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Table 2.
Measurements of the H2 emission lines detected in the EMIR and-or X-shooter spectra of 4C12.50.
| EMIR |
X-shooter |
|||||
|---|---|---|---|---|---|---|
| Line | λ | Flux ×10−16 | FWHM | Flux ×10−16 | FWHM | |
| (μm) | (ergs cm−2 s−1) | (km s−1) | (ergs cm−2 s−1) | (km s−1) | ||
| H2 2–0 S(1) | 1.1622 | out | out | 2.20±0.21 | 455±35 | |
| H2 1–0 S(7) | 1.7480 | out | out | 5.10±0.37 | 461±23 | |
| H2 1–0 S(5) | 1.8358 | 11.4±0.40 | 471±8 | 12.50±0.60 | 465±15 | |
| H2 1–0 S(4) | 1.8920 | 3.65±0.18 | 424±17 | 4.31±0.15 | 389±14 | |
| H2 1–0 S(3) | 1.9576 | 20.1±0.3 | 418±12 | 16.7±0.4 | 424±21 | |
| H2 1–0 S(2) | 2.0338 | 6.03±0.24 | 453±9 | 5.51±0.84 | 457±66 (ns) | |
| H2 1–0 S(1) | 2.1218 | 20.0±1.9 | 446±26 | 21.30±1.10 | 435±9 | |
Notes. H2 1-0S(1) is on the red edge of the EMIR spectrum. The S(3) measurements are based on a simple, 1-Gaussian fit of the line profile above the broad pedestal.
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