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Table 4

Multi-wavelength photometry of H14290028.

Survey/ Filter Total Foreg. Backg.a
facility [μJy] [μJy] [μJy]

SDSS u <4.9
g 5.9 ± 0.8
r 20.5 ± 1.1
i 35.3 ± 1.9
z 61.9 ± 7.4
VIKING Z 52.7 ± 3.1
Y 78.8 ± 5.9
J 133.9 ± 6.7
H 192 ± 12 134.8 ± 8.4 6.4 ± 0.6b
K s 380 ± 12 224.7 ± 6.9 17.4 ± 1.5b
HST F110W 98.8 ± 4.2 78.1 ± 3.5 2.6 ± 0.3b

Survey/ Filter Total Foreg. Backg.
facility [mJy] [mJy] [mJy]

Spitzer 3.6 μm 0.614 ± 0.003
4.5 μm 0.673 ± 0.004
WISE 3.4 μm 0.558 ± 0.014
4.6 μm 0.653 ± 0.020
12 μm 5.39 ± 0.15
22 μm 6.22 ± 0.76
Herschel 100 μm 821 ± 28
160 μm 1164 ± 32
250 μm 778 ± 6
350 μm 467.0 ± 7.0
500 μm 227.0 ± 8.0
IRAM-30 1.2 mm 10.3 ± 2.5
ALMA 1.28 mm 5.86 ± 0.99 0.543 ± 0.098c
2.8 mm 0.54 ± 0.11
JVLA 7 GHz 0.91 ± 0.08 <0.03 0.175 ± 0.023c

Notes. Upper limits are set at the 3σ level.

(a)

Intrinsic (demagnified) fluxes.

(b)

Estimated via direct analysis of high-resolution HST F110W, Keck AO H and Ks imaging and demagnified by μ = 7.9 ± 0.8 in the former and μ = 8.9 ± 0.7 in the Keck bands.

(c)

Assumed to be equal to the total flux and demagnified by μ = 10.8 ± 2 at 1.28 mm and μ = 5.2 ± 0.5 at 7 GHz (Table 3).

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