gan, Z.C.Li, J.C.Liu, X.X.Bai, Z.D.Wu, S.J.Jin, L.Y.Zhang, X.Q.Yu, L.Li, H.B.Sun, G.Lian, Q.W.Fan, W.P.Liu Proton spectroscopic factor of the 12C ground state from the 12C(11B, 12C) 11B elastic transfer reaction NUCLEAR REACTIONS 12C(11B, 11B), (11B, 12C)11B, E=50 MeV; measured particle spectra, angular distributions using Q3D magnetic spectrometer at the HI-13 tandem accelerator of CIAE facility. 12C; deduced optical potential parameters, proton spectroscopic factor for 12C g.s., DWBA calculations. Comparison with previous experimental and theoretical results.
doi: 10.1103/PhysRevC.90.067601
2014WU03 Phys.Rev. C 89, 054315 (2014) Z.D.Wu, B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, S.Q.Yan, E.T.Li, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, J.J.He, S.J.Jin, L.Jing, L.Li, Z.C.Li, G.Lian, J.C.Liu, Y.P.Shen, Y.B.Wang, X.Q.Yu, S.Zeng, D.H.Zhang, L.Y.Zhang, W.J.Zhang, W.P.Liu Proton widths of the low-lying 16F states from the 15N(7Li, 6Li)16N reaction NUCLEAR REACTIONS 15N(7Li, 7Li), (7Li, 6Li), E=34.5, 44 MeV; measured particle spectra, elastic and inelastic σ(θ) using Q3D magnetic spectrograph at CIAE facility. 16N; deduced levels, J, π, asymptotic normalization coefficients (ANCs), spectroscopic factors. DWBA analysis. 16F; deduced proton and single-particle widths, spectroscopic factors for first four levels from mirror analogy with 16N. Comparison with previous experimental results and compilation.
doi: 10.1103/PhysRevC.89.054315
2014WU07 Ann.Nucl.Energy 73, 17 (2014) Z.Wu, H.Liang, J.Li, Z.Zhang, Y.Han Theoretical calculations and evaluations of n + 32, 33, 34, 36, nat.S reactions NUCLEAR REACTIONS 32,33,34,36S, S(n, n), (n, n'), (n, X), (n, p), (n, t), (n, xn), (n, xp), E<200 MeV; calculated σ, σ(θ, E), σ(θ). APMN nuclear model code, comparison ENDF/B-VII, JENDL-4, and TENDL-2012 libraries.
doi: 10.1016/j.anucene.2014.05.032
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
2013LI09 Phys.Rev. C 87, 017601 (2013) Z.H.Li, Y.J.Li, J.Su, B.Guo, E.T.Li, K.J.Dong, X.X.Bai, Z.C.Li, J.C.Liu, S.Q.Yan, Y.B.Wang, S.Zeng, G.Lian, B.X.Wang, S.J.Jin, X.Liu, W.J.Zhang, W.Z.Huang, Q.W.Fan, L.Gan, Z.D.Wu, W.P.Liu New determination of the proton spectroscopic factor in 9Be from the 13C(9Be, 8Li)14N angular distribution NUCLEAR REACTIONS 13C(9Be, 8Li)14N, 12,13C(9Be, 9Be), E=40 MeV; measured particle spectra, Eα, differential s(θ) using Q3D magnetic spectrometer at HI-13 tandem accelerator facility in Beijing. 9Be; deduced proton spectroscopic factor for g.s. Optical model and DWBA analysis. Comparison with previous experimental and theoretical studies. Relevance to astrophysical S factor for 8Li(p, γ)9Be reaction.
doi: 10.1103/PhysRevC.87.017601
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
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
2011WU01 Nucl.Instrum.Methods Phys.Res. B269, 671 (2011) Calculation of cross-sections for p+ 92, 94, 95, 96, 97, 98, 100Mo reactions up to 160 MeV NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(p, p), (p, p'), (p, α), (p, nα), (p, pα), (p, n), (p, 2n), (p, 3α), (p, 3n), (p, 4n), (p, 4n2p), (p, 3He), (p, np), E<200 MeV; calculated σ. MEND nuclear reaction model code.
doi: 10.1016/j.nimb.2011.01.126
2010FA10 Nucl.Phys. A834, 183c (2010) G.T.Fan, W.Xu, C.J.Lin, B.J.Xu, F.Jia, G.W.Fan, H.M.Jia, L.F.Yang, Y.J.Li, Q.Y.Pan, W.Luo, X.X.Xu, Z.D.Wu Systematic uncertainty studies for precision measurement on electric polarizabilities of 3He and 4He
doi: 10.1016/j.nuclphysa.2009.12.034
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
2010TI01 Int.J.Mod.Phys. E19, 307 (2010) J.Tian, X.Li, S.Yan, Z.Wu, Z.Li Kinematic correlation of the ternary fission for the system 197Au + 197Au NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; measured reaction fragments; deduced mass number distributions, dynamical modes of ternary fission.
doi: 10.1142/S0218301310014777
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
2010ZH46 Phys.Rev. C 82, 054609 (2010) H.Q.Zhang, C.J.Lin, F.Yang, H.M.Jia, X.X.Xu, Z.D.Wu, F.Jia, S.T.Zhang, Z.H.Liu, A.Richard, C.Beck Near-barrier fusion of 32S+90, 96Zr: The effect of multi-neutron transfers in sub-barrier fusion reactions NUCLEAR REACTIONS 90Zr(32S, X), E=100-130 MeV: 96Zr(32S, X), E=95-130 MeV; measured particle spectra of fusion evaporation residues (ER), E-TOF plot of ER and beam-like particles (BLP), fusion σ(E, θ); deduced barrier distributions. Comparison with coupled-channel (CC) calculations and with data for 96Zr(40Ca, X) reaction. Effects of multi-neutron transfers.
doi: 10.1103/PhysRevC.82.054609
2009JI02 Chin.Phys.Lett. 26, 032301 (2009) F.Jia, C.-J.Lin, H.-Q.Zhang, F.Yang, H.-M.Jia, X.-X.Xu, Z.-D.Wu, Z.-H.Liu, G.-L.Zhang, C.-L.Zhang Experimental Evidence of Two-Proton Emissions from 18Ne Excited State NUCLEAR REACTIONS 197Au(18Ne, 18Ne'), E not given; measured Ep, Ip. 18Ne; deduced level energies. Two proton decay.
doi: 10.1088/0256-307X/26/3/032301
2009WU01 Chin.Phys.Lett. 26, 022503 (2009) Z.-D.Wu, C.-J.Lin, H.-Q.Zhang, Z.-H.Liu, F.Yang, G.-P.An, C.-L.Zhang, G.-L.Zhang, H.-M.Jia, X.-X.Xu, C.-L.Bai, N.Yu, F.Jia Optical Potential Parameters for Halo Nucleus System 6He+12C from Transfer Reaction 11B(7Li, 6He)12C NUCLEAR REACTIONS 11B(7Li, 6He), E=18.3, 28.3 MeV; analyzed σ(θ). 12C(6He, 7Li); deduced optical potential parameters.
doi: 10.1088/0256-307X/26/2/022503
2008AN17 Chin.Phys.Lett. 25, 4237 (2008) G.-P.An, C.-J.Lin, H.-Q.Zhang, Z.-H.Liu, F.Yang, G.-L.Zhang, C.-L.Zhang, Z.-D.Wu, F.Jia, H.-M.Jia, X.-X.Xu, C.-L.Bai, N.Yu Optical Potential Parameters of Weakly Bound Nuclear System 17F+13C NUCLEAR REACTIONS 16O(14N, 14N), (14N, 13C), E=76.2, 57.0 MeV; measured σ(θ). Compared results to model calculations.
doi: 10.1088/0256-307X/25/12/014
2008JI03 Chin.Phys.Lett. 25, 2834 (2008) H.-M.Jia, C.-J.Lin, H.-Q.Zhang, Z.-H.Liu, F.Yang, F.Jia, C.-L.Zhang, G.-P.An, Z.-D.Wu, X.-X.Xu, C.-L.Bai, N.Yu Surface Diffuseness Anomaly in 16O+208Pb Quasi-elastic Scattering at Backward Angle NUCLEAR REACTIONS 208Pb(16O, 16O'), E=40.50-80.25 MeV; measured quasi=elastic scattering excitation function at backward angles.
doi: 10.1088/0256-307X/25/8/028
2008KA21 Nucl.Data Sheets 109, 1655 (2008) Nuclear Data Sheets for A = 124 COMPILATION 124Pd, 124Ag, 124In, 124Sn, 124Sb, 124Te, 124I, 124Xe, 124Cs, 124Ba, 124La, 124Ce, 124Pr; compiled, evaluated structure data.
doi: 10.1016/j.nds.2008.06.001
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
2006ZH12 Chin.Phys.Lett. 23, 1146 (2006) C.-L.Zhang, H.-Q.Zhang, C.-J.Lin, M.Ruan, Z.-H.Liu, F.Yang, X.-K.Wu, P.Zhou, G.-P.An, H.-M.Jia, Z.-D.Wu, X.-X.Xu.C.-L.Bai Unusual Threshold Anomaly in the 6Li+208Pb System NUCLEAR REACTIONS 208Pb(6Li, 6Li), E=25-46 MeV; measured elastic σ(θ); deduced optical potential parameters, effects of coupling to breakup channel.
doi: 10.1088/0256-307X/23/5/023
2004WA08 Phys.Rev. C 69, 034608 (2004) N.Wang, Z.Li, Z.Wu, J.Tian, Y.X.Zhang, M.Liu Further development of the improved quantum molecular dynamics model and its application to fusion reactions near the barrier NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 114,132Sn, 140Ce, 208Pb; calculated binding energies, radii. NUCLEAR REACTIONS 48Ca, 90Zr(40Ca, X), 16O, 208Pb(16O, X), 131I(131I, X), 208Pb(54Cr, X), 230Th(32S, X), 250Fm(12C, X), E not given; calculated static Coulomb barriers. 48Ca(40Ca, X), E(cm)=52, 54, 58, 60 MeV; calculated fusion probability. 48Ca, 48Ti, 90,96Zr(40Ca, X), E(cm)=48-112 MeV; 46Ti(46Ti, X), E(cm)=58-72 MeV; 89Y(32S, X), (34S, X), E(cm)=72-92 MeV; 92Zr(28Si, X), (35Cl, X), E(cm)=65-100 MeV; 64Ni(132Sn, X), E(cm)=140-168 MeV; calculated fusion σ. Improved quantum molecular dynamics model, comparison with data.
doi: 10.1103/PhysRevC.69.034608
2003WA37 High Energy Phys. and Nucl.Phys. (China) 27, 309 (2003) X.-D.Wang, S.-W.Xu, Z.-K.Li, Y.-X.Xie, Z.-Y.Wu, F.-R.Xu, B.Guo, C.-G.Leng, C.-F.Wang, Y.Yu β-Delayed Proton Decay of 93Pd
2003WU06 Chin.Phys.Lett. 20, 1702 (2003) Z.-Y.Wu, F.-R.Xu, E.-G.Zhao, C.-K.Zheng Spherical and Deformed Shell Closures in Superheavy nuclei NUCLEAR STRUCTURE 270Hs, 298Fl, 306Og; calculated energy vs deformation. 250,252,254,256Fm, 252,254,256No, 256Rf, 260Sg, 264Hs; calculated binding energies. 270,288Hs, 298Fl, 304120; calculated single-particle levels. 250,252,254,256Fm, 252,254,256No, 256,262Rf, 260,266Sg, 264,266,270Hs, 270,280Ds, 284,286Cn, 288,290,292,298Fl, 292,294Lv, 292,294Og; calculated deformation, α-decay energy, T1/2. Macroscopic-microscopic model, comparisons with data.
doi: 10.1088/0256-307X/20/10/314
1999GO04 Chin.Phys.Lett. 16, 95 (1999) Q.-B.Gou, Y.-T.Zhu, H.-S.Xu, Z.-Y.Wei, J.Lu, Y.-H.Zhang, Q.Wang, S.-L.Li, Z.-L.Wu Angular Distributions of Intermediate Mass Fragments Emitted in 30 MeV/u 40Ar Induced Reactions NUCLEAR REACTIONS 58,64Ni, 115In(40Ar, X), E=30 MeV/nucleon; measured intermediate mass fragments σ(θ) vs charge; deduced interaction time, other reaction mechanism features.
doi: 10.1088/0256-307X/16/2/007
1997AR02 Phys.Rev. C55, 788 (1997) Preferred Modes of Decay in Nuclear Fragmentation NUCLEAR STRUCTURE 120Sn; 240Pu; calculated partial widths ratio related quantity vs energy following fragmentation; deduced preferred modes of decay related features. Transition state theory.
doi: 10.1103/PhysRevC.55.788
1997XU02 Chin.Phys.Lett. 14, 413 (1997) H.-S.Xu, Y.-T.Zhu, Z.-Y.Wei, J.Lu, Q.Wang, S.-L.Li, Y.-H.Zhang, Y.-X.Xie, Z.-L.Wu, Q.-Z.Zhao, Q.-B.Gou Target Dependence of N/Z Ratio of the Fragments Produced in 30 MeV/u 40Ar Induced Reactions NUCLEAR REACTIONS 58,64Ni, 115In(40Ar, X), E=30 MeV/nucleon; measured intermediate mass fragments charge, mass, energy distributions; deduced target dependence, fragmentation process features.
1990XI02 Phys.Rev. C41, R1355 (1990) L.Xiong, J.Q.Wu, Z.G.Wu, C.M.Ko, J.H.Shi Dielectron Production in Proton-Nucleus Reactions NUCLEAR REACTIONS 9Be(p, e+e-), E=1.05, 2.1, 4.9 GeV; calculated invariant mass spectra.
doi: 10.1103/PhysRevC.41.R1355
1988LI15 Chin.J.Nucl.Phys. 10, 52 (1988) Li Jianwei, Wu Zhihua, Wu Songmao, Song Linggen, Yu Junsheng Measurements of the Cross Sections of the Reactions 115In(n, 2n)114mIn and 113In(n, 2n)112mIn NUCLEAR REACTIONS 113,115In(n, 2n), E=12.7-18.6 MeV; measured isomer production σ(E). 115In(n, 2n), E=15.75 MeV; measured isomer production. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30782. 1987GR23 Phys.Rev.Lett. 59, 1080 (1987) N.Grion, R.Rui, F.M.Rozon, T.Anderl, J.Ernst, D.R.Gill, M.Hanna, J.J.Kraushaar, R.R.Johnson, R.Olszewski, M.E.Sevior, G.Sheffer, G.R.Smith, R.P.Trelle, Z.Wu Measurement of the 16O(π+, π+π-) Reaction at T(π+) = 280 MeV NUCLEAR REACTIONS 16O(π+, π+π-), E=280 MeV; measured σ(E(π+), θ(π+), θ(π-)), σ(E(π+)). Tof.
doi: 10.1103/PhysRevLett.59.1080
1987WA29 Chin.J.Nucl.Phys. 9, 193 (1987) Wang Xiaozhong, Tang Hongqing, Zhang Ying, Xu Jun, Yu Chunying, Yu Zhirong, Wu Zhongming, Bai Xixiang Preequilibrium Effect in the Neutron Angular Distribution of the 40Ar(α, n)43Ca Reaction NUCLEAR REACTIONS, MECPD 40Ar(α, n), E=26 MeV; measured σ(En, θn). Gas target, tof. Exciton model.
1986FA15 Chin.J.Nucl.Phys. 8, 102 (1986) Fan Guoying, Zhu Yongtai, Miao Hobin, Li Songli, Yin Xu, Wang Qi, Feng Enpu, Shen Wenqing, Jin Genming, Zhan Wenlong, Wu Zhongli, Xie Yuonxiang, Song Shizhan, Guo Zhongyan, Qiao Weimin, Cai Jin-Gxiang, Wang Xiaoming Study of α-Particle Emission Mechanism in N + Ni Reaction at 96 MeV NUCLEAR REACTIONS 58Ni(14N, αX), E=96 MeV; measured Eα, αX-coin; deduced α-emission mechanism, shadow effect. ΔE-E telescopes.
1985SO11 Chin.J.Nucl.Phys. 7, 58 (1985) Song Linggen, Wu Songmao, Xu Zhizheng, Yu Junsheng, Wu Zhihua Measurement of Inelastic Cross Sections for the Reaction 87Sr(n, n')87mSr NUCLEAR REACTIONS 87Sr(n, n'), E=0.9-1.8, 3.2-5.7 MeV; measured σ(E), isomer production.Enriched target, activation techniques. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32503. 1984LI26 Chin.J.Nucl.Phys. 6, 250 (1984) Ling Yinsheng, Wu Zumei, Tu Chuanshi Group Theoretical Disscussion about the Energy Spectrum of Odd A Nucleus by Enlarging the Fermions Configuration Space NUCLEAR STRUCTURE 159Tb; calculated levels, B(E2). Group theoretical methods.
1982GU16 Chin.J.Nucl.Phys. 4, 209 (1982) Guo Zhendi, Qian Jinhua, Wu Zhihua, Xu Zhizheng, He Mianhong, Huang Shibin, Yang Fujia The γ Resonant Absorption Experiments of the 9.966 MeV Bound State in 24Mg and the 12.33 MeV Unbound State in 28Si NUCLEAR REACTIONS 24Mg(γ, γ'), E=9.983 MeV; 28Si(γ, γ'), E=12.33 MeV; measured level widths. Resonant absorption method, proton capture reaction gamma source.
1979CH42 Chin.J.Nucl.Phys. 1, 31 (1979) Chu Yung-Tai, Fan Guo-Ying, Wu Zhong-Li, Feng En-Pu, Liang Guo-Zhao, Li Fa-Wei, Jiao Dun-Long, Li Xian-Hui, Guo Ying-Xiang, Xia Guo-Zhong, Su Ying-Quan, Xiao Qin-Pian The Research of Scattering and Transfer Reaction of 12C with 12C NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), (12C, 11C), (12C, 13N), E=49, 60, 72.5 MeV; measured σ(θ). Optical model, zero-range DWBA analyses.
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