NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = Zhang Guishan Found 91 matches. 2024BA01 Nucl.Instrum.Methods Phys.Res. A1058, 168912 (2024) H.Bai, H.Yi, Y.Sun, Z.Cui, Y.Hu, J.Liu, C.Xia, W.Cao, T.Fan, G.Zhang, R.Fan, Y.Li, W.Jiang, Y.Chen, Y.Lv, W.Jia, Z.Zhang, H.Chen, Z.Chen, M.Zhao, C.Feng, S.Liu Measurement of cross section for the 232Th(n, f) reaction using a time projection chamber NUCLEAR REACTIONS 232Th(n, F), E=5 MeV; measured reaction products; deduced σ. Comparison with JENDL-4, ROSFOND-2010, CENDL-3.2, ENDF/B-VIII.0, and BROND-3.1 libraries.
doi: 10.1016/j.nima.2023.168912
2024CH17 Eur.Phys.J. A 60, (2024) Y.Chen, Y.Qiu, Q.Li, Sh.Tang, Y.Yang, Zh.Ren, W.Jiang, R.Fan, H.Yi, R.Liu, J.Tang, H.Jing, Ch.Lan, Y.Li, Zh.Tan, Q.An, J.Bai, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Zh.Chen, Z.Cui, Ch.Feng, K.Gao, X.Gao, M.Gu, Ch.Han, Z.Han, G.He, Y.He, Y.Hong, Y.Hu, H.Huang, X.Huang, H.Jiang, Zh.Jiang, L.Kang, B.Li, Ch.Li, J.Li, X.Li, J.Liu, Sh.Liu, X.Liu, Z.Long, G.Luan, Ch.Ning, M.Niu, B.Qi, J.Ren, X.Ruan, Zh.Song, K.Sun, Zh.Sun, X.Tang, B.Tian, L.Wang, P.Wang, Zh.Wang, Zh.Wen, X.Wu, X.Wu, L.Xie, X.Yang, L.Yu, T.Yu, Y.Yu, G.Zhang, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Zh.Zhang, L.Zhou, Zh.Zhou, K.Zhu Measurement of the neutron flux of CSNS Back-n ES#1 under small collimators from 0.5 eV to 300 MeV NUCLEAR REACTIONS 235U(n, F), 6Li(n, X), E=0.0000005-300 MeV; measured reaction products, En, In, TOF; deduced σ, neutron flux and uncertainties. China Spallation Neutron Source (CSNS).
doi: 10.1140/epja/s10050-024-01272-z
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
2024JI02 At.Data Nucl.Data Tables 157, 101648 (2024) Sh.Jiang, B.Deng, G.Zhang, Y.Wang, Sh.Nie, X.Wang The study of atomic structure parameters for n = 4 - n = 3 transitions in Mg-like ions with 15<Z<30 ATOMIC PHYSICS Z=15-30; calculated energy levels, wavelengths, line strengths, absorption oscillator strengths, and transition probabilities in Mg-like ions with multiconfiguration Dirac–Hartree–Fock (MCDHF) and relativistic configuration interaction (RCI) methods.
doi: 10.1016/j.adt.2024.101648
2024ZH08 Phys.Rev. C 109, 024606 (2024) L.-L.Zhou, J.-J.Cai, L.-Q.Li, Z.-L.Wang, R.Zhu, X.-Y.Zhang, X.-R.Zhang, L.Zhu, G.Zhang, F.-Sh.Zhang Fusion enhancement in the collisions with 44Ca beams and the production of neutron-deficient 245-250Lr isotopes
doi: 10.1103/PhysRevC.109.024606
2023LI22 J.Phys.(London) G50, 045106 (2023) J.Liu, Z.Cui, Y.Hu, H.Bai, Y.Yang, X.Ruan, C.Xia, J.Chen, G.Zhang, Y.M.Gledenov, E.Sansarbayar, G.Khuukhenkhuu, L.Krupa, I.Chuprakov, H.Huang, J.Ren, Q.Fan, Y.Gao, X.Yang 63Cu(n, α)60Co cross sections in the MeV region NUCLEAR REACTIONS 63Cu(n, α), 238U(n, F), E=4.5-10.5 MeV; measured reaction products, Eγ, Iγ; deduced σ using both the direct measurement method and the activation method, preference of ENDF/B-VII.1 over ENDF/B-VIII.0 library. Comparison with TALYS-1.9 calculations. The 4.5 MV Van de Graaff accelerator at Peking University (PKU) and the HI-13 tandem accelerator at the China Institute of Atomic Energy (CIAE).
doi: 10.1088/1361-6471/acb960
2023LI24 Phys.Lett. B 842, 137985 (2023) J.Liu, Z.Cui, Y.Hu, H.Bai, Z.Chen, C.Xia, T.Fan, J.Chen, G.Zhang, X.Ruan, H.Huang, J.Ren, H.Chen 12C(n, n, + 3α) and 12C(n, α0)9Be cross sections in the MeV neutron energy region NUCLEAR REACTIONS 12C(n, n3α), (α, α), E=9.5-14.67 MeV; measured reaction products; deduced σ. Comparison with R-matrix RAC code analysis, JEFF-3.1/A library. The HI-13 tandem accelerator and Cockcroft-Walton generator at China Institute of Atomic Energy (CIAE).
doi: 10.1016/j.physletb.2023.137985
2023LI30 Eur.Phys.J. A 59, 106 (2023) J.Liu, H.Bai, H.Jiang, G.Zhang Ratios of the cross sections for the 10B(n, α)7Li reaction to the 6Li(n, t)4He reaction NUCLEAR REACTIONS 10B(n, α), 6Li(n, t), E=0.000001-1 MeV; analyzed available data; deduced σ(θ), σ ratios. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries.
doi: 10.1140/epja/s10050-023-00992-y
2023WA17 Phys.Lett. B 843, 138034 (2023) W.Wang, C.Lv, X.Zhang, C.Fu, B.Guo, H.Cai, L.Chen, L.Cheng, C.He, J.He, L.Li, X.Xi, D.Yuan, G.Zhang, W.Sun, Z.Zhang, J.Zhang, Y.Ma First measurement of the 7Li(D, n) astrophysical S-factor in laser-induced full plasma NUCLEAR REACTIONS 7Li(d, n), E(cm)<0.7 MeV; measured reaction products, En, In; deduced neutron yields, neutron groups, astrophysical S-factor. The Shenguang-II laser facility, the National Laboratory on High Power Lasers and Physics, Shanghai, China.
doi: 10.1016/j.physletb.2023.138034
2023WA35 Eur.Phys.J. A 59, 224 (2023) J.Wang, J.Ren, W.Jiang, X.Ruan, Q.Sun, J.Hu, B.Jiang, J.Bao, Q.Zhang, G.Luan, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, J.Bai, P.Cao, Q.Chen, Y.Chen, Z.Chen, Z.Cui, A.Fan, R.Fan, C.Feng, F.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, Y.Hu, W.Jia, H.Jiang, Z.Jiang, Z.Jin, L.Kang, B.Li, C.Li, G.Li, J.Li, Q.Li, Y.Li, J.Liu, R.Liu, S.Liu, C.Ning, B.Qi, Z.Ren, Z.Song, K.Sun, Z.Tan, J.Tang, S.Tang, L.Wang, P.Wang, Z.Wang, Z.Wen, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, Y.Yu, G.Zhang, L.Zhang, M.Zhang, X.Zhang, Y.Zhang, Y.Zhang, Z.Zhang, M.Zhao, L.Zhou, K.Zhu, J.Zhang Determination of the 232Th(n, γ) cross section from 10 to 200 keV at the Back-n facility at CSNS NUCLEAR REACTIONS 232Th, 197Au(n, γ), E=10-200 keV; measured reaction products, En, In, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VIII.0, CENDL-3.2, JENDL-5 libraries and TALYS 1.96 calculations. The back-streaming white neutron beam-line (Back-n) of China Spallation Neutron Source (CSNS).
doi: 10.1140/epja/s10050-023-01126-0
2023ZH01 At.Data Nucl.Data Tables 149, 101547 (2023) G.Zhang, B.Deng, J.Yang, K.Tang, B.Meng, X.Zhang Wavelengths, transition rates, weight oscillator strengths and line strengths for He-like to Ne-like cobalt ions ATOMIC PHYSICS Co; calculated wavelengths, transition rates, absorption oscillator strengths, and line strengths for the 2s-3p, 2p-3s, and 2p-3d electric dipole (E1) transitions in He-like to Ne-like cobalt ions using the multi-configuration Dirac–Hartree–Fock (MCDHF) and Relativistic Configuration Interaction (RCI) methods. Comparison with available data.
doi: 10.1016/j.adt.2022.101547
2022FE02 Phys.Rev.Lett. 128, O52501 (2022) J.Feng, W.Wang, C.Fu, L.Chen, J.Tan, Y.Li, J.Wang, Y.Li, G.Zhang, Y.Ma, J.Zhang Femtosecond Pumping of Nuclear Isomeric States by the Coulomb Collision of Ions with Quivering Electrons RADIOACTIVITY 83Kr(IT); measured decay products, X-rays; deduced T1/2. Femtosecond pumping of nuclear isomeric states by the Coulomb excitation of ions with the quivering electrons induced by laser fields.
doi: 10.1103/PhysRevLett.128.052501
2022GL02 Eur.Phys.J. A 58, 86 (2022) Yu.M.Gledenov, Z.Cui, J.Liu, H.Jiang, Y.Hu, H.Bai, J.Chen, G.Zhang, E.Sansarbayar, G.Khuukhenkhuu, L.Krupa, I.Chuprakov, Y.Han, X.Ruan, H.Huang, J.Ren Cross section of the 232Th(n, f) reaction in the MeV neutron energy region NUCLEAR REACTIONS 232Th(n, F), E=1.5-12 MeV; measured fission products; deduced σ. Comparison with ENDF/B-VIII.0, JEFF-3.3, FENDL-3.2, ROSFOND 2010, CENDL-3.2, BROND-3.1, JENDL-4.0 libraries, TALYS-1.9 code calculations. Peking University (PKU) and China Institute of Atomic Energy (CIAE), using the 4.5 MV Van de Graaff accelerator and the HI-13 tandem accelerator, respectively.
doi: 10.1140/epja/s10050-022-00716-8
2022JI04 Chin.Phys.C 46, 024001 (2022) H.Jiang, Z.Cui, Y.Hu, J.Liu, H.Bai, J.Chen, G.Zhang, Y.M.Gledenov, E.Sansarbayar, G.Khuukhenkhuu, L.Krupa, I.Chuprakov, X.Ruan, H.Huang, J.Ren, Q.Fan Cross-section measurements for the 58, 60, 61Ni(n, α)55, 57, 58Fe reactions at 8.50, 9.50 and 10.50 MeV neutron energies NUCLEAR REACTIONS 58,60,61Ni(n, α), E=8.50, 9.50, 10.50 MeV; measured reaction products, En, In; deduced σ and uncertainties. Comparison with TALYS-1.9 calculations, available data. The HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE).
doi: 10.1088/1674-1137/ac3412
2022LI03 J.Phys.(London) G49, 25106 (2022) J.Li, G.Zhang, X.Zhang, Y.Zhang, Z.Liu and F.-S.Zhang Production of unknown neutron-rich transuranium isotopes 245-249Np, 248-251Pu, 248-254Am, and 252-254Cm in multinucleon transfer reactions NUCLEAR REACTIONS 238U, 248Cm(238U, X), E(cm)=800 MeV; 249Bk(238U, X), E not given; analyzed available data. 245,246,247,248Np, 248,249,250,251Pu, 248,249,250,251Am, 252,253,254,255Cm; calculated production σ in multinucleon transfer (MNT) reactions using the dinuclear system model with GEMINI code.
doi: 10.1088/1361-6471/ac44ad
2022LI39 Phys.Rev. C 106, 014606 (2022) J.-J.Li, N.Tang, Y.-H.Zhang, X.-R.Zhang, G.Zhang, F.-S.Zhang Theoretical study on the production of neutron-rich transuranium nuclei with radioactive beams in multinucleon transfer reactions NUCLEAR REACTIONS 248Cm(136Xe, X)229Pu/230Pu/231Pu/232Pu/233Pu/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/254Pu/233Am/234Am/235Am/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/259Cf/260Cf/261Cf/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es/261Es/262Es , E(cm)=533 MeV; 249Cf(136Xe, X)229Pu/230Pu/231Pu/232Pu/233Pu/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/230Am/231Am/232Am/233Am/234Am/235Am/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/233Cm/234Cm/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/236Bk/237Bk/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/237Cf/238Cf/239Cf/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/259Cf/260Cf/261Cf/240Es/241Es/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es, E(cm)=526 MeV; 238U(92Kr, X)/229Np/230Np/231Np/232Np/233Np/234Np/235Np/236Np/237Np/238Np/239Np/240Np/241Np/242Np/243Np/244Np/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf, E(cm)=357 MeV; 238U(132Sn, X), 230Np/231Np/232Np/233Np/234Np/235Np/236Np/237Np/238Np/239Np/240Np/241Np/242Np/243Np/244Np/245Np/246Np/247Np/248Np/249Np/250Np/251Np/252Np/253Np/254Np/255Np/232Pu/233Pu/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/254Pu/255Pu/256Pu/257Pu/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/256Am/257Am/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/259Cm/260Cm/261Cm/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/261Bk/262Bk/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cm/258Cm/259Cm/260Cm/261Cm/262Cm/263Cm/264Cm, E(cm)=478, 521, 564 MeV; 238U(144Xe, X), 236Np/237Np/238Np/239Np/240Np/241Np/242Np/243Np/244Np//245Np/246Np/247Np/248Np/249Np/250Np/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/265Bk/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cm/258Cm/259Cm/260Cm/261Cm/262Cm, E(cm)=511 MeV; calculated σ of the isotopes production, driving potential during the transfer of nucleons. Dinuclear system model (DNS) calculations performed with GEMINI++ code. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.014606
2022LI45 Phys.Rev. C 106, 024601 (2022) Production of unknown Fl isotopes in proton evaporation channels within the dinuclear system model NUCLEAR REACTIONS 243Am(48Ca, n), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E(cm)=190-225 MeV; 248Cm(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E(cm)=195-220 MeV;249Bk(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E(cm)=195-225 MeV;249Cf(48Ca, 3n), E(cm)=205-215 MeV;244Am(48Ca, np), (48Ca, 2np), (48Ca, 3np), (48Ca, 4np), E*=25-70 MeV; 255Es(36S, np), (36S, 2np), (36S, 3np), (36S, 4np), E*=25-70 MeV;239Pa(54Cr, np), (54Cr, 2np), (54Cr, 3np), (54Cr, 4np), E*=25-70 MeV; calculated evaporation residues σ(E). 255Es(36S, X), (34S, X), (36S, X), E*=20-70 MeV; calculated capture σ(E), driving potential as a function of the mass asymmetry, fusion probability, fission barrier. 255Es(36S, np), (36S, 2np), (36S, 3np), (36S, 4np), (36S, np), (34S, 2np), (34S, 3np), (34S, 4np), (32S, np), (32S, 2np), (32S, 3np), (32S, 4np)E*=25-70 MeV; calculated survival probability. 255Es(36S, np)289Fl, E*=37.2 MeV;255Es(36S, 2np)288Fl, E*=38.8 MeV; 255Es(36S, 3np)287Fl, E*=45.5 MeV;255Es(36S, 4np)286Fl, E*=53.8 MeV;243Am(48Ca, np)289Fl, E*=30.9 MeV;243Am(48Ca, 2np)288Fl, E*=37.3 MeV;243Am(48Ca, 3np)287Fl, E*=45.8 MeV;243Am(48Ca, 4np)286Fl, E*=55.1 MeV;239Pa(54Cr, np)291Fl, E*=33.6 MeV; 239Pa(54Cr, 2np)290Fl, E*=37.2 MeV;239Pa(54Cr, 3np)288Fl, E*=4.1 MeV;239Pa(54Cr, 4np)288Fl, E*=53.4 MeV;244Am(48Ca, np)290Fl, E*=30.9 MeV;244Am(48Ca, 2np)289Fl, E*=38.4 MeV;244Am(48Ca, 3np)288Fl, E*=45.8 MeV;244Am(48Ca, 4np)287Fl, E*=55.4 MeV; calculated production σ. Dinuclear system model. Comparison to available experimental data.
doi: 10.1103/PhysRevC.106.024601
2022LI60 Phys.Rev. C 106, 054610 (2022) J.Liu, H.jiang, Z.Cui, Y.Hu, H.Bai, J.Chen, G.Zhang, Yu.M.Gledenov, E.Sansarbayar, G.Khuukhenkhuu, N.Battsooj, L.Krupa, I.Chuprakov, X.Ruan, H.Huang, J.Ren, Q.Fan Cross sections of the 40Ca(n α0)37Ar and 40Ca(n α)37Ar reactions in the 8.50-9.50 MeV neutron energy range NUCLEAR REACTIONS 40Ca(n, α), E=8.5-9.5 MeV; measured En, In, Eα, Iα; deduced total and (n, α0) σ(E), σ forward to backward ratio, compound, preequilibrium and direct contributions. Comparison to other experimental results, evaluated data (ENDF/B-VIII.0, JENDL-5, JEFF-3.3, CENDL-3.2, ROSFOND-2010, TENDL-2019) and TALYS-1.9 calculations. Twin gridded ionization chamber (GIC) used as charged particle detector, and the EJ-309 liquid scintillator as the neutron detector. Monoenergetic neutron beam from 2H(d, n) at HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE).
doi: 10.1103/PhysRevC.106.054610
2022ZH42 Phys.Rev. C 106, 014625 (2022) Y.-H.Zhang, G.Zhang, J.-J.Li, Z.Liu, A.V.Yeremin, F.-S.Zhang Production cross sections of 243-248No isotopes in fusion reactions NUCLEAR REACTIONS 208Pb(48Ca, X), E(cm)=165-220 MeV; 238U(20Ne, X), E(cm)=95-14 MeV; 242Pu(16O, X), E(cm)=80-130 MeV; 232Th(26Mg, X), E(cm)=110-160 MeV; 208Pb(48Ca, 2n), E(cm)=170-245 MeV; 208Pb(48Ca, 3n), E(cm)=180-258 MeV; 208Pb(48Ca, 4n), E(cm)=190-275 MeV; 208Pb(48Ca, 5n), E(cm)=200-280 MeV; 208Pb(40Ca, 2n), E(cm)=160-190 MeV; 208Pb(40Ca, 3n), E(cm)=170-200 MeV; 208Pb(40Ca, 4n), E(cm)=175-215 MeV; 208Pb(40Ca, 5n), E(cm)=200-220 MeV; 208Pb(44Ca, 2n), E(cm)=170-200 MeV; 208Pb(44Ca, 3n), E(cm)=175-210 MeV; 208Pb(44Ca, 4n), E(cm)=175-215 MeV; 208Pb(44Ca, 5n), E(cm)=180-225 MeV; 233U(20Ne, 4n), E(cm)=90-135 MeV; 233U(20Ne, 5n), E(cm)=105-140 MeV; 233U(20Ne, n), E(cm)=115-140 MeV; 235U(20Ne, 4n), E(cm)=90-135 MeV; 235U(20Ne, 5n), E(cm)=100-140 MeV; 235U(20Ne, n), E(cm)=110-140 MeV; 238U(20Ne, 4n), E(cm)=90-135 MeV; 238U(20Ne, 5n), E(cm)=95-140 MeV; 238U(20Ne, n), E(cm)=105-140 MeV; calculated σ(E), time evolution of binding energies and root-mean-square charge radii for 48Ca and 208Pb, excitation functions, static barrier in collision, evolution density profile for heads-on collision, production σ for new isotopes - 243,244,245,246,247,248No.Improved quantum molecular dynamical model (ImQMD) incorporated with a statistical model and the dinuclear system (DNS) model calculations. Comparison to available experimental data.
doi: 10.1103/PhysRevC.106.014625
2022ZH54 J.Phys.(London) G49, 095104 (2022) X.-r.Zhang, G.Zhang, J.-j.Li, Z.Liu, Y.-x.Yang, F.-s.Zhang Production mechanism and prediction cross sections of unknown neutron-rich 263-265, 267-269Lr isotopes in multinucleon transfer reactions based on the dinuclear system model NUCLEAR REACTIONS 235U(40Ar, X), E(cm)=184.6 MeV; 249Bk(130Te, X)263Lr/264Lr/265Lr/267Lr/268Lr/269Lr, E(cm)=526.7 MeV; analyzed available data; calculated production σ.
doi: 10.1088/1361-6471/ac81df
2022ZH71 Phys.Rev. C 106, 064602 (2022) G.Zhang, E.Sansarbayar, Yu.M.Gledenov, G.Khuukhenkhuu, L.Krupa, N.S.Gustova, M.G.Voronyuk, I.Chuprakov, N.Battsooj, I.Wilhelm, M.Solar, R.Sykora, Z.Kohout, J.Liu, Y.Hu, Z.Cui Cross sections of the 91Zr(n, α)88Sr reaction in the 3.9-5.3 MeV neutron energy region NUCLEAR REACTIONS 91Zr(n, α), E=3.9, 4.3, 5.0, 5.3 MeV; measured Eα, Iα, In; deduced total σ(E) and exclusive (n, α0) σ(E), α-cluster preformation factor. Comparison to TALYS-1.9 calculations and evaluated data (ENDF/B-VIII.0, JENDL-5.0, JEFF-3.3, CENDL-3.2, BROND, TENDL-2019). Twin gridded ionization chamber (GIC) with a common cathode, supplemented by a fission chamber and coupled with 3He counters at EG-5 Van de Graaff accelerator of the Frank Laboratory of Neutron Physics (JINR).
doi: 10.1103/PhysRevC.106.064602
2021GO23 Nucl.Instrum.Methods Phys.Res. A1015, 165753 (2021) A.Goasduff, D.Mengoni, F.Recchia, J.J.Valiente-Dobon, R.Menegazzo, G.Benzoni, D.Barrientos, M.Bellato, N.Bez, M.Biasotto, N.Blasi, C.Boiano, A.Boso, S.Bottoni, A.Bracco, S.Brambilla, D.Brugnara, F.Camera, S.Capra, A.Capsoni, P.Cocconi, S.Coelli, M.L.Cortes, F.C.L.Crespi, G.de Angelis, F.J.Egea, C.Fanin, S.Fantinel, A.Gadea, E.R.Gamba, A.Gambalonga, C.Gesmundo, G.Gosta, A.Gottardo, A.Gozzelino, E.T.Gregor, M.Gulmini, J.Ha, K.Hadynska-Klek, A.Illana, R.Isocrate, G.Jaworski, P.R.John, S.M.Lenzi, S.Leoni, S.Lunardi, M.Magalini, N.Marchini, B.Million, V.Modamio, A.Nannini, D.R.Napoli, G.Pasqualato, J.Pellumaj, R.M.Perez-Vidal, S.Pigliapoco, M.Polettini, C.Porzio, A.Pullia, L.Ramina, G.Rampazzo, M.Rampazzo, M.Rebeschini, K.Rezynkina, M.Rocchini, M.Romanato, D.Rosso, A.Saltarelli, M.Scarcioffolo, M.Siciliano, D.A.Testov, D.Tomasella, F.Tomasi, N.Toniolo, C.A.Ur, S.Ventura, F.Veronese, E.Viscione, V.Volpe, O.Wieland, I.Zanon, S.Ziliani, G.Zhang, D.Bazzacco The GALILEO γ-ray array at the Legnaro National Laboratories
doi: 10.1016/j.nima.2021.165753
2021HU08 Chin.Phys.C 45, 024003 (2021) M.Huang, A.Bonasera, S.Zhang, H.Zheng, D.X.Wang, J.C.Wang, N.Song, X.Tang, L.Lu, G.Zhang, Z.Kohley, M.R.D.Rodrigues, Y.G.Ma, S.J.Yennello Four α correlations in nuclear fragmentation: a game of resonances NUCLEAR REACTIONS 70Zn(70Zn, X), 64Zn(64Zn, X), 64Ni(64Ni, X), E=35 MeV/nucleon; measured reaction products, Eα, Iα. 4He; deduced yields, correlation functions, strong resonances among α-particles.
doi: 10.1088/1674-1137/abce52
2021JI16 Symmetry 13, 2278 (2021) H.Jian, Y.Gao, F.Dai, J.Liu, X.Xu, C.Yuan, K.Kaneko, Y.Sun, P.Liang, G.Shi, L.Sun, L.Xayavong, C.Lin, J.Lee, Z.Li, Y.Yang, P.Li, R.Fan, S.Zha, H.Zhu, J.Li, Q.Gao, Z.Zhang, R.Chen, J.Wang, D.Wang, H.Wu, K.Wang, Y.Lam, F.Duan, P.Ma, Z.Gao, Q.Hu, Z.Bai, J.Ma, J.Wang, F.Zhong, C.Wu, D.Luo, Y.Jiang, Y.Liu, D.Hou, R.Li, N.Ma, W.Ma, G.Yu, D.Patel, S.Jin, Y.Wang, Y.Yu, Q.Zhou, P.Wang, L.Hu, X.Wang, H.L.Zang, Q.Zhao, L.Yang, P.Wen, F.Yang, H.Jia, G.Zhang, M.Pan, X.Wang, H.Sun, M.Wang, Z.Hu, X.Zhou, Y.Zhang, H.Xu, M.Liu, H.-J.Ong, W.Yang β-Delayed γ Emissions of 26P and Its Mirror Asymmetry RADIOACTIVITY 26P(β+), (EC) [from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation using RIBBL1 at HRIBF, Lanzhou facility]; measured Eγ, Iγ, βγ-coin, T1/2 of 26P decay. 26Si; deduced levels, J, π, β++ϵ feedings, logft, mirror asymmetry parameter from comparison with the ϵ decay of mirror nucleus 26Na to 26Mg, mirror-energy differences (MEDs), and halo structure in 26P. Comparison with shell-model calculations. NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P/27S, E=80.6 MeV/nucleon; measured reaction products, particle-identification (PID) plot of ΔE vs TOF for the ions separated using RIBBL1 separator at HRIBF, Lanzhou facility.
doi: 10.3390/sym13122278
2021LI35 Eur.Phys.J. A 57, 232 (2021); Erratum Eur.Phys.J. A 57, 252 (2021) X.Liu, Y.Yang, R.Liu, Z.Wen, J.Wen, Z.Han, Y.Chen, H.Jing, H.Yi, J.Bao, Z.Ren, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the neutron total cross sections of aluminum at the back-n white neutron source of CSNS NUCLEAR REACTIONS 27Al(n, X), E<20 MeV; measured reaction products, En, In; deduced neutron transmission, total σ and uncertainties. Comparison withENDF/B-VIII.0, JEFF-3.3 and CENDL-3.2 library evaluations, EXFOR compilations. Spallation Neutron Source Science Center.
doi: 10.1140/epja/s10050-021-00513-9
2021RE01 Nucl.Instrum.Methods Phys.Res. A985, 164703 (2021) J.Ren, X.Ruan, W.Jiang, J.Bao, G.Luan, Q.Zhang, H.Huang, Y.Nie, Z.Ge, Q.An, H.Bai, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, Z.Cui, R.Fan, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, Q.Mu, C.Ning, B.Qi, Z.Ren, Y.Song, Z.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, L.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Background study for (n, γ) cross section measurements with C6D6 detectors at CSNS Back-n NUCLEAR REACTIONS 197Au, Pb, C, 181Ta, 59Co(n, γ), E<400 MeV; measured reaction products, Eγ, Iγ; deduced σ.
doi: 10.1016/j.nima.2020.164703
2021SA47 Phys.Rev. C 104, 044620 (2021); Erratum Phys.Rev. C 105, 049902 (2022) E.Sansarbayar, Yu.M.Gledenov, I.Chuprakov, G.Khuukhenkhuu, G.S.Ahmadov, L.Krupa, G.Zhang, H.Jiang, Z.Cui, Y.Hu, J.Liu, N.Battsooj, I.Wilhelm, M.Solar, R.Sykora, Z.Kohout Cross sections for the 35Cl(n, α)32P reaction in the 3.3-5.3 MeV neutron energy region NUCLEAR REACTIONS 35Cl(n, α)32P, E=3.3, 3.9, 4.3, 4.5, 4.8, 5.0, 5.1, 5.3 MeV; measured Eα, Iα, relative and absolute neutron fluxes, σ(E) using gridded ionization chamber (GIC) at EG-5 Van de Graaff accelerator EG-5 of FLNP-JINR; deduced α cluster preformation factor as function of incident neutron energy. 238U(n, F), E=5.0 MeV; measured fission fragments and absolute neutron flux. Comparison with theoretical calculations using TALYS-1.9 code, and with evaluated data in ENDF/B-VIII.0, FENDL-3.1c, JEFF-3.3, and BROND-3.1.
doi: 10.1103/PhysRevC.104.044620
2021ZH16 Phys.Rev. C 103, 024608 (2021) X.-R.Zhang, G.Zhang, J.-J.Li, S.H.Cheng, Z.Liu, F.-S.Zhang Effects of nucleus orientation on transfer process and production of unknown neutron-rich isotopes with Z = 62-75 in 204Hg + 232Th based on the dinuclear system model NUCLEAR REACTIONS 166Er(86Kr, X), E(cm)=464 MeV; calculated mass and charge distributions of total kinetic energy (TKE) of the primary binary fragments. 232Th(204Hg, X)168Sm/169Sm/170Eu/171Eu/172Eu/172Gd/173Gd/174Gd/175Gd/175Tb/176Tb/177Tb/177Dy/178Dy/179Dy/180Dy/179Ho/180Ho/181Ho/182Ho/181Er/182Er/183Er/184Er/185Er/182Tm/183Tm/184Tm/185Tm/186Tm/187Tm/186Yb/187Yb/188Yb/189Yb/190Yb/189Lu/190Lu/191Lu/192Lu/193Lu/191Hf/192Hf/193Hf/194Hf/195Hf/195Ta/196Ta/197Ta/198W/199W/200Re/201Re/202Re, E(cm)=678.1 MeV; calculated potential energies for the tip-to-tip and side-to-side configurations, production σ. Dinuclear system (DNS) model. Comparison with available experimental data.
doi: 10.1103/PhysRevC.103.024608
2020BA03 Chin.Phys.C 44, 014003 (2020) H.Bai, R.Fan, H.Jiang, Z.Cui, Y.Hu, G.Zhang, Z.Chen, W.Jiang, H.Yi, J.Tang, L.Zhou, Q.An, J.Bao, P.Cao, Q.Chen, Y.Chen, P.Cheng, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the differential cross sections and angle-integrated cross sections of the 6Li(n, t)4He reaction from 1.0 eV to 3.0 MeV at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), E=0.000001-3 MeV; measured reaction products; deduced σ. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries, experimental data.
doi: 10.1088/1674-1137/44/1/014003
2020GE06 Chin.Phys.C 44, 104102 (2020) Z.Ge, G.Zhang, S.Cheng, Yu.S.Tsyganov, F.-S.Zhang Calculations of the α-decay properties of Z = 120, 122, 124, 126 isotopes RADIOACTIVITY 285,286,287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294Og, 287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339120, 294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339122, 300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339124, 306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339126(α); calculated Q-values, T1/2 using the generalized liquid drop model (GLDM), Royer's formula, and universal decay law (UDL). Comparison with available data.
doi: 10.1088/1674-1137/abab00
2020JI06 Nucl.Instrum.Methods Phys.Res. A973, 164126 (2020) W.Jiang, H.Bai, H.Jiang, H.Yi, R.Fan, G.Zhang, J.Tang, Z.Sun, C.Ning, K.Sun, K.Gao, Z.Cui, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Y.Song, Z.Song, H.Sun, X.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Application of a silicon detector array in (n, lcp) reaction cross-section measurements at the CSNS Back-n white neutron source NUCLEAR REACTIONS 6Li(n, t), 10B(n, α), E<1 MeV; measured reaction products, En, In; deduced σ. Comparison with experimental data, ENDF/B-VIII.0, JEFF-3.3, ROSFOND evaluated libraries.
doi: 10.1016/j.nima.2020.164126
2020JI10 Chin.Phys.C 44, 114102 (2020) H.Jiang, Z.Cui, Y.Hu, J.Liu, J.Chen, G.Zhang, Yu.M.Gledenov, E.Sansarbayar, G.Khuukhenkhuu, L.Krupa, I.Chuprakov Cross-section measurements for 58, 60, 61Ni(n, α)55, 57, 58Fe reactions in the 4.50 - 5.50 MeV neutron energy region NUCLEAR REACTIONS 58,60,61Ni(n, α), E4.5-5.5 MeV; measured reaction products, En, In, Eα, Iα; deduced σ. Comparison with available data, TALYS-1.9 calculations.
doi: 10.1088/1674-1137/abadf2
2020LI33 Nucl.Instrum.Methods Phys.Res. A980, 164506 (2020) Q.Li, H.Jing, B.Zhou, C.Ning, J.Tang, J.Ren, H.Yi, X.Zhu, L.Zhang, W.Jiang, R.Fan, J.Bao, C.Feng, X.Ruan, Y.Chen, L.Zhou, Y.Li, Z.Tan, Y.Chen, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, M.Gu, F.Guo, C.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, L.Kang, M.Kang, B.Li, L.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Y.Ma, B.Qi, Z.Song, H.Sun, X.Sun, Z.Sun, H.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Neutron and γ background measurements of the experimental halls at the CSNS back-streaming white neutron source
doi: 10.1016/j.nima.2020.164506
2020RE11 Phys.Rev. C 102, 034604 (2020) Z.Ren, Y.Yang, J.Wen, H.Guo, Z.Wen, R.Liu, Z.Han, W.Sun, X.Liu, Q.Chen, T.Ye, Q.An, H.Bai, J.Bao, P.Cao, Y.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the 236U(n, f) cross section for neutron energies from 0.4 MeV to 40 MeV from the back-streaming white neutron beam at the China Spallation Neutron Source NUCLEAR REACTIONS 235,236U(n, F), E AP 0.4-40 MeV beam from the China Spallation Neutron Source (CSNS)-Back-streaming white neutron source (WNS); measured fission fragments, energy spectra, time-of-flight using Fast Ionization Chamber Spectrometer; deduced 236U(n, F)/235U(n, F) cross section ratios. Comparison with theoretical calculation using the UNF code, and with evaluated data in JENDL-4.0, CENDL-3.1, and ENDF/B-VIII.0 libraries.
doi: 10.1103/PhysRevC.102.034604
2020WE04 Ann.Nucl.Energy 140, 107301 (2020) J.Wen, Y.Yang, Z.Wen, R.Liu, X.Liu, Z.Han, Q.Chen, Z.Ren, Q.An, H.Bai, J.Bao, P.Cao, Y.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, C.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, H.Jing, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, S.Liu, G.Luan, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, Q.Wu, X.Wu, X.Wu, L.Xie, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurement of the U-238/U-235 fission cross section ratio at CSNS - Back-in WNS NUCLEAR REACTIONS 235,238U(n, F), E=1-20 MeV; measured reaction products, fission fragments, Eγ, Iγ; deduced neutron resonances, σ. Comparison with ENDF/B-VIII.0 library evaluations.
doi: 10.1016/j.anucene.2019.107301
2020ZH18 Bull.Rus.Acad.Sci.Phys. 84, 485 (2020) G.Zhang, C.A.T.Sokhna, F.S.Zhang The Production of the Isotopes with Z = 98-106 in the Multinucleon Transfer Reaction 238U + 251Cf
doi: 10.3103/S106287382004036X
2020ZH22 Int.J.Mod.Phys. E29, 2030004 (2020) L.Zhu, C.Li, C.-C.Guo, J.Su, P.W.Wen, G.Zhang, F.-S.Zhang Theoretical progress on production of isotopes in the multinucleon transfer process NUCLEAR REACTIONS 238U(64Ni, X), E(cm)=307.5 MeV; 208Pb(124Xe, X), E(cm)=50 MeV; 186W(160Gd, X), E=503 MeV; calculated transfer σ for production of neutron-rich transuranium nuclei.
doi: 10.1142/S0218301320300040
2020ZH28 Phys.Rev. C 102, 024617 (2020) G.Zhang, J.-J.Li, X.-R.Zhang, B.Li, C.A.T.Sokhna, C.Wang, Z.Liu, F.-S.Zhang Role of the quasifission yields in the multinucleon transfer reactions of 136Xe + 208Pb NUCLEAR REACTIONS 208Pb(136Xe, X), (136Xe, F), E(cm)=526 MeV; calculated mass distributions with and without the quasifission yields, σ(A) as function of the angular momentum, production σ of Hg, Pb, and Po isotopes contributed from quasifission yields, quasifission yields and excitation energies of 202Hg and 208Hg, isotopic distribution σ(Z) of Hg, Pb and Po isotopes. Dinuclear system (DNS) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.024617
2019BA08 Phys.Rev. C 99, 024619 (2019) H.Bai, H.Jiang, Y.Lu, Z.Cui, J.Chen, G.Zhang, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu, Xi.Ruan, H.Huang, J.Ren, Q.Fan 56, 54Fe (n, α) 53, 51Cr cross sections in the MeV region NUCLEAR REACTIONS 54,56Fe(n, α), E=5.5, 7.7, 8.5, 9.5, 10.5 MeV; measured α-particles, E(n), I(n), and σ(E) using twin-gridded ionization chamber for charged particle detection and 238U fission chamber for neutron fluence at the 4.5-MV Van de Graaff accelerator of Peking University (PKU). Comparison with theoretical calculations using TALYS-1.8 code, and evaluated data in ENDF-B/VII.1, JEFF-3.3, JENDL-4.0, and several other libraries.
doi: 10.1103/PhysRevC.99.024619
2019BA33 Appl.Radiat.Isot. 152, 180 (2019) H.Bai, H.Jiang, Y.Lu, Z.Cui, J.Chen, G.Zhang Determination of the number of 238U target nuclei and simulation of the neutron induced fission fragment energy spectrum RADIOACTIVITY 238U(α); measured decay products, Eα, Iα; deduced energy spectrum of neutron induced fission fragments. Comparison with Monte Carlo calculations.
doi: 10.1016/j.apradiso.2019.06.026
2019BA47 Eur.Phys.J. A 55, 219 (2019) H.Bai, Z.Wang, H.Jiang, Z.Cui, Y.Hu, J.Chen, G.Zhang, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu Cross sections of the 10B(n, α)7Li two-body and 10B(n, t2α) three-body reactions at 4.0, 4.5 and 5.0 MeV
doi: 10.1140/epja/i2019-12908-x
2019CH37 Eur.Phys.J. A 55, 115 (2019), Erratum Eur.Phys.J. A 55, 145 (2019) Y.Chen, G.Luan, J.Bao, H.Jing, L.Zhang, Q.An, H.Bai, P.Cao, Q.Chen, P.Cheng, Z.Cui, R.Fan, C.Feng, M.Gu, F.Guo, Ch.Han, Z.Han, G.He, Y.He, Y.He, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, H.Jiang, W.Jiang, L.Kang, M.Kang, B.Li, L.Li, Q.Li, X.Li, Y.Li, Y.Li, R.Liu, S.Liu, X.Liu, Y.Ma, C.Ning, B.Qi, J.Ren, X.Ruan, Z.Song, H.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, J.Tang, P.Wang, Q.Wang, T.Wang, Y.Wang, Z.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, H.Yi, L.Yu, T.Yu, Y.Yu, G.Zhang, J.Zhang, L.Zhang, Q.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Neutron energy spectrum measurement of the Back-n white neutron source at CSNS
doi: 10.1140/epja/i2019-12808-1
2019GE08 Eur.Phys.J. A 55, 166 (2019) Z.Ge, G.Zhang, S.Cheng, Y.Li, N.Su, W.Guo, Yu.S.Tsyganov, F.-S.Zhang Theoretical predictions for α-decay properties of 283-339Og using a shell-effect induced generalized liquid-drop model RADIOACTIVITY Sg, Bh, Hs, Mt, Ds, Rg, Cn, Nh, Fl, Mc, Lv, Ts, Og(α) [all known isotopes]; compiled Qα, T1/2 available experimental values and calculations using Royer's formula, Universal Decay Law (UDL), Generalized Liquid-Drop Model (GLDM) with and without shell correction; calculated 283-339Og α-particle preformation factor.
doi: 10.1140/epja/i2019-12864-5
2019JI07 Chin.Phys.C 43, 124002 (2019) H.Jiang, W.Jiang, H.Bai, Z.Cui, G.Zhang, R.Fan, H.Yi, C.Ning, L.Zhou, J.Tang, Q.An, J.Bao, Y.Bao, P.Cao, H.Chen, Q.Chen, Y.Chen, Y.Chen, Z.Chen, C.Feng, K.Gao, M.Gu, C.Han, Z.Han, G.He, Y.He, Y.Hong, H.Huang, W.Huang, X.Huang, X.Ji, X.Ji, Z.Jiang, H.Jing, L.Kang, M.Kang, B.Li, C.Li, J.Li, L.Li, Q.Li, X.Li, Y.Li, R.Liu, S.Liu, X.Liu, G.Luan, Q.Mu, B.Qi, J.Ren, Z.Ren, X.Ruan, Z.Song, Y.Song, H.Sun, K.Sun, X.Sun, Z.Sun, Z.Tan, H.Tang, X.Tang, B.Tian, L.Wang, P.Wang, Q.Wang, T.Wang, Z.Wang, J.Wen, Z.Wen, Q.Wu, X.Wu, X.Wu, L.Xie, Y.Yang, L.Yu, T.Yu, Y.Yu, L.Zhang, Q.Zhang, X.Zhang, Y.Zhang, Z.Zhang, Y.Zhao, L.Zhou, Z.Zhou, D.Zhu, K.Zhu, P.Zhu Measurements of differential and angle-integrated cross sections for the 10B(n, α)7Li reaction in the neutron energy range from 1.0 eV to 2.5 MeV NUCLEAR REACTIONS 10B(n, α), E=0.000001-2.5 MeV; measured reaction products, Eα, Iα; deduced σ(θ), σ and uncertainties. Comparison with ENDF/B-VIII.0, JEFF-3.3, CENDL-3.1 and JENDL 4.0 libraries.
doi: 10.1088/1674-1137/43/12/124002
2019LI08 Phys.Rev. C 99, 024602 (2019) C.Li, X.Xu, J.Li, G.Zhang, B.Li, C.A.T.Sokhna, Z.Ge, F.Zhang, P.Wen, F.-S.Zhang Production of new neutron-rich heavy nuclei with Z=56--80 in the multinucleon transfer reactions of 136Xe + 198Pt NUCLEAR REACTIONS 198Pt(136Xe, X), E=5.25, 6.20, 7.98, 10.0, 15.0 MeV/nucleon; calculated σ(E) for isotopic distribution of primary and secondary fragments in A=110-230 and Z=52, 54, 56, 74, 76, 78, 80, 82, 84 region, average energy difference after multi-nucleon transfer (MNT), average excitation energy of primary target like fragments as a function of mass number, differential σ(θ) of secondary target like fragments: 198,200,202,204,206Pt, 196,198,200,202,204Os, 190,192,194,196,198W, 186,188,190,192,194Hf. Improved quantum molecular dynamics (ImQMD), ImQMD+GEMINI and GRAZING calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.024602
2019LI13 Phys.Rev. C 99, 034619 (2019) C.Li, C.A.T.Sokhna, X.Xu, J.Li, G.Zhang, B.Li, Z.Ge, F.-S.Zhang Isospin equilibration in multinucleon transfer reaction at near-barrier energies NUCLEAR REACTIONS 208Pb(124Xe, X), E(cm)=450 MeV; calculated single-particle potentials of neutrons and protons, time evolution of density profiles and isospin asymmetry, and neutron and proton transfer coefficients for the neutron and proton as function of symmetry energy coefficients. 208Pb(58Ni, X), E=328.4, 345 MeV; calculated isotope production σ(E) from Mn to Ni, total kinetic energy TKE-mass distributions and N/Z ratios of primary binary fragments. Improved quantum molecular dynamics model (ImQMD). Comparison with experimental values for 208Pb(58Ni, X) reaction.
doi: 10.1103/PhysRevC.99.034619
2019XU06 Chin.Phys.C 43, 064105 (2019) X.-X.Xu, G.Zhang, J.-J.Li, B.Li, C.A.T.Sokhna, X.-R.Zhang, X.-X.Yang, S.-H.Cheng, Y.-H.Zhang, Z.-S.Ge, C.Li, Z.Liu, F.-S.Zhang Production of exotic neutron-deficient isotopes near N, Z = 50 in multinucleon transfer reactions NUCLEAR REACTIONS 124Sn(40Ca, X), E=128.5 MeV; 112Sn(48Ca, X), (40Ca, X), (58Ni, X), (106Cd, X), E(cm)=280 MeV; 112Sn(106Cd, X)101Sb/112Sb/103Te/106I/107I, E(cm)=300, 500, 780 MeV; calculated production σ. Comparison with experimental data.
doi: 10.1088/1674-1137/43/6/064105
2019ZH17 Phys.Rev. C 99, 044605 (2019) S.Zhang, A.Bonasera, M.Huang, H.Zheng, D.X.Wang, J.C.Wang, L.Lu, G.Zhang, Z.Kohley, Y.G.Ma, S.J.Yennello Strongly resonating bosons in hot nuclei NUCLEAR REACTIONS 64,70Zn(70Zn, X), (64Zn, X), 64Zn, 64Ni(64Zn, X), (64Ni, X), E=35 MeV/nucleon; analyzed experimental data from 4π NIMROD array at K150 cyclotron facility of Texas A and M University; deduced relative kinetic energy distribution of 2α events, excitation-energy distributions of 12C from 3α events, and 3Li from 3p events, probability ratios of direct-decay of 12C states into 3α particles of equal energies (DDE), and into a linear-decay (LD), probability ratios of decay of Hoyle state (HS) when 8Be g.s. energy is consistent with two α relative kinetic energies, or when the second largest energy is twice that of the 8Be g.s. energy. 8Be, 12C; discussed energy levels in hot nuclear matter, excitation of 12C states through multiresonance processes, and decay of 12C Hoyle state through 8Be.
doi: 10.1103/PhysRevC.99.044605
2019ZH36 Pramana 93, 61 (2019) Scattering of neutrons on α-particles in three-dimensional space
doi: 10.1007/s12043-019-1824-1
2019ZH38 Phys.Rev. C 100, 024613 (2019) G.Zhang, C.A.T.Sokhna, Z.Liu, F.-S.Zhang Production of neutron-rich isotopes 264, 266, 268, 269Rf by multinucleon transfer reactions based on 238U beam NUCLEAR REACTIONS 248Cm(238U, X), E=1760 MeV; calculated production cross sections of Z=97-100, A=235-265 isotopes, and compared to experimental data. 248Cf(238U, X), E(cm)=847.1 MeV; 249Bk(238U, X), E(cm)=892.1 MeV; 252Cf(238U, X), E(cm)=889.6 MeV; calculated production cross sections and driving potentials of A=250-271 Rf isotopes. 252Cf(238U, X), E(cm)=889.6 MeV; calculated N/Z ratio distribution of primary fragments as function of angular momentum, primary and final production cross sections of A=255-270 Rf isotopes. 252Cf(238U, X), E(cm)=849.1, 889.6, 970.4 MeV; calculated primary and final production cross sections of A=250-275 Rf isotopes. 248Cf(238U, X)264Rf/266Rf/268Rf/269Rf, E(cm)=847.1 MeV; 249Bk(238U, X)264Rf/266Rf/268Rf/269Rf, E(cm)=892.1 MeV; 252Cf(238U, X)264Rf/266Rf/268Rf/269Rf, E(cm)=849.1, 889.6, 970.4 MeV; calculated counts per day for 264,266,268,269Rf isotopes, with the highest counts for 238U+252Cf reaction. Dinuclear system (DNS) model with GEMINI++ code.
doi: 10.1103/PhysRevC.100.024613
2018GE06 Phys.Rev. C 98, 034312 (2018) Z.Ge, C.Li, J.Li, G.Zhang, B.Li, X.Xu, C.A.T.Sokhna, X.Bao, H.Zhang, Yu.S.Tsyganov, F.-S.Zhang Effect of shell corrections on the α-decay properties of 280-305Fl isotopes RADIOACTIVITY 280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305Fl(α), (SF); calculated Q(α) and half-lives using GLDM, the GLDM with shell correction, the UFM and the Royer's formula, and shell correction energies of the even-even nuclei. 285,286,287,288,289Fl, 281,283,285Cn, 277,279,281Ds, 273,275Hs, 269,271Sg(α); calculated T1/2 using Royer's, UDL, UFM, and GLDM formulas, and by input of experimental Q(α) values. Comparison with experimental values.
doi: 10.1103/PhysRevC.98.034312
2018GL03 Phys.Rev. C 98, 034605 (2018) Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu, H.Bai, H.Jiang, Y.Lu, Z.Cui, J.Chen, G.Zhang Measurement of the cross sections of the 25Mg (n, α) 22Ne reaction in the 4-6 MeV region NUCLEAR REACTIONS 25Mg(n, α), E=4.0-6.0 MeV; measured Eα, Iα, σ(E) using enriched target and a twin-gridded ionization chamber for charged particle detection at the 4.5 MV Van de Graaff accelerator of Peking University Comparison with previous experimental values, evaluated data libraries, and theoretical predictions.
doi: 10.1103/PhysRevC.98.034605
2018LI02 Phys.Lett. B 776, 278 (2018) C.Li, P.Wen, J.Li, G.Zhang, B.Li, X.Xu, Z.Liu, S.Zhu, F.-S.Zhang Production mechanism of new neutron-rich heavy nuclei in the 136Xe + 198Pt reaction NUCLEAR REACTIONS 136Xe(198Pt, X)199Pt/203Pt/208Pt, E=7.98 MeV/nucleon; analyzed available data; calculated σ.
doi: 10.1016/j.physletb.2017.11.060
2018LI34 Phys.Rev. C 98, 014626 (2018) J.Li, C.Li, G.Zhang, B.Li, X.Xu, Z.Liu, Yu.S.Tsyganov, F.-S.Zhang Theoretical study on production of unknown neutron-deficient 280-283Fl and neutron-rich 290-292Fl isotopes by fusion reactions NUCLEAR REACTIONS 239,240,242,244Pu(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-65 MeV; 242Pu(44Ca, 2n), (44Ca, 3n), (44Ca, 4n), (44Ca, 5n), E*=30-70 MeV; 249Cf(36S, 2n), (36S, 3n), (36S, 4n), (36S, 5n), E*=30-70 MeV; 250Cm(44Ar, 4n), (44Ar, 5n), E*=30-65 MeV; 248,250Cm(46Ar, 3n), (46Ar, 4n), (46Ar, 5n); calculated evaporation residue σ(E) using dinuclear system (DNS) model. 280,281,282,283,291,292,293Fl; calculated production cross sections using hot fusion reaction mechanism. Comparison with available experimental data.
doi: 10.1103/PhysRevC.98.014626
2018WU05 Phys.Rev. C 97, 064602 (2018) S.Wuenschel, K.Hagel, M.Barbui, J.Gauthier, X.G.Cao, R.Wada, E.J.Kim, Z.Majka, R.Planeta, Z.Sosin, A.Wieloch, K.Zelga, S.Kowalski, K.Schmidt, C.Ma, G.Zhang, J.B.Natowitz Experimental survey of the production of α-decaying heavy elements in 238U+232Th reactions at 7.5-6.1 MeV/nucleon NUCLEAR REACTIONS 232Th(238U, X), (197Au, X), E=6.1 MeV/nucleon; measured reaction products, Eα, α(θ), Eα(t) of reaction product decays, (recoil)α-coin, differential σ(θ) using Big-Sol Superconducting-Solenoid Time of Flight Spectrometer at Texas A and M; deduced α-decay and spontaneous fission T1/2 of recoils and α-decay T1/2 of daughter nuclides, and of correlated pairs, thick target differential cross sections. Comparison with previous experimental results, and theoretical predictions.
doi: 10.1103/PhysRevC.97.064602
2018ZH30 Phys.Rev. C 98, 014613 (2018) G.Zhang, C.Li, P.-W.Wen, J.-J.Li, X.-X.Xu, B.Li, Z.Liu, F.-S.Zhang Production of neutron-rich 209-212Pt isotopes based on a dinuclear system model NUCLEAR REACTIONS 208Pb(64Ni, X)180Os/181Os/182Os/183Os/184Os/185Os/186Os/187Os/188Os/189Os/190Os/191Os/192Os/193Os/194Os/195Os/196Os/187Pt/188Pt/189Pt/190Pt/191Pt/192Pt/193Pt/194Pt/195Pt/196Pt/197Pt/198Pt/199Pt/200Pt/201Pt/202Pt/192Hg/193Hg/194Hg/195Hg/196Hg/197Hg/198Hg/199Hg/200Hg/201Hg/202Hg/203Hg/204Hg/205Hg/206Hg/207Hg, E(cm)=268 MeV; calculated isotopic production σ, and cross sections for production of A=50 to 200 masses. 208Pb(133Sn, X), (145Xe, X), (238U, X), E(cm)=1.10Vc; calculated driving potential for neutron pickup and stripping channels. 198Pt, 204Hg, 208Pb(133Sn, X), 208Pb(145Xe, X), (238U, X)190Pt/191Pt/192Pt/193Pt/194Pt/195Pt/196Pt/197Pt/198Pt/199Pt/200Pt/201Pt/202Pt/203Pt/204Pt/205Pt/206Pt/207Pt/208Pt/209Pt, E(cm)=1.10Vc; calculated production σ for Pt isotopes. 209,210,211,212Pt; calculated production cross sections in 208Pb+145Xe and 204Hg+133Sn reactions via multinucleon transfer reactions. Dinuclear system (DNS) model. Comparison with available experimental data.
doi: 10.1103/PhysRevC.98.014613
2017LI16 Phys.Rev. C 95, 054612 (2017) J.Li, C.Li, G.Zhang, L.Zhu, Z.Liu, F.-S.Zhang Production cross sections of neutron-rich 261-263No isotopes NUCLEAR REACTIONS 208Pb(48Ca, X), E*=10-45 MeV; 244Pu(18O, X), (22O, 4n), E*=30-70 MeV; calculated capture σ(E*). Compared with experimental data for 208Pb+48Ca. 244Pu(18O, 3n), (18O, 4n), (18O, 5n), 244Pu(22O, 3n), (22O, 4n), (22O, 5n), E*(CN)=20-80 MeV; calculated survival probabilities. 208Pb(48Ca, n), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E*(CN)=10-55 MeV; 228,230Th(26Mg, 3n), (26Mg, 4n), (26Mg, 5n), E*(CN)=35-75 MeV; 242,244Pu(18O, 3n), (18O, 4n), (18O, 5n), (22O, 3n), (22O, 4n), (22O, 5n), E*(CN)=30-80 MeV; calculated σ(E). 228Th(26Mg, 5n)249No, E=164.9 MeV; 204Pb(48Ca, 2n)250No, E=216.7 MeV; 206Pb(48Ca, 4n)250No, E=242.2 MeV; 228Th(26Mg, 4n)250No, E=140.4 MeV; 206Pb(48Ca, 3n)251No, E=226.2 MeV; 244Cm(12C, 5n)251No, E=83.0 MeV; 206Pb(48Ca, 2n)252No, E=217.1 MeV; 230Th(26Mg, 4n)252No, E=135.8 MeV; 244Cm(12C, 4n)252No, E=73.3 MeV; 206Pb(48Ca, n)253No, E=217.4 MeV; 207Pb(48Ca, 2n)253No, E=216.7 MeV; 230Th(26Mg, 3n)253No, E=133.6 MeV; 244Cm(13C, 4n)253No, E=72.8 MeV; 246Cm(12C, 5n)253No, E=83.0 MeV; 208Pb(48Ca, 2n)254No, E=216.7 MeV; 244Cm(13C, 3n)254No, E=69.8 MeV; 246Cm(12C, 4n)254No, E=72.0 MeV; 246Cm(13C, 5n)254No, E=78.5 MeV; 242Pu(18O, 5n)255No, E=106.8 MeV; 246Cm(13C, 4n)255No, E=69.5 MeV; 248Cm(12C, 5n)255No, E=77.8 MeV; 242Pu(18O, 4n)256No, E=93.9 MeV; 246Cm(13C, 3n)256No, E=67.5 MeV; 248Cm(12C, 4n)256No, E=71.2 MeV; 248Cm(13C, 5n)256No, E=74.8 MeV; 242Pu(18O, 3n)257No, E=91.8 MeV; 244Pu(18O, 5n)257No, E=105.8 MeV; 248Cm(12C, 3n)257No, E=69.2 MeV; 248Cm(13C, 4n)257No, E=70.5 MeV; 244Pu(18O, 4n)258No, E=95.0 MeV; 248Cm(13C, 3n)258No, E=71.1 MeV; 242Pu(22O, 5n)259No, E=106.9 MeV; 244Pu(18O, 3n)259No, E=90.7 MeV; 242Pu(22O, 4n)260No, E=93.8 MeV; 242Pu(22O, 3n)261No, E=91.6 MeV; 244Pu(22O, 5n)261No, E=100.8 MeV; 244Pu(22O, 4n)262No, E=92.1 MeV; 244Pu(22O, 3n)263No, E=89.9 MeV; calculated production σ, and compared with experimental data. Dinuclear system (DNS) model for fusion-evaporation (FE) reaction.
doi: 10.1103/PhysRevC.95.054612
2017SC09 Phys.Rev. C 95, 054618 (2017) K.Schmidt, X.Cao, E.J.Kim, K.Hagel, M.Barbui, J.Gauthier, S.Wuenschel, G.Giuliani, M.R.D.Rodrigues, H.Zheng, M.Huang, N.Blando, A.Bonasera, R.Wada, C.Botosso, G.Liu, G.Viesti, S.Moretto, G.Prete, S.Pesente, D.Fabris, Y.El Masri, T.Keutgen, S.Kowalski, A.Kumar, G.Zhang, J.B.Natowitz α-conjugate neck structures in the collisions of 35 MeV/nucleon 40Ca with 40Ca NUCLEAR REACTIONS 40Ca(40Ca, X), E=35 MeV/nucleon; measured reaction products, yields of the heaviest fragments, average excitation energy vs exit channel separation energy, events for α particles and α-conjugate nuclei, excitation energy distributions, excitation functions, and projectile-like fragments in the exit channels using the NIMROD-ISiS 4π array at the K500 superconducting cyclotron of the Texas A and M University; deduced hierarchy effect, dominance of α-conjugate exit channels in a subset of events with a total α-conjugate A=40 and Z=20, source-frame-invariant velocity plots for α-like and two fragment α-like exit channels, parallel velocity distributions for α-conjugate exit channels, de-excitation of α-conjugate nuclei, and the dynamics of collisions leading to projectile-like fragment exit channels.
doi: 10.1103/PhysRevC.95.054618
2017WA32 Phys.Rev. C 96, 034611 (2017) T.Wang, G.Li, L.Zhu, O.Hen, G.Zhang, Q.Meng, L.Wang, H.Han, H.Xia Aspects of charge distribution measurement for 252Cf(sf) RADIOACTIVITY 252Cf(SF); measured charge distribution and yields of fission fragments of Z=33-43, charge dispersion of A=101 nuclei 101Y, 101Zr, 101Nb, 101Mo, and 101Tc using grid-ionization chamber (GIC) and a gas ΔE-E detector coupled with a surface-barrier detector; deduced kinetic energy averaged widths as function of atomic mass A, widths of charge distributions, Charge polarization as a function of the mass number of primary fission fragments, average most probable charge as a function of mass number of light fragments. Comparison with theoretical calculations.
doi: 10.1103/PhysRevC.96.034611
2017WA42 Phys.Rev. C 96, 044620 (2017) Z.Wang, H.Bai, L.Zhang, H.Jiang, Y.Lu, J.Chen, G.Zhang, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu Cross section measurement for the 10B (n, t2α) three-body reaction at 4.0, 4.5, and 5.0 MeV. I. Prediction of the experimental spectrum NUCLEAR REACTIONS 10B(n, t2α), E=4.0, 4.5, 5.0 MeV; calculated complete final-state phase space for the 7Li**, 8Be, and breakup channels, one-dimensional and two-dimensional experimental spectra using LUNF code, and as described in the experimental details of a companion article 2017Wa23.
doi: 10.1103/PhysRevC.96.044620
2017WA43 Phys.Rev. C 96, 044621 (2017) Z.Wang, H.Bai, L.Zhang, H.Jiang, Y.Lu, J.Chen, G.Zhang, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu Cross section measurement for the 10B (n, t2α) three-body reaction at 4.0, 4.5, and 5.0 MeV. II. Experimental setup and results NUCLEAR REACTIONS 10B(n, t2α), E=4.0, 4.5, 5.0 MeV; 10B(n, α)7Li, E=thermal; measured particle spectra, grid-anode two-dimensional spectra using a twin gridded ionization chamber (GIC) and double-coincidence technique at the 4.5 MV Van de Graaff accelerator of Peking University; deduced σ(E). Comparison with previous measurements and evaluated libraries ENDF/B-VII.1, JENDL-4.0, and CN-RAC2016.
doi: 10.1103/PhysRevC.96.044621
2015HA04 Eur.Phys.J. A 51, 12 (2015) J.Han, J.Liu, X.Liu, X.Fan, Z.Wang, J.Chen, G.Zhang, Yu.M.Gledenov, M.V.Sedysheva, L.Krupa, G.Khuukhenkhuu, P.J.Szalanski Differential and angle-integrated cross sections for the 40Ca(n, α)37Ar reaction from 4.0 to 6.5 MeV NUCLEAR REACTIONS 40Ca(n, α), E=4.0, 4.5, 5.0, 5.5, 6.0, 6.5 MeV; measured reaction products using GIS (gridded ionization chamber); deduced σ, σ(θ) to discrete states; calculated σ, σ(θ) using TALYS-1.6. Cross sections compared also to other data.
doi: 10.1140/epja/i2015-15012-5
2015WA31 Phys.Rev. C 92, 044601 (2015) Z.Wang, X.Fan, L.Zhang, H.Bai, J.Chen, G.Zhang, Yu.M.Gledenov, M.V.Sedysheva, L.Krupa, G.Khuukhenkhuu Cross sections of the 56Fe (n, α)53Cr and 54Fe (n, α)51Cr reactions in the MeV region NUCLEAR REACTIONS 56Fe(n, α)53Cr, E=5.5, 6.5 MeV; 54Fe(n, α)51Cr, E=4.0, 4.5, 5.5, 6.5 MeV; measured Eα, Iα, σ(E) at Van de Graaff Accelerator of Peking University. Comparison with TALYS-1.6 code calculations, previous experimental data, and several evaluated libraries of reaction cross section data.
doi: 10.1103/PhysRevC.92.044601
2014GL01 Phys.Rev. C 89, 064607 (2014) Yu.M.Gledenov, M.V.Sedysheva, V.A.Stolupin, G.Zhang, J.Han, Z.Wang, X.Fan, X.Liu, J.Chen, G.Khuukhenkhuu, P.J.Szalanski Cross sections of the 57Fe(n, α)54Cr and 63Cu(nα)60Co reactions in the MeV region NUCLEAR REACTIONS 57Fe(n, α)54Cr, 63Cu(n, α)60Co, E=5.0, 5.5, 6.0, 6.5 MeV; measured particle spectra, σ(E), reaction spectra at Van de Graaff Accelerator facility of Peking University. Comparison with TALYS-1.4 code predictions, previous experimental results, and several evaluated libraries.
doi: 10.1103/PhysRevC.89.064607
2011GL03 J.Korean Phys.Soc. 59, 1693s (2011) Y.Gledenov, M.Sedysheva, G.Zhang, J.Zhang, H.Wu, J.Liu, J.Chen, P.Koehler, G.Khuukhenkhuu, P.Szalanski Investigation of (n, α) Reaction for Rare-earth Elements in the MeV Neutron Energy Region NUCLEAR REACTIONS 143Nd(n, α), E=4.0, 5.0, 6.0 MeV;147Sm(n, α), E=5.0, 6.0 MeV;149Sm(n, α), E=6 MeV; measured Eα, Iα; deduced σ; calculated σ using TALYS; deduced optical model parameter. Compared with other data, ENDF/B-VI-8, ENDF/B-VII.0, JEFF3.1, JENDL3.3.
doi: 10.3938/jkps.59.1693
2011ZH50 Phys.Rev.Lett. 107, 252502 (2011) G.Zhang, Yu.M.Gledenov, G.Khuukhenkhuu, M.V.Sedysheva, P.J.Szalanski, P.E.Koehler, Yu.N.Voronov, J.Liu, X.Liu, J.Han, J.Chen 149Sm(n, α)146Nd Cross Sections in the MeV Region NUCLEAR REACTIONS 149Sm(n, α), E=4.5, 5.0, 5.5, 6.0, 6.5 MeV; measured Eα, Iα, En, In; deduced σ. Comparison with TALYS code calculations and evaluated nuclear libraries.
doi: 10.1103/PhysRevLett.107.252502
2011ZH51 J.Korean Phys.Soc. 59, 1705s (2011) G.Zhang, J.Zhang, H.Wu, J.Liu, J.Chen, Y.Gledenov, M.Sedysheva, G.Khuukhenkhuu, P.Szalanski 64Zn and 67Zn (n, α) Reactions in the MeV Neutron Energy Region NUCLEAR REACTIONS 64Zn(n, α), E=2.5, 4.0, 5.0, 5.5, 6.0 MeV; measured Eα, Iα(θ); deduced σ, σ(θ). 67Zn(n, α), E=4.0, 5.0, 6.0 MeV; measured Eα, Iα; deduced σ. σ compared with other data, JEF-2.2, JEFF-3.1/A, TENDL-2009, JENDL/HE-2007 below 20 MeV.
doi: 10.3938/jkps.59.1705
2010GL03 Phys.Rev. C 82, 014601 (2010) Yu.M.Gledenov, G.Zhang, G.Khuukhenkhuu, M.V.Sedysheva, P.J.Szalanski, P.E.Koehler, J.Liu, H.Wu, X.Liu, J.Chen Cross-section measurement and analysis for the 149Sm(n, γ)146Nd reaction at 6.0 MeV NUCLEAR REACTIONS 149Sm(n, α), E=6.0 MeV; measured σ. Comparison with statistical-model calculations using TALYS code and with existing evaluations in various databases such as ENDF/B-VII.
doi: 10.1103/PhysRevC.82.014601
2010ZH01 Appl.Radiat.Isot. 68, 180 (2010) G.Zhang, H.Wu, J.Zhang, J.Liu, Y.Yin, J.Chen, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu, P.E.Koehler, P.J.Szalanski Cross section measurement for the 95Mo(n, α)92Zr reaction at 4.0, 5.0 and 6.0 MeV NUCLEAR REACTIONS 95Mo(n, α), E=4, 5, 6 MeV; measured Iα, Eα, reaction fragments; deduced σ. Comparison with ENDF/B-VII.0, JEFF-3.1/A and JENDL-3.3 libraries.
doi: 10.1016/j.apradiso.2009.09.013
2010ZH28 Eur.Phys.J. A 43, 1 (2010) G.Zhang, H.Wu, J.Zhang, J.Liu, J.Chen, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu, P.J.Szalanski Cross-section measurement for the 67Zn(n, α)64Ni reaction at 6.0 MeV NUCLEAR REACTIONS 67Zn(n, α), E=6.0 MeV; measured Eα, Iα, σ. Comparison with other data and TALYS calculation.
doi: 10.1140/epja/i2009-10886-2
2010ZH47 Phys.Rev. C 82, 054619 (2010) G.Zhang, Yu.M.Gledenov, G.Khuukhenkhuu, M.V.Sedysheva, P.J.Szalanski, J.Liu, H.Wu, X.Liu, J.Chen, V.A.Stolupin Cross sections of the 67Zn(n, α)64Ni reaction at 4.0, 5.0, and 6.0 MeV NUCLEAR REACTIONS 67Zn(n, α)64Ni, E=4.0, 5.0, 6.0 MeV; measured Eα, Iα, partial σ to 64Ni g.s. and total σ. Comparison with previous measurements, evaluations and calculations using TALYS code.
doi: 10.1103/PhysRevC.82.054619
2009GL02 Phys.Rev. C 80, 044602 (2009) Yu.M.Gledenov, M.V.Sedysheva, V.A.Stolupin, G.Zhang, J.Zhang, H.Wu, J.Liu, J.Chen, G.Khuukhenkhuu, P.E.Koehler, P.J.Szalanski Cross sections of the 143Nd(n, α)140Ce and 147Sm(n, α)144Nd reactions in the MeV neutron energy region NUCLEAR REACTIONS 143Nd(n, α)140Ce, E=4.0, 5.0, 6.0 MeV; 147Sm(n, α)144Nd, E=5.0, 6.0 MeV; measured α spectra, σ, forward and backward α rates. 143Nd, 147Sm(n, α), E=0.5 keV-20 MeV; compared present and previous measured cross sections with several evaluations, and calculations from TALYS code.
doi: 10.1103/PhysRevC.80.044602
2009ZH01 Appl.Radiat.Isot. 67, 46 (2009) G.Zhang, J.Zhang, L.Guo, H.Wu, J.Chen, G.Tang, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu, P.J.Szalanski Measurement of cross sections for the 147Sm(n, α)144Nd reaction at 5.0 and 6.0 MeV NUCLEAR REACTIONS 147Sm(n, α), E=5.0, 6.0 MeV; measured Eα, Iα, cross sections. Compared results to existing data.
doi: 10.1016/j.apradiso.2008.07.005
2008ZH15 Nucl.Sci.Eng. 160, 123 (2008) G.Zhang, J.Zhang, R.Cao, L.Guo, J.Chen, Yu.M.Gledenov, M.V.Sedysheva, G.Khuukhenkhuu, P.J.Szalanski Measurement of Differential Cross Section for the 64Zn(n, α)61Ni Reaction at 2.54, 4.00, and 5.50 MeV NUCLEAR REACTIONS 64Zn(n, α), E=2.54, 4.00, 5.50 MeV; measured Eα, Iα, σ(θ).
doi: 10.13182/NSE160-123
2008ZH20 Appl.Radiat.Isot. 66, 1427 (2008) G.Zhang, L.Guo, R.Cao, J.Zhang, J.Chen Cross-section measurement for the 10B(n, α)7Li reaction at 4.0 and 5.0 MeV NUCLEAR REACTIONS 10B(n, α), E=4.0, 5.0; 238U(n, F), E=4.0 MeV; measured σ; gridded ionization chamber; comparison with previous results and JENDL-3.3, ENDF/B-VII evaluations.
doi: 10.1016/j.apradiso.2008.07.035
2007ZH12 Nucl.Sci.Eng. 156, 115 (2007) G.Zhang, R.Cao, J.Chen, G.Tang, Yu.M.Gledenov, M.Sedysheva, G.Khuukhenkhuu Differential Cross-Section measurement for the 64Zn(n, α)61Ni Reaction at 5.03 and 5.95 MeV NUCLEAR REACTIONS 64Zn(n, α), E=5.03, 5.95 MeV; measured Eα, σ(θ); deduced angle-integrated σ.
doi: 10.13182/NSE07-A2690
2007ZH42 Appl.Radiat.Isot. 65, 1314 (2007) P.Zhu, Z.Yuan, J.Chen, Z.Liu, G.Zhang, Z.Shi, H.Lu Measurement of neutron capture cross sections for 141Pr from 0.5 to 1.6 MeV NUCLEAR REACTIONS 141Pr(n, γ), E=0.54, 1.09, 1.59 MeV; measured Eγ, Iγ, cross sections using the activation method. Compared results to model calculations.
doi: 10.1016/j.apradiso.2007.07.015
2006ZH07 Nucl.Sci.Eng. 153, 41 (2006) G.Zhang, R.Cao, J.Chen, G.Tang, Yu.M.Gledenov, M.Sedysheva, G.Khuukhenkhuu Differential and Angle-Integrated Cross-Section Measurement for the 6Li(n, t)4He Reaction at En = 1.05, 1.54, and 2.25 MeV NUCLEAR REACTIONS 6Li(n, t), E=1.05, 1.54, 2.25 MeV; measured σ(θ); deduced angle-integrated σ. Comparison with previous results.
doi: 10.13182/NSE153-41
2006ZH27 Nucl.Instrum.Methods Phys.Res. A566, 615 (2006) G.Zhang, J.Chen, G.Tang, Yu.M.Gledenov, M.Sedysheva, G.Khuukhenkhuu Measurement of differential and angle-integrated cross sections of the 6Li(n, t)4He reaction in the MeV neutron energy range NUCLEAR REACTIONS 6Li(n, t), E=1.05-4.42 MeV; measured σ(θ); deduced angle-integrated σ. Comparison with previous results.
doi: 10.1016/j.nima.2006.06.064
2005HU14 J.Radioanal.Nucl.Chem. 265, 499 (2005) D.Huang, P.Wang, X.Chen, W.Tian, B.Ni, L.Zhang, G.Zhang, C.Liu, L.Liu Half-life of 97Zr, re-measured RADIOACTIVITY 97Zr(β-) [from Zr(n, X)]; measured T1/2.
doi: 10.1007/s10967-005-0854-y
2003GL06 Bull.Rus.Acad.Sci.Phys. 67, 760 (2003) Yu.M.Gledenov, M.V.Sedysheva, P.V.Sedyshev, A.Oprea, G.Khuukhenkhuu, Z.Chen, Y.Chen, J.Yuan, G.Tang, G.Zhang, J.Andrzejewski, P.J.Szalanski (nα)-reactions on medium-mass nuclei at En = 4.5 - 6.75 MeV NUCLEAR REACTIONS 39K, 40Ca, 64Zn(n, α), E=4.5-6.75 MeV; measured σ, σ(θ). Comparison with previous work, model predictions. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31506. 2003GL08 Bull.Rus.Acad.Sci.Phys. 67, 1784 (2003) Yu.M.Gledenov, M.V.Sedysheva, P.V.Sedyshev, A.Oprea, G.Khuukhenkhuu, Z.Chen, Y.Chen, J.Yuan, G.Tang, G.Zhang, J.Andrzejewski, P.J.Szalanski Two-section ionization chamber α-spectrometer for nuclear reaction studies NUCLEAR REACTIONS 36Ar, 39K, 40Ca, 64Zn(n, α), E ≈ 5-6.5 MeV; measured σ(E), σ. 64Zn(n, α), E=5 MeV; measured Eα, angular distribution. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31559. 2003YU09 Nucl.Sci.Eng. 144, 108 (2003) J.Yuan, Z.Chen, G.Tang, G.Zhang, J.Chen, Z.Shi, Yu.M.Gledenov, M.Sedysheva, G.Khuukhenkhuu Angular Distribution and Cross-Section Measurements for 64Zn(n, α)61Ni Reaction at 5.0, 5.7, and 6.5 MeV NUCLEAR REACTIONS 64Zn(n, α), E=5.0, 5.7, 6.5 MeV; measured σ(θ); deduced integrated σ.
doi: 10.13182/NSE03-A2346
2003ZH40 Nucl.Sci.Eng. 143, 86 (2003) G.Zhang, G.Tang, J.Chen, Z.Shi, Z.Chen, Yu.M.Gledenov, M.Sedysheva, G.Khuukhenkhuu Measurement of Differential Cross Sections of the 6Li(n, t)4He Reaction at 1.85 and 2.67 MeV NUCLEAR REACTIONS 6Li(n, t), E=1.85, 2.67 MeV; measured σ(θ); deduced angle-integrated σ.
doi: 10.13182/NSE03-A2320
2002ZH35 Nucl.Sci.Eng. 142, 203 (2002) G.Zhang, G.Tang, J.Chen, S.Zhang, Z.Shi, J.Yuan, Z.Chen, Yu.M.Gledenov, M.Sedysheva, G.Khuukhenkhuu Differential Cross-Section Measurement for the 10B(n, α)7Li Reaction NUCLEAR REACTIONS 10B(n, α), E=4.17, 5.02, 5.74, 6.52 MeV; measured σ(θ); deduced angle-integrated σ.
doi: 10.13182/NSE02-A2300
2001ZH11 Nucl.Sci.Eng. 137, 107 (2001) G.Zhang, Z.Shi, G.Tang, J.Chen, G.Liu, H.Lu Interference of the Low-Energy Neutrons on Activation Cross-Section Measurement of the 186W(n, γ)187W Reaction NUCLEAR REACTIONS 186W(n, γ), E=0.5-1.5 MeV; measured σ. Activation technique, effects of interference from low-energy neutrons discussed. Comparisons with previous results, evaluated data.
doi: 10.13182/NSE01-A2179
2000ZH01 Nucl.Sci.Eng. 134, 89 (2000) X.Zhang, Z.Chen, Y.Chen, G.Tang, G.Zhang, J.Chen, Yu.M.Gledenov, G.Khuukhenkhuu Measurements and Calculations of the 39K and 40Ca(n, α) Cross Sections at En = 4.5 to 6.5 MeV NUCLEAR REACTIONS 39K(n, α), E=4.5, 5.5, 6.5 MeV; 40Ca(n, α), E=5, 6 MeV; measured σ, σ(θ), σ(E, θ). Comparison with model calculations.
doi: 10.13182/NSE00-A2102
2000ZH05 Nucl.Sci.Eng. 134, 312 (2000) G.Zhang, G.Tang, J.Chen, Z.Shi, G.Liu, X.Zhang, Z.Chen, Yu.M.Gledenov, M.Sedysheva, G.Khuukhenkhuu Differential Cross-Section Measurement for the 6Li(n, t)4He Reaction at 3.67 and 4.42 MeV NUCLEAR REACTIONS 6Li(n, t), E=3.67, 4.42 MeV; measured σ(θ); deduced angle-integrated σ. Gridded ionization chamber.
doi: 10.13182/NSE00-A2119
2000ZH10 Phys.Rev. C61, 054607 (2000) X.Zhang, Z.Chen, Y.Chen, J.Yuan, G.Tang, G.Zhang, J.Chen, Yu.M.Gledenov, G.Khuukhenkhuu, M.Sedysheva Dispersion Relations for (n, n), (n, p), and (n, α) Reactions on 39K and 40Ca NUCLEAR REACTIONS 39K(n, α), E=4.5, 5.5, 6.5 MeV; 40Ca(n, α), E=5, 6 MeV; measured σ, σ(E, θ); deduced optical model parameters, dispersion relations. 39K, 40Ca(n, n), (n, p), (n, α), E=4-70 MeV; calculated σ. Dispersive optical model.
doi: 10.1103/PhysRevC.61.054607
1989SC08 Phys.Rev. C39, 1827 (1989) H.R.Schelin, A.Galonsky, C.K.Gelbke, L.Heilbronn, W.G.Lynch, T.Murakami, M.B.Tsang, X.Yang, G.Zhang, B.A.Remington, F.Deak, A.Kiss, Z.Seres, J.Kasagi Neutron Inclusive Measurements in 14N + Ag Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, nX), E=35 MeV/nucleon; measured σ(θn, En); deduced angle integrated σ.
doi: 10.1103/PhysRevC.39.1827
1982SA32 Chin.J.Nucl.Phys. 4, 318 (1982) Sa Benhao, Su Zongdi, Zhang Guishan, Shi Yijing, Huang Zuqia Direct Simulation of Deep Inelastic Scattering of Heavy-Ions. (I). One Parameter Distribution NUCLEAR REACTIONS 58Ni(40Ar, X), E=280 MeV; analyzed data; deduced single nucleon transfer probability. Statistical spectroscopy method, direct simulation, Lagrange equation.
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