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B2+和B+离子的静态偶极极化率和超极化率的理论研究

陈池婷 吴磊 王霞 王婷 刘延君 蒋军 董晨钟

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B2+和B+离子的静态偶极极化率和超极化率的理论研究

陈池婷, 吴磊, 王霞, 王婷, 刘延君, 蒋军, 董晨钟

Theoretical study of static dipole polarizabilities and hyperpolarizability of B2+ and B+ ions

Chen Chi-Ting, Wu Lei, Wang Xia, Wang Ting, Liu Yan-Jun, Jiang Jun, Dong Chen-Zhong
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  • 利用相对论组态相互作用模型势方法计算了B2+和B+离子的波函数、能级和振子强度, 进一步得到B2+离子2s1/2, 2p1/2, 2p3/2, 3s1/2态的电偶极极化率和基态2s1/2的超极化率, 以及B+离子2s2 1S0与2s2p 3P0态的电偶极极化率. B2+离子2p1/2和2p3/2的偶极极化率为负值, 基态2s1/2的超极化率的贡献主要来自于与极化率相关的$ {{\rm{\alpha }}}^{1}{{\rm{\beta }}}_{0} $项. 对于B+离子, 钟跃迁2s2p 3P0 → 2s2 1S0在室温下的黑体辐射频移是0.01605 Hz, 该黑体辐射频移比碱土金属原子的钟跃迁黑体辐射频移小1—2个数量级.
    The wave functions, energy levels, and oscillator strengths of B2+ ions and B+ ions are calculated by using a relativistic potential model, which is named the relativistic configuration interaction plus core polarization (RCICP) method.The presently calculated energy levels are in very good agreement with experimental energy levels tabulated in NIST Atomic Spectra Database, with difference no more than 0.05%.The presently calculated oscillator strengths agree very well with NIST and some available theoretical results. The difference is no more than 0.6%. By using these energy levels and oscillator strengths, the electric-dipole static polarizability of the 2s1/2, 2p1/2, 2p3/2, and 3s1/2 state and static hyperpolarizability of the ground state 2s1/2 for B2+ ion, as well as electric-dipole static polarizability of the 2s2 1S0 state and 2s2p 3P0 state for B+ ion are determined, respectively. The polarizability of the 2p1/2 state and 2p3/2 state of B2+ ion are negative. The main reason is that the absorption energy of the 2p1/2,3/2 → 2s1/2 resonance transition is negative. The contribution to the polarizability of the 2p1/2 state and 2p3/2 state are both negative. For the tensor polarizability of the 2p3/2 state, the main contribution from the 2p3/2 → 2s1/2 transition and 2p3/2 → 3d5/2 transition are 2.4963 a.u. and –0.2537 a.u., respectively, and the present RCICP result is 2.1683 a.u. The largest contribution to the hyperpolarizability of the ground state 2s1/2 originates from the term of $ {\alpha }^{1}{\beta }_{0} $. The electric-dipole static polarizability of the 2s2 1S0 state and 2s2p 3P0 state of B+ ion are 9.6220 a.u. and 7.7594 a.u., respectively. The presently calculated blackbody radiation (BBR) shift of the 2s2p 3P0 → 2s2 1S0 clock transition is 0.01605 Hz. This BBR shift is one or two orders of magnitude smaller than that for alkaline-earth-metal atom.
      通信作者: 蒋军, phyjiang@yeah.net
    • 基金项目: 国家重点研发计划(批准号: 2022YFA1602500)、国家自然科学基金(批准号: 12174316)、西北师范大学青年教师科研能力提升计划(批准号: NWNU-LKQN2020-10)和甘肃省创新基础研究群体项目基金(批准号: 20JR5RA541)资助的课题.
      Corresponding author: Jiang Jun, phyjiang@yeah.net
    • Funds: Project supported by the National Key Research and Development Program of China (Grant No. 2022YFA1602500), the National Natural Science Foundation of China (Grant No. 12174316), the Young Teachers Scientific Research Ability Promotion Plan of Northwest Normal University, China (Grant No. NWNU-LKQN2020-10), and the Funds for Innovative Fundamental Research Group Project of Gansu Province, China (Grant No. 20JR5RA541).
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  • 表 1  B2+离子的截断参数$ {\rho }_{l, j} $(单位: a.u.)

    Table 1.  Cut-off parameters $ {\rho }_{l, j} $ of B2+ ions (in a.u.).

    Statej$ {\rho }_{l, j} $
    2s1/20.72951
    2p1/20.67398
    3/20.67164
    3d3/20.91441
    5/20.91355
    下载: 导出CSV

    表 2  B2+离子的基态和部分低激发态相对于原子实的能级, 实验值(Expt.) [33]是来自于NIST的数据(单位: a.u.), “Diff.”表示用RCICP方法计算的结果与NIST结果之差的百分比

    Table 2.  Energy levels of the ground state and some low-lying states of B2+ ions relative to atomic core. Experimental values (Expt.) [33] are from the NIST data (in a.u.). “Diff.” denotes the difference in percentage from calculated by RCICP method and NIST results.

    StatejRCICPExpt.[33]Diff./%
    2s1/2–1.3939235–1.39392350
    2p1/2–1.1735867–1.17358670
    3/2–1.1734313–1.17343130
    3s1/2–0.5728008–0.57286320.01
    3p1/2–0.5146980–0.51477300.01
    3/2–0.5146520–0.51472740.01
    3d3/2–0.5005686–0.50056860
    5/2–0.5005553–0.50055530
    4s1/2–0.3108609–0.31089050.01
    4p1/2–0.2874707–0.28750980.01
    3/2–0.2874514–0.28749200.01
    4d3/2–0.2815308–0.28153240
    5/2–0.2815252–0.28152680
    4f5/2–0.2812848–0.28127050.01
    7/2–0.2812820–0.28126760.01
    5s1/2–0.1948639–0.19487930.01
    5p1/2–0.1831864–0.18320670.01
    3/2–0.1831765–0.18319700.01
    5d3/2–0.1801535–0.18015520
    5/2–0.1801507–0.18015230
    5f5/2–0.1800204–0.18001380
    7/2–0.1800190–0.18001240
    下载: 导出CSV

    表 3  B2+离子基态和部分低激发态之间跃迁的振子强度, “Diff.”表示用RCICP方法计算的结果与NIST结果[41]之差的百分比

    Table 3.  Oscillator strengths of transitions between the ground state and some low-lying states of B2+ ions. “Diff.” represents the difference in percentage form calculated by RCICP method and NIST results.

    TransitionsRCICPRMBPT[42]HR[43]NIST[41]Diff./%
    2s1/2→2p1/20.1212510.1211010.1210760.120990.22
    2s1/2→2p3/20.2427230.2425010.2423990.242150.24
    2s1/2→3p1/20.0510840.051080.01
    2s1/2→3p3/20.1020610.102400.33
    2p1/2→3s1/20.0463080.0462880.046360.11
    2p1/2→3d3/20.6379370.638000.01
    2p1/2→4s1/20.0081930.0082330.49
    2p1/2→4d3/20.1225730.122800.19
    2p3/2→3s1/20.0463460.0463380.046360.03
    2p3/2→3d3/20.0638060.063810.01
    2p3/2→3d5/20.5742840.574300
    2p3/2→4s1/20.0081980.0082360.46
    2p3/2→4d3/20.0122560.012280.20
    2p3/2→4d5/20.1103230.110500.16
    3s1/2→3p1/20.2032930.203100.10
    3s1/2→3p3/20.4069420.40680.04
    3s1/2→4p1/20.0487450.048500.51
    3s1/2→4p3/20.0973570.097000.37
    下载: 导出CSV

    表 4  B2+离子基态与部分低激发态的静态电偶极标量极化率与张量极化率以及主要跃迁的贡献(单位: a.u.)

    Table 4.  Static electric-dipole scalar and tensor polarizability of the ground state and some low-lying state of B2+ ions and breakdowns of the contributions of individual transitions (in a.u.).

    2s1/22p1/22p3/2 3s1/2
    Contr.$ {\alpha }_{}^{{\rm{S}}} $FCPC [44]Contr.$ {\alpha }_{}^{{\rm{S}}} $Contr.$ {\alpha }_{}^{{\rm{S}}} $$ {\alpha }^{{\rm{T}}} $Contr.$ {\alpha }_{}^{{\rm{S}}} $
    2p1/22.49752.4953[44]2s1/2–2.49752s1/2–2.49632.49633p1/260.218
    2p3/24.99264.9872[44]3d3/21.40843d5/21.2684–0.25373p3/2120.35
    Remains0.34330.3453[44]Remains0.4959Remains0.6371–0.0743Remains2.3125
    Core[30]0.01950.0195[44]Core0.0195Core0.0195Core0.0195
    Total7.85297.8473[44]Total–0.5737Total–0.57132.1683Total182.90
    CICP[45]7.8460–0.56938182.94
    SCC[46]7.85
    FCG[47]7.8591
    下载: 导出CSV

    表 5  B2+离子基态的超极化率及其中间态对超极化率的贡献(单位: a.u.)

    Table 5.  Hyperpolarizability of the ground state of B2+ ion and the contributions to the hyperpolarizability (in a.u.).

    Contributions$ {\gamma }_{0}\left(2{\rm{s}}\right) $$ {\gamma }_{0}^{{\rm{C}}}\left(2{\rm{s}}\right) $
    $ \dfrac{1}{18}T({\rm{s}}, {{\rm{p}}}_{1/2}, {\rm{s}}, {{\rm{p}}}_{1/2}) $1.251(1)1.250
    $ -\dfrac{1}{18}T({\rm{s}}, {{\rm{p}}}_{1/2}, {\rm{s}}, {{\rm{p}}}_{3/2}) $2.501(1)2.500
    $ -\dfrac{1}{18}T({\rm{s}}, {{\rm{p}}}_{3/2}, {\rm{s}}, {{\rm{p}}}_{1/2}) $2.501(1)2.500
    $ \dfrac{1}{18}T({\rm{s}}, {{\rm{p}}}_{3/2}, {\rm{s}}, {{\rm{p}}}_{3/2}) $5.001(1)5.000
    $T({\rm{s} }, { {\rm{p} } }_{ {j}^{'} }, {\rm{s} }, { {\rm{p} } }_{ {j}^{''} })$11.255(5)11.250
    $\dfrac{1}{18}T({\rm{s} }, { {\rm{p} } }_{1/2}{, {\rm{d} } }_{3/2}, { {\rm{p} } }_{1/2})$9.588(8)9.580
    $\dfrac{1}{18\sqrt{10} }T({\rm{s} }, { {\rm{p} } }_{1/2}{, {\rm{d} } }_{3/2}, { {\rm{p} } }_{3/2})$1.917(2)1.915
    $\dfrac{1}{18\sqrt{10} }T({\rm{s} }, { {\rm{p} } }_{3/2}{, {\rm{d} } }_{3/2}, { {\rm{p} } }_{1/2})$1.917(2)1.915
    $\dfrac{1}{180}T({\rm{s} }, { {\rm{p} } }_{3/2}{, {\rm{d} } }_{3/2}, { {\rm{p} } }_{3/2})$0.383(1)0.382
    $\dfrac{1}{30}T({\rm{s} }, { {\rm{p} } }_{3/2}{, {\rm{d} } }_{5/2}, { {\rm{p} } }_{3/2})$20.692(16)20.676
    $T({\rm{s} }, { {\rm{p} } }_{ {j}^{'} }{, {\rm{d} } }_{j}, { {\rm{p} } }_{ {j}^{''} })$34.497(28)34.469
    $ {\alpha }^{1}{\beta }_{0} $134.364(586)133.778
    RCICP–1063.346(6.645)–1056.701
    UCHF[50]–1160
    CHF[49]–1120
    下载: 导出CSV

    表 6  B+基态和部分低激发态相对于原子实的能级值, 实验值(Expt.) [51]是来自于NIST的数据(单位: a.u.), “Diff.”表示用RCICP方法计算的结果与NIST结果之差的百分比

    Table 6.  Energy levels of the ground state and some low-lying states of B+ ions relative to atomic core. Experimental values (Expt.) are from the NIST data (in a.u.). “Diff.” denotes the difference in percentage from calculated by RCICP method and NIST results.

    StateRCICPExpt.[51]Diff./%
    2$ {{\rm{s}}}^{2}{{}_{}{}^{1}{\rm{S}}}_{0} $–2.318347–2.3183470
    2s2p$ {{}_{}{}^{3}{\rm{P}}}_{0} $–2.148235–2.1482330
    2s2p$ {{}_{}{}^{3}{\rm{P}}}_{1} $–2.148205–2.1482050
    2s2p$ {{}_{}{}^{3}{\rm{P}}}_{2} $–2.148178–2.1481320
    2s2p$ {{}_{}{}^{1}{\rm{P}}}_{1} $–1.9832–1.9839270.03
    2$ {{\rm{p}}}^{2}{{}_{}{}^{3}{\rm{P}}}_{0} $–1.867621–1.8676730
    2$ {{\rm{p}}}^{2}{{}_{}{}^{3}{\rm{P}}}_{1} $–1.867634–1.8676340
    2$ {{\rm{p}}}^{2}{{}_{}{}^{3}{\rm{P}}}_{2} $–1.867565–1.8675730
    2$ {{\rm{p}}}^{2}{{}_{}{}^{1}{\rm{D}}}_{2} $–1.852917–1.8519470.05
    2$ {{\rm{p}}}^{2}{{}_{}{}^{1}{\rm{S}}}_{0} $–1.736452–1.7366790.01
    2s3s $ {{}_{}{}^{3}{\rm{S}}}_{1} $–1.727042–1.7270530
    2s3s $ {{}_{}{}^{1}{\rm{S}}}_{0} $–1.690800–1.6912930.03
    2s3p $ {{}_{}{}^{3}{\rm{P}}}_{0} $–1.662206–1.6622800
    2s3p $ {{}_{}{}^{3}{\rm{P}}}_{1} $–1.662167–1.6622770.01
    2s3p $ {{}_{}{}^{3}{\rm{P}}}_{2} $–1.662006–1.6622610.02
    2s3p $ {{}_{}{}^{1}{\rm{P}}}_{1} $–1.661601–1.6617650.01
    2s3d $ {{}_{}{}^{3}{\rm{D}}}_{1} $–1.631934–1.6319360
    2s3d $ {{}_{}{}^{3}{\rm{D}}}_{2} $–1.631720–1.6319360.01
    2s3d $ {{}_{}{}^{1}{\rm{D}}}_{2} $–1.613116–1.6135450.03
    $ 2{\rm{s}}4{\rm{s}}{{}_{}{}^{3}{\rm{S}}}_{1} $–1.560411–1.5604230
    $ 2{\rm{s}}4{\rm{s}}{{}_{}{}^{1}{\rm{S}}}_{0} $–1.552914–1.5531770.02
    $ 2{\rm{s}}4{\rm{p}} $ $ {{}_{}{}^{1}{\rm{P}}}_{1} $–1.540973–1.5410750.01
    $ 2{\rm{s}}4{\rm{p}} $ $ {{}_{}{}^{3}{\rm{P}}}_{1} $–1.5366–1.53670.01
    $ 2{\rm{s}}4{\rm{p}} $ $ {{}_{}{}^{3}{\rm{P}}}_{2} $–1.536439–1.5367260.02
    $ 2{\rm{s}}4{\rm{p}} $ $ {{}_{}{}^{3}{\rm{P}}}_{0} $–1.536693–1.5367260
    $ 2{\rm{s}}4{\rm{d}} $ $ {{}_{}{}^{3}{\rm{D}}}_{2} $–1.524938–1.5252100.02
    $ 2{\rm{s}}4{\rm{d}} $ $ {{}_{}{}^{3}{\rm{D}}}_{1} $–1.525198–1.5252100
    下载: 导出CSV

    表 7  B+离子基态和部分低激发态之间电偶极跃迁的振子强度(单位: a.u.)

    Table 7.  Oscillator strengths of electric-dipole transitions between the ground state and some low-lying states of B+ ions (in a.u.).

    TransitionRCICPCICP[45]BCICP[52]MCHF-BP[53]MCHF[54]NIST.[41]
    2s2 1S0 2s2p 1P11.000920.999071.0021.0010.9976(22)0.9990
    2s2 1S0→2s3p 1P10.108290.109590.1080.10870.1093(3)0.1090
    2s2 1S0→2s4p 1P10.053310.05300.0514
    2s2 1S02s5p 1P10.022440.02300.0241
    2s2p 3P02p2 3P10.341130.342980.3650.34300.3427(2)0.3400
    2s2p 3P0 2s3s 3S10.064370.063770.063970.0640
    2s2p 3P02s3d 3D10.476570.476270.4730.47590.4750
    2s2p 3P02s4s 3S10.011700.0115
    2s2p 3P02s4d 3D10.124800.1250.1260
    下载: 导出CSV

    表 8  B+离子2s2 1S0 和2s2p 3P0的电偶极极化率

    Table 8.  Electric-dipole polarizability of 2s2 1S0 and 2s2p 3P0 states of B+ ions

    2s2 1S02s2p 3P0
    Contributions polarizability/a.u.Contributions polarizability/a.u.
    2s2 1S0→2s2p 1P18.91492s2p 3P0→2p2p 3P14.3326
    2s2 1S0→2s3p 1P10.25112s2p 3P0→2s3d 3D11.7878
    Remains0.4365Remains1.6195
    Core0.0195Core0.0195
    RCICP9.6220RCICP7.7594
    CI[55]9.5750CI[55]7.7790
    CI+MBPT[55]9.6130CI+MBPT[55]7.7690
    CI+all-orders[55]9.6240CI+all-order[55]7.7720
    CCD+ST [56]9.5660
    CICP[45]9.6441CICP[45]7.7798
    PRCC[29]9.4130
    CCSDpT[57]10.395(22)
    RRV[58]9.6210
    下载: 导出CSV
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