!MOLECULE HF pure-rot from JPL, vib-rot from HITRAN !MOLECULAR WEIGHT 20. ! NUMBER OF ENERGY LEVELS 16 !LEVEL + ENERGY(cm^-1) + WEIGHT + QNUM(v,J) 1 0.000000000 1.0 0,0 2 41.110983186 3.0 0,1 3 123.282117860 5.0 0,2 4 246.411770260 7.0 0,3 5 410.347964465 9.0 0,4 6 614.888349113 11.0 0,5 7 859.781218521 13.0 0,6 8 1144.725393803 15.0 0,7 9 1469.371544334 17.0 0,8 10 3961.4224986000 1.0 1,0 11 4000.9891779732 3.0 1,1 12 4080.0730466364 5.0 1,2 13 4198.5752354112 7.0 1,3 14 4356.3477180000 9.0 1,4 15 4553.1936439500 11.0 1,5 16 4788.8677826052 13.0 1,6 ! NUMBER OF RADIATIVE TRANSITIONS 19 !TRANS + U + L + A(s^-1) + FREQ(GHz) + E_u/k(K) + WAVENUMBER(cm^-1) 1 2 1 2.423E-02 1232.47627000 59.15 41.11098 2 3 2 2.322E-01 2463.42814000 177.38 82.17112 3 4 3 8.371E-01 3691.33465000 354.53 123.12967 4 5 4 2.049E+00 4914.68257000 590.40 163.93616 5 6 5 4.070E+00 6131.96840000 884.69 204.54045 6 7 6 7.092E+00 7341.70200110 1237.03 244.89282 7 8 7 1.130E+01 8542.41202530 1647.00 284.94419 8 9 8 1.685E+01 9732.64655900 2114.10 324.64614 9 14 6 1.156E+02 112166.128 6267.8 3741.45934 10 13 5 1.179E+02 113568.197 6040.8 3788.22729 11 12 4 1.225E+02 114930.274 5870.3 3833.66127 12 11 3 1.341E+02 116250.734 5756.5 3877.70708 13 10 2 1.979E+02 117527.983 5699.6 3920.31152 14 11 1 6.317E+01 119946.638 5756.5 4000.98918 15 12 2 7.383E+01 121085.037 5870.3 4038.96207 16 13 3 7.675E+01 122174.214 6040.8 4075.29314 17 14 4 7.695E+01 123212.780 6267.8 4109.93594 18 15 5 7.581E+01 124199.390 6551.0 4142.84570 19 16 6 7.382E+01 125132.754 6890.1 4173.97940 !NUMBER OF COLL PARTNERS 2 !COLLISIONS BETWEEN 1 HF-H2 scaled from HF-He by Reese et al 2005, A&A 430, 1139 !NUMBER OF COLLISIONAL TRANSITIONS 36 !NUMBER OF TEMPERATURES 8 !TEMPERATURES 1 10 30 50 80 100 200 300 !TRANS + UP + LOW + RATES [cm3 s-1] 1 2 1 7.58e-13 1.34e-12 2.49e-12 3.94e-12 6.27e-12 7.87e-12 1.54e-11 2.21e-11 2 3 2 8.27e-12 1.09e-11 1.04e-11 1.14e-11 1.37e-11 1.54e-11 2.42e-11 3.24e-11 3 3 1 1.37e-13 1.85e-13 2.42e-13 3.60e-13 6.27e-13 8.56e-13 2.44e-12 4.43e-12 4 4 3 1.04e-11 1.35e-11 1.34e-11 1.50e-11 1.80e-11 2.00e-11 2.98e-11 3.86e-11 5 4 2 8.91e-13 1.05e-12 1.08e-12 1.29e-12 1.72e-12 2.06e-12 4.31e-12 7.07e-12 6 4 1 3.28e-13 3.97e-13 4.14e-13 4.85e-13 6.01e-13 6.76e-13 9.91e-13 1.24e-12 7 5 4 9.49e-12 1.28e-11 1.31e-11 1.52e-11 1.87e-11 2.11e-11 3.26e-11 4.24e-11 8 5 3 9.61e-13 1.23e-12 1.31e-12 1.60e-12 2.15e-12 2.57e-12 5.12e-12 8.03e-12 9 5 2 1.68e-13 2.18e-13 2.41e-13 3.03e-13 4.22e-13 5.12e-13 1.02e-12 1.60e-12 10 5 1 7.39e-14 8.96e-14 9.75e-14 1.22e-13 1.72e-13 2.10e-13 4.37e-13 6.92e-13 11 6 5 8.29e-12 1.06e-11 1.11e-11 1.32e-11 1.69e-11 1.95e-11 3.22e-11 4.31e-11 12 6 4 8.71e-13 1.08e-12 1.18e-12 1.46e-12 2.04e-12 2.49e-12 5.15e-12 8.14e-12 13 6 3 1.21e-13 1.50e-13 1.67e-13 2.14e-13 3.13e-13 3.91e-13 8.95e-13 1.54e-12 14 6 2 6.32e-14 7.65e-14 8.58e-14 1.12e-13 1.67e-13 2.13e-13 5.09e-13 8.87e-13 15 6 1 1.35e-14 1.60e-14 1.80e-14 2.38e-14 3.67e-14 4.77e-14 1.28e-13 2.41e-13 16 7 6 7.16e-12 8.26e-12 8.84e-12 1.07e-11 1.42e-11 1.68e-11 2.97e-11 4.13e-11 17 7 5 7.47e-13 8.48e-13 9.38e-13 1.20e-12 1.72e-12 2.14e-12 4.71e-12 7.65e-12 18 7 4 1.08e-13 1.20e-13 1.35e-13 1.76e-13 2.67e-13 3.41e-13 8.57e-13 1.57e-12 19 7 3 4.41e-14 4.92e-14 5.65e-14 7.58e-14 1.19e-13 1.56e-13 4.22e-13 8.03e-13 20 7 2 1.45e-14 1.57e-14 1.80e-14 2.45e-14 3.95e-14 5.29e-14 1.58e-13 3.20e-13 21 7 1 2.53e-15 2.69e-15 3.09e-15 4.24e-15 7.00e-15 9.53e-15 3.17e-14 7.03e-14 22 8 7 5.74e-12 6.24e-12 6.77e-12 8.38e-12 1.15e-11 1.38e-11 2.61e-11 3.75e-11 23 8 6 5.84e-13 6.28e-13 7.03e-13 9.15e-13 1.37e-12 1.73e-12 4.08e-12 6.74e-12 24 8 5 8.91e-14 9.49e-14 1.08e-13 1.44e-13 2.25e-13 2.94e-13 8.08e-13 1.50e-12 25 8 4 2.80e-14 3.01e-14 3.49e-14 4.81e-14 7.85e-14 1.06e-13 3.22e-13 6.35e-13 26 8 3 9.75e-15 1.03e-14 1.20e-14 1.68e-14 2.80e-14 3.85e-14 1.26e-13 2.61e-13 27 8 2 2.95e-15 3.10e-15 3.63e-15 5.08e-15 8.68e-15 1.21e-14 4.39e-14 9.68e-14 28 8 1 6.91e-16 7.30e-16 8.53e-16 1.20e-15 2.07e-15 2.91e-15 1.10e-14 2.55e-14 29 9 8 4.47e-12 4.63e-12 5.09e-12 6.40e-12 9.02e-12 1.10e-11 2.23e-11 3.37e-11 30 9 7 4.33e-13 4.52e-13 5.12e-13 6.78e-13 1.04e-12 1.34e-12 3.39e-12 5.89e-12 31 9 6 6.62e-14 6.92e-14 8.00e-14 1.10e-13 1.77e-13 2.38e-13 7.14e-13 1.42e-12 32 9 5 1.81e-14 1.90e-14 2.21e-14 3.09e-14 5.21e-14 7.18e-14 2.44e-13 5.42e-13 33 9 4 6.03e-15 6.35e-15 7.47e-15 1.06e-14 1.83e-14 2.56e-14 9.22e-14 2.15e-13 34 9 3 2.00e-15 2.11e-15 2.50e-15 3.60e-15 6.39e-15 9.11e-15 3.60e-14 9.15e-14 35 9 2 6.78e-16 7.16e-16 8.52e-16 1.23e-15 2.23e-15 3.24e-15 1.38e-14 3.67e-14 36 9 1 1.77e-16 1.90e-16 2.25e-16 3.25e-16 5.88e-16 8.53e-16 3.74e-15 1.03e-14 ! PARTNER 2, collisions between: 4 Electron-impact excitation cross sections for radiatively allowed transitions ! NUMBER OF COLLISIONAL TRANSITIONS 19 ! NUMBER OF COLLISIONAL TEMPERATURES 12 ! COLLISIONAL TEMPERATURES 10.0 20.0 30.0 50.0 75.0 100.0 150.0 200.0 300.0 500.0 750.0 1000.0 ! COLLISION RATES 1 2 1 7.4E-07 1.2E-06 1.4E-06 1.5E-06 1.4E-06 1.2E-06 8.8E-07 6.9E-07 5.0E-07 4.2E-07 4.1E-07 3.8E-07 2 3 2 3.5E-07 6.3E-07 8.4E-07 1.1E-06 1.2E-06 1.3E-06 1.2E-06 1.0E-06 7.5E-07 4.8E-07 3.8E-07 3.6E-07 3 4 3 2.1E-07 4.0E-07 5.5E-07 7.9E-07 9.7E-07 1.1E-06 1.1E-06 1.1E-06 8.8E-07 6.0E-07 4.2E-07 3.5E-07 4 5 4 1.4E-07 2.8E-07 4.0E-07 5.9E-07 7.6E-07 8.7E-07 9.7E-07 9.9E-07 9.1E-07 6.8E-07 4.8E-07 3.8E-07 5 6 5 1.1E-07 2.1E-07 3.0E-07 4.6E-07 6.1E-07 7.2E-07 8.5E-07 9.0E-07 8.9E-07 7.2E-07 5.4E-07 4.2E-07 6 7 6 8.3E-08 1.6E-07 2.4E-07 3.7E-07 5.0E-07 6.0E-07 7.4E-07 8.1E-07 8.4E-07 7.4E-07 5.8E-07 4.5E-07 7 8 7 6.7E-08 1.3E-07 1.9E-07 3.0E-07 4.2E-07 5.1E-07 6.5E-07 7.3E-07 7.9E-07 7.3E-07 6.0E-07 4.8E-07 8 9 8 5.6E-08 1.1E-07 1.6E-07 2.6E-07 3.6E-07 4.5E-07 5.7E-07 6.6E-07 7.3E-07 7.2E-07 6.1E-07 5.1E-07 9 14 6 6.5E-12 1.3E-11 1.9E-11 3.2E-11 4.8E-11 6.4E-11 9.6E-11 1.3E-10 1.9E-10 3.0E-10 4.2E-10 5.3E-10 10 13 5 6.2E-12 1.2E-11 1.9E-11 3.1E-11 4.7E-11 6.2E-11 9.2E-11 1.2E-10 1.8E-10 2.9E-10 4.1E-10 5.1E-10 11 12 4 6.1E-12 1.2E-11 1.8E-11 3.1E-11 4.6E-11 6.1E-11 9.1E-11 1.2E-10 1.8E-10 2.8E-10 4.0E-10 5.1E-10 12 11 3 6.4E-12 1.3E-11 1.9E-11 3.2E-11 4.8E-11 6.3E-11 9.5E-11 1.3E-10 1.8E-10 3.0E-10 4.2E-10 5.3E-10 13 10 2 9.0E-12 1.8E-11 2.7E-11 4.5E-11 6.7E-11 8.9E-11 1.3E-10 1.8E-10 2.6E-10 4.2E-10 5.9E-10 7.4E-10 14 11 1 2.6E-12 5.2E-12 7.8E-12 1.3E-11 2.0E-11 2.6E-11 3.9E-11 5.1E-11 7.6E-11 1.2E-10 1.7E-10 2.2E-10 15 12 2 2.9E-12 5.9E-12 8.8E-12 1.5E-11 2.2E-11 2.9E-11 4.3E-11 5.7E-11 8.5E-11 1.4E-10 1.9E-10 2.4E-10 16 13 3 2.9E-12 5.8E-12 8.8E-12 1.5E-11 2.2E-11 2.9E-11 4.3E-11 5.7E-11 8.5E-11 1.4E-10 1.9E-10 2.4E-10 17 14 4 2.8E-12 5.6E-12 8.5E-12 1.4E-11 2.1E-11 2.8E-11 4.2E-11 5.5E-11 8.2E-11 1.3E-10 1.9E-10 2.4E-10 18 15 5 2.7E-12 5.4E-12 8.0E-12 1.3E-11 2.0E-11 2.7E-11 4.0E-11 5.3E-11 7.8E-11 1.3E-10 1.8E-10 2.3E-10 19 16 6 2.5E-12 5.0E-12 7.6E-12 1.3E-11 1.9E-11 2.5E-11 3.7E-11 5.0E-11 7.3E-11 1.2E-10 1.7E-10 2.1E-10 ! ! Prepared by J. H. Black 2008-8-14; ! e-impact rates added 2010-3-18; ! He rates scaled to H2 by F. van der Tak 2010-11-2 ! ! Vibration-rotation transition frequencies from D. Goddon et al. 1991, J. Molec. Spectrosc., 147, 392. ! A-values computed from the transition dipole moments and fit to the Herman-Wallis factors of ! Pine, Fried, Elkins 1985, J. Molec. Spectrosc., 109, 30. These are similar -- but not identical -- ! to the values in HITRAN2004. Pure rotational transitions from JPL database. ! Electron impact rates were calculated in the Coulomb-Born approximation.