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Table 4
Convergence of the integrated intensities Σ (× 10-17 cm/molecules) as a function of the cutoffs on the lower energy E (in cm-1), the line intensity I (in cm/molecule), and the rotational quantum number J.
| Wavenumbers ≤ 6400 cm-1 | Wavenumbers ≤ 5200 cm-1 | ||||
| T | 80 K | 160 K | 296 K | 500 K | 700 K |
| Lower energy cut-off | Integrated intensities | ||||
| E ≤ 500 | 2.551 | 2.473 | 1.969 | 0.986 | 0.413 |
| E ≤ 1000 | 2.553 | 2.549 | 2.382 | 1.516 | 0.752 |
| E ≤ 2000 | 2.553 | 2.552 | 2.545 | 2.255 | 1.580 |
| E ≤ 3000 | 2.552 | 2.552 | 2.468 | 2.117 | |
| E ≤ 4000 | 2.552 | 2.512 | 2.381 | ||
| E ≤ 5000 | 2.517 | 2.475 | |||
| E ≤ 6000 | 2.518 | 2.494 | |||
| E ≤ 7000 | 2.496 | ||||
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| Intensity cutoff | |||||
| I ≥ 10-21 | 2.281 | 2.152 | 1.853 | 1.052 | 0.363 |
| I ≥ 10-22 | 2.475 | 2.425 | 2.278 | 1.804 | 1.142 |
| I ≥ 10-23 | 2.533 | 2.517 | 2.463 | 2.231 | 1.799 |
| I ≥ 10-24 | 2.548 | 2.544 | 2.525 | 2.414 | 2.189 |
| I ≥ 10-25 | 2.552 | 2.550 | 2.545 | 2.489 | 2.387 |
| I ≥ 5 × 10-26 | 2.553 | 2.551 | 2.548 | 2.501 | 2.423 |
| I ≥ 10-26 | 2.552 | 2.552 | 2.518 | 2.479 | |
| I ≥ 5 × 10-27 | 2.496 | ||||
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| Rotational cutoff | |||||
| J ≤ 15 | 2.499 | 2.167 | 1.591 | 1.051 | 0.762 |
| J ≤ 20 | 2.550 | 2.464 | 2.120 | 1.622 | 1.258 |
| J ≤ 30 | 2.553 | 2.551 | 2.506 | 2.279 | 2.027 |
| J ≤ 40 | 2.552 | 2.550 | 2.480 | 2.373 | |
| J ≤ 50 | 2.552 | 2.514 | 2.474 | ||
| J ≤ 60 | 2.518 | 2.493 | |||
| J ≤ 71 | 2.496 | ||||
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| Number of lines | 388 954 | 828 897 | 2 904 094 | 12 742 100 | 58 848 859 |
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