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Table 2:

Prediction of low-lying (J<6) rotational transitions (in MHz) of CH2D+ up to 1.5 THz.

J'K'aK'c JKa Kc
This work (1) (2)

22 0    22 1
23 015.03 $\pm$ 0.42 23 016.83 $\pm$ 1.18 23 015.95 $\pm$ 0.46
43 1    43 2 34 063.57 $\pm$ 0.77 34 070.76 $\pm$ 2.13 34 065.77 $\pm$ 0.68
11 0    11 1 67 273.80 $\pm$ 0.86 67 272.91 $\pm$ 1.78 67 273.71 $\pm$ 1.35
32 1    32 2 101 479.95 $\pm$ 0.96 101 487.42 $\pm$ 4.28 101 482.82 $\pm$ 2.03
53 2    53 3 116 348.72 $\pm$ 2.51 116 361.74 $\pm$ 5.69 116 343.38 $\pm$ 2.32
21 1    21 2 201 753.84 $\pm$ 1.60 201 752.39 $\pm$ 5.12 201 753.99 $\pm$ 4.04
42 2    42 3 251 004.10 $\pm$ 1.85 251 019.73 $\pm$ 8.30 251 006.92 $\pm$ 5.02
10 1    00 0 278 690.53 $\pm$ 0.44 278 693.05 $\pm$ 2.51 278 691.62 $\pm$ 5.57
31 2    31 3 398 038.11 $\pm$ 1.39 398 036.25 $\pm$ 9.26 398 037.70 $\pm$ 7.96
52 3    52 4 466 146.23 $\pm$ 3.85 466 163.41 $\pm$ 11.9 466 137.32 $\pm$ 9.32
21 2    11 1 490 011.00 $\pm$ 0.79 490 015.33 $\pm$ 4.16 490 012.30 $\pm$ 9.80
20 2    10 1 534 279.32 $\pm$ 0.71 534 282.33 $\pm$ 4.45 534 279.91 $\pm$ 10.7
21 1    11 0 624 491.04 $\pm$ 0.86 624 494.81 $\pm$ 5.70 624 492.58 $\pm$ 12.5
41 3    41 4 637 668.62 $\pm$ 1.84 637 663.21 $\pm$ 12.8  
32 2    30 3 666 868.24 $\pm$ 0.93 666 865.74 $\pm$ 8.50  
31 3    21 2 722 356.35 $\pm$ 0.86 722 357.77 $\pm$ 5.92  
30 3    20 2 757 259.87 $\pm$ 0.79 757260.81 $\pm$ 6.15  
42 3    40 4 798 820.76 $\pm$ 1.66 798 814.54 $\pm$ 9.80  
32 2    22 1 835 464.15 $\pm$ 0.98 835 467.35 $\pm$ 6.20  
51 4    51 5 890 257.97 $\pm$ 3.59 890 243.87 $\pm$ 15.0  
32 1    22 0 913 929.07 $\pm$ 1.23 913 937.95 $\pm$ 8.27  
31 2    21 1 918 640.62 $\pm$ 0.86 918 641.64 $\pm$ 7.22  
43 2    41 3 921 337.21 $\pm$ 1.72 921 351.70 $\pm$ 14.2  
53 3    51 4 937 383.22 $\pm$ 2.61 937 400.94 $\pm$ 10.8  
41 4    31 3 945 401.66 $\pm$ 1.43 945 400.35 $\pm$ 7.41  
40 4    30 3 963 383.72 $\pm$ 1.30 963 382.76 $\pm$ 7.60  
52 4    50 5 970 995.05 $\pm$ 3.23 970 979.36 $\pm$ 12.7  
42 3    32 2 1 095 336.24 $\pm$ 1.13 1 095 331.57 $\pm$ 7.16  
43 2    33 1 1 147 303.78 $\pm$ 1.36 1 147 313.43 $\pm$ 8.22  
51 5    41 4 1 161 984.97 $\pm$ 2.96 1 161 989.15 $\pm$ 8.60  
50 5    40 4 1 169 118.83 $\pm$ 2.90 1 169 123.51 $\pm$ 8.69  
43 1    33 0 1 176 099.37 $\pm$ 1.56 1 176 114.69 $\pm$ 9.40  
41 3    31 2 1 185 032.17 $\pm$ 1.15 1 185 027.31 $\pm$ 7.61  
42 2    32 1 1 244 860.39 $\pm$ 1.45 1 244 863.87 $\pm$ 9.48  
52 4    42 3 1 341 293.12 $\pm$ 1.74 1 341 288.32 $\pm$ 7.64  
51 4    41 3 1 414 574.32 $\pm$ 2.20 1 414 569.81 $\pm$ 7.75  
53 3    43 2 1 430 620.33 $\pm$ 1.78 1 430 619.04 $\pm$ 8.53  
54 2    44 1 1 439 955.31 $\pm$ 3.73 1 439 977.95 $\pm$ 10.7  
54 1    44 0 1 447 413.00 $\pm$ 3.73 1 447 437.27 $\pm$ 11.0  

References. (1) CDMS; (2) Rösslein et al. (1991).


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