========================================================================= Supplementary data associated with the paper "A Full Analytic Potential Energy Curve for the $a\,^3\Sigma^+$ State of KLi from a limited vibrational data set" by H. Salami, A.J. Ross, P. Crozet, W. Jastrzebski, P. Kowalczyk and R.J. Le Roy, Journal of Chemical Physics (accepted, April 2007) Experimental Data for a-state KLi in the input format for program DPotFit used to perform the analysis reported in this paper. As discussed there, the known X-state dissociation limit and molecular constants were used to re-state fluoescence transitions from the directly-excited upper-state levels as pseudo photoassociation (PA) level energies, relative to the a-state asymptote. While parity splittings are not resolved, the labelling (p' & p") is retained as it is required by the code. ========================================================================= 0 0 'PA' 'a3' 39 6 % v' J' ES1 ES2 mass1 mass2 6 1 31 1 -11.630 0.005 % v" p' J" p" wavenumber uncertainty [cm-1] 6 1 29 1 -3.592 0.005 % P,R from B 1pi - e: 12ja6020 5 -1 33 1 -7.320 0.005 % 10jul002 7 -1 25 1 -1.413 0.005 8 -1 23 1 -5.034 0.005 8 -1 21 1 -0.372 0.005 8 -1 25 1 -9.591 0.050 6 -1 30 1 -7.603 0.005 % 12jul003 6 -1 32 1 -15.633 0.005 6 -1 29 1 -3.588 0.005 % 11jul009.add 6 -1 31 1 -11.629 0.005 8 -1 22 1 -2.691 0.005 5 1 23 1 38.211 0.005 % 10ja6010 5 1 25 1 29.953 0.005 7 1 4 1 42.278 0.005 % 12ja6023 7 1 6 1 40.606 0.005 7 1 7 1 39.549 0.005 7 1 9 1 36.999 0.005 8 1 4 1 26.485 0.005 8 1 6 1 25.028 0.005 8 1 7 1 24.103 0.005 8 1 9 1 21.884 0.005 9 1 9 1 10.730 0.005 7 1 5 1 41.513 0.005 % 12ja6005 7 1 7 1 39.551 0.005 8 1 5 1 25.821 0.005 8 1 7 1 24.105 0.005 7 1 8 1 38.348 0.005 7 1 10 1 35.509 0.005 8 1 8 1 23.056 0.005 8 1 10 1 20.591 0.005 9 1 8 1 11.690 0.005 9 1 10 1 9.659 0.005 7 1 6 1 40.615 0.005 % 20ja6007 7 1 8 1 38.354 0.005 7 1 9 1 37.002 0.005 7 1 11 1 33.882 0.005 8 1 6 1 25.034 0.005 8 1 8 1 23.060 0.005 8 1 9 1 21.886 0.005 8 1 11 1 19.183 0.005 9 1 9 1 10.735 0.005 9 1 11 1 8.499 0.005 7 1 10 1 35.511 0.005 % 23ja6009.add 7 1 12 1 32.110 0.005 8 1 10 1 20.593 0.005 8 1 12 1 17.656 0.005 9 1 10 1 9.661 0.005 9 1 12 1 7.246 0.005 10 1 10 1 2.606 0.005 10 1 12 1 0.807 0.005 7 1 8 1 38.352 0.005 % 23ja6015 7 1 10 1 35.515 0.005 8 1 8 1 23.065 0.005 8 1 10 1 20.600 0.005 9 1 10 1 9.676 0.005 7 1 11 1 33.881 0.005 7 1 13 1 30.208 0.005 8 1 11 1 19.180 0.005 8 1 13 1 16.014 0.005 9 1 11 1 8.497 0.005 9 1 13 1 5.916 0.005 7 -1 23 1 4.734 0.005 % 13ja6017 7 -1 21 1 10.626 0.005 6 -1 28 1 0.392 0.005 5 -1 29 1 12.019 0.005 6 -1 22 1 22.749 0.005 % 12jul001 6 -1 20 1 29.384 0.005 5 -1 22 1 42.128 0.005 7 -1 22 1 7.730 0.005 6 -1 12 1 50.606 0.005 % 19ja6010 6 -1 10 1 54.423 0.005 6 -1 14 1 46.170 0.005 5 -1 12 1 73.090 0.005 5 -1 10 1 77.296 0.005 5 -1 14 1 68.201 0.005 7 -1 12 1 32.111 0.005 7 -1 10 1 35.513 0.005 7 -1 14 1 28.178 0.005 8 -1 12 1 17.660 0.005 8 -1 10 1 20.607 0.005 8 -1 14 1 14.280 0.005 7 -1 5 1 41.515 0.005 % 11ja6029 7 -1 7 1 39.550 0.005 7 -1 9 1 37.000 0.005 8 -1 5 1 25.821 0.005 8 -1 7 1 24.107 0.005 8 -1 9 1 21.887 0.005 9 -1 7 1 12.575 0.005 7 -1 6 1 40.608 0.005 % 11ja6017 7 -1 8 1 38.349 0.005 7 -1 10 1 35.508 0.005 8 -1 6 1 25.026 0.005 8 -1 8 1 23.061 0.005 8 -1 10 1 20.593 0.005 7 -1 9 1 37.005 0.005 % 23ja6007.add 7 -1 11 1 33.880 0.005 7 -1 13 1 30.207 0.005 8 -1 9 1 21.886 0.005 8 -1 11 1 19.184 0.005 8 -1 13 1 16.019 0.005 9 -1 11 1 8.493 0.005 9 -1 13 1 5.913 0.005 10 -1 11 1 1.729 0.005 5 1 16 1 62.645 0.005 % 20jul005.add 5 1 18 1 56.415 0.005 % these go with the P,R lines 6 1 16 1 41.133 0.005 6 1 18 1 35.528 0.005 7 1 16 1 23.728 0.005 7 1 18 1 18.806 0.005 8 1 18 1 6.351 0.005 8 1 16 1 10.492 0.005 -1 -1 -1 1 -1.000 0.005 54 17 'FS' 'a3' 39 6 5 1 16 1 12525.018 0.005 % collisional system 3sig - 3sig 5 1 18 1 12518.791 0.005 % 20jul005.add, 6 1 16 1 12503.511 0.005 % 18ja6002.add, 6 1 18 1 12497.908 0.005 % 12jul009.add 7 1 16 1 12486.102 0.005 7 1 18 1 12481.185 0.005 8 1 16 1 12472.869 0.005 8 1 18 1 12468.721 0.005 -1 -1 -1 1 -1.000 0.005 54 14 'FS' 'a3' 39 6 % collisional system 3sig - 3sig 6 1 13 1 12500.587 0.005 % 20jul005.add, 6 1 15 1 12495.842 0.005 % 18ja6002.add, 7 1 15 1 12478.134 0.005 % 12jul009.add -1 -1 -1 1 -1.000 0.005 54 15 'FS' 'a3' 39 6 % collisional system 3sig - 3sig 6 1 16 1 12496.465 0.005 % 20jul005.add, 6 1 14 1 12501.496 0.005 % 18ja6002.add, 7 1 16 1 12479.059 0.005 % 12jul009.add 7 1 14 1 12483.505 0.005 8 1 16 1 12465.822 0.005 -1 -1 -1 1 -1.000 0.005 54 16 'FS' 'a3' 39 6 % collisional system 3sig - 3sig 6 1 15 1 12502.476 0.005 % 20jul005.add, 6 1 17 1 12497.152 0.005 % 18ja6002.add, 7 1 15 1 12484.766 0.005 % 12jul009.add 7 1 17 1 12480.076 0.005 8 1 17 1 12467.209 0.005 -1 -1 -1 1 -1.000 0.005 54 18 'FS' 'a3' 39 6 % collisional system 3sig - 3sig 6 1 17 1 12504.615 0.005 % 20jul005.add, 6 1 19 1 12498.735 0.005 % 18ja6002.add, 7 1 17 1 12487.536 0.005 % 12jul009.add 7 1 19 1 12482.399 0.005 8 1 19 1 12470.387 0.005 8 1 17 1 12474.666 0.005 -1 -1 -1 1 -1.000 0.005 54 19 'FS' 'a3' 39 6 % collisional system 3sig - 3sig 6 1 18 1 12505.779 0.005 % 20jul005.add, 6 1 20 1 12499.639 0.005 % 18ja6002.add, 7 1 18 1 12489.055 0.005 % 12jul009.add 8 1 18 1 12476.598 0.005 8 1 20 1 12472.174 0.005 -1 -1 -1 1 -1.000 0.005 54 20 'FS' 'a3' 39 6 % collisional system 3sig - 3sig 6 1 19 1 12507.028 0.005 6 1 21 1 12500.625 0.005 7 1 19 1 12490.677 0.005 -1 -1 -1 1 -1.000 0.005 54 13 'FS' 'a3' 39 6 % collisional system 3sig - 3sig 7 1 14 1 12477.285 0.005 -1 -1 -1 1 -1.000 0.005 54 21 'FS' 'a3' 39 6 % collisional system 3sig - 3sig 6 1 20 1 12508.336 0.005 -1 -1 -1 1 -1.000 0.005 ========================================================================= END OF FILE =========================================================================