Table 6.
l-type resonance constants (in cm−1) for 16O12C32S
| Vib. state v1 v2 v3 |
qv0×104 | qvJ×1010 |
|---|---|---|
| 0 1 0 | 2.121 938 68(53)a | 1.424 13(102)b |
| 0 2 0 | 2.086 287(47) | 0.659(35) |
| 0 1 1 | 2.285 201(291) | 3.593(114) |
| 0 3 0 | 2.064 232(39) | 0.252(22) |
| 0 2 1 | 2.222 23(145) | 1.898(64) |
| 0 4 0 | 2.018 56(408) | −12.49(345) |
| 0 1 2 | 2.447 445(564) | 6.146(177) |
| 0 3 1 | 2.183 365(144) | 1.475 6(245) |
| 1 1 0 | 2.155 327(274) | 3.764(70) |
| 0 5 0 | 2.019 577(583) | −1.318(375) |
| 0 2 2 | 2.365(100) | 2.76(137) |
| 0 4 1 | 2.127 48(95) | −1.168(169) |
| 0 1 3 | 2.596 1(162) | 3.2(120) |
| 1 2 0 | 2.130 1(102) | 6.6(28) |
| 0 3 2 | 2.302 77(231) | 2.93(90) |
| 1 1 1 | 2.373 76(132) | 8.57(31) |
| 0 2 3 | [2.42] | [0.6587]c |
| 1 3 0 | 2.100 35(154) | 2.06(87) |
| 1 2 1 | [2.255 63] | [3.7] |
| 1 1 2 | 2.709 0(144) | 47.6(85) |
a
The uncertainty in the last digits (twice the estimated standard error) is given in parentheses.
b
Also included in the fit was a higher order term qvJJ = 0.574(44) × 10−15.
c
The values enclosed in square brackets were fixed during the analysis.