Acta Physica Sinica, Volume. 68, Issue 3, 033101-1(2019)

Spectrum and transition characteristics of low excited state of strontium chloride molecule

Dong-Lan Wu*... Jin-Hong Yuan, Yu-Feng Wen, Xue-Feng Zeng and An-Dong Xie |Show fewer author(s)
Figures & Tables(7)
Potential energy curves of 14 excited states of Sr35Cl.Sr35Cl分子14个激发态的势能曲线
Permanent dipole moments of 5 bound states of Sr35Cl.Sr35Cl分子5个束缚态的电偶极矩
Transition dipole moments of 5 bound states of Sr35Cl.Sr35Cl分子5个束缚态的跃迁偶极矩
  • Table 1.

    Spectroscopic constants of the 5 bound states.

    5个束缚态的光谱常数

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    Table 1.

    Spectroscopic constants of the 5 bound states.

    5个束缚态的光谱常数

    Λ-S态Te/cm−1Re/nm $\omega $e/cm−1$\omega $e$\chi $e/cm−1Be/cm−1104αe/cm−1De/eV Re附近主要电子组态(%)
    $ {{\rm{X}}^{2}}\Sigma^+$0.00.2575309.780.86820.10164.1313.7036 $\text{σ}$27 $\text{σ}$28 $\text{σ}$α9 $\text{σ}$03 $\text{π}$24 $\text{π}$2(78.8) 6 ${\rm{\sigma }}$27 $\text{σ}$28 $\text{σ}$09 $\text{σ}$α3 $\text{π}$24 $\text{π}$2(7.5)
    理论[26]0.00.2553130.930.1037
    实验[15]0.00.257302[27]0.95[27]
    实验[16]0.0302.448−0.95020.10164.524
    实验[12]0.0302.30.950
    $ {{\rm{A}}^{2}}\Pi$15779.160.2518330.690.10612.0131.6736 $\text{σ}$27 $\text{σ}$28 $\text{σ}$09 $\text{σ}$03 $\text{π}$ααβ 4 $\text{π}$2(85.7)
    理论[26]147300.2523230.950.1055
    实验[15]148180.255309[27]0.98[27]
    实验[16]14966.727309.6250.9960.10304.606
    $ {{\rm{B}}^{2}}\Sigma^+$16612.740.2538318.670.48740.10432.5991.9376 $\text{σ}$27 $\text{σ}$28 $\text{σ}$α9 $\text{σ}$03 $\text{π}$24 $\text{π}$2(78.8) 6 ${\rm{\sigma }}$27 $\text{σ}$28 $\text{σ}$09 $\text{σ}$α3 $\text{π}$24 $\text{π}$2(7.6)
    理论[26]157140.2533190.990.1055
    实验[15]157190.255306[27]0.98[27]0.1030[16]
    实验[12]15719.5306.40.98
    $ {{\rm{C}}^{2}}\Pi$33532.990.3477425.5715.56910.0554−11.9321.5466 $\text{σ}$27 $\text{σ}$28 $\text{σ}$09 $\text{σ}$03 $\text{π}$ααβ 4 $\text{π}$2(59.7) 6 $\text{σ}$27 $\text{σ}$28 $\text{σ}$29 $\text{σ}$03 $\text{π}$24 $\text{π}$2(13.4) 6 $\text{σ}$27 $\text{σ}$α8 $\text{σ}$β9 $\text{σ}$03 $\text{π}$ααβ2(9.8) 6 $\text{σ}$27 $\text{σ}$α8 $\text{σ}$α9 $\text{σ}$03 $\text{π}$αββ 4 $\text{π}$2(2.7)
    理论[26]266880.2592780.830.1095
    实验[27]260992700.72
    $ {{\rm{3}}^{2}}\Sigma^+$36625.550.3519392.4910.45440.0544−12.5671.1406 $\text{σ}$27 $\text{σ}$α8 $\text{σ}$29 $\text{σ}$03 $\text{π}$24 $\text{π}$2(51.0) 6 $\text{σ}$27 $\text{σ}$28 $\text{σ}$09 $\text{σ}$α3 $\text{π}$24 $\text{π}$2(16.4) 6 $\text{σ}$27 $\text{σ}$28 $\text{σ}$α9 $\text{σ}$03 $\text{π}$ααβ 4 $\text{π}$2(4.6) 6 $\text{σ}$27 $\text{σ}$28 $\text{σ}$α9 $\text{σ}$03 $\text{π}$β4 $\text{π}$ααβ (4.6) 6 $\text{σ}$27 $\text{σ}$28 $\text{σ}$α9 $\text{σ}$03 $\text{π}$24 $\text{π}$2(2.5) 6 $\text{σ}$27 $\text{σ}$28 $\text{σ}$α9 $\text{σ}$03 $\text{π}$αββ 4 $\text{π}$2(1.6) 6 $\text{σ}$27 $\text{σ}$28 $\text{σ}$09 $\text{σ}$α3 $\text{π}$α4 $\text{π}$αββ (1.6) 6 $\text{σ}$27 $\text{σ}$α8 $\text{σ}$09 $\text{σ}$03 $\text{π}$44 $\text{π}$2(1.5) 6 $\text{σ}$27 $\text{σ}$α8 $\text{σ}$09 $\text{σ}$03 $\text{π}$24 $\text{π}$4(1.5)
    理论[26]279790.2483581.010.1095
    实验[15]28822344[27]1.04[27]0.1030[16]
  • Table 2. The Gv, Bv and Dv of , , , and states of Sr35Cl. Sr35Cl分子 , , , 和 的Gv, BvDv

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    Table 2. The Gv, Bv and Dv of , , , and states of Sr35Cl. Sr35Cl分子 , , , 和 的Gv, BvDv

    v0123456789
    $ {{\rm{X}}^{2}}\Sigma^+$Gv/cm−10308.69615.44919.341220.801520.911820.072118.052414.532709.33
    Bv/cm−10.1013890.1009640.1005670.1002090.0998150.0993690.0989100.0984670.0980430.097629
    108Dv/cm−14.3518394.3645774.4674934.4975144.3622264.2425424.2343604.2860164.3341244.353049
    $ {{\rm{A}}^{2}}\Pi$Gv/cm−115953.7416281.8316598.4316930.6217269.0117605.6517940.0418272.5918603.5218933.04
    Bv/cm−10.1062340.1064620.1060950.1051370.1046040.1042350.1038590.1034750.1030820.102679
    108Dv/cm−14.4619095.1115093.2534763.3327904.0078704.1303234.0855464.0409973.9761383.938946
    $ {{\rm{B}}^{2}}\Sigma^+$Gv/cm−116777.5817097.7717402.4617705.6318020.4418339.1618656.6918972.4419286.6019599.30
    Bv/cm−10.1042600.1041680.1043920.1036970.1028310.1022970.1019000.1015150.1011300.100741
    108Dv/cm−14.4167175.3420624.9473743.1209033.5004124.1294284.2737334.2441994.2064114.139361
    $ {{\rm{C}}^{2}}\Pi$Gv/cm−133822.2534298.6834607.2134880.8135124.5735352.1535566.0135770.8535971.2536169.15
    Bv/cm−10.0560490.0573540.0589120.0599950.0609740.0620710.0630320.0638430.0645150.065071
    108Dv/cm−10.2930931.0697201.3715962.1282872.4330733.0235763.3866363.3825633.4265463.529599
    $ {{\rm{3}}^{2}}\Sigma^+$Gv/cm−136879.5637294.0237638.5637944.0738221.4338480.1638726.9938965.8239199.0239428.18
    Bv/cm−10.0550790.0564810.0577580.0590280.0602420.0613770.0624320.0634140.0643320.065193
    108Dv/cm−10.3630520.6909091.0026581.3738201.6905301.9227242.1223552.3005062.4539552.583320
  • Table 3. The Franck-Condon factors of the transitions − , − , − and − . Sr35Cl分子 — , — , — 和 — 跃迁的Franck-Condon因子

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    Table 3. The Franck-Condon factors of the transitions − , − , − and − . Sr35Cl分子 — , — , — 和 — 跃迁的Franck-Condon因子

    v′′ = 0 123456789
    $ {{\rm{A}}^{2}}\Pi$$ {{\rm{X}}^{2}}\Sigma^+ $
    v′ = 0 0.6568880.2666080.0620270.0115630.0021700.0005200.0001630.0000480.0000070.000000
    10.2723080.1924200.3209470.1506850.4664790.0125670.0335440.0086550.0001740.000137
    20.0617410.3651000.0125910.2360030.2009350.0863560.0275680.0075570.0017910.000312
    30.0083780.1451530.3304340.0134760.1323920.2007670.1123950.0414330.0120930.002903
    40.0006410.0274990.2111700.2311620.0645890.0620860.1849830.1349770.0582630.018761
    50.0000400.0030150.0539250.254280.1324670.1155280.0187740.1558780.1511980.077211
    60.0000040.0001820.0082210.0846230.2713970.0583930.1511180.0008030.1173800.157174
    70.0000000.0000210.0062530.0163980.1179200.2630550.0147020.1649390.0051130.077068
    80.0000000.0000000.0000520.0016740.0275470.1514180.2336230.0000680.1572080.024940
    90.0000000.0000000.0000070.0001180.0036270.0418880.1812830.1902250.0086300.133109
    $ {{\rm{B}}^{2}}\Sigma^+$$ {{\rm{X}}^{2}}\Sigma^+ $
    v′ = 0 0.8612880.1254940.0119270.0010650.0001420.0000470.0000250.0000910.0000000.000000
    10.1296920.6037950.2200010.0383320.0062510.0013650.0004110.0001200.0000190.000000
    20.0086500.2413210.3600720.2841630.0813080.0186460.0044560.0011090.0002260.000018
    30.0003650.0276610.3525670.1793850.2882150.1125840.0300790.0072270.0016000.000265
    40.0000020.0017070.0514620.4119030.0833780.2685330.1316410.0392810.0096680.002055
    50.0000010.0000170.0038430.0784230.4214330.0347300.2469760.1487900.0496630.012870
    60.0000000.0000000.0001170.0063410.1089180.4073820.0094020.2212960.1637110.061334
    7 80.000000 0.0000000.000003 0.0000020.000001 0.0000070.000333 0.0000020.009581 0.0007630.141252 0.0141680.381199 0.1733210.000074 0.3466870.190975 0.0038010.174597 0.158106
    90.0000000.0000000.0000000.0000000.0000000.0012720.0204840.2036050.3064370.017104
    $ {{\rm{C}}^{2}}\Pi$$ {{\rm{X}}^{2}}\Sigma^+ $
    v′ = 0 0.0000020.0000570.0004000.0024910.0132570.0483810.1211070.2111640.2459630.199742
    10.0000280.0007550.0039230.0164780.0547110.1124990.1290550.0630350.0004780.054393
    20.0002160.0045360.0180570.0528610.1106480.1195270.0404560.0023850.0591840.058927
    30.0008940.0142940.0426880.0831920.0970650.0336970.0039200.0602620.0398650.000817
    $ {{\rm{3}}^{2}}\Sigma^+$$ {{\rm{X}}^{2}}\Sigma^+ $
    v′ = 0 0.0000050.0001600.0010140.0055830.0259730.0820350.1746250.2632660.2377440.147940
    10.0000720.0017260.0079850.0289590.0808610.1332680.1068900.0189460.0193480.137924
    20.0004440.0081220.0281470.0686990.1140640.0856950.0083410.0255440.0751680.024261
    30.0018870.0256140.0640480.0967490.0764640.0079490.0236640.0622440.0101840.021472
    40.0058230.0573750.0987150.0792070.0134590.0154200.0562150.0104800.0186870.044825
    50.0131040.0910740.0990090.0274500.0056030.0519270.0167730.0124480.0409660.001448
    60.0234670.1091480.0623360.0000390.0432340.0333130.0033660.0422120.0047520.023015
    70.0365520.1060160.0203160.0190850.0558070.0017340.0350280.0170510.0126990.031310
    80.0520500.0858670.0004310.0518610.0280880.0115620.0372560.0008330.0361760.001957
    90.0695480.0571890.0085290.0609070.0017910.0384890.0087130.0246660.0152290.013407
  • Table 4. Radiative lifetimes of the transitions − , − and − . Sr35Cl分子 — , — 和 — 跃迁的辐射寿命

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    Table 4. Radiative lifetimes of the transitions − , − and − . Sr35Cl分子 — , — 和 — 跃迁的辐射寿命

    TransitionRadiative lifetimes/ns
    v′ = 0 v′ = 1 v′ = 2
    $ {{\rm{A}}^{2}}\Pi $$ {{\rm{X}}^{2}}\Sigma^+ $31.2331.3531.56
    $ {{\rm{B}}^{2}}\Pi $$ {{\rm{X}}^{2}}\Sigma^+ $38.8338.8939.12
    $ {{\rm{C}}^{2}}\Pi$$ {{\rm{X}}^{2}}\Sigma^+ $25.9226.0126.18
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Dong-Lan Wu, Jin-Hong Yuan, Yu-Feng Wen, Xue-Feng Zeng, An-Dong Xie. Spectrum and transition characteristics of low excited state of strontium chloride molecule[J]. Acta Physica Sinica, 2019, 68(3): 033101-1

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Received: Sep. 26, 2018

Accepted: --

Published Online: Oct. 28, 2019

The Author Email:

DOI:10.7498/aps.68.20181770

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