NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = G.Zhang Found 206 matches. Showing 1 to 100. [Next]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
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
2023HU10 Phys.Rev. C 107, 044309 (2023) Z.Huang, G.X.Zhang, C.X.Yuan, G.L.Zhang, D.Mengoni, B.S.Cai, S.P.Hu, H.Q.Zhang, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, D.Bazzacco, D.R.Napoli, F.Galtarossa, F.Recchia, G.de Angelis, M.Siciliano, R.Menegazzo, S.M.Lenzi Level scheme study of 91Mo: Weak-coupling approximation in the N=50 region NUCLEAR REACTIONS 89Y(6Li, X)91Mo, E=34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 91Mo; deduced levels, J, π, transition intensities, angular distribution from oriented nuclei (ADO) ratios, δ, T1/2 for two isomeric states, high-spin states, B(E2), configurations. Comparison with shell-model calculation employing the JUN45 interaction (KSHELL code). GALILEO ψ-ray spectrometer consisting of 25 Compton-suppressed HPGe tapered detectors at Tandem-XTU accelerator (INFN-LNL, Italy).
doi: 10.1103/PhysRevC.107.044309
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
2023QI06 Phys.Rev. C 108, 014325 (2023) L.-J.Qi, D.-M.Zhang, S.Luo, G.-Q.Zhang, P.-C.Chu, X.-J.Wu, X.-H.Li Cluster radioactivity preformation probability of trans-lead nuclei in the NpNn scheme RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 223Ac(14C);228Th(20O);231Pa(23F);230Th, 231Pa, 232,233,234U(24Ne);233U(25Ne);234U(26Ne);234U, 236,238Pu(28Mg), 238Pu(30Mg);238Pu(32Si);242Cm(34Si); calculated cluster preformation probability. Comparison of results obtained with unified fission model (model dependent approach), cluster formation model (microscopic approach) and Wei model (analytical formula).
doi: 10.1103/PhysRevC.108.014325
2023RE11 Phys.Rev. C 108, 044301 (2023) Z.Ren, J.-B.Lu, G.-X.Dong, Y.Zheng, Y.-H.Wu, T.-J.Gao, P.-Y.Yang, Y.Hao, K.-Y.Ma, X.-G.Wu, C.-B.Li, Z.Huang, G.-X.Zhang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, D.Testov, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, D.Mengoni, D.Bazzacco, G.-L.Zhang Level scheme of 92Nb and observation of an oblate collective rotational band
doi: 10.1103/PhysRevC.108.044301
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
2022HU22 Phys.Rev. C 106, 064331 (2022) Z.Huang, G.X.Zhang, G.L.Zhang, S.P.Hu, S.M.Lenzi, D.Mengoni, J.L.Ferreira, Y.F.Lv, J.B.Lu, B.Paes, E.N.Cardozo, H.Q.Zhang, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, D.Bazzacco, P.R.John, D.R.Napoli, F.Galtarossa, F.Recchia, G.de.Angelis, M.Siciliano, R.Menegazzo, J.Lubian Level scheme study of 92Mo: Searching for evidence of core excitation NUCLEAR REACTIONS 89Y(6Li, 3n), E=34 MeV; measured Eγ, Iγ; γγ-coin, γγ(θ). 92Mo; deduced levels, J, π, δ, B(E1), T1/2 of excited states, high-spin states, angular distribution from the oriented nuclei (ADO) ratio, configurations. Comparison to JUN45 and JJGLEM shell-model calculation. GALILEO γ-array consisting of 25 Compton suppressed HPGe and 8 BGO crystals served as the anti-Compton shield of each HPGe at XTU Tandem accelerator (INFN Legnaro National Laboratory).
doi: 10.1103/PhysRevC.106.064331
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
2022RE11 Phys.Rev. C 106, 024323 (2022), Erratum Phys.Rev. C 107, 049902 (2023) Z.Ren, J.-B.Lu, G.-L.Zhang, Y.-H.Wu, T.-J.Gao, K.-Y.Ma, Z.Huang, G.-X.Zhang, M.-L.Wang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, D.Mengoni, D.Bazzacco Reinvestigation of the level structures of the N=49 isotones 89Zr and 91Mo NUCLEAR REACTIONS 89Y(6Li, 4n2p)89Zr, (6Li, 4n)91Mo, E=34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(ADO), (particle)γ-coin using GALILEO array with 25 BGO-Compton-suppressed HPGe detectors for γ rays, and EUCLIDES 4π Si-ball array for charged particles at the Tandem-XTU accelerator of INFN-LNL, Legnaro. 89Zr, 91Mo; deduced high-spin levels, J, π, ADO ratios, multipolarities, configurations. 91Nb, 92Mo; deduced ADO ratios for certain γ-transitions. Comparison with spherical-basis shell-model calculations. NUCLEAR STRUCTURE 89Zr, 91Mo; calculated levels, J, π, components of the wave functions and their partitions for spherical configurations for protons and neutrons. Comparison with experimental data. Systematics of energies in N=49 isotones: 9/2+, 13/2+, 17/2+, 21/2+, 23/2+ and 25/2+ states in 89Zr, 91Mo, 93Ru, 95Pd, and those of 8+, 9+, 10+, 12+, 13+ and 14+ in 88Y, 90Nb, 92Tc, 94Rh.
doi: 10.1103/PhysRevC.106.024323
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
2022ZH52 Phys.Rev. C 106, 034604 (2022) Simulating fusion reactions from Coulomb explosions within a transport approach NUCLEAR REACTIONS 2H(d, 3He), E=2-10 keV; calculated fusion σ(E), reaction rate at different temperatures, time evolution of the Coulomb explosion of deuterium clusters induced by high intensity laser beams, neutron production rate in Coulomb explosion. EPOCH model framework - typical particle-in-cell (PIC) transport approach, to simulate the Coulomb explosion of clusters with electrons completely stripped by laser beams, modified to incorporate fusion reactions by introducing nuclear inelastic scattering channels.
doi: 10.1103/PhysRevC.106.034604
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
2021HU12 Eur.Phys.J. A 57, 137 (2021) Z.Huang, G.X.Zhang, S.P.Hu, B.Paes, E.N.Cardozo, J.L.Ferreira, M.J.Ermamatov, G.L.Zhang, J.B.Lu, M.Mazzocco, Y.F.Lv, H.Q.Zhang, H.B.Sun, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, F.Recchia, D.Mengoni, D.Bazzacco, J.Lubian, X.B.Qin, H.M.Zhao Angular distribution of γ rays emitted by oriented nuclei: the case of 92Mo formed in the reaction 6Li + 89Y NUCLEAR REACTIONS 89Y(6Li, X)92Mo, E=34 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, J, π, γ-ray angular distributions, E1, M2 transition strengths, mixing ratios and T1/2. Comparison with the NushellX calculation using the jjglem interaction.
doi: 10.1140/epja/s10050-021-00443-6
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
2021RO14 Eur.Phys.J. A 57, 143 (2021) C.H.Rong, J.Rangel, Y.S.Wu, G.L.Zhang, G.X.Zhang, C.J.Lin, E.N.Cardozo, X.Y.Wang, L.Yang, N.R.Ma, D.X.Wang, L.J.Sun, H.M.Jia, F.Yang, J.S.Wang, Y.Y.Yang, J.B.Ma, P.Ma, Z.Bai, S.W.Xu, F.F.Duan, X.B.Qin, H.M.Zhao, J.Lubian Study of quasi-elastic scattering of 17F+208Pb at energies around Coulomb barrier NUCLEAR REACTIONS 208Pb(17F, 17F), E=94.5 MeV; measured reaction products. 17F; deduced σ(θ), σ. Comparison with continuum discretized coupled channel method (CDCC) calculations.
doi: 10.1140/epja/s10050-021-00454-3
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
2021SH23 Phys.Rev. C 103, L061301 (2021) G.Z.Shi, J.J.Liu, Z.Y.Lin, H.F.Zhu, X.X.Xu, L.J.Sun, P.F.Liang, C.J.Lin, J.Lee, C.X.Yuan, S.M.Wang, Z.H.Li, H.S.Xu, Z.G.Hu, Y.Y.Yang, R.F.Chen, J.S.Wang, D.X.Wang, H.Y.Wu, K.Wang, F.F.Duan, Y.H.Lam, P.Ma, Z.H.Gao, Q.Hu, Z.Bai, J.B.Ma, J.G.Wang, F.P.Zhong, C.G.Wu, D.W.Luo, Y.Jiang, Y.Liu, D.S.Hou, R.Li, N.R.Ma, W.H.Ma, G.M.Yu, D.Patel, S.Y.Jin, Y.F.Wang, Y.C.Yu, Q.W.Zhou, P.Wang, L.Y.Hu, X.Wang, H.L.Zang, P.J.Li, Q.R.Gao, H.Jian, S.X.Zha, F.C.Dai, R.Fan, Q.Q.Zhao, L.Yang, P.W.Wen, F.Yang, H.M.Jia, G.L.Zhang, M.Pan, X.Y.Wang, H.H.Sun, X.H.Zhou, Y.H.Zhang, M.Wang, M.L.Liu, H.J.Ong, W.Q.Yang β-delayed two-proton decay of 27S at the proton-drip line RADIOACTIVITY 27S(β+2p)[from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation and purification of fragments using RIBLL1 at HIRFL-Lanzhou facility, and implanted into three W1-type double-sided silicon strip detectors (DSSDs)]; measured reaction products, E(p), I(p), pp-coin, p(θ), half-life of 27S decay using Si detectors surrounded by HPGe detectors; deduced branching ratio of β+2p decay, identified as a two-proton transition, dominantly sequential, via the isobaric-analog state (IAS) in 27P to the ground state of 25Al.
doi: 10.1103/PhysRevC.103.L061301
2021YA01 Phys.Lett. B 813, 136045 (2021) L.Yang, C.J.Lin, H.Yamaguchi, J.Lei, P.W.Wen, M.Mazzocco, N.R.Ma, L.J.Sun, D.X.Wang, G.X.Zhang, K.Abe, S.M.Cha, K.Y.Chae, A.Diaz-Torres, J.L.Ferreira, S.Hayakawa, H.M.Jia, D.Kahl, A.Kim, M.S.Kwag, M.La Commara, R.Navarro-Perez, C.Parascandolo, D.Pierroutsakou, J.Rangel, Y.Sakaguchi, C.Signorini, E.Strano, X.X.Xu, F.Yang, Y.Y.Yang, G.L.Zhang, F.P.Zhong, J.Lubian Insight into the reaction dynamics of proton drip-line nuclear system 17F+58Ni at near-barrier energies NUCLEAR REACTIONS 58Ni(17F, 17F), (17F, X), E=43.6, 47.5, 55.7, 63.1 MeV; measured reaction products, Eα, Iα, Ep, Ip. 16O, 17F; deduced σ, σ(θ) quasielastic scattering and fusion.
doi: 10.1016/j.physletb.2020.136045
2021YA16 Chin.Phys.C 45, 054104 (2021) Y.-J.Yao, C.-J.Lin, L.Yang, N.-R.Ma, D.-X.Wang, G.-l.Zhang, G.-X.Zhang, H.-M.Jia, F.Yang, F.-P.Zhong, P.i-W.Wen, X.-B.Qin, H.-M.Zhao Relative probabilities of breakup channels in reactions of 6, 7Li with 209Bi at energies around and above the Coulomb barrier NUCLEAR REACTIONS 209Bi(6Li, X), (7Li, X), E=30, 40, 47 MeV; measured reaction products, Eα, Iα, Ep, Ip, α-p coin., α-α-coin.; deduced σ(E), relative probabilities of the breakup channels.
doi: 10.1088/1674-1137/abe3ee
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
2020LI06 Phys.Rev. C 101, 024305 (2020) P.F.Liang, L.J.Sun, J.Lee, S.Q.Hou, X.X.Xu, C.J.Lin, C.X.Yuan, J.J.He, Z.H.Li, J.S.Wang, D.X.Wang, H.Y.Wu, Y.Y.Yang, Y.H.Lam, P.Ma, F.F.Duan, Z.H.Gao, Q.Hu, Z.Bai, J.B.Ma, J.G.Wang, F.P.Zhong, C.G.Wu, D.W.Luo, Y.Jiang, Y.Liu, D.S.Hou, R.Li, N.R.Ma, W.H.Ma, G.Z.Shi, G.M.Yu, D.Patel, S.Y.Jin, Y.F.Wang, Y.C.Yu, Q.W.Zhou, P.Wang, L.Y.Hu, X.Wang, H.L.Zang, P.J.Li, Q.Q.Zhao, H.M.Jia, L.Yang, P.W.Wen, F.Yang, G.L.Zhang, M.Pan, X.Y.Wang, H.H.Sun, Z.G.Hu, R.F.Chen, M.L.Liu, W.Q.Yang, Y.M.Zhao Simultaneous measurement of β-delayed proton and γ emission of 26P for the 25Al(p, γ)26Si reaction rate RADIOACTIVITY 26P(β+), (β+p)[from 9Be(32S, X), E=806 MeV/nucleon, followed by in-flight separation by the RIBLL1 fragment separator at HIRFL-Lanzhou]; measured E(p), I(p), Eγ, Iγ, βp- and βγ-coin, half-life of the decay of 26P from correlated events of 26P implants and successive decays using three double-sided silicon strip detectors (DSSDs), five Clover-type HPGe detectors, and five quadrant silicon detectors (Q SDs). 26Si; deduced levels, J, π, Γp and Γγ of 5929, 3+ state. Comparison with previous experimental data, and with shell-model calculations. NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P, E=806 MeV/nucleon; measured reaction products and TOF-ΔE spectrum using in-flight separation by the RIBLL1 fragment separator at HIRFL-Lanzhou. 25Al(p, γ)26Si, T=0.03-1.1 GK; deduced energies and strengths of resonances, corresponding astrophysical reaction rates, and compared with data in JINA REACLIB database.
doi: 10.1103/PhysRevC.101.024305
2020LI12 Phys.Rev. C 101, 044313 (2020) C.B.Li, G.L.Zhang, C.X.Yuan, G.X.Zhang, S.P.Hu, W.W.Qu, Y.Zheng, H.Q.Zhang, D.Mengoni, D.Testov, J.J.Valiente-Dobon, H.B.Sun, N.Wang, X.G.Wu, G.S.Li, M.Mazzocco, A.Gozzelino, C.Parascandolo, D.Pierroutsakou, M.La Commara, F.Recchia, A.I.Sison, S.Bakes, I.Zanon, S.Aydin, D.Bazzacco New level scheme and shell model description of 212Rn NUCLEAR REACTIONS 209Bi(6Li, 3n)212Rn, E=28, 30, 34 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using GALILEO array at the Tandem-XTU accelerator of Legnaro National Laboratory. 212Rn; deduced levels, J, π, multipolarities, B(E2), B(E3), configurations. Comparison with large-scale shell-model calculations with multiparticle configurations. Systematics of low-, and medium-spin levels in N=126 isotones: 210Po, 212Rn, 214Ra and 216Th. Systematics of 3- to 0+ and 15/2- to 9/2+ excitation energies in N=126 and 127 isotones of Z=82-91. NUCLEAR STRUCTURE 212Rn; calculated levels, J, π, amplitudes of shell-model multiparticle configurations for different levels, B(M1), B(E2), B(E3) using large-scale shell-model calculations with multiparticle configurations. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.044313
2020LI28 Phys.Rev. C 102, 024301 (2020) J.J.Liu, J.Lee, H.Watanabe, S.Nishimura, G.X.Zhang, J.Wu, P.M.Walker, P.H.Regan, P.-A.Soderstrom, H.Kanaoka, Z.Korkulu, P.S.Lee, A.Yagi, A.C.Dai, F.R.Xu, D.S.Ahn, T.Alharbi, H.Baba, F.Browne, A.M.Bruce, R.J.Carroll, K.Y.Chae, Zs.Dombradi, P.Doornenbal, A.Estrade, N.Fukuda, C.Griffin, E.Ideguchi, N.Inabe, T.Isobe, S.Kanaya, I.Kojouharov, F.G.Kondev, T.Kubo, S.Kubono, N.Kurz, I.Kuti, S.Lalkovski, G.J.Lane, C.S.Lee, E.J.Lee, G.Lorusso, G.Lotay, C.-B.Moon, I.Nishizuka, C.R.Nita, A.Odahara, Z.Patel, V.H.Phong, Zs.Podolyak, O.J.Roberts, H.Sakurai, H.Schaffner, C.M.Shand, Y.Shimizu, T.Sumikama, H.Suzuki, H.Takeda, S.Terashima, Zs.Vajta, J.J.Valiente-Dobon, Z.Y.Xu Isomeric and β-decay spectroscopy of 173, 174Ho RADIOACTIVITY 173,174Ho(β-)[from 9Be(238U, F), E=345 MeV/nucleon, followed by separation of fission fragments using BigRIPS separator and ZeroDegree spectrometer and implantation in WAS3ABi at RIBF-RIKEN facility]; measured Eγ, Iγ, Eβ, conversion electrons, βγ-, (ce)γ- and γγ-coin, half-lives of 173Ho and 174Ho decays from γ-decay curves, half-life of an isomer in 173Ho using double-sided silicon strip detectors (DSSD) and the EURICA γ-ray spectrometer. 174Er; deduced levels, J, π, β feedings, logft, configurations. 173Ho; deduced level, isomer, J, π. 174Ho; deduced J, π and configuration of ground state. 173,174Ho, 173,174Er; calculated levels, J, π, deformation parameters β2, γ and β4, configurations using configuration-constrained potential energy surface (PES) calculations. Systematics of yrast g.s. bands in N=106 isotones: 172Dy, 174Er, 176Yb, 178Hf, 180W, 182Os. Systematics of experimental logft values in decays of 168Ho, 171,173Er, 174,176Tm, 178Lu. Systematics of Weisskopf hindrance factors in odd-A Ho isotopes: 159,161,163,165,167Ho.
doi: 10.1103/PhysRevC.102.024301
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
2020RO16 Chin.Phys.C 44, 104003 (2020) C.-H.Rong, G.-L.Zhang, L.Gan, Z.-Ho.Li, L.C.Brandao, E.N.Cardozo, M.R.Cortes, Y.-J.Li, Ju.Su, S.-Q.Yan, S.Zeng, G.Lian, B.Guo, Y.-B.Wang, W.-P.Liu, J.Lubian The angular distributions of elastic scattering of 12, 13C+Zr NUCLEAR REACTIONS 90,91,92,94,96Zr(12C, 12C), (13C, 13C), E=66, 64 MeV; measured reaction products; deduced σ, the neutron spectroscopic amplitudes using the optical model and coupled channel calculations.
doi: 10.1088/1674-1137/abab8d
2020WA07 Eur.Phys.J. A 56, 31 (2020) M.Wang, W.J.Sun, B.H.Sun, J.Li, L.H.Zhu, Y.Zheng, G.L.Zhang, L.C.He, W.W.Qu, F.Wang, T.F.Wang, C.Xiong, C.Y.He, G.S.Li, J.L.Wang, X.G.Wu, S.H.Yao, C.B.Li, H.W.Li, S.P.Hu, J.J.Liu The ΔI = 2 bands in 109In: possible antimagnetic rotation NUCLEAR REACTIONS 100Mo(14N, 5n), E=78 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using two low-energy photon detectors and nine BGO-Compton-suppressed HPGe detectors at CIAE-Beijing. 109In; deduced levels, J, π, multipolarities, anti-magnetic rotational band, alignments, configurations. Comparison with calculations using titled axis cranking calculation in the framework of covariant density function theory (TAC-CDFT), and with previous experimental results. Systematics of bands based on πg7/2 orbital in 107,109,111,113In. See also 2018Wa15, a related experiment from the same laboratory.
doi: 10.1140/epja/s10050-020-00039-6
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
2019CA04 Phys.Rev. C 99, 014606 (2019) X.G.Cao, E.J.Kim, K.Schmidt, K.Hagel, M.Barbui, J.Gauthier, S.Wuenschel, G.Giuliani, M.R.D.Rodriguez, S.Kowalski, H.Zheng, M.Huang, A.Bonasera, R.Wada, N.Blando, G.Q.Zhang, C.Y.Wong, A.Staszczak, Z.X.Ren, Y.K.Wang, S.Q.Zhang, J.Meng, J.B.Natowitz Examination of evidence for resonances at high excitation energy in the 7 α disassembly of 28Si NUCLEAR REACTIONS 12C(28Si, X), (28Si, 7α), E=35 MeV/nucleon; measured Eα, Iα, excitation functions for the α-conjugate exit channels using the 4π NIMROD-ISiS array for charged particle detection at the K500 superconducting cyclotron facility of Texas A and M. 28Si; deduced resonances at high excitation energies, shapes of 7α events in the de-excitation of projectile-like nuclei; calculated energies, J, π, configurations, quadrupole deformation of toroidal high-spin isomers using covariant functional PC-PK1 and DD-ME2.
doi: 10.1103/PhysRevC.99.014606
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
2019GH07 Nucl.Phys. A990, 294 (2019) Assessment of the quality of different pocket formulas in reproducing experimental sub-barrier fusion cross sections
doi: 10.1016/j.nuclphysa.2019.07.012
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
2019LA13 Astrophys.J. 879, 23 (2019) L.Lamia, M.Mazzocco, R.G.Pizzone, S.Hayakawa, M.La Cognata, C.Spitaleri, C.A.Bertulani, A.Boiano, C.Boiano, C.Broggini, A.Caciolli, S.Cherubini, G.D'Agata, H.da Silva, R.Depalo, F.Galtarossa, G.L.Guardo, M.Gulino, I.Indelicato, M.La Commara, G.La Rana, R.Menegazzo, J.Mrazek, A.Pakou, C.Parascandolo, D.Piatti, D.Pierroutsakou, S.M.R.Puglia, S.Romano, G.G.Rapisarda, A.M.Sanchez-Benitez, M.L.Sergi, O.Sgouros, F.Soramel, V.Soukeras, R.Sparta, E.Strano, D.Torresi, A.Tumino, H.Yamaguchi, G.L.Zhang Cross-section Measurement of the Cosmologically Relevant 7Be(n, α)4He Reaction over a Broad Energy Range in a Single Experiment NUCLEAR REACTIONS 2H(7Be, 2α), E<2 MeV; measured reaction products, Ep, Ip. 8Be; deduced σ, astrophysical reaction rates. Trojan Horse Method.
doi: 10.3847/1538-4357/ab2234
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
2019LV02 Chin.Phys.C 43, 104102 (2019) Y.-F.Lv, J.-B.Lu, G.-L.Zhang, Y.-H.Wu, C.-X.Yuan, G.-J.Fu, G.-X.Zhang, Z.Huang, M.-L.Wang, S.-P.Hu, H.-B.Sun, H.-Q.Zhang, C.-Q.Li, K.-Y.Ma, Y.-J.Ma, Yu.-Z.Liu, D.Testov, P.R.John, J.J.Valiente-Dobon, A.Goasduff, M.Siciliano, F.Galtarossa, F.Recchia, D.Mengoni, D.Bazzacco Low-lying states of 92, 93Nb excited in the reactions induced by the weakly-bound nucleus 6Li near the Coulomb barrier NUCLEAR REACTIONS 89Y(6Li, X)92Nb/93Nb, E=34 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, level schemes.
doi: 10.1088/1674-1137/43/10/104102
2019MA46 Eur.Phys.J. A 55, 87 (2019) N.R.Ma, L.Yang, C.J.Lin, H.Yamaguchi, D.X.Wang, L.J.Sun, M.Mazzocco, H.M.Jia, S.Hayakawa, D.Kahl, S.M.Cha, G.X.Zhang, F.Yang, Y.Y.Yang, C.Signorini, Y.Sakaguchi, K.Abe, M.La Commara, D.Pierroutsakou, C.Parascandolo, E.Strano, A.Kim, K.Y.Chae, M.S.Kwag, G.L.Zhang, M.Pan, X.X.Xu, P.W.Wen, F.P.Zhong, H.H.Sun, G.Guo MITA: A Multilayer Ionization-chamber Telescope Array for low-energy reactions with exotic nuclei NUCLEAR REACTIONS 58Ni(17F, 17F'), E=55.7 MeV; measured ToF of different isotopes recorded by MITA, reaction products; deduced protons and α counts vs E, σ(θ) vs θ.
doi: 10.1140/epja/i2019-12765-7
2019WA24 Int.J.Mod.Phys. E28, 1950039 (2019) K.Wang, A.Bonasera, H.Zheng, G.Q.Zhang, Y.G.Ma, W.Q.Shen The role of the Heisenberg principle in constrained molecular dynamics model NUCLEAR REACTIONS 12C(p, p), E<250 MeV; 197Au(197Au, X), E=35 MeV/nucleon; 238U(238U, X), E=15 MeV/nucleon; analyzed available data; calculated σ(θ), charge density distributions.
doi: 10.1142/S0218301319500393
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
2019ZH22 Chin.Phys.C 43, 064102 (2019) S.Zhang, J.C.Wang, A.Bonasera, M.R.Huang, H.Zheng, G.Q.Zhang, Z.Kohley, Y.G.Ma, S.J.Yennello Triple α-particle resonances in the decay of hot nuclear systems NUCLEAR REACTIONS 70Zn(70Zn, X), 64Zn(64Zn, X)12C, E=35 MeV/nucleon; analyzed available data. 8Be; deduced 3α systems, relative energies, Efimov states.
doi: 10.1088/1674-1137/43/6/064102
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
2019ZH49 Phys.Lett. B 799, 135036 (2019) G.X.Zhang, H.Watanabe, G.D.Dracoulis, F.G.Kondev, G.J.Lane, P.H.Regan, P.-A.Soderstrom, P.M.Walker, K.Yoshida, H.Kanaoka, Z.Korkulu, P.S.Lee, J.J.Liu, S.Nishimura, J.Wu, A.Yagi, D.S.Ahn, T.Alharbi, H.Baba, F.Browne, A.M.Bruce, M.P.Carpenter, R.J.Carroll, K.Y.Chae, C.J.Chiara, Zs.Dombradi, P.Doornenbal, A.Estrade, N.Fukuda, C.Griffin, E.Ideguchi, N.Inabe, T.Isobe, S.Kanaya, I.Kojouharov, T.Kubo, S.Kubono, N.Kurz, I.Kuti, S.Lalkovski, T.Lauritsen, C.S.Lee, E.J.Lee, C.J.Lister, G.Lorusso, G.Lotay, E.A.McCutchan, C.-B.Moon, I.Nishizuka, C.R.Nita, A.Odahara, Z.Patel, V.H.Phong, Zs.Podolyak, O.J.Roberts, H.Sakurai, H.Schaffner, D.Seweryniak, C.M.Shand, Y.Shimizu, T.Sumikama, H.Suzuki, H.Takeda, S.Terashima, Zs.Vajta, J.J.Valiente-Dobon, Z.Y.Xu, S.Zhu Interplay of quasiparticle and vibrational excitations: First observation of isomeric states in 168Dy and 169Dy RADIOACTIVITY 168,169Dy(β-) [from be(238U, X), E=345 MeV/nucleon]; measured decay products, Eγ, Iγ, X-rays; deduced level energies, J, π, B(E2), isomer T1/2. Comparison with deformed QRPA and multi-quasiparticle calculations.
doi: 10.1016/j.physletb.2019.135036
2018CO08 Phys.Rev. C 97, 044613 (2018) G.Colucci, G.Montagnoli, A.M.Stefanini, H.Esbensen, D.Bourgin, P.Colovic, L.Corradi, M.Faggian, E.Fioretto, F.Galtarossa, A.Goasduff, J.Grebosz, F.Haas, M.Mazzocco, F.Scarlassara, C.Stefanini, E.Strano, S.Szilner, M.Urbani, G.L.Zhang Isotopic effects in sub-barrier fusion of Si + Si systems NUCLEAR REACTIONS 30Si(30Si, X), E=47-90 MeV; measured fusion evaporation residues (ERs), fusion σ(E) at the XTU tandem accelerator facility of LNL-INFN-Legnaro. Comparison with previous experimental results, 28Si+28Si data, and with theoretical calculations using coupled-channels method with aM3Y+repulsion potential, and including one- and two-phonon excitations and the mutual excitations of the low-lying 2+ and 3- states in projectiles and targets.
doi: 10.1103/PhysRevC.97.044613
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
2018MO05 Phys.Rev. C 97, 024610 (2018) G.Montagnoli, A.M.Stefanini, C.L.Jiang, K.Hagino, F.Galtarossa, G.Colucci, S.Bottoni, C.Broggini, A.Caciolli, P.Colovic, L.Corradi, S.Courtin, R.Depalo, E.Fioretto, G.Fruet, A.Gal, A.Goasduff, M.Heine, S.P.Hu, M.Kaur, T.Mijatovic, M.Mazzocco, D.Montanari, F.Scarlassara, E.Strano, S.Szilner, G.X.Zhang Fusion hindrance for the positive Q-value system 12C+30Si NUCLEAR REACTIONS 12C(30Si, X), E=34-80 MeV; measured reaction products, fusion σ(E) at the XTU Tandem accelerator of INFN-LN, Legnaro. Comparison with coupled-channel calculations using Woods Saxon (WS) and Yukawa-plus-exponential (YPE) potentials.
doi: 10.1103/PhysRevC.97.024610
2018QU04 Chin.Phys.C 42, 074001 (2018) W.-W.Qu, G.-L.Zhang, G.-Y.Tian, Z.-Q.Chen, S.-P.Xu, R.Wada Angular distribution measurement for 12C fragmentation via 12C + 12C scattering at 100 MeV/u NUCLEAR REACTIONS 12C(12C, X)9Be/10B/11B, E=100 MeV/nucleon; measured reaction products; deduced σ(θ). Comparison with theoretical calculations.
doi: 10.1088/1674-1137/42/7/074001
2018TE06 Phys.Rev.Lett. 121, 242501 (2018) S.Terashima, L.Yu, H.J.Ong, I.Tanihata, S.Adachi, N.Aoi, P.Y.Chan, H.Fujioka, M.Fukuda, H.Geissel, G.Gey, J.Golak, E.Haettner, C.Iwamoto, T.Kawabata, H.Kamada, X.Y.Le, H.Sakaguchi, A.Sakaue, C.Scheidenberger, R.Skibinski, B.H.Sun, A.Tamii, T.L.Tang, D.T.Tran, K.Topolnicki, T.F.Wang, Y.N.Watanabe, H.Weick, H.Witala, G.X.Zhang, L.H.Zhu Dominance of Tensor Correlations in High-Momentum Nucleon Pairs Studied by (p, pd) Reaction NUCLEAR REACTIONS 16O(p, pd), E=392 MeV; measured reaction products; deduced σ, σ(θ, E), isospin character of p-n pairs at large relative momentum. Comparison with the DWIA calculations.
doi: 10.1103/PhysRevLett.121.242501
2018WA15 Phys.Rev. C 98, 014304 (2018), Erratum Phys.Rev. C 102, 069903 (2020) M.Wang, Y.Y.Wang, L.H.Zhu, B.H.Sun, G.L.Zhang, L.C.He, W.W.Qu, F.Wang, T.F.Wang, Y.Y.Chen, C.Xiong, J.Zhang, J.M.Zhang, Y.Zheng, C.Y.He, G.S.Li, J.L.Wang, X.G.Wu, S.H.Yao, C.B.Li, H.W.Li, S.P.Hu, J.J.Liu New high-spin structure and possible chirality in 109In NUCLEAR REACTIONS 100Mo(14N, 5n), E=78 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) using two low-energy photon detectors and nine BGO-Compton-suppressed HPGe detectors at CIAE-Beijing. 109In; deduced levels, J, π, multipolarities, bands, alignments, configurations, and possible chiral partner bands. Comparison with calculations using titled axis cranking calculation in the framework of covariant density function theory (TAC-CDFT), and with previous experimental results. Systematics of yrast states in 103,105,107,109,111,113In.
doi: 10.1103/PhysRevC.98.014304
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
2018ZH06 Phys.Rev. C 97, 014611 (2018) G.L.Zhang, G.X.Zhang, S.P.Hu, Y.J.Yao, J.B.Xiang, H.Q.Zhang, J.Lubian, J.L.Ferreira, B.Paes, E.N.Cardozo, H.B.Sun, J.J.Valiente-Dobon, D.Testov, A.Goasduff, P.R.John, M.Siciliano, F.Galtarossa, R.Francesco, D.Mengoni, D.Bazzacco, E.T.Li, X.Hao, W.W.Qu One-neutron stripping processes to excited states of 90Y* in the 89Y(6Li, 5Li)90Y* reaction NUCLEAR REACTIONS 89Y(6Li, 5Li)90Y*, E=22, 34 MeV; measured in-beam and off-beam Eγ, Iγ, γγ- and pγ-coin, ΔE-E for protons, deuterons, tritons, and α particles, one-neutron stripping σ(E) using GALILEO array for γ rays and 4π Si-ball EUCLIDES for particles at the Tandem-XTU accelerator of Legnaro National Laboratory. 90Y, 93Mo; deduced level schemes. Comparisons of cross sections with parameter-free coupled reaction channel calculations.
doi: 10.1103/PhysRevC.97.014611
2018ZH18 Phys.Rev. C 97, 044618 (2018) G.L.Zhang, G.X.Zhang, C.J.Lin, J.Lubian, J.Rangel, B.Paes, J.L.Ferreira, H.Q.Zhang, W.W.Qu, H.M.Jia, L.Yang, N.R.Ma, L.J.Sun, D.X.Wang, L.Zheng, X.X.Liu, X.T.Chu, J.C.Yang, J.S.Wang, S.W.Xu, P.Ma, J.B.Ma, S.L.Jin, Z.Bai, M.R.Huang, H.L.Zang, B.Yang, Y.Liu Angular distribution of elastic scattering induced by 17F on medium-mass target nuclei at energies near the Coulomb barrier NUCLEAR REACTIONS 89Y(17F, 17F), E=50, 59 MeV, [17F secondary beam from 1H(17O, n), E=7.6 MeV/nucleon primary reaction]; measured reaction products, 17F scattered particles, differential σ(θ, E) using DSSD and SSD detector telescopes at RIBLL facility in Lanzhou. 16F, 90Zr; calculated spectroscopic amplitudes for excited levels in the coupled reaction channels (CRC) formalism for one-proton transfer reactions using the Sao Paulo double-folding potential. Comparison with Continuum-discretized coupled-Channels (CDCC) calculations.
doi: 10.1103/PhysRevC.97.044618
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
2017GU08 Acta Phys.Pol. B48, 601 (2017) L.A.Gurgi, P.H.Regan, P.-A.Soderstrom, H.Watanabe, P.M.Walker, Zs.Podolyak, S.Nishimura, T.A.Berry, P.Doornenbal, G.Lorusso, T.Isobe, H.Baba, Z.Y.Xu, H.Sakurai, T.Sumikama, W.N.Catford, A.M.Bruce, F.Browne, G.J.Lane, F.G.Kondev, A.Odahara, J.Wu, H.L.Liu, F.R.Xu, Z.Korkulu, P.Lee, J.J.Liu, V.H.Phong, A.Yagi, G.X.Zhang, T.Alharbi, R.J.Carroll, K.Y.Chae, Zs.Dombradi, A.Estrade, N.Fukuda, C.Griffin, E.Ideguchi, N.Inabe, H.Kanaoka, I.Kojouharov, T.Kubo, S.Kubono, N.Kurz, I.Kuti, S.Lalkovski, E.J.Lee, C.S.Lee, G.Lotay, C.B.Moon, I.Nishizuka, C.R.Nita, Z.Patel, O.J.Roberts, H.Schaffner, C.M.Shand, H.Suzuki, H.Takeda, S.Terashima, Zs.Vajta, S.Kanaya, J.J.Valiente-Dobon Isomer Spectroscopy of Neutron-rich 165, 167Tb NUCLEAR REACTIONS 9Be(238U, f), E=345 MeV/nucleon; measured fission products β-delayed discrete Eγ, Iγ, X-rays, γγ-coin, Xγ-coin using HPGe. 165,167Tb; deduced neutron-rich deformed nuclei γ-ray spectra, levels, J, π, isomeric states interpreted as hindered E1 decay from single quasi-proton Nilsson configuration to rotational states built on single quasi-proton gs, levels populated in isomeric decays.
doi: 10.5506/APhysPolB.48.601
2017GU24 Radiat.Phys.Chem. 140, 493 (2017) L.A.Gurgi, P.H.Regan, P.-A.Soderstrom, H.Watanabe, P.M.Walker, Zs.Podolyak, S.Nishimura, T.A.Berry, P.Doornenbal, G.Lorusso, T.Isobe, H.Baba, Z.Y.Xu, H.Sakurai, T.Sumikama, W.N.Catford, A.M.Bruce, F.Browne, G.J.Lane, F.G.Kondev, A.Odahara, J.Wu, H.L.Liu, F.R.Xu, Z.Korkulu, P.Lee, J.J.Liu, V.H.Phong, A.Yag, G.X.Zhang, T.Alharbi, R.J.Carroll, K.Y.Chae, Zs.Dombradi, A.Estrade, N.Fukuda, C.Griffin, E.Ideguchi, N.Inabe, H.Kanaoka, I.Kojouharov, T.Kubo, S.Kubono, N.Kurz, I.Kuti, S.Lalkovski, E.J.Lee, C.S.Lee, G.Lotay, C.-B.Moon, I.Nishizuka, C.R.Nita, Z.Patel, O.J.Roberts, H.Schaffner, C.M.Shand, H.Suzuki, H.Takeda, S.Terashima, Zs.Vajta, S.Yoshida, J.J.Valiente-Dobon Isomer spectroscopy of neutron-rich 168Tb103 NUCLEAR REACTIONS 9Be(238U, X)168Tb, E=350 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, isomeric state T1/2. Comparison with blocked BCS pairing Nilsson calculations for a well-deformed prolate shape, available data.
doi: 10.1016/j.radphyschem.2016.12.011
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
2017LI28 Nucl.Instrum.Methods Phys.Res. B410, 158 (2017) L.X.Liu, H.W.Wang, Y.G.Ma, X.G.Cao, X.Z.Cai, J.G.Chen, G.L.Zhang, J.L.Han, G.Q.Zhang, J.F.Hu, X.H.Wang, W.J.Li, Z.Yan, H.J.Fu Measurements of the total cross section of natBe with thermal neutrons from a photo-neutron source NUCLEAR REACTIONS 9Be(n, X), E=0.007-0.1 eV; measured reaction products, En, In, time-of-flight; deduced σ. Comparison with available data.
doi: 10.1016/j.nimb.2017.08.022
2017LV01 Phys.Rev. C 95, 024614 (2017) M.Lv, Y.G.Ma, J.H.Chen, D.Q.Fang, G.Q.Zhang Medium effect on the nuclear modification factor of protons and pions in intermediate-energy heavy ion collisions
doi: 10.1103/PhysRevC.95.024614
2017QU02 Phys.Rev. C 95, 044616 (2017) W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto Repulsive three-body force and channel-coupling effects via 12C+12C scattering at 100A MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=100 MeV/nucleon; measured scattered 12C using Grand Raiden high-resolution magnetic spectrometer, and 10B, 11C and other particles by the energy loss and time-of-flight (TOF) information, differential cross sections for the ground state, 4.44 MeV, 2+ state, and the sum of the 7.65 MeV, 0+ and the 9.64 MeV, 3- states in 12C using the Ring Cyclotron facility at RCNP-Osaka. Comparison with microscopic coupled-channel calculations, using the double folding method with three different complex G-matrix interactions, the ESC, CEG07b, and MPa.
doi: 10.1103/PhysRevC.95.044616
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
2017WA05 Phys.Rev. C 95, 014608 (2017) K.Wang, Y.G.Ma, G.Q.Zhang, X.G.Cao, W.B.He, W.Q.Shen Giant dipole resonance in proton capture reactions using an extended quantum molecular dynamics model NUCLEAR REACTIONS 11B(p, γ)12C, E=30-60 MeV; 27Al(p, γ)28Si, E=30-90 MeV; 39K(p, γ)40Ca, E=25-80 MeV; , 67Co(p, γ)68Ni, E=20-90 MeV; calculated GDR γ spectra, GDR parameters such as peak energies, strengths, and FWHM, dipole moments and temperature of the proton-capture systems as functions of incident energies, GDR width as a function of temperature. Extended quantum molecular dynamics (EQMD) model for giant dipole resonance in proton capture reactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.014608
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
2017WU04 Phys.Rev.Lett. 118, 072701 (2017) J.Wu, S.Nishimura, G.Lorusso, P.Moller, E.Ideguchi, P.-H.Regan, G.S.Simpson, P.-A.Soderstrom, P.M.Walker, H.Watanabe, Z.Y.Xu, H.Baba, F.Browne, R.Daido, P.Doornenbal, Y.F.Fang, G.Gey, T.Isobe, P.S.Lee, J.J.Liu, Z.Li, Z.Korkulu, Z.Patel, V.Phong, S.Rice, H.Sakurai, L.Sinclair, T.Sumikama, M.Tanaka, A.Yagi, Y.L.Ye, R.Yokoyama, G.X.Zhang, T.Alharbi, N.Aoi, F.L.Bello Garrote, G.Benzoni, A.M.Bruce, R.J.Carroll, K.Y.Chae, Z.Dombradi, A.Estrade, A.Gottardo, C.J.Griffin, H.Kanaoka, I.Kojouharov, F.G.Kondev, S.Kubono, N.Kurz, I.Kuti, S.Lalkovski, G.J.Lane, E.J.Lee, T.Lokotko, G.Lotay, C.-B.Moon, H.Nishibata, I.Nishizuka, C.R.Nita, A.Odahara, Zs.Podolyak, O.J.Roberts, H.Schaffner, C.Shand, J.Taprogge, S.Terashima, Z.Vajta, S.Yoshida 94 β-Decay Half-Lives of Neutron-Rich 55Cs to 67Ho: Experimental Feedback and Evaluation of the r-Process Rare-Earth Peak Formation RADIOACTIVITY 144,145,146,147,148,149,150,151Cs, 146,147,148,149,150,151,152,153,154Ba, 148,149,150,151,152,153,154,155,156La, 150,151,152,153,154,155,156,157,158Ce, 153,154,155,156,157,158,159,160Pr, 156,157,158,159,160,161,162Nd, 159,160,161,162,163Pm, 160,161,162,163,164,165,166Sm, 161,162,163,164,165,166,167,168Eu, 165,166,167,168,169,170Gd, 166,167,168,169,170,171,172Tb, 169,170,171,172,172m,173Dy, 172,173,174,175Ho, 174mEr(β-)[from Be(238U, X), E=345 MeV/nucleon]; measured and analyzed reaction products using BigRIPS separator and ZeroDegree Spectrometer (ZDS), γ rays, half-lives by (implant)β correlations using WAS3ABi and EURICA detection systems at RIBF-RIKEN facility; deduced Gamow-Teller strength functions, r-process abundance pattern in the solar system. Comparison with previous experimental half-lives, and with three theoretical calculations using FRDM+QRPA, KTUY+GT2, and RHB+pn-RQRPA models. Numerical values of half-lives listed in supplementary file.
doi: 10.1103/PhysRevLett.118.072701
2016FA10 Phys.Rev. C 94, 044621 (2016) D.Q.Fang, Y.G.Ma, X.Y.Sun, P.Zhou, Y.Togano, N.Aoi, H.Baba, X.Z.Cai, X.G.Cao, J.G.Chen, Y.Fu, W.Guo, Y.Hara, T.Honda, Z.G.Hu, K.Ieki, Y.Ishibashi, Y.Ito, N.Iwasa, S.Kanno, T.Kawabata, H.Kimura, Y.Kondo, K.Kurita, M.Kurokawa, T.Moriguchi, H.Murakami, H.Ooishi, K.Okada, S.Ota, A.Ozawa, H.Sakurai, S.Shimoura, R.Shioda, E.Takeshita, S.Takeuchi, W.D.Tian, H.W.Wang, J.S.Wang, M.Wang, K.Yamada, Y.Yamada, Y.Yasuda, K.Yoneda, G.Q.Zhang, T.Motobayashi Proton-proton correlations in distinguishing the two-proton emission mechanism of 23Al and 22Mg NUCLEAR REACTIONS 12C(23Al, 2pX), (23Al, 2p21Na), (23Al, 2p20Ne), E=57.4 MeV/nucleon; 12C(22Mg, 2pX), (22Mg, 2p20Ne), E=53.5 MeV/nucleon, [secondary 22Mg and 23Al beams from 12C(28Si, X), E=135 MeV/nucleon primary reaction]; measured fragments and protons using ΔE-E detectors at RIBF-RIKEN facility; deduced proton-proton momentum correlation function for decays into p+p+X, p+p+20Na, and p+p+21Na channels, effective source sizes from calculations using the CRAB code with a Gaussian source, mechanism of two-proton emission.
doi: 10.1103/PhysRevC.94.044621
2016GU16 Phys.Rev. C 94, 044605 (2016) M.F.Guo, G.L.Zhang, P.R.S.Gomes, J.Lubian, E.Ferioli Negligible suppression of the complete fusion of 6, 7Li on light targets, at energies above the barrier NUCLEAR REACTIONS 12,13C, 16O, 24Mg(6Li, X), (7Li, X), E=2-12 MeV; calculated complete fusion σ(E) using coupled-channel (CC) approach. Comparison with from predictions of the statistical evaporation code CASCADE, and with experimental values. Discussed breakup process and breakup threshold anomaly (BTA).
doi: 10.1103/PhysRevC.94.044605
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