Abstract
Dunham type parameters obtained from global processing of experimental vibrational–rotational and rotational transition frequencies of 14N16O and 16OH molecules are used for constructing RKR curves of potential energy. Pointwise defined potentials are approximated by expansions in the variable \({{z}_{S}} = (r - {{r}_{e}}){\text{/}}r\). Potential energy functions of the abovementioned molecules are calculated nonempirically using the Molpro software. The obtained results are compared with literature data.
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Translated by A. Nikol’skii
Appendices
APPENDIX A
Potential energy function and spin-orbit splitting of vibrational levels of the 14N16O molecule
r, Å | Eν, cm–1 | ξ/2, cm–1 | r, Å | Eν, cm–1 | ξ/2, cm–1 |
0.80 | 132 651.70 | 26.89 | 2.20 | 49 986.47 | 27.01 |
0.90 | 50 547.33 | 41.59 | 2.25 | 50 386.37 | 26.65 |
0.95 | 28 182.21 | 46.84 | 2.30 | 50 708.45 | 26.39 |
1.00 | 13 903.04 | 50.64 | 2.35 | 50 968.83 | 26.20 |
1.05 | 5478.20 | 53.33 | 2.40 | 51 180.45 | 26.06 |
1.10 | 1253.38 | 55.15 | 2.45 | 51 353.46 | 25.96 |
1.15 | 2.00 | 56.47 | 2.50 | 51 495.84 | 25.89 |
1.20 | 815.94 | 57.14 | 2.55 | 51 613.85 | 25.84 |
1.25 | 3025.04 | 57.44 | 2.60 | 51 712.33 | 25.80 |
1.30 | 6137.32 | 57.46 | 2.65 | 51 795.07 | 25.77 |
1.35 | 9793.70 | 57.17 | 2.70 | 51 865.06 | 25.75 |
1.40 | 13 733.63 | 56.62 | 2.75 | 51 924.65 | 25.74 |
1.45 | 17 768.58 | 55.81 | 2.80 | 51 975.72 | 25.72 |
1.50 | 21 762.07 | 54.68 | 2.85 | 52 019.77 | 25.72 |
1.55 | 25 614.58 | 53.19 | 2.90 | 52 057.98 | 25.71 |
1.60 | 29 252.68 | 51.27 | 2.95 | 52 091.38 | 25.71 |
1.65 | 32 621.90 | 48.90 | 3.00 | 52 120.73 | 25.70 |
1.70 | 35 682.67 | 46.12 | 3.20 | 52 209.24 | 25.70 |
1.75 | 38 409.16 | 43.03 | 3.40 | 52 268.01 | 25.70 |
1.80 | 40 790.24 | 39.87 | 3.60 | 52 307.52 | 25.71 |
1.85 | 42 830.47 | 36.88 | 3.80 | 52 332.39 | 25.71 |
1.90 | 44 549.00 | 34.27 | 4.00 | 52 346.76 | 25.71 |
1.95 | 45 975.87 | 32.12 | 4.20 | 52 354.58 | 25.72 |
2.00 | 47 146.93 | 30.43 | 4.40 | 52 358.79 | 25.72 |
2.05 | 48 099.47 | 29.15 | 4.60 | 52 361.16 | 25.72 |
2.10 | 48 869.25 | 28.20 | 4.80 | 52 362.63 | 25.72 |
2.15 | 49 488.79 | 27.51 | 5.00 | 52 363.64 | 25.72 |
APPENDIX B
Potential energy function and spin-orbit splitting of vibrational levels of the 16OH molecule
r, Å | Eν, cm–1 | ξ/2, cm–1 | r, Å | Eν, cm–1 | ξ/2, cm–1 |
0.60 | 74 846.55 | 70.43 | 2.10 | 33 620.31 | 62.62 |
0.65 | 48 074.00 | 69.73 | 2.15 | 34 107.04 | 61.51 |
0.70 | 29 145.71 | 69.22 | 2.20 | 34 522.59 | 60.42 |
0.75 | 16 786.42 | 68.94 | 2.25 | 34 876.21 | 59.37 |
0.80 | 8764.58 | 68.77 | 2.30 | 35 176.43 | 58.39 |
0.85 | 3853.27 | 68.70 | 2.35 | 35 430.90 | 57.47 |
0.90 | 1174.35 | 68.70 | 2.40 | 35 646.38 | 56.65 |
0.95 | 93.56 | 68.76 | 2.45 | 35 828.78 | 55.89 |
1.00 | 150.65 | 68.96 | 2.50 | 35 983.18 | 55.21 |
1.05 | 1010.01 | 69.08 | 2.55 | 36 113.92 | 54.61 |
1.10 | 2410.09 | 69.64 | 2.60 | 36 224.69 | 54.08 |
1.15 | 4214.91 | 69.74 | 2.65 | 36 318.62 | 53.61 |
1.20 | 6242.42 | 69.84 | 2.70 | 36 398.34 | 53.21 |
1.25 | 8400.99 | 69.94 | 2.75 | 36 466.06 | 52.85 |
1.30 | 10 618.29 | 70.05 | 2.80 | 36 523.64 | 52.55 |
1.35 | 12 839.02 | 70.13 | 2.85 | 36 573.87 | 52.29 |
1.40 | 15 021.30 | 70.21 | 2.90 | 36 615.43 | 52.06 |
1.45 | 17 133.67 | 70.24 | 2.95 | 36 650.05 | 51.87 |
1.50 | 19 152.71 | 70.22 | 3.00 | 36 681.17 | 51.71 |
1.55 | 21 061.36 | 70.15 | 3.20 | 36 764.46 | 51.26 |
1.60 | 22 847.54 | 69.98 | 3.40 | 36 809.70 | 51.03 |
1.65 | 24 503.26 | 69.73 | 3.60 | 36 834.75 | 50.91 |
1.70 | 26 023.96 | 69.37 | 3.80 | 36 848.90 | 50.85 |
1.75 | 27 408.05 | 68.90 | 4.00 | 36 857.10 | 50.82 |
1.80 | 28 656.62 | 68.30 | 4.20 | 36 861.98 | 50.80 |
1.85 | 29 773.13 | 67.59 | 4.40 | 36 864.99 | 50.80 |
1.90 | 30 763.08 | 66.75 | 4.60 | 36 866.91 | 50.79 |
1.95 | 31 633.75 | 65.82 | 4.80 | 36 868.18 | 50.79 |
2.00 | 32 393.74 | 64.80 | 5.00 | 36 869.06 | 50.79 |
2.05 | 33 052.58 | 63.72 |
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Borkov, Y.G., Sulakshina, O.N., Kozlov, S.V. et al. RKR Potentials of 14N16O and 16OH Molecules in the Electronic Ground State. Opt. Spectrosc. 128, 1921–1926 (2020). https://doi.org/10.1134/S0030400X20120887
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DOI: https://doi.org/10.1134/S0030400X20120887