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Search: Author = J.J.Li

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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, 69}V, 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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 - ^{243,244,245,246,247,248}No.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, 267-269}Lr 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)=1.10V_c; 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)=1.10V_c; calculated production σ for Pt isotopes. ^{209,210,211,212}Pt; 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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