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Table C.1.

Photometry of our F200W dropouts.

ID Names fF435W [nJy] fF606W [nJy] fF814W [nJy] fF105W [nJy] fF125W [nJy] fF140W [nJy] fF160W [nJy]
U-31863 BUDIARA −3.60 ± 5.20 2.39 ± 5.90
U-34120 VICIADGO 5.23 ± 5.04 −0.78 ± 3.79 2.78 ± 5.82 −12.64 ± 14.84 −23.42 ± 5.60
U-53105 - −0.16 ± 4.45 3.72 ± 4.20 0.89 ± 4.95 −8.68 ± 7.16 23.44 ± 12.48 −14.71 ± 6.42
U-75985 LIZZAN 6.49 ± 4.21 2.83 ± 1.79 3.54 ± 2.84 −6.22 ± 3.19 −0.41 ± 4.01 −0.58 ± 2.75
U-80918 NASPE 1.41 ± 5.50 0.82 ± 4.33 −3.99 ± 5.51 12.79 ± 7.30 12.96 ± 13.28 −1.67 ± 6.48
U-100588 - 0.96 ± 4.16 −3.88 ± 5.46 0.20 ± 5.79 11.57 ± 7.28 −3.61 ± 13.06 −6.38 ± 6.68
U-106373 - −1.85 ± 5.60 0.50 ± 3.81 1.17 ± 6.25 4.08 ± 4.60 7.77 ± 4.18
U-112842 CURION −1.33 ± 3.25 −1.35 ± 4.02 −10.16 ± 6.45 6.15 ± 5.87 6.68 ± 9.75 −13.74 ± 4.78
A-22691 ARCERIO 3.06 ± 3.55 4.13 ± 3.66 5.74 ± 10.02 5.39 ± 8.89
A-26130 - 0.00 ± 5.17 −6.18 ± 5.62 17.32 ± 14.25 12.02 ± 11.93
A-76468 - −1.23 ± 4.62 5.85 ± 7.08 12.42 ± 12.55 −9.45 ± 10.53


ID Names f F 090 W [ nJy ] Mathematical equation: $ \mathrm{f}_{\mathrm{F090W}} \, \mathrm{[nJy]} $ f F 115 W [ nJy ] Mathematical equation: $ \mathrm{f}_{\mathrm{F115W}} \, \mathrm{[nJy]} $ f F 150 W [ nJy ] Mathematical equation: $ \mathrm{f}_{\mathrm{F150W}} \, \mathrm{[nJy]} $ f F 200 W [ nJy ] Mathematical equation: $ \mathrm{f}_{\mathrm{F200W}} \, \mathrm{[nJy]} $ f F 277 W [ nJy ] Mathematical equation: $ \mathrm{f}_{\mathrm{F277W}} \, \mathrm{[nJy]} $ f F 356 W [ nJy ] Mathematical equation: $ \mathrm{f}_{\mathrm{F356W}} \, \mathrm{[nJy]} $ f F 410 M [ nJy ] Mathematical equation: $ \mathrm{f}_{\mathrm{F410M}} \, \mathrm{[nJy]} $ f F 444 W [ nJy ] Mathematical equation: $ \mathrm{f}_{\mathrm{F444W}} \, \mathrm{[nJy]} $

U-31863 BUDIARA 5.64 ± 3.55 4.61 ± 2.53 3.18 ± 1.98 10.18 ± 1.33 11.66 ± 1.49 11.70 ± 1.56
U-34120 VICIADGO 5.78 ± 3.46 3.14 ± 1.73 2.84 ± 2.54 1.57 ± 1.91 10.04 ± 1.84 9.28 ± 1.32 12.34 ± 2.49 7.30 ± 1.30
U-53105 - 3.31 ± 3.97 3.74 ± 3.62 7.66 ± 4.04 6.33 ± 3.53 9.41 ± 2.10 13.24 ± 2.02 16.02 ± 4.58 23.06 ± 3.91
U-75985 LIZZAN 1.15 ± 1.17 1.43 ± 2.01 −0.54 ± 1.89 1.64 ± 1.17 5.47 ± 1.07 9.40 ± 1.23 3.38 ± 2.13 4.32 ± 1.03
U-80918 NASPE 4.14 ± 3.60 −10.81 ± 9.89 3.98 ± 2.81 12.56 ± 2.13 16.43 ± 2.43 14.88 ± 3.94 8.44 ± 2.06
U-100588 - −2.86 ± 4.14 −1.75 ± 3.02 5.01 ± 4.11 0.58 ± 3.34 −1.12 ± 2.18 −0.93 ± 2.11 23.04 ± 5.03 27.83 ± 2.22
U-106373 - 2.83 ± 1.88 2.75 ± 3.08 3.08 ± 2.83 4.31 ± 2.34 1.03 ± 1.35 6.67 ± 1.86 18.34 ± 2.64 17.20 ± 1.86
U-112842 CURION 0.83 ± 2.41 0.99 ± 2.80 −0.49 ± 1.74 −0.81 ± 1.77 5.18 ± 1.46 31.34 ± 3.37 32.08 ± 1.64
A-22691 ARCERIO 1.02 ± 2.16 0.59 ± 2.09 2.65 ± 1.79 7.9 ± 1.83 9.32 ± 1.66 8.99 ± 2.97
A-26130 - 4.05 ± 2.95 1.09 ± 4.63 0.98 ± 3.63 11.21 ± 3.12 14.38 ± 2.23 25.04 ± 5.45 19.46 ± 4.87
A-76468 - 4.37 ± 2.94 3.75 ± 3.41 3.56 ± 2.79 6.55 ± 2.12 8.87 ± 2.13 18.45 ± 4.25 24.66 ± 3.36

Notes. We flagged with “-” all those observations that are not available in a certain band. Negative flux values are likely produced by local over-subtractions of the background, and they were treated in our analysis as upper limits.

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