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The electronic structures and single point energy of 14 lowest electronic states of 88Sr 79Br molecule are optimized by using the internal contraction multi-reference configuration interaction method and relativistic effective core pseudo-potential basis. Because 88Sr 79Br molecule belongs to heavy element system, the single point energy must be corrected to obtain more accurate spectral parameters. Therefore, Davidson is introduced to correct the energy inconsistency, nuclear valence correlation is used to correct the electron correlation effect of inner shell and valence shell, and the relativistic scalar effect is corrected by calculating the third-order Douglas-Kroll-Hess Hamilton single electron integral. According to the single point energy calculated by the modified optimization, the potential energy curves, electric dipole moments, and transition dipole moments of 14 lowest electronic states are obtained. Using the latest LEVEL8.0 program to fit the modified potential energy curve, the spectral constants, molecular constants and vibration energy levels of 5 lowest bound states of 88Sr 79Br molecule are given. In order to explain the changing trend of spectral constants of homologous compounds, the spectral parameters of each compound are compared and analyzed in this paper. At the same time, the vibration energy levels and molecular constants of 88Sr 81Br molecule are also fitted and calculated for analyzing the influence of isotopes. The comparative analysis shows that the results of 88Sr 79Br molecule are in better agreement with the experimental values. Finally, the Franck-Condon factors are gained by fitting the optimized single point energy and transition dipole moment of 88Sr 79Br molecule. The transition band with the largest factor and obvious diagonalization is selected by analyzing the Franck-Condon factor of each transition band, and whether it meets the conditions for selecting laser cooling molecular system is judged. The radiation lifetimes of the transitions from the lowest two excited states to the ground state are calculated by combining the transition dipole moment, Franck-Condon factor, single point energy and vibration energy level of each electronic state. The results of this paper are in good agreement with the experimental values, which shows that the method in this paper is reliable. These spectral characteristic parameters provide theoretical support for further experimental measurement and construction of molecular laser cooling scheme of 88Sr 79Br molecule.
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Λ-S 态 Te/cm–1 Re/nm ωe/cm–1 ωeχe/cm–1 Be/cm–1 αe/(10–4cm–1) De/eV Re附近主要电子组态/% X2Σ+ 0.0 0.2740 216.17 0.499 0.0538 1.731 3.310 11σ212σα13σ06π47π2(80.2)
11σ212σ013σα6π47π2(6.9)理论[28] 0.0 0.2746 212.78 0.509 0.0535 — — 理论[29] 0.0 0.2799 205.6 0.53 0.051 1.742 — 实验[30] 0.0 0.2735 216 0.51 0.0541 — — A2Π 14679.348 0.2701 222.38 0.5346 0.0549 1.213 1.334 11σ212σ013σ06π47π3(86.1) 理论[28] 14657 0.272 220 0.57 0.0544 — — 理论[29] 14269.9 0.275 215.1 0.54 0.052 1.241 — 实验[30] 14850 0.2717 222 0.53 0.0545 — — B2Σ+ 15376.803 0.2702 223.03 0.5272 0.0552 1.799 1.597 11σ212σ013σα6π47π2(79.2)
11σ212σα13σ06π47π2(6.1)理论[28] 15208 0.2710 220.5 0.52 0.0547 — — 理论[29] 15222.8 0.2749 214.5 0.56 0.053 1.831 — 实验[30] 15352 0.2701 222 0.53 0.0552 — — C2Π 24947.818 0.3373 201.07 0.5012 0.0515 2.369 1.500
11σ212σ213σ06π37π3(80.0)
11σ212σ013σ06π47π3(2.2)
11σ212σ013σ06π37π4(2.8)
11σα12σα13σ06π47π3(2.7)理论[28] 25491 0.2810 197 0.49 0.0509 — — 理论[29] 25323.2 0.285 191.2 0.46 0.049 2.477 — 实验[30] 24665 — 205 0.49 — — — 32Σ+ 29079.756 0.3548 238.98 0.4556 0.0542 1.653 1.109 11σ212σα13σ06π47π2(1.3)
11σα12σ213σ06π47π2(69.4)
11σ212σ013σα6π47π2(5.3)
11σ212σα13σ06π37π3(2.9)
11σ212σ013σα6π47π1(.9)理论[28] 28117 0.266 242 0.54 0.0567 — — 理论[29] 27228.9 0.27 235.8 0.54 0.055 1.660 — 实验[30] 28958 — 247 0.55 — — — 
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ν 0 1 2 3 4 5 6 7 8 9 X2Σ+ Gν/cm–1 0 217.21 422.31 648.92 863.52 1077.13 1289.84 1501.60 1712.39 1922.24 Bν/cm–1 0.054170 0.054003 0.053836 0.053663 0.053494 0.053330 0.053165 0.052997 0.052827 0.052659 Dν/(10–8cm–1) 1.299301 1.303053 1.284638 1.297713 1.299115 1.295311 1.296435 1.298790 1.296092 1.292529 A2Π Gν/cm–1 14691.87 14934.23 15175.25 15415.96 15656.46 15896.12 16134.07 16369.73 16603.1 16834.89 Bν/cm–1 0.055780 0.055620 0.055462 0.055295 0.055124 0.054976 0.054861 0.054772 0.054687 0.054578 Dν/(10–8cm–1) 1.347703 1.355108 1.331605 1.313371 1.331860 1.390480 1.454430 1.476056 1.452901 1.372534 B2Σ+ Gν/cm–1 15376.52 15507.84 15738.33 15967.89 16196.74 16425.06 16652.61 16878.97 17103.8 17327.04 Bν/cm–1 0.055152 0.054998 0.054842 0.054679 0.054501 0.054326 0.054170 0.054020 0.053860 0.053722 Dν/(10–8cm–1) 1.383536 1.380925 1.382206 1.370045 1.352258 1.361286 1.370500 1.430538 1.454700 1.453644 C2Π Gν/cm–1 25067.11 25478.29 25768.5 25995.01 26202.12 26394.03 26575.33 26748.69 26915.65 27077.76 Bν/cm–1 0.051613 0.051929 0.052694 0.053118 0.0536173 0.053991 0.054389 0.054762 0.055104 0.055412 Dν/(10–8cm–1) 7.342555 2.052993 4.137982 4.629906 5.880088 6.862856 7.6697626 8.6153136 9.298999 9.430722 32Σ+ Gν/cm–1 31178.79 31534.74 31825.03 32085.24 32324.03 32546.51 32756.77 32958.15 33153 33342.76 Bν/cm–1 0.052457 0.052986 0.053498 0.053999 0.054484 0.054959 0.055414 0.055843 0.056246 0.056634 Dν/(10–8cm–1) 8.487942 1.681584 2.237826 2.904620 3.611947 4.250499 4.782100 5.233730 5.676720 6.069434 DownLoad:
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ν''= 0 1 2 3 4 5 6 7 8 9 A2Π–X2Σ+ ν'= 0 0.645022 0.336688 0.098008 0.017772 0.002264 0.000225 0.000019 0.000001 0.000000 0.000000 1 0.436688 0.083076 0.303189 0.190372 0.661533 0.165378 0.003316 0.000568 0.000087 0.000011 2 0.098008 0.434973 0.000835 0.180970 0.223953 0.113214 0.036827 0.009054 0.001812 0.000305 3 0.017772 0.293991 0.318827 0.055875 0.070256 0.256239 0.170741 0.062531 0.018499 0.004301 4 0.002263 0.053921 0.247678 0.100225 0.125148 0.010981 0.177146 0.190350 0.089728 0.031718 5 0.000225 0.009392 0.099735 0.271659 0.024898 0.160484 0.001473 0.098532 0.170079 0.114744 6 0.000019 0.001159 0.022742 0.145408 0.236122 0.000076 0.155129 0.024834 0.046417 0.151117 7 0.000000 0.000110 0.003473 0.042832 0.181875 0.178132 0.014614 0.150355 0.062132 0.011646 8 0.000000 0.000008 0.000391 0.008050 0.068736 0.202633 0.095379 0.050504 0.073401 0.096387 9 0.000000 0.000000 0.000034 0.001075 0.015763 0.098088 0.204697 0.042685 0.089124 0.031198 B2Σ+–X2Σ+ ν'= 0 0.825605 0.238234 0.033347 0.002666 0.000142 0.000006 0.000000 0.000000 0.000000 0.000000 1 0.388234 0.634880 0.110814 0.094271 0.088490 0.062873 0.040384 0.000047 0.000006 0.000000 2 0.033347 0.414395 0.520552 0.090304 0.084878 0.077853 0.067309 0.051175 0.000165 0.000020 3 0.002666 0.083449 0.366773 0.423286 0.082800 0.072301 0.061320 0.014268 0.002657 0.000419 4 0.000142 0.009678 0.107691 0.317402 0.350042 0.097638 0.0602219 0.055584 0.023573 0.005001 5 0.000006 0.000654 0.052162 0.087692 0.280018 0.317641 0.083112 0.07925 0.068340 0.044978 6 0.000000 0.000000 0.000117 0.006341 0.098918 0.277382 0.309402 0.081296 0.063711 0.051334 7 0.000000 0.000000 0.000093 0.003861 0.057313 0.055610 0.245025 0.292709 0.036511 0.075513 8 0.000000 0.000000 0.000004 0.000245 0.007248 0.080579 0.069675 0.186559 0.227752 0.010265 9 0.000000 0.000000 0.000000 0.000012 0.000552 0.012263 0.036322 0.069989 0.121499 0.152774 DownLoad:
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Transition Radiative lifetimes/ns ν′ = 0 ν′ = 1 ν′ = 2 A2Π–X2Σ+ 32.23 32.35 32.56 B2Σ+–X2Σ+ 40.93 40.95 41.22 DownLoad:
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[1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] [17] [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] [29] [30] [31] [32] [33] [34] [35] [36]
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