Table A1 of the paper "The infrared dielectric function of solid para-hydrogen" S.C.Kettwich D.T. Anderson M.A. Walker A.V. Tuntsov 2015 Monthly Notices of the Royal Astronomical Society (in press) Excited electronic states of the H2 molecule accessible by photo-absorption from the ground rovibrational state of the ground electronic state X $^1\Sigma_g^+$ All excited states have rotational quantum number J = 1 so the lines are in every case R(0). Columns are as follows: i is an integer, assigned for indexing purposes v is the vibrational quantum number of upper state E is the transition wavenumber (1/cm) A is the transition rate from excited to ground state (MHz) Atot is total transition rate out of excited state (MHz) i v E A Atot 1 0 90242.36 3. 1900. 2 1 91558.74 11. 1700. 3 2 92838.45 22. 1600. 4 3 94083.81 35. 1500. 5 4 95295.51 47. 1400. 6 5 96474.38 56. 1400. 7 6 97620.29 61. 1300. 8 7 98735.16 64. 1200. 9 8 99818.26 59. 1200. 10 9 100869.90 59. 1100. 11 10 101891.40 48. 1100. 12 11 102882.25 47. 1000. 13 12 103844.59 32. 980. 14 13 104776.54 35. 940. 15 14 105689.44 3.1 970. 16 15 106556.97 24. 870. 17 16 107404.52 27. 840. 18 17 108227.25 16. 800. 19 18 109021.56 16. 780. 20 19 109791.23 10. 750. 21 20 110533.82 11. 720. 22 21 111252.73 6.2 700. 23 22 111944.84 6.9 680. 24 23 112614.62 2.2 670. 25 24 113256.20 4.6 640. 26 25 113870.94 9.5 660. 27 26 114467.73 3.0 620. 28 27 115033.96 3.8 610. 29 28 115574.95 2.0 600. 30 29 116087.47 2.4 610. 31 30 116569.72 1.4 610. 32 31 117015.15 1.6 630. 33 32 117420.53 0.91 640. 34 33 117773.65 0.98 670. 35 34 118062.74 0.50 720. 36 35 118257.91 0.33 800. 37 36 118338.00 0.23 820. 38 37 118365.91 0.0085 1000. 39 0 99151.62 96. 1200. 40 1 101457.30 160. 1200. 41 2 103628.99 160. 1100. 42 3 105660.98 150. 1000. 43 4 107581.03 88. 1100. 44 5 109361.86 64. 1100. 45 6 111012.74 45. 1100. 46 7 112530.28 32. 1100. 47 8 113917.99 14. 1000. 48 9 115154.15 10. 1100. 49 10 116237.75 8.1 1100. 50 11 117151.28 5.3 1100. 51 12 117870.00 3.4 1100. 52 13 118350.03 1.6 1100. 53 0 110529.44 6.4 380. 54 1 112404.59 20. 320. 55 2 114117.96 24. 270. 56 3 115646.83 20. 210. 57 4 116932.23 23. 160. 58 5 117883.94 9.3 130. 59 6 118177.72 1.2 340. 60 0 112935.70 22. 360. 61 1 115155.74 45. 350. 62 2 117251.54 40. 350. 63 9 124354.91 16.2 18000. 64 21 127131.03 30.9 36000. 65 27 128338.40 25.2 99000. 66 34 129441.46 19.9 81000. 67 39 130291.46 4.6 84000. 68 40 130461.44 8.9 18000. 69 42 130604.57 1.7 60000. 70 46 131194.00 1.64 9000. 71 47 131354.26 0.45 45000. 72 49 131494.17 2.59 21000. 73 50 131634.37 0.36 18000. 74 57 132471.39 0.34 15000. 75 58 132557.43 1.40 36000. 76 59 132631.27 1.23 9000. 77 60 132805.65 0.38 24000. 78 3 124113. 27.9 10000. 79 4 125971. 3.6 10000. 80 5 127667. 10.6 10000. 81 6 129252. 17.4 10000. 82 7 130742. 5.9 10000. 83 8 132117. 5.2 10000. 84 9 133364. 3.6 10000. 85 10 134498. 1.7 300000. 86 11 135510. 1.48 330000. 87 12 136403. 0.88 120000. 88 13 137201. 0.85 120000. 89 14 137797. 1.21 120000. 90 15 138327. 0.40 210000. 91 16 138680. 0.43 210000. 92 2 123922. 15.7 3000. 93 3 125728. 15.8 1500. 94 4 127600. 54.3 21000. 95 5 129287. 35.7 69000. 96 6 130610. 2.8 75000. 97 7 132036. 6.5 12000. 98 8 133141. 3.1 15000. 99 9 134023. 5.1 330000.