Table B.2
Selected astrophysically relevant 
transitions calculated at 10 K below 400 GHz (intensity, expressed in log(Icalc), and frequency, fcalc) and comparison with the present measurements (exp).
 |
 |
J′− J″ |  |
F′− F″ (a) | log(Icalc) (b) | fcalc (b) | fexp | Unc. | fexp − fcalc (b) |
|---|---|---|---|---|---|---|---|---|---|
| 111−000 | 0–1 | 1.5–0.5 | 1–0 | −1.39 | 220 220.494 | ||||
| 0–1 | 1.5–0.5 | 2–1 | −0.99 | 220 220.818 | 220 220.926 | 0.100 | 0.108 | ||
| 1–0 | 1.5–0.5 | 2–1 | 2–1 | −1.34 | 220 459.218 | ||||
| 1–0 | 1.5–0.5 | 2–1 | 1–1 | −1.45 | 220 490.591 | ||||
| 1–0 | 1.5–0.5 | 2–1 | 3–2 | −0.84 | 220 497.347 | 220 497.313 | 0.100 | −0.034 | |
| 1–0 | 1.5–0.5 | 1–0 | 2–1 | −1.02 | 220 498.190 | ||||
| 1–0 | 1.5–0.5 | 2–1 | 2–2 | −1.28 | 220 542.420 | ||||
| 0–1 | 0.5–0.5 | 1–1 | −1.38 | 220 569.669 | |||||
| 1–0 | 0.5–0.5 | 1–1 | 2–1 | −1.24 | 220 811.659 | ||||
| 1–0 | 0.5–0.5 | 1–1 | 1–2 | −1.35 | 220 843.440 | ||||
| 1–0 | 0.5–0.5 | 1–1 | 2–2 | −1.38 | 220 894.860 | ||||
| 212−101 | 0–1 | 2.5–1.5 | 3–2 | −0.86 | 272 160.133 | 272 160.058 | 0.050 | −0.075 | |
| 0–1 | 2.5–1.5 | 2–1 | −1.05 | 272 161.429 | 272 161.443 | 0.100 | 0.014 | ||
| 0–1 | 1.5–0.5 | 2–1 | −1.08 | 272 314.812 | |||||
| 1–0 | 2.5–1.5 | 3–2 | 4–3 | −0.75 | 272 436.717 | 272 436.693 | 0.050 | −0.024 | |
| 1–0 | 2.5–1.5 | 2–1 | 3–2 | −0.88 | 272 438.070 | 272 438.116 | 0.050 | 0.046 | |
| 1–0 | 2.5–1.5 | 3–2 | 2–1 | −1.21 | 272 442.401 | ||||
| 1–0 | 2.5–1.5 | 3–2 | 3–2 | −0.99 | 272 446.851 | ||||
| 1–0 | 2.5–1.5 | 2–1 | 2–1 | −1.18 | 272 447.243 | ||||
| 1–0 | 1.5–0.5 | 2–1 | 2–1 | −1.25 | 272 577.158 | ||||
| 1–0 | 1.5–0.5 | 1–0 | 2–1 | −1.10 | 272 589.726 | 272 589.844 | 0.050 | 0.118 | |
| 1–0 | 1.5–0.5 | 2–1 | 3–2 | −0.91 | 272 592.746 | 272 592.698 | 0.050 | −0.048 | |
| 313−202 | 0–1 | 3.5–2.5 | 4–3 | −0.90 | 322 157.218 | 322 157.465 | 0.100 | 0.247 | |
| 0–1 | 3.5–2.5 | 3–2 | −1.03 | 322 158.774 | |||||
| 0–1 | 2.5–1.5 | 2–1 | −1.23 | 322 229.666 | 322 229.731 | 0.100 | 0.065 | ||
| 0–1 | 2.5–1.5 | 3–2 | −1.04 | 322 232.906 | 322 232.743 | 0.100 | −0.163 | ||
| 1–0 | 3.5–2.5 | 4–3 | 5–4 | −0.81 | 322 433.683 | 322 433.702 | 0.050 | 0.019 | |
| 1–0 | 3.5–2.5 | 3–2 | 4–3 | −0.91 | 322 435.231 | 322 435.218 | 0.050 | −0.013 | |
| 1–0 | 3.5–2.5 | 4–3 | 4–3 | −0.95 | 322 438.364 | 322 438.442 | 0.100 | 0.078 | |
| 1–0 | 3.5–2.5 | 4–3 | 3–2 | −1.08 | 322 438.882 | ||||
| 1–0 | 3.5–2.5 | 3–2 | 3–2 | −1.08 | 322 439.438 | 322 439.500 | 0.150 | 0.062 | |
| 1–0 | 3.5–2.5 | 3–2 | 2–1 | −1.27 | 322 439.785 | 322 439.500 | 0.150 | −0.285 | |
| 1–0 | 2.5–1.5 | 3–2 | 2–1 | −1.30 | 322 503.234 | ||||
| 1–0 | 2.5–1.5 | 2–1 | 2–1 | −1.28 | 322 504.199 | ||||
| 1–0 | 2.5–1.5 | 3–2 | 3–2 | −1.09 | 322 506.538 | 322 506.633 | 0.100 | 0.095 | |
| 1–0 | 2.5–1.5 | 2–1 | 3–2 | −1.04 | 322 510.538 | ||||
| 1–0 | 2.5–1.5 | 3–2 | 4–3 | −0.91 | 322 513.186 | 322 512.721 | 0.100 | −0.465 | |
| 414−303 | 0–1 | 4.5–3.5 | 5–4 | −1.08 | 370 307.411 | ||||
| 0–1 | 4.5–3.5 | 4–3 | −1.18 | 370 309.055 | |||||
| 0–1 | 3.5–2.5 | 3–2 | −1.31 | 370 327.000 | |||||
| 0–1 | 3.5–2.5 | 4–3 | −1.18 | 370 329.627 | |||||
| 1–0 | 4.5–3.5 | 5–4 | 6–5 | −1.01 | 370 583.580 | ||||
| 1–0 | 4.5–3.5 | 4–3 | 5–4 | −1.09 | 370 585.209 | ||||
| 1–0 | 4.5–3.5 | 5–4 | 5–4 | −1.11 | 370 585.966 | ||||
| 1–0 | 4.5–3.5 | 5–4 | 4–3 | −1.20 | 370 586.994 | ||||
| 1–0 | 4.5–3.5 | 4–3 | 4–3 | −1.21 | 370 587.292 | ||||
| 1–0 | 4.5–3.5 | 4–3 | 3–2 | −1.34 | 370 588.255 | ||||
| 1–0 | 3.5–2.5 | 3–2 | 2–1 | −1.54 | 370 599.860 | ||||
| 1–0 | 3.5–2.5 | 4–3 | 3–2 | −1.34 | 370 602.441 | ||||
| 1–0 | 3.5–2.5 | 3–2 | 3–2 | −1.34 | 370 604.078 | ||||
| 1–0 | 3.5–2.5 | 4–3 | 4–3 | −1.21 | 370 606.235 | ||||
| 1–0 | 3.5–2.5 | 3–2 | 4–3 | −1.19 | 370 608.246 | ||||
| 1–0 | 3.5–2.5 | 4–3 | 5–4 | −1.09 | 370 610.538 |
Notes. For each cluster of transitions (involving a common 
), an intensity cutoff of a factor 4 of the strongest component is used. Frequencies, experimental uncertainties (Unc.), and residuals (fexp −fcalc) are expressed in MHz; Icalc in nm2 MHz. Intensities have been determined using a partition function Q(10 K) = 259.1302 determined using Pickett’s SPCAT program. (a)The quantum number F only exists for the ortho levels (see text).
(b) Predictions from the final fit.
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