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    Zhang Tian-Cheng, Pan Gao-Yuan, Yu You-Jun, Dong Chen-Zhong, Ding Xiao-Bin
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    • The ionization energy of the superheavy element Og ( Z= 118) and its homolog elements Ar, Kr, Xe, Rn, and their ions are systematically calculated by using the GRASP2K program based on the multi-configuration Dirac-Hartree-Fock (MCDHF) method, taking into account relativistic effects, electron correlation effects between valence shell electrons, quantum electrodynamics effects, and Breit interaction. To reduce the uncertainty of the ionization energy derived from electron correlation effects which are not fully considered, the ionization potential of the superheavy element Og 0–2+and its homolog element Rn 0–2+are extrapolated by the extrapolation method. The ionization energy of extrapolated Rn 0–5+and Og 5+coincide well with experimental and other theoretical values. These results can be used to predict the unknown physical and chemical properties of the atoms and compounds of the superheavy element Og. In addition, the calculation results of the electron orbital binding energy of the atomic valence shell of the superheavy element Og and its homolog elements Ar, Kr, Xe, and Rn under relativistic and non-relativistic conditions show that owing to the relativistic effect, there occur strong orbital contraction phenomena in the 7s orbital and 7p 1/2orbital and strong splitting phenomena in the 7p 1/2orbital and 7p 3/2orbital of Og, which may cause the physical and chemical properties of the superheavy element Og to differ from those of other homologs.
          Corresponding author:Dong Chen-Zhong,dongcz@nwnu.edu.cn; Ding Xiao-Bin,dingxb@nwnu.edu.cn
        • Funds:Project supported by the National Key R&D Program of China (Grant No. 2017YFA0402300), the National Natural Science Foundation of China (Grant Nos. U1832126, 11874051), the Funds for Innovative Fundamental Research Group Project of Gansu Province, China (Grant No. 20JR5RA541), and the Doctoral Research Funds of Lanzhou City University, China (Grant No. LZCU-BS2019-50).
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      • 电子组态 关联模型 活动空间 组态波函数数目
        Og (J= 0+)
        [Rn]5f146d107s27p6 DHF {n7l1} 1
        7SD {n7l2} 14
        8SD 7SD + {n8l3} 143
        9SD 8SD + {n9l4} 468
        10SD 9SD + {n10l4} 987
        11SD 10SD + {n11l4} 1700
        12SD 11SD + {n12l4} 2607
        Og1+(J= 3/2)
        [Rn]5f146d107s27p5 DHF {n7l1} 1
        7SD {n7l2} 51
        8SD 7SD + {n8l3} 758
        9SD 8SD + {n9l4} 2738
        10SD 9SD + {n10l4} 5982
        11SD 10SD + {n11l4} 10490
        12SD 11SD + {n12l4} 16262
        Og2+(J= 2+)
        [Rn]5f146d107s27p4 DHF {n7l1} 2
        7SD {n7l2} 76
        8SD 7SD + {n8l3} 1054
        9SD 8SD + {n9l4} 3841
        10SD 9SD + {n10l4} 8404
        11SD 10SD + {n11l4} 14743
        12SD 11SD + {n12l4} 22858
        Og3+(J= 3/2)
        [Rn]5f146d107s27p3 DHF {n7l1} 3
        7SD {n7l2} 66
        8SD 7SD + {n8l3} 802
        9SD 8SD + {n9l4} 2816
        10SD 9SD + {n10l4} 6094
        11SD 10SD + {n11l4} 10636
        12SD 11SD + {n12l4} 16442
        Og4+(J= 0+)
        [Rn]5f146d107s27p2 DHF {n7l1} 2
        7SD {n7l2} 22
        8SD 7SD + {n8l3} 163
        9SD 8SD + {n9l4} 500
        10SD 9SD + {n10l4} 1031
        11SD 10SD + {n11l4} 1756
        12SD 11SD + {n12l4} 2675
        Og5+(J= 1/2)
        [Rn]5f146d107s27p1 DHF {n7l1} 1
        7SD {n7l2} 13
        8SD 7SD + {n8l3} 96
        9SD 8SD + {n9l4} 293
        10SD 9SD + {n10l4} 606
        11SD 10SD + {n11l4} 1035
        12SD 11SD + {n12l4} 1580
        Og6+(J= 0+)
        [Rn]5f146d107s2 DHF {n7l1} 1
        7SD {n7l2} 5
        8SD 7SD + {n8l3} 17
        9SD 8SD + {n9l4} 38
        10SD 9SD + {n10l4} 68
        11SD 10SD + {n11l4} 107
        12SD 11SD + {n12l4} 155
        DownLoad: CSV

        元素 MCDHF NIST[48] α β 外推值 误差 Others
        IP1
        Ar 15.50 15.76* 0.26
        Kr 13.74 14.00* 0.26 0.00
        Xe 11.85 12.13* 0.28 0.02
        Rn 10.48 10.75* (0.32) (0.04) 10.80 0.04 10.76[12]
        Og 8.53 (0.38) (0.06) 8.91 0.06 8.86[13]
        8.87[20]
        8.91[22]
        8.84[23]
        8.88[12]
        IP2
        Ar 27.36 27.63* 0.27
        Kr 24.06 24.36* 0.30 0.03
        Xe 20.63 20.98* 0.35 0.05
        Rn 18.65 21.40±1.90 (0.42) (0.07) 19.07 0.07 18.99[12]
        Og 15.80 (0.51) (0.09) 16.31 0.09 16.19[12]
        IP3
        Ar 40.45 40.74*±0.01 0.29
        Kr 35.49 35.84*±0.02 0.35 0.06
        Xe 30.60 31.05*±0.04 0.45 0.10
        Rn 28.21 29.40±1.00 (0.59) (0.14) 28.80 0.14
        Og 24.28 (0.77) (0.18) 25.05 0.18
        IP4
        Ar 58.96 59.58±0.18 0.62
        Kr 50.48 50.85*±0.11 0.37
        Xe 42.11 42.20*±0.20 0.09
        Rn 37.88 36.90±1.70 (0.44) 38.32 1.53
        Og 32.70 (0.55) 33.25 0.99
        IP5
        Ar 74.60 74.84±0.17 0.24
        Kr 64.08 64.69*±0.20 0.61
        Xe 54.38 54.10*±0.50 –0.28
        Rn 52.83 52.90±1.90 (0.44) 53.27 2.13
        Og 55.37 (0.55) 55.92 2.24
        IP6
        Ar 91.13 91.29* 0.16
        Kr 78.07 78.49*±0.20 0.42
        Xe 66.16 66.70* 0.54
        Rn 64.42 64.00±2.00 (0.44) 64.86 2.59
        Og 67.04 (0.55) 67.59 2.70
        DownLoad: CSV

        轨道 Ar Kr Xe Rn Og
        R NR R NR R NR R NR R NR
        $ {n\mathrm{s}}_{1/2} $ 1.29 1.28 1.19 1.15 1.01 0.94 1.07 0.87 1.30 0.77
        $ {n\mathrm{p}}_{1/2} $ 0.60 0.59 0.54 0.52 0.49 0.46 0.54 0.43 0.74 0.39
        $ {n\mathrm{p}}_{3/2} $ 0.59 0.59 0.51 0.52 0.44 0.46 0.38 0.43 0.31 0.39
        DownLoad: CSV
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      Metrics
      • Abstract views:3418
      • PDF Downloads:60
      • Cited By:0
      Publishing process
      • Received Date:25 April 2022
      • Accepted Date:05 July 2022
      • Available Online:22 October 2022
      • Published Online:05 November 2022

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