Table C.1.
Comparison of the NIRCam photometry of GN-z11 with the NIRSpec spectroscopy.
| Filter | Prism flux | Grating flux | Grating |
|---|---|---|---|
| nJy | nJy | ||
| F090W −1.0 ± 1.7 | 1.4 ± 0.9 | −3.0 ± 3.8 | G140M |
| F115W 1.2 ± 1.5 | 0.6 ± 0.9 | −3.6 ± 1.7 | G140M |
| F150W 99.2 ± 1.6 | 100.0 ± 1.1 | 103.0 ± 3.3 | G140M |
| F200W 135.2 ± 1.5 | 133.8 ± 1.0 | 139.7 ± 2.9 | G235M |
| F277W 112.0 ± 1.0 | 115.1 ± 0.9 | 132.8 ± 3.5 | G235M |
| F335M 107.2 ± 1.9 | 113.0 ± 1.3 | 127.2 ± 4.1 | G395M |
| F356W 106.7 ± 1.0 | 112.5 ± 1.0 | 124.3 ± 2.9 | G395M |
| F410M 109.9 ± 1.4 | 112.8 ± 1.8 | 108.3 ± 5.0 | G395M |
| F444W 121.0 ± 1.3 | 118.68 ± 1.5 | 114.7 ± 4.5 | G395M |
The NIRCam photometry of GN-z11 in a 
-diameter aperture (column 2) from Tacchella et al. (2023) is compared with that inferred from the spectroscopy in the low-dispersion prism (column 3) and medium-dispersion gratings (flux in column 4, and grating which overlaps that filter in column 5). The spectroscopic measurements use the 3-pixel extraction.
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