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Table 2

Comparison between the database built in Sect. 2.2 and a previously available line list.

J K p L J K p L F (a) F (b) ΔF (c)
3 2 1 o1 2 2 1 o1 124964.268 124987.573 −23
3 2 1 e0 2 2 1 e0 125018.701 125031.220 −13
3 2 2 o1 2 2 2 o1 125031.220 125018.714 13
4 3 2 e1 3 3 2 e1 166297.556 166622.635 −325
4 3 1 e1 3 3 1 e1 166297.679 166622.635 −325
4 2 1 o1 3 2 1 o1 166608.434 166584.647 24
4 2 2 o1 3 2 2 o1 166775.754 166789.815 −14
5 3 2 e1 4 3 2 e1 207868.305 208290.307 −422
5 3 1 e1 4 3 1 e1 207868.736 208289.062 −420
6 5 1 e1 5 5 1 e1 249400.639 249405.569 −5
6 5 2 e1 5 5 2 e1 249400.639 249405.569 −5
6 4 1 e1 5 4 1 e1 249429.563 249419.799 10
6 4 2 e1 5 4 2 e1 249429.563 249419.799 10
6 3 2 e1 5 3 2 e1 249436.550 249975.994 −539
6 3 1 e1 5 3 1 e1 249437.730 249972.691 −535
7 3 2 e1 6 3 2 e1 291001.713 291651.893 −650
7 3 1 e1 6 3 1 e1 291004.306 291644.451 −640
7 2 1 o1 6 2 1 o1 291477.556 291514.936 −37
7 6 1 o1 6 6 1 o1 291501.533 291509.826 −8
7 6 2 o1 6 6 2 o1 291501.533 291509.826 −8
7 6 1 e0 6 6 1 e0 291509.860 291514.936 −5
7 6 2 e0 6 6 2 e0 291509.860 291514.936 −5
8 3 2 e1 7 3 2 e1 332563.111 333350.925 −788
8 3 1 e1 7 3 1 e1 332568.325 333335.082 −767
8 2 1 e1 7 2 1 e1 332719.680 332718.625 1
8 6 1 e0 7 6 1 e0 333151.638 333159.463 −8
8 6 2 e0 7 6 2 e0 333151.638 333159.463 −8
8 7 1 o1 7 7 1 o1 333159.539 333163.863 −4
8 7 2 o1 7 7 2 o1 333159.539 333163.863 −4
8 3 1 o1 7 3 1 o1 333335.082 333336.082 −1
8 4 1 e0 7 4 1 e0 333354.017 333350.239 4
8 4 2 e0 7 4 2 e0 333354.783 333350.239 5

Notes. The transition frequencies reported in Table 2 of Mukhopadhyay (2016b) are compared to those calculated in this work. Only transitions with a discrepancy larger than 0.5 MHz appear. Transitions are assigned using the rotational quantum numbers J, K, p (Coudert et al. 2021) and the torsional label (Su & Quade 1989b) of the upper and lower levels. (a) The frequency calculated in this work is given in MHz. (b)The frequency reported in Mukhopadhyay (2016b) is given in MHz. (c) The difference between the frequency calculated in this work and that reported in Mukhopadhyay (2016b) is given in MHz.

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