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Table 1:

Calculated frequencies and intensities of $\Delta F = \Delta N$ rotational transitions in the $X^{2}\Sigma ^{+}$ (v=0) ground state of AlO. The constants from Yamada et al. (1990) have been used, with the exception that the sign of $\gamma _{\rm D}$ has been reversed. 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)
2 1 3 0 2 38 278.080 0.0
3 1 4 0 3 38 281.977 6.0
2 2 2 1 1 76 502.453 0.0
2 2 4 1 3 76 553.373 11.8
3 2 4 1 3 76 559.315 17.7
2 2 3 1 2 76 568.067 4.1
3 2 5 1 4 76 579.518 28.9
3 2 3 1 2 76 677.262 9.4
2 3 5 2 4 114 831.410 43.0
2 3 2 2 1 114 832.298 5.5
2 3 3 2 2 114 835.198 14.1
2 3 4 2 3 114 841.162 26.4
2 3 1 2 0 114 846.559 0.0
3 3 5 2 4 114 850.440 55.2
3 3 6 2 5 114 865.239 76.2
3 3 4 2 3 114 866.448 38.4
3 3 3 2 2 114 888.139 25.1
3 3 2 2 1 114 899.206 15.1
2 4 6 3 5 153 108.310 100.8
3 4 1 3 0 153 109.961 10.3
2 4 5 3 4 153 117.008 73.1
2 4 4 3 3 153 118.588 50.7
2 4 3 3 2 153 121.600 33.2
2 4 2 3 1 153 132.878 19.9
3 4 2 3 1 153 133.226 38.8
3 4 6 3 5 153 133.628 121.9
3 4 5 3 4 153 135.760 94.0
3 4 4 3 3 153 141.151 71.0
3 4 3 3 2 153 142.358 52.6
3 4 7 3 6 153 145.778 155.0
3 5 2 4 1 191 379.947 48.1
2 5 7 4 6 191 382.536 192.2
2 5 6 4 5 191 390.676 151.2
2 5 5 4 4 191 394.726 116.6
3 5 3 4 2 191 398.164 96.1
2 5 4 4 3 191 399.767 88.1
3 5 4 4 3 191 406.813 119.3
3 5 5 4 4 191 409.199 148.4
3 5 6 4 5 191 409.272 183.5
2 5 3 4 2 191 410.177 65.3
3 5 7 4 6 191 411.477 224.7
3 5 8 4 7 191 422.055 272.3
3 6 3 5 2 229 648.771 114.4
2 6 8 5 7 229 653.036 324.2
2 6 7 5 6 229 660.782 267.5
3 6 4 5 3 229 664.971 186.9
2 6 6 5 5 229 665.912 218.4
2 6 5 5 4 229 671.899 176.7
3 6 5 5 4 229 673.641 221.8
3 6 6 5 5 229 677.782 264.1
3 6 7 5 6 229 680.325 313.5
2 6 4 5 3 229 681.974 142.0
3 6 8 5 7 229 684.329 370.3
3 6 9 5 8 229 693.846 434.8
3 7 4 6 3 267 913.912 216.3
2 7 9 6 8 267 918.911 503.3
2 7 8 6 7 267 926.336 428.6
3 7 5 6 4 267 929.255 317.9
2 7 7 6 6 267 931.998 362.9
3 7 6 6 5 267 938.051 366.9
2 7 6 6 5 267 938.489 305.6
3 7 7 6 6 267 943.172 424.6
3 7 8 6 7 267 947.009 490.7
2 7 5 6 4 267 948.413 256.7
3 7 9 6 8 267 951.860 565.4
3 7 10 6 9 267 960.593 649.0
3 8 5 7 4 306 174.001 360.4
2 8 10 7 9 306 179.316 735.8
2 8 9 7 8 306 186.459 641.1
3 8 6 7 5 306 189.028 495.5
2 8 8 7 7 306 192.386 556.4
3 8 7 7 6 306 197.956 561.0
2 8 7 7 6 306 199.154 481.4
3 8 8 7 7 306 203.668 636.4
3 8 9 7 8 306 208.233 721.4
2 8 6 7 5 306 209.009 416.0
3 8 10 7 9 306 213.497 816.2
3 8 11 7 10 306 221.612 921.0
3 9 6 8 5 344 428.006 553.1
2 9 11 8 10 344 433.426 1028.0
2 9 10 8 9 344 440.311 911.0
3 9 7 8 6 344 443.008 726.3
2 9 9 8 8 344 446.356 805.1
3 9 8 8 7 344 452.051 810.4
2 9 8 8 7 344 453.276 710.3
3 9 9 8 8 344 458.123 905.6
2 9 7 8 6 344 463.087 626.2
3 9 10 8 9 344 463.112 1011.7
3 9 11 8 10 344 468.561 1128.8
3 9 12 8 11 344 476.168 1257.0
3 10 7 9 6 382 675.021 800.6
2 10 12 9 11 382 680.433 1385.7
2 10 11 9 10 382 687.074 1244.3
3 10 8 9 7 382 690.169 1016.2
2 10 10 9 9 382 693.151 1115.3
3 10 9 9 8 382 699.297 1121.2
2 10 9 9 8 382 700.137 998.3
3 10 10 9 9 382 705.589 1238.4
2 10 8 9 7 382 709.915 893.4
3 10 11 9 10 382 710.818 1367.7
3 10 12 9 11 382 716.327 1509.1
3 10 13 9 12 382 723.495 1662.8
3 11 8 10 7 420 914.194 1109.0
2 11 13 10 12 420 919.531 1814.6
2 11 12 10 11 420 925.941 1646.9
3 11 9 10 8 420 929.595 1371.1
2 11 11 10 10 420 931.991 1492.6
3 11 10 10 9 420 938.778 1499.0
2 11 10 10 9 420 938.985 1351.5
3 11 11 10 10 420 945.191 1640.4
2 11 9 10 8 420 948.726 1223.6
3 11 12 10 11 420 950.546 1794.9
3 11 13 10 12 420 956.037 1962.7
3 11 14 10 13 420 962.823 2143.9


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