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Table 2

Measured frequencies and residuals (νobsνcalc) in MHz for the rotational transitions of 1,2-diethynylbenzene.

νobs νobsνcalc
21,2–11,1 3718.0808 0.0082
20,2–10,1 4036.5597 0.0035
21,1–11,0 4771.1493 0.0098
31,3–21,2 5464.9715 0.0021
32,2–22,1 6366.9270 0.0179
31,2–21,1 6988.1538 −0.0062
32,1–22,0 7047.7281 −0.0014
41,4–31,3 7137.2432 0.0024
40,4–30,з 7234.7818 0.0101
42,3–32,2 8321.0133 0.0126
51,5–41,4 8763.9657 −0.0065
50,5–40,4 8797.2933 0.0047
41,3–31,2 8946.2760 0.0079
43,1–33,0 9085.2485 0.0254
42,2–32,1 9562.8878 −0.0070
52,4–42,3 10155.5724 −0.0046
61,6–51,5 10 370.0747 −0.0058
60,6–50,5 10 380.0387 −0.0021
51,4–41,3 10 602.2929 0.0044
53,3–43,2 10 933.8954 0.0132
53,2–43,1 11 725.7060 −0.0168
52,3–42,2 11 877.3150 −0.0207
62,5–52,4 11 884.2907 −0.0088
71,7–61,6 11 968.7362 −0.0038
70,7–60,6 11 971.4924 −0.0038

Notes. The standard asymmetric-top notation, , where J is the total rotational angular-momentum quantum number and Ka, Kc represent the quantum numbers for the projection of the angular momentum onto the symmetry axis (a- or c-axis) in the two limiting cases of prolate and oblate symmetric tops, respectively, is used to denote the rotational levels involved in each transition.

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