NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of April 27, 2024.

Search: Author = X.R.Zhang

Found 9 matches.

Back to query form

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics