Table 1.
NIRCam and MIRI photometry.
| Filter | Units | Obs. | Cont. level |
|---|---|---|---|
| NIRCam/F115W | nJy | 31 ± 9 | – |
| NIRCam/F150W | nJy | 118 ± 9 | – |
| NIRCam/F182M | nJy | 177 ± 11 | 154 ± 12 |
| NIRCam/F200W | nJy | 201 ± 7 | 185 ± 8 |
| NIRCam/F210M | nJy | 175 ± 14 | 164 ± 14 |
| NIRCam/F277W | nJy | 161 ± 3 | 161 ± 3 |
| NIRCam/F335M | nJy | 130 ± 7 | 123 ± 7 |
| NIRCam/F356W | nJy | 153 ± 3 | 150 ± 3 |
| NIRCam/F410M | nJy | 133 ± 6 | 129 ± 6 |
| NIRCam/F444W | nJy | 163 ± 4 | 140 ± 4 |
| MIRIM/F560W | nJy | 368 ± 26 | 156 ± 31 |
| MIRIM/F770W | nJy | 274 ± 20 | 212 ± 22 |
| MIRIM/F1000W | nJy | 249 ± 77 | 237 ± 77† |
| MIRIM/F2100W | μJy | < 2.6 | < 2.6 |
Notes. The third and fourth columns display the observed and continuum level, i.e. the measured photometry and the continuum fluxes after subtracting the emission line contribution (see Sect. 3.2), respectively. We adopted 3σ upper limits for F2100W. †: The continuum level for F1000W was derived assuming a [S III]λλ9071,9533/Hα = 0.17 (see Sect. 4.1).
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