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Table 4
Spectroscopic parameters for the H-in-plane configuration.
| Parameter | Value | Parameter | Value | ||
|
|
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| A | 17 281. 949 265(420) | HKJJ × 109 | −210.249(540) | ||
| B | 6540. 604 314(110) | HJJJ × 109 | 2.332(19) | ||
| C | 5041. 990 952(120) | hKK × 109 | −601.454(3897) | ||
| hKJ × 109 | 330.458(839) | ||||
| ΔKK × 103 | 41. 404 648(2200) | hJJ × 109 | 1.322(7) | ||
| ΔKJ × 103 | −7. 932 466(660) | ||||
| ΔJJ × 103 | 5. 806 476(90) | LKKKK × 1012 | −14.173(2998) | ||
| δK × 103 | −5. 786 705(1000) | LKKKJ × 1012 | 4.787(720) | ||
| δJ × 103 | 1. 787 297(26) | LKJJJ × 1012 | −4.897(72) | ||
| lKKJ × 1012 | 4.777(839) | ||||
| HKKK × 109 | 123. 268(4797) | lKJJ × 1012 | 7.766(162) | ||
| HKKJ × 109 | 611. 220(1469) | ||||
Notes. Parameters are in MHz. Numbers in parentheses are one standard deviation in the same units as the last digit. These parameters are involved in the pure rotational Hamiltonian in the second of Eqs. (10) of Margulès et al. (2009).
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