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NSR database version of April 11, 2024.

Search: Author = J.J.Li

Found 29 matches.

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2023LI17      Int.J.Mod.Phys. E32, 2330002 (2023)

J.-J.Li, N.Tang, Y.-H.Zhang, M.-H.Zhang, C.Wang, X.-R.Zhang, L.Zhu, F.-S.Zhang

Progress on production cross-sections of unknown nuclei in fusion evaporation reactions and multinucleon transfer reactions

NUCLEAR REACTIONS 232Th(204Hg, X), E(cm)=678.1 MeV; 249Bk(238U, X), E(cm)=823.4 MeV; 248Cm(238U, X), E(cm)=824.9 MeV; calculated σ in fusion evaporation (FE) reactions and multinucleon transfer (MNT) reactions.

doi: 10.1142/S0218301323300023
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2023LI44      Phys.Rev. C 108, 025810 (2023)

J.J.Li, A.Sedrakian, F.Weber

Universal relations for compact stars with heavy baryons

doi: 10.1103/PhysRevC.108.025810
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2023LI65      Astrophys.J. 957, 41 (2023)

J.-J.Li, A.Sedrakian

New Covariant Density Functionals of Nuclear Matter for Compact Star Simulations

doi: 10.3847/1538-4357/acfa73
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2023TA03      Phys.Rev. C 107, 014603 (2023)

N.Tang, B.Li, J.-J.Li, F.-S.Zhang

Production of 61Ca, 63Sc, 65Ti, 68, 69V, 71Cr, 77Fe and 79Co in projectile fragmentation with radioactive ion beams at 1A GeV

NUCLEAR REACTIONS 9Be(69Cu, X)37Ar/38Ar/39Ar/40Ar/41Ar/42Ar/43Ar/44Ar/39K/40K/41K/42K/43K/44K/45K/46K/41Ca/42Ca/43Ca/44Ca/45Ca/46Ca/47Ca/43Sc/44Sc/45Sc/46Sc/47Sc/48Sc/49Sc/50Sc/45Ti/46Ti/47Ti/48Ti/49Ti/50Ti/51Ti/52Ti/48V/49V/50V/51V/52V/53V/54V/55V/50Cr/51Cr/52Cr/53Cr/54Cr/55Cr/56Cr/57Cr/53Mn/54Mn/55Mn/56Mn/57Mn/58Mn/59Mn, E=98.1 MeV/nucleon; calculated isotopes production σ. 9Be(81Ga, X)48Ca/49Ca/50Ca/51Ca/52Ca/53Ca/54Ca/55Ca/56Ca/49Sc/50Sc/51Sc/52Sc/53Sc/54Sc/55Sc/56Sc/57Sc/58Sc/59Sc/60Sc/52Ti/53Ti/54Ti/55Ti/56Ti/57Ti/58Ti/59Ti/60Ti/61Ti/62Ti/63Ti/56V/57V/58V/59V/60V/61V/62V/63V/64V/65V/56Cr/57Cr/58Cr/59Cr/60Cr/61Cr/62Cr/63Cr/64Cr/65Cr/66Cr/67Cr/59Mn/60Mn/61Mn/62Mn/63Mn/64Mn/65Mn/66Mn/67Mn/68Mn/69Mn/62Fe/63Fe/64Fe/65Fe/66Fe/67Fe/68Fe/69Fe/70Fe/71Fe/72Fe/64Co/65Co/66Co/67Co/68Co/69Co/70Co/71Co/72Co/73Co, E=1 GeV/nucleon; 9Be(84Ga, X)48Ca/49Ca/50Ca/51Ca/52Ca/53Ca/54Ca/55Ca/56Ca/57Ca/58Ca/59Ca/60Ca/51Sc/52Sc/53Sc/54Sc/55Sc/56Sc/57Sc/58Sc/59Sc/60Sc/61Sc/53Ti/54Ti/55Ti/56Ti/57Ti/58Ti/59Ti/60Ti/61Ti/62Ti/63Ti/64Ti/57V/58V/59V/60V/61V/62V/63V/64V/65V/66V/58Cr/59Cr/60Cr/61Cr/62Cr/63Cr/64Cr/65Cr/66Cr/67Cr/68Cr/69Cr/60Mn/61Mn/62Mn/63Mn/64Mn/65Mn/66Mn/67Mn/68Mn/69Mn/70Mn/71Mn/72Mn/64Fe/65Fe/66Fe/67Fe/68Fe/69Fe/70Fe/71Fe/72Fe/73Fe/74Fe/75Fe/66Co/67Co/68Co/69Co/70Co/71Co/72Co/73Co/74Co/75Co/76Co/77Co, E=1 GeV/nucleon; 9Be(86Ga, X)48Ca/49Ca/50Ca/51Ca/52Ca/53Ca/54Ca/55Ca/56Ca/57Ca/58Ca/59Ca/60Ca/61Ca/51Sc/52Sc/53Sc/54Sc/55Sc/56Sc/57Sc/58Sc/59Sc/60Sc/61Sc/62Sc/63Sc/54Ti/55Ti/56Ti/57Ti/58Ti/59Ti/60Ti/61Ti/62Ti/63Ti/64Ti/65Ti/57V/58V/59V/60V/61V/62V/63V/64V/65V/66V/67V/68V/69V/59Cr/60Cr/61Cr/62Cr/63Cr/64Cr/65Cr/66Cr/67Cr/68Cr/69Cr/70Cr/71Cr/62Mn/63Mn/64Mn/65Mn/66Mn/67Mn/68Mn/69Mn/70Mn/71Mn/72Mn/73Mn/74Mn/75Mn/65Fe/66Fe/67Fe/68Fe/69Fe/70Fe/71Fe/72Fe/73Fe/74Fe/75Fe/76Fe/77Fe/67Co/68Co/69Co/70Co/71Co/72Co/73Co/74Co/75Co/76Co/77Co/78Co/79Co, E=1 GeV/nucleon; calculated isotopes production σ. Isospin-dependent Boltzmann-Langevin equation (IBLE) model. Comparison of model predictions with experimental data for 9Be(69Cu, X) reaction.

doi: 10.1103/PhysRevC.107.014603
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2023ZH09      Phys.Rev. C 107, 024604 (2023)

Y.-H.Zhang, J.-J.Li, N.Tang, X.-R.Zhang, Z.Liu, F.-S.Zhang

Production cross sections of new neutron-rich isotopes with Z=92-106 in the multinucleon transfer reaction 197Au + 232Th

NUCLEAR REACTIONS 232Th(197Au, X)258Es/259Es/260Es/261Es/262Es/260Fm/261Fm/262Fm/263Fm/261Md/262Md/263Md/264Md/265Md/261No/263No/264No/265No/266No/267No/263Lr/265Lr/267Lr/268Lr/264Rf/266Rf/268Rf/269Rf/270Rf/264Db/265Db/269Db/271Db/267Sg/268Sg/270Sg/272Sg/273Sg, E(cm)=690.69;232Th(197Au, X)243U/244U/245U/246U/247U/248U/249U/246Np/247Np/248Np/249Np/250Np/251Np/252Np/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/254Pu/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/256Am/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/252Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/257Cf/258Cf/259Cf/260Cf/261Cf/258Es/259Es/260Es/261Es/262Es, E(cm)=756.47 MeV; calculated production σ. 232Th(197Au, X), E=690.7, 723.6, 756.5 MeV;232Th(186W, X), E=681, 2 MeV;232Th(238U, X), E=823.8; calculated final isotopic production σ for U, Np, Pu, Am, Cm, Bk, Cf, Es, Fm, Md, No, Lr, Rf, Db and Sg isotopes, calculated driving potentials, potential energy surfaces. 232Th(197Au, X), E=690.7, 723.6, 756.5, 789.4 MeV; interaction time as a function of the impact parameter. 249Cf(136Xe, X), E(cm)=567 MeV; calculated final production σ for Pu, Am, Cm, Bk, Cf, Es isotopes. Calculations performed within the framework of dinuclear system (DNS) model with a decay model GEMINI++. Comparison to experimental data.

doi: 10.1103/PhysRevC.107.024604
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2022HA10      Phys.Rev. C 105, 044302 (2022)

J.X.Han, Y.Liu, Y.L.Ye, J.L.Lou, X.F.Yang, T.Baba, M.Kimura, B.Yang, Z.H.Li, Q.T.Li, J.Y.Xu, Y.C.Ge, H.Hua, Z.H.Yang, J.S.Wang, Y.Y.Yang, P.Ma, Z.Bai, Q.Hu, W.Liu, K.Ma, L.C.Tao, Y.Jiang, L.Y.Hu, H.L.Zang, J.Feng, H.Y.Wu, S.W.Bai, G.Li, H.Z.Yu, S.W.Huang, Z.Q.Chen, X.H.Sun, J.J.Li, Z.W.Tan, Z.H.Gao, F.F.Duan, J.H.Tan, S.Q.Sun, Y.S.Song

Observation of the π2σ2-bond linear-chain molecular structure in 16C

NUCLEAR REACTIONS 2H(16C, X)16C/2H/1H/2H/3H/3He/4He/5He/6He/6Li/7Li/8Li/9Li/7Be/8Be/9Be/10Be/11Be/12Be, E=23.5 MeV/nucleon; measured reaction products, recoil 2H, 8Be and other outgoing particles; deduced Q-value spectra for breakup of excited states of 16C into 4He+12Be and 6He+10Be channels, angular correlation between 4He and 12Be decay fragments from the 16.5 MeV resonance in 16C, and 6He and 10Be fragments from the 19.4 MeV resonance in 16C. 16C; deduced excitation energy spectra reconstructed from 4He+12Be+2 H and 6He+10Be+2H channels, levels, resonances, total width. Comparison with previous experimental data, and with antisymmetrized molecular dynamics (AMD) theoretical calculations. Secondary 16C beam produced in 9Be(18O, X), E=59.6 MeV/nucleon primary reaction at the HIRFL-RIBLL facility in Lanzhou.

doi: 10.1103/PhysRevC.105.044302
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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
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2022TA17      Phys.Rev. C 106, 034601 (2022)

N.Tang, X.-R.Zhang, J.-J.Li, P.-W.Wen, F.-S.Zhang

Production of unknown neutron-rich isotopes with Z=99-102 in multinucleon transfer reactions near the Coulomb barrier

NUCLEAR REACTIONS 248Cm(86Kr, X)235Am/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/245Fm/246Fm/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm , E(cm)=386 MeV; calculated capture probability, isotopic production σ, σ dependence on angular momentum of 251Es and 254Fm reaction products. 249Cf(112Sn, X)230Bk/231Bk/232Bk/233Bk/234Bk/235Bk/236Bk/237Bk/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/231Cf/232Cf/233Cf/234Cf/235Cf/236Cf/237Cf/238Cf/239Cf/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/239Es/240Es/241Es/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/240Fm/241Fm/242Fm/243Fm/244Fm/245Fm/246Fm/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm, E=475 MeV; 249Cf(124Sn, X)238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/237Cf/238Cf/239Cf/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/239Es/240Es/241Es/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es/240Fm/241Fm/242Fm/243Fm/244Fm/245Fm/246Fm/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm/258Fm/259Fm/260Fm/261Fm/262Fm, E=468 MeV; 249Cf(132Sn, X)239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/259Cf/260Cf/261Cf/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es/261Es/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm/258Fm/259Fm/260Fm/261Fm/262Fm/263Fm/264Fm/265Fm/250Md/251Md/252Md/253Md/254Md/255Md/256Md/257Md/258Md/259Md/260Md/261Md/262Md/263Md/264Md/265Md/266Md/253No/254No/255No/256No/257No/258No/259No/260No/261No/262No/263No/264No/265No/266No/267No/268No, E=463 MeV; calculated isotope production σ, driving potential. Theoretical framework of a hybrid model combining the dinuclear system model and the GRAZING model. Comparison to experimental data.

doi: 10.1103/PhysRevC.106.034601
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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
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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
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2021YU04      Chin.Phys.C 45, 084002 (2021)

H.-z.Yu, J.Li, Y.-L.Ye, B.Yang, C.-J.Lin, H.-M.Jia, J.-L.Lou, X.-F.Yang, T.Baba, Q.-T.Li, Y.-C.Ge, Z.-H.Li, H.Hua, J.-Y.Xu, Z.-H.Yang, J.Feng, H.-L.Zang, Q.Liu, W.Jiang, Y.Liu, J.-J.Li, W.Liu, S.-W.Bai, J.Chen, J.-X.Han, J.-H.Chen, K.Ma, D.-X.Wang, L.Yang, N.-R.Ma, L.-J.Sun

Novel evidence for the σ-bond linear-chain molecular structure in 14C

NUCLEAR REACTIONS 7Li(11B, α)14C, E=55 MeV; measured reaction products, Eα, Iα. 4He, 10Be; deduced Q-values, energy levels, J, π. Comparison with theoretically predicted band head of the positive-parity σ-bond linear-chain molecular band.

doi: 10.1088/1674-1137/ac04a0
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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
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2020LI14      Phys.Rev.Lett. 124, 192501 (2020)

Y.Liu, Y.L.Ye, J.L.Lou, X.F.Yang, T.Baba, M.Kimura, B.Yang, Z.H.Li, Q.T.Li, J.Y.Xu, Y.C.Ge, H.Hua, J.S.Wang, Y.Y.Yang, P.Ma, Z.Bai, Q.Hu, W.Liu, K.Ma, L.C.Tao, Y.Jiang, L.Y.Hu, H.L.Zang, J.Feng, H.Y.Wu, J.X.Han, S.W.Bai, G.Li, H.Z.Yu, S.W.Huang, Z.Q.Chen, X.H.Sun, J.J.Li, Z.W.Tan, Z.H.Gao, F.F.Duan, J.H.Tan, S.Q.Sun, Y.S.Song

Positive-Parity Linear-Chain Molecular Band in 16C

NUCLEAR REACTIONS 2H(16C, X)2H, E=23.5 MeV/nucleon; measured reaction products, Eα, Iα. 16C; deduced excitation energies, spin parities, total decay widths of the resonances in 16C. Comparison with AMD calculations.

doi: 10.1103/PhysRevLett.124.192501
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2020LI51      Phys.Rev. C 102, 064601 (2020)

J.J.Li, C.A.Bertulani, Y.Liu, J.L.Lou, D.Y.Pang, X.H.Sun, B.Yang, X.F.Yang, Y.L.Ye

Eikonal method for charge-exchange reactions at intermediate energies

NUCLEAR REACTIONS 26Mg, 120Sn(3He, t), E=140 MeV/nucleon; 13C(13N, 13C), E=105 MeV/nucleon; calculated differential σ(θ) and relativistic kinematical quantities for intermediate and high energy heavy-ion charge exchange reactions using Eikonal method and the DWBA model, with effective nucleon-nucleon interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.064601
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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
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2019GE09      Phys.Rev. C 100, 051301 (2019)

J.Geng, J.J.Li, W.H.Long, Y.F.Niu, S.Y.Chang

Pseudospin symmetry restoration and the in-medium balance between nuclear attractive and repulsive interactions

NUCLEAR STRUCTURE 48Ca, 90Zr, 132Sn, 208Pb, 310126; calculated Proton shell gaps and the splittings of the neighboring pseudospin symmetry (PS) partners using RMF Lagrangians PKA1, PKO3, and the RMF ones DD-ME2, PK1, NL3*, and compared with available experimental data. 208Pb; calculated contributions to the binding energy from various channels given by the RHF Lagrangian PKA1, proton pseudospin orbital (PSO) splittings using PKA1, PKO3, DD-ME2, and the tentative parametrizations. Relativistic Hartree-Fock (RHF) approach.

doi: 10.1103/PhysRevC.100.051301
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2019LI01      Phys.Lett. B 788, 192 (2019)

J.J.Li, W.H.Long, J.Margueron, N.Van Giai

48Si: An atypical nucleus?

NUCLEAR STRUCTURE 48Si; calculated energy levels, J, π, pairing gap, the onset of doubly magicity using the relativistic Hartree-Fock Lagrangian PKA1.

doi: 10.1016/j.physletb.2018.11.034
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2019LI15      Astrophys.J. 874, L22 (2019)

J.J.Li, A.Sedrakian

Implications from GW170817 for δ-isobar Admixed Hypernuclear Compact Stars

doi: 10.3847/2041-8213/ab1090
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2019LI48      Chin.Phys.C 43, 124102 (2019)

J.-J.Li, D.-Y.Pang, Y.-L.Ye, J.-L.Lou, X.-F.Yang, Y.Liu, B.Yang

Improved eikonal approach for charge exchange reactions at intermediate energies

NUCLEAR REACTIONS 12,13C, 26Mg, 120Sn(3He, 3He), (3He, t), E=140 MeV/nucleon; calculated σ(θ). Comparison with available data.

doi: 10.1088/1674-1137/43/12/124102
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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
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2019YA07      Phys.Rev. C 99, 064315 (2019)

B.Yang, Y.L.Ye, J.Feng, C.J.Lin, H.M.Jia, Z.H.Li, J.L.Lou, Q.T.Li, Y.C.Ge, X.F.Yang, H.Hua, J.Li, H.L.Zang, Q.Liu, W.Jiang, C.G.Li, Y.Liu, Z.Q.Chen, H.Y.Wu, C.G.Wang, W.Liu, X.Wang, J.J.Li, D.W.Luo, Y.Jiang, S.W.Bai, J.Y.Xu, N.R.Ma, L.J.Sun, D.X.Wang, Z.H.Yang, J.Chen

Investigation of the 14C+ α molecular configuration in 18O by means of transfer and sequential decay reaction

NUCLEAR REACTIONS 9Be(13C, α)18O*, E=65 MeV; measured recoil α particles and the two decay fragments 14C+α using an array of six charged-particle telescopes, Eα, Iα, (recoil)α-coin, αα-coin, invariant- and missing-mass spectrum, and angular correlation for the 10.3-MeV (4+) state at the HI-13 tandem accelerator of CIAE-Beijing. 18O; deduced levels, 14C+α resonant states, total widths, J, π, α-decay branching ratios, bands. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.99.064315
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2019YA09      Chin.Phys.C 43, 084001 (2019)

B.Yang, Y.-L.Ye, J.-L.Lou, X.-F.Yang, J.-J.Li, Y.Liu, W.Liu, H.-Z.Yu

Spin determination by in-plane angular correlation analysis in various coordinate systems

NUCLEAR STRUCTURE 18O; analyzed available data; deduced J, π.

doi: 10.1088/1674-1137/43/8/084001
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2018LI45      Eur.Phys.J. A 54, 133 (2018)

J.J.Li, W.H.Long, A.Sedrakian

Hypernuclear stars from relativistic Hartree-Fock density functional theory

doi: 10.1140/epja/i2018-12566-6
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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
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2018ZH59      Sci. Rep. 8, 4121 (2018)

L.Q.Zhang, C.H.Zhang, J.J.Li, Y.C.Meng, Y.T.Yang, Y.Song, Z.N.Ding, T.X.Yan

Damage to epitaxial GaN layer on Al2O3 by 290-MeV 238U32+ ions irradiation

NUCLEAR REACTIONS Ga, N(238U, X), E=290 MeV; measured reaction products; deduced the nano-hillocks, Al, O, and C elements appear on the GaN surface, along with a spiral-like, layered volcanic-cone structure formed at the highest-fluence irradiation, dislocation density increase, no N and Ga vacancies. Atomic force microscopy (AFM), scanning electron microscopy (SEM), high-resolution X-ray diffraction (HRXRD), and Raman scattering spectroscopy.

doi: 10.1038/s41598-018-22321-w
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2017BE16      Phys.Rev. C 96, 024304 (2017)

M.Belabbas, J.J.Li, J.Margueron

Finite-temperature pairing re-entrance in the drip-line nucleus 48Ni

NUCLEAR STRUCTURE 48Ni; calculated temperature-averaged proton pairing gap versus temperature based on SLY4-5 and SIII Skyrme interactions, proton pairing gap as function of the temperature based on FT-RHFB PKA1 and PKO3 effective Lagrangians, temperature evolution of proton quasiparticle energies corresponding to states around the Fermi energy. Finite-temperature Hartree-Fock-Bogoliubov (FT-HFB) and relativistic Hartree-Fock-Bogoliubov (FT-RHFB) theories.

doi: 10.1103/PhysRevC.96.024304
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2016LI02      Phys.Lett. B 753, 97 (2016)

J.J.Li, J.Margueron, W.H.Long, N.Van Giai

Magicity of neutron-rich nuclei within relativistic self-consistent approaches

NUCLEAR STRUCTURE 24O, 48Si, 52,54Ca; calculated single particle energies, spin orbital splittings; deduce magicity. Relativistic Hartree-Fock-Bogoliubov theory.

doi: 10.1016/j.physletb.2015.12.004
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2015LI25      Phys.Rev. C 92, 014302 (2015)

J.J.Li, J.Margueron, W.H.Long, N.Van Giai

Pairing phase transition: A finite-temperature relativistic Hartree-Fock-Bogoliubov study

NUCLEAR STRUCTURE 124Sn; calculated neutron pairing gaps, density, binding energy, compression modulus, symmetry energy, and nonrelativistic effective masses, critical temperature and the occupation number of continuum states, contributions of the continuum states to the pairing and neutron numbers. Z=20-50, N=50; Z=32-76, N=82; Z=52-98, N=126; Z=28, N=22-68; Z=50, N=46-126; Z=82, N=96-184; calculated and compared critical temperatures in FT-RHFB with PKA1, PKO1, DD-ME2 and the Gogny pairing interaction D1S. 68Ni, 174Sn; calculated neutron pairing gaps as a function of temperature using FT-RHFB with Gogny D1S and DDCI pairing forces, and FT-RHF-BCS with DDCI pairing force. 120,160Sn; calculated entropy and specific heat as a function of temperature using FT-RH(F)B and FTRH(F) theories and several different interactions. Self-consistent finite-temperature RHFB (FT-RHFB) theory in a Dirac Woods-Saxon (DWS) basis with a large number of Lagrangians.

doi: 10.1103/PhysRevC.92.014302
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2013LI51      Chin.Phys.C 37, 114101 (2013)

C.Li, J.-L.Tian, Y.-J.Qin, J.-J.Li, N.Wang

Determination of the nucleon-nucleon interaction in the ImQMD model by nuclear reactions at the Fermi energy region

NUCLEAR REACTIONS 40Ca(40Ca, X), E=10-45 MeV/nucleon; 120Sn(129Xe, X), E=32, 45 MeV/nucleon; 197Au(197Au, X), E=35, 50 MeV/nucleon; 197Au(238U, X), E=15 MeV/nucleon; calculated charge fragment distribution, multiplicity. Improved quantum molecular dynamic model.

doi: 10.1088/1674-1137/37/11/114101
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