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Table 2:

Calculated frequencies and intensities of $\Delta F = \Delta N$ rotational transitions in the $X^{2}\Sigma ^{+}$ (v=1) ground state of AlO. The constants from Goto et al. (1994) have been used. The intensities are calculated according to a Hund's case $(b\beta _{J})-(b\beta _{J})$ formula (B1) from Bacis et al. (1973), at a temperature of 230 K.
G N' F' N'' F'' Freq/MHz Int. (230 K)
3 1 4 0 3 37 916.433 6.0
2 1 3 0 2 37 940.955 0.0
2 2 2 1 1 75 811.789 0.0
3 2 4 1 3 75 851.618 17.7
3 2 5 1 4 75 865.649 28.9
2 2 4 1 3 75 868.870 11.8
2 2 3 1 2 75 877.360 4.1
3 2 3 1 2 75 973.826 9.5
2 3 2 2 1 113 785.454 5.5
2 3 3 2 2 113 793.040 14.1
2 3 1 2 0 113 793.103 0.0
3 3 5 2 4 113 794.111 55.3
2 3 5 2 4 113 799.247 43.0
3 3 6 2 5 113 803.169 76.2
2 3 4 2 3 113 803.475 26.4
3 3 4 2 3 113 815.224 38.4
3 3 3 2 2 113 841.408 25.1
3 3 2 2 1 113 857.193 15.1
2 4 3 3 2 151 726.258 33.2
2 4 6 3 5 151 728.377 100.8
2 4 4 3 3 151 728.480 50.8
3 4 6 3 5 151 728.774 121.9
2 4 2 3 1 151 730.961 19.9
2 4 5 3 4 151 731.788 73.1
3 4 1 3 0 151 735.211 10.3
3 4 7 3 6 151 735.526 155.0
3 4 5 3 4 151 735.995 94.1
3 4 4 3 3 151 746.268 71.1
3 4 2 3 1 151 750.044 38.8
3 4 3 3 2 151 752.710 52.6
2 5 7 4 6 189 654.765 192.3
2 5 4 4 3 189 656.532 88.1
2 5 5 4 4 189 656.893 116.7
3 5 2 4 1 189 657.138 48.1
2 5 6 4 5 189 657.809 151.2
3 5 7 4 6 189 658.131 224.8
2 5 3 4 2 189 660.290 65.3
3 5 6 4 5 189 660.900 183.6
3 5 8 4 7 189 663.606 272.4
3 5 5 4 4 189 665.779 148.5
3 5 3 4 2 189 666.704 96.1
3 5 4 4 3 189 668.783 119.3
2 6 8 5 7 227 577.375 324.3
3 6 3 5 2 227 577.836 114.5
2 6 7 5 6 227 580.197 267.6
2 6 6 5 5 227 580.377 218.5
2 6 5 5 4 227 580.899 176.8
3 6 8 5 7 227 582.496 370.5
3 6 7 5 6 227 583.325 313.6
2 6 4 5 3 227 584.223 142.1
3 6 4 5 3 227 585.035 187.0
3 6 6 5 5 227 585.713 264.2
3 6 5 5 4 227 587.022 221.9
3 6 9 5 8 227 587.174 435.0
3 7 4 6 3 265 494.808 216.4
2 7 9 6 8 265 495.305 503.5
2 7 8 6 7 265 497.970 428.9
2 7 7 6 6 265 498.736 363.1
2 7 6 6 5 265 499.743 305.8
3 7 5 6 4 265 500.733 318.0
3 7 8 6 7 265 501.362 490.9
3 7 9 6 8 265 501.526 565.7
3 7 7 6 6 265 502.401 424.8
3 7 6 6 5 265 502.741 367.1
2 7 5 6 4 265 502.824 256.9
3 7 10 6 9 265 505.661 649.3
3 8 5 7 4 303 406.685 360.6
2 8 10 7 9 303 407.706 736.2
2 8 9 7 8 303 410.250 641.4
2 8 8 7 7 303 411.355 556.7
3 8 6 7 5 303 411.841 495.8
2 8 7 7 6 303 412.650 481.7
3 8 7 7 6 303 413.888 561.4
3 8 9 7 8 303 413.915 721.8
3 8 8 7 7 303 414.147 636.7
3 8 10 7 9 303 414.638 816.7
2 8 6 7 5 303 415.571 416.3
3 8 11 7 10 303 418.377 921.5
3 9 6 8 5 341 312.432 553.4
2 9 11 8 10 341 313.756 1028.6
2 9 10 8 9 341 316.193 911.6
3 9 7 8 6 341 317.083 726.7
2 9 9 8 8 341 317.503 805.7
2 9 8 8 7 341 318.976 710.7
3 9 8 8 7 341 319.162 811.0
3 9 9 8 8 341 319.813 906.2
3 9 10 8 9 341 320.090 1012.4
3 9 11 8 10 341 321.146 1129.5
2 9 7 8 6 341 321.779 626.6
3 9 12 8 11 341 324.576 1257.8
3 10 7 9 6 379 211.141 801.2
2 10 12 9 11 379 212.637 1386.7
2 10 11 9 10 379 214.978 1245.2
3 10 8 9 7 379 215.433 1016.9
2 10 10 9 9 379 216.413 1116.1
3 10 9 9 8 379 217.532 1122.0
2 10 9 9 8 379 217.995 999.0
3 10 10 9 9 379 218.444 1239.3
3 10 11 9 10 379 219.058 1368.7
3 10 12 9 11 379 220.313 1510.2
2 10 8 9 7 379 220.702 894.0
3 10 13 9 12 379 223.494 1664.0
3 11 8 10 7 417 101.951 1109.8
2 11 13 10 12 417 103.541 1816.1
2 11 12 10 11 417 105.791 1648.2
3 11 9 10 8 417 105.972 1372.1
2 11 11 10 10 417 107.299 1493.7
3 11 10 10 9 417 108.077 1500.2
2 11 10 10 9 417 108.943 1352.5
3 11 11 10 10 417 109.166 1641.7
3 11 12 10 11 417 110.003 1796.3
3 11 13 10 12 417 111.379 1964.3
2 11 9 10 8 417 111.564 1224.5
3 11 14 10 13 417 114.346 2145.7


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