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NSR database version of April 11, 2024.

Search: Author = Z.H.Wu

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2023WU05      Nucl.Phys. A1036, 122671 (2023)

Z.-H.Wu, H.-B.Fu, T.Zhong, D.Huang, D.-D.Hu, X.-G.Wu

α0(980)-meson twist-2 distribution amplitude within the QCD sum rules and investigation of D → α0(980)(→ ηπ)e+ ve

doi: 10.1016/j.nuclphysa.2023.122671
Citations: PlumX Metrics


2019CH53      J.Radioanal.Nucl.Chem. 322, 1605 (2019)

Y.Chen, S.-H.Huang, R.i-X.Hu, Y.-G.Zhao, L.-L.Li, J.-J.Zhou, C.Li, J.-L.Zhang, Z.-H.Wu

Age determination for uranium standard samples by 231Pa/235U radiochronometer

doi: 10.1007/s10967-019-06922-x
Citations: PlumX Metrics


2018LI33      Phys.Rev. C 98, 014618 (2018)

F.Li, L.Zhu, Z.-H.Wu, X.-B.Yu, J.Su, C.-C.Guo

Predictions for the synthesis of superheavy elements Z=119 and 120

NUCLEAR REACTIONS 238U, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-60 MeV; calculated evaporation residue σ(E), and compared with available experimental data. 252Es(40Ca, 3n), E(cm)=204.08 MeV; 252Es(42Ca, 3n), E(cm)=203.00 MeV; 249Cf(45Sc, 3n), E(cm)=211.09 MeV; 255Es(40Ca, 4n), E(cm)=207.02 MeV; 254Es(40Ca, 3n), E(cm)=203.60 MeV; 247Bk(47Ti, 3n), E(cm)=219.19 MeV; 248Bk(46Ti, 3n), E(cm)=217.76 MeV; 242Cm(51V, 2n), E(cm)=225.86 MeV; 248Cf(45Sc, 2n), E(cm)=209.29 MeV; 241Am(52Cr, 2n), E(cm)=231.94 MeV; 252Es(44Ca, 3n), E(cm)=204.27 MeV; 253Es(43Ca, 3n), E(cm)=202.49 MeV; 254Es(42Ca, 3n), E(cm)=201.65 MeV; 251Cf(45Sc, 3n), E(cm)=210.03 MeV; 249Bk(47Ti, 3n), E(cm)=217.18 MeV; 248Bk(48Ti, 3n), E(cm)=219.47 MeV; 245Cm(51V, 3n), E(cm)=229.29 MeV; 247Bk(49Ti, 3n), E(cm)=222.17 MeV; 246Cm(50V, 3n), E(cm)=225.70 MeV; 244Cm(51V, 2n), E(cm)=224.00 MeV; 255Es(42Ca, 4n), E(cm)=205.95 MeV; 243Am(53Cr, 3n), E(cm)=236.20 MeV; 254Es(43Ca, 4n), E(cm)=206.90 MeV; 253Es(44Ca, 4n), E(cm)=210.94 MeV; 243Am(52Cr, 2n), E(cm)=229.49 MeV; 254Es(44Ca, 3n), E(cm)=201.64 MeV; 255Es(43Ca, 3n), E(cm)=201.49 MeV; 255Es(44Ca, 4n), E(cm)=207.59 MeV; 252Es(46Ca, 3n), E(cm)=206.00 MeV; 248Bk(50Ti, 3n), E(cm)=222.48 MeV; 247Cm(51V, 3n), E(cm)=226.83 MeV; 254Cf(45Sc, 4n), E(cm)=211.93 MeV; 249Bk(49Ti, 3n), E(cm)=218.88 MeV; 254Es(46Ca, 3n), E(cm)=203.64 MeV; 255Es(46Ca, 4n), E(cm)=210.13 MeV; 252Es(48Ca, 3n), E(cm)=208.42 MeV; 255Es(46Ca, 3n), E(cm)=204.13; 254Es(48Ca, 3n), E(cm)=205.96 MeV; 255Es(48Ca, 4n), E(cm)=212.72 MeV; 242Cm(50Cr, 2n), E(cm)=234.22 MeV; 249Cf(46Ti, 3n), E(cm)=222.89 MeV; 248Cf(46Ti, 2n), E(cm)=219.12 MeV; 257Fm(40Ca, 5n), E(cm)=222.66 MeV; 257Fm(40Ca, 4n), E(cm)=211.66 MeV; 257Fm(40Ca, 3n), E(cm)=205.66 MeV; 251Cf(46Ti, 3n), E(cm)=220.39 MeV; 252Es(45Sc, 3n), E(cm)=214.17 MeV; 250Cf(46Sc, 2n), E(cm)=218.88 MeV; 247Bk(50V, 3n), E(cm)=231.13 MeV; 244Cm(52Cr, 2n), E(cm)=234.88 MeV; 245Cm(52Cr, 3n), E(cm)=240.80 MeV; 243Cm(53Cr, 2n), E(cm)=236.02 MeV; 247Cm(50Cr, 3n), E(cm)=235.12 MeV; 257Fm(42Ca, 3n), E(cm)=205.29 MeV; 254Es(45Sc, 3n), E(cm)=213.40 MeV; 257Fm(43Ca, 4n), E(cm)=210.97 MeV; 257Fm(44Ca, 3n), E(cm)=205.27 MeV; 257Fm(46Ca, 3n), E(cm)=207.84 MeV; 250Cm(53Cr, 3n), E(cm)=234.59 MeV; 257Fm(48Ca, 3n), E(cm)=211.07 MeV; calculated production σ for Z=119 and 120 superheavy isotopes. Dinuclear system (DNS) model.

doi: 10.1103/PhysRevC.98.014618
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2018WU06      Phys.Rev. C 97, 064609 (2018)

Z.-H.Wu, L.Zhu, F.Li, X.-B.Yu, J.Su, C.-C.Guo

Synthesis of neutron-rich superheavy nuclei with radioactive beams within the dinuclear system model

NUCLEAR REACTIONS 242,244Pu, 243Am, 245,248,250Cm, 249Bk, 250,251Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-60 MeV; 234Th(42S, 2n), (42S, 3n), (42S, 4n), (42S, 5n), E*=20-65 MeV; 234Th, 244Pu(46Ar, 2n), (46Ar, 3n), (46Ar, 4n), (46Ar, 5n), E*=20-65 MeV; 234Th, 238U, 248Cm, 255Es(44Cl, 2n), (44Cl, 3n), (44Cl, 4n), (44Cl, 5n), E*=20-65 MeV; 228Ra(45Cl, 2n), (45Cl, 3n), (45Cl, 4n), (45Cl, 5n), E*=20-65 MeV; 244Pu, 248Cm(43Cl, 2n), (43Cl, 3n), (43Cl, 4n), (43Cl, 5n), E*=20-65 MeV; 244Pu, 254Cf, 255Es(41S, 2n), (41S, 3n), (41S, 4n), (41S, 5n), E*=20-65 MeV; 257Fm(42Ar, 2n), (42Ar, 3n), (42Ar, 4n), (42Ar, 5n), E*=20-65 MeV; 260Md(38Cl, 2n), (38Cl, 3n), (38Cl, 4n), (38Cl, 5n), E*=20-65 MeV; calculated evaporation residue σ. 228Ra(45Cl, 2n), E*=36.0 MeV; 228Ra(46Cl, 3n), E*=46.0 MeV; 226Ra(47Cl, 2n), E*=36.0 MeV; 234Th(42S, 4n), E*=43.0 MeV; 228Ra(46Ar, 2n), E*=34.0 MeV; 234Th(43S, 5n), E*=51.0 MeV; 234Th(42S, 3n), E*=41.0 MeV; 234Th(43S, 4n), E*=46.0 MeV; 234Th(44S, 5n), E*=59.0 MeV; 234Th(44Cl, 2n), E*=37.0 MeV; 234Th(45Cl, 3n), E*=44.0 MeV; 228Ra(50K, 2n), E*=36.0 MeV; 234Th(46Ar, 2n), E*=34.0 MeV; 238U(43S, 3n), E*=41.0 MeV; 238U(42S, 2n), E*=37.0 MeV; 238U(44Cl, 3n), E*=38.0 MeV; 238U(43Cl, 2n), E*=36.0 MeV; 238U(43S, 3n), E*=41.0 MeV; 234Th(47K, 2n), E*=33.0 MeV; 244Pu(41S, 3n), E*=38.0 MeV; 244Pu(42S, 4n), E*=42.0 MeV; 238U(46Ar, 2n), E*=33.0 MeV; 244Pu(43Cl, 4n), E*=44.0 MeV; 242Pu(44Cl, 3n), E*=37.0 MeV; 244Pu(42Cl, 3n), E*=38.0 MeV; 244Pu(46Ar, 4n), E*=38.0 MeV; 244Pu(45Ar, 3n), E*=44.0 MeV; 242Pu(46Ar, 2n), E*=33.0 MeV; 248Cm(43Cl, 4n), E*=38.0 MeV; 250Cm(42Cl, 5n), E*=43.0 MeV; 248Cm(44Cl, 5n), E*=43.0 MeV; 248Cm(44Cl, 4n), E*=38.0 MeV; 250Cm(42Cl, 4n), E*=39.0 MeV; 250Cm(43Cl, 5n), E*=45.0 MeV; 254Cf(41S, 5n), E*=40.0 MeV; 253Cf(42S, 5n), E*=40.0 MeV; 250Cm(44Ar, 4n), E*=37.0 MeV; 255Es(41S, 5n), E*=40.0 MeV; 254Cf(42Cl, 5n), E*=40.0 MeV; 253Cf(43Cl, 5n), E*=39.0 MeV; 255Es(41S, 4n), E*=37.0 MeV; 253Cf(43Cl, 4n), E*=36.0 MeV; 254Cf(42Cl, 4n), E*=37.0 MeV; 250Cm(48Ca, 4n), E*=35.0 MeV; 248Cm(48Ca, 2n), E*=31.0 MeV; 250Cm(46Ca, 2n), E*=35.0 MeV; 255Es(44Cl, 5n), E*=40.0 MeV; 254Cf(44Ar, 4n), E*=36.0 MeV; 257Fm(41S, 4n), E*=37.0 MeV; 250Cm(48Ca, 3n), E*=31.0 MeV; 255Es(44Cl, 4n), E*=36.0 MeV; 253Cf(46Ar, 4n), E*=34.0 MeV; 254Cf(46Ar, 5n), E*=41.0 MeV; 250Cf(48Ca, 3n), E*=34.0 MeV; 250Cm(49Ti, 4n), E*=42.0 MeV; 252Cf(46Ca, 3n), E*=36.0 MeV; 260Md(38Cl, 3n), E*=41.0 MeV; 260Md(39Cl, 4n), E*=42.0 MeV; 257Fm(42Ar, 4n), E*=41.0 MeV; 251Cf(48Ca, 3n), E*=30.0 MeV; 252Cf(48Ca, 4n), E*=38.0 MeV; 250Cm(49Ti, 3n), E*=34.0 MeV; 257Fm(42Ar, 3n), E*=33.0 MeV; 257Fm(43Ar, 4n), E*=38.0 MeV; 260Md(39Cl, 3n), E*=37.0 MeV; 244Pu(43Cl, n), E*=40.0 MeV; 238Cm(48Ca, 2np), E*=41.0 MeV; 254Cf(41S, 5n), E*=40.0 MeV; 248Cm(48Ca, 2nα), E*=46.0 MeV; 248Cm(43Cl, 4n), E*=38.0 MeV; 242Pu(48Ca, 2np), E*=35.0 MeV; 248Cm(44Cl, 4n), E*=38.0 MeV; 242Pu(48Ca, np), E*=40.0 MeV; 244Pu(48Ca, 3np), E*=45.0 MeV; 255Es(41S, 5n), E*=40.0 MeV; 245Cm(48Ca, np), E*=32.0 MeV; 249Bk(48Ca, 2nα), E*=37.0 MeV; 255Es(41S, 4n), E*=37.0 MeV; 248Cm(48Ca, 3np), E*=44.0 MeV; 249Bk(48Ca, nα), E*=32.0 MeV; calculated evaporation residue σ, and optimal incident beam energies. 48Ca(238U, 2n), (238U, 3n), (238U, 4n), E(cm)=184.13-214.13 MeV; calculated evaporation residue σ, potential energy surface, driving potential, survival and complete fusion probabilities, and capture σ. Dinuclear system model. 271Db, 272,273Sg, 276Bh, 278Hs, 279Mt, 282Ds, 283Rg, 286Cn, 287,288Nh, 290Fl, 291,292Mc, 294,295Lv, 295,296Og; calculated evaporation residue σ, and optimal incident beam energies for various reactions. Comparison with available experimental data. Relevance to synthesis of neutron-rich superheavy nuclei using radioactive ion beams, such as those at ATLAS-ANL.

doi: 10.1103/PhysRevC.97.064609
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