Table 6.
Radio loudness.
Source | mz | S2500 Å | S4400 Å | S5 GHz | R2500 Å | R4400 Å |
---|---|---|---|---|---|---|
(mag) | (mJy) | (mJy) | (mJy) | |||
(1) | (2) | (3) | (4) | (5) | (6) | (7) |
J0131−0321 | (c)18.08 | 0.046 | 0.061 |
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J0741+2520 | (c)18.44 | 0.033 | 0.043 |
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J0836+0054 | (c, 1)18.83 | 0.022 | 0.029 |
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J0913+5919 | (c)20.81 | 0.0037 | 0.0049 |
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J1034+2033 | (c)19.70 | 0.010 | 0.014 |
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J1146+4037 | (c)19.30 | 0.015 | 0.020 |
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J1427+3312 | (c, 1)18.87 | 0.021 | 0.027 |
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J1614+4640 | (c)19.71 | 0.010 | 0.013 |
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J2228+0110 | (b, 1)22.28 | 0.00089 | 0.0012 |
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J2245+0024 | (a)21.72 | 0.0016 | 0.0021 |
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Notes. Column 1: source name. Column 2: z-band AB magnitude. Columns 3−4: rest-frame 2500 Å and 4400 Å flux density, which are calculated assuming a UV power law Sν ∝ ν−0.5 with z-band photometry data. Column 5: rest-frame 5 GHz flux density predicted from our spectral fit. Columns 6−7: radio loudness. (1)z-band magnitude is contaminated by the strong Lyα line emission.
References. (a)Sharp et al. (2001); (b)Zeimann et al. (2011); (c)SDSS.
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