Table A.2.
Spectroscopic parametersa, b of HSO.
| Parameter | This work | Cazzoli et al. (2016) |
| A0 / MHz | 299483.868(80) | 299483.90(12) |
| B0 / MHz | 20502.78627(60) | 20502.7847(10) |
| C0 / MHz | 19135.69995(60) | 19135.6989(10) |
| DN / kHz | 29.46847(79) | 29.4675(13) |
| DNK / kHz | 904.870(69) | 904.18(11) |
| DK / MHz | 26.122(74) | 26.24(11) |
| d1 / kHz | -2.02578(30) | -2.02504(43) |
| d2 / kHz | -0.35319(34) | -0.35187(30) |
| HN / mHz | -29.56(51) | -28.42(75) |
| HNK / Hz | 3.896(53) | 2.779(88) |
| HKN / Hz | 134.8(42) | 144.7(43) |
| HK / kHz | [6.43] | [6.43] |
| h1 × 102 / mHz | [-8.32] | [-8.32] |
| h2 / mHz | 5.09(36) | [3.69] |
| h3 / mHz | 1.07(18) | 1.10(22) |
| LNK / mHz | -59.6(18) | -11.4(32) |
| LKKN / Hz | 1.709(84) | – |
| ϵaa / MHz | -10366.131(70) | -10366.15(10) |
| ϵbb / MHz | -426.630(10) | -426.633(17) |
| ϵcc / MHz | 0.205(12) | 0.191(21) |
 / MHz |
377.951(13) | 377.971(16) |
 c / MHz |
2.9760(75) | 2.979(10) |
 c / kHz |
-1.637(23) | -1.676(32) |
 c / MHz |
0.0569(27) | 0.0638(36) |
 c / kHz |
-0.125(22) | -0.114(30) |
| aF(H) / MHz | -35.842(13) | -35.72(50) |
| Taa(H) / MHz | -11.917(30) | -11.932(86) |
| Tbb(H) / MHz | 10.45(12) | 10.45(14) |
| Tab(H) d / MHz | [-7.53] | [-7.53] |
| Caa(H) / kHz | [-20.18] | [-20.18] |
| Cbb(H) / kHz | [2.51] | [2.51] |
| Ccc(H) / kHz | [-1.52] | [-1.52] |
Notes. (a) Watson S-reduction. Uncertainties (1σ) are in units of the last significant digit. (b) Values given in square brackets are kept fixed at the computed values, see Cazzoli et al. (2016) for details. (c) Centrifugal-distortion dependence of the electron spin-rotation constants, as given by Endo et al. (1981). (d) The negative sign means the sign of Tab is opposite to that of 1/2(ϵab + ϵba).
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