9 NOV 2016 EXOMOL VO IN KURUCZ FORMAT The EXOMOL linelist VOMYT for 51VO by McKemmish, L.K., Yurchenko, S.N., and Tennyson, J. 2016, MNRAS 463, 771-793, has been reformatted and edited down from 277,131,624 to 49,274,820 lines by eliminating lines with log gf less than -7.999. It includes the states X,A,A',B,C,D,a,b,c,d,e,f,g. The label for A' is changed to @. File VOMYT.ASC has air wavelengths. 17 AUG 2012 VO A-X, B-X, and C-X This is a quick and dirty calculation that ignores hyperfine splitting and perturbations and may have the parities exchanged or the lambda doubling ef levels exchanged. I started from a program that works correctly for triplets and modified it for quartets. The details should not affect the total opacity. All the line positions are predicted. There are good laboratory data available only for the lowest one or two vibrational levels of each state. It should possible in the future to determine the energy levels for those states and to substitute in the real energies and wavelengths. The references for the rotational and vibrational constants are X 4Sigma- V=0 Cheung, A., Taylor, A., and Merer, A. 1982. JMS 82, 391-409. V=1 Cheung, A., Taylor, A., and Merer, A. 1982. JMS 82, 391-409. V>1-15 Harrington, J., Seel, R., Hebert, G., and Nicholls, R. 1970. York University Centre fo Research in Experimental Space Science, Identification Atlas of Molecular Spectra 7. The VO C-X Yellow-Green and B-X Red Systems. A 4Pi V=0 Cheung, A., Taylor, A., and Merer, A. 1982. JMS 82, 391-409. V>0-15 Cheung, A., Taylor, A., and Merer, A. 1982. JMS 82, 391-409. Merer, A., Huang, G., Cheung, A., and Taylor, A. 1987. JMS 125, 465-503. B 4Pi V=0 Adam, A., Barnes, M., Berno, B., Bower, R., and Merer, A. 1995. JMS 170, 94-130. V=1 Cheung, A., Hajigeorgiou, P., Huang, G., and Huang, S. 1994. JMS 163, 443-458. V>1-15 Harrington et al 1970. op. cit. C 4Sigma- V=0 Cheung, A., Hansen, R., and Merer, A. 1982. JMS 91, 165-208. V>0-15 Harrington et al 1970. op. cit. and in partition function only A' 4Phi V=0-15 Merer, A., Huang, G., Cheung, A., and Taylor, A. 1987. JMS 125, 465-503. f values A=0.003, B=0.027, and C=0.068 are from Karlsson, L., Lindgren, B., Lundevall, C., and Sassenberg, U. 1997. JMS 181, 274-278 and are assumed to be band f values. D0 was taken as 6.41 eV = 51700 cm-1 from Huber and Herzberg. For the 4Pi states the RKR potentials did not converge to the limit, possibly because they dissociate to excited states, but the levels used are deep in the well so they should be reasonable. Frank-Condon factors were computed from the RKR potentials. Honl-London factors were computed up to J=199.5 and line lists were computed up to J=199.5 . The files are VOAX.ASC (1611872 lines), VOBX.ASC (1841400), VOCX.ASC (1056247), and VO.ASC (4509519). VO has been added to the reading program RMOLECASC.FOR . The partition function was computed up to the smaller of E(J=299.5) and 51700 cm-1, partly to make up for missing doublets. The equilibrium constant computed for 1000 < T < 6000 is 823.00 6.41 4.7617E+01 1.0876E-03 1.7055E-07 1.6406E-11 8.1447E-16 Spot Checks N gf E(ev) Plez VO 00 00 017 + P1 .1496E-01 9441.325 .018 A Cheung 9441.077 Plez VO 00 00 017 + Q1 .3053E-01 9458.709 .018 A Cheung 9463.059 Plez VO 00 00 017 + R1 .1565E-01 9477.092 .018 A Cheung 9478.474 gf 1058.2140 -1.850 15.5 112.997 14.5 9560.293 X00e1 A00e1 9447.296 .0141 1056.4513 -1.540 15.5 112.997 15.5 9576.056 X00e1 A00f1 9463.059 .0288 1054.6898 -1.830 15.5 112.997 16.5 9591.861 X00e1 A00e1 9478.863 .0148 N gf E(eV) Plez VO 00 00 017 + TR42 .1010E+00 12725.932 .021 B Adam 12728.637 Plez VO 00 00 017 + SQ42 .1593E+00 12706.525 .021 B Adam 12709.323 Plez VO 00 00 017 + RP42 .6168E-01 12688.164 .021 B Adam 12692.364 gf 787.6725 -1.098 16.5 150.571 15.5 12842.711 X00f2 B00f4 12692.140 .0798 786.6088 -0.679 16.5 150.571 16.5 12859.873 X00f2 B00e4 12709.302 .209 785.4836 -0.870 16.5 150.571 17.5 12878.080 X00f2 B00f4 12727.509 .135 N gf E(eV) Plez VO 00 00 017 + P1 .4494E+00 17390.012 .018 C Plez VO 00 00 017 + Q1 missing Plez VO 00 00 017 + R1 .4752E+00 17422.572 .018 C gf 574.6898 -0.480 15.5 112.997 14.5 17508.864 X00e1 C00e1 17395.867 .331 574.2346 -2.809 15.5 112.997 15.5 17522.655 X00e1 C00f1 17409.657 .00155 573.7476 -0.453 15.5 112.997 16.5 17537.431 X00e1 C00e1 17424.434 .352