Table 2
Catalogue of z, Y, and J-dropouts in A2667.
Source | RA | Dec | H | ΔH | Stell. | FWHM | μ | μ | Δμ | Q1 | Q2 | Q3 | Q |
![]() |
Final |
(J2000) | (J2000) | [″] | high-z | low-z | |||||||||||
|
|||||||||||||||
z1 | 23:51:45.837 | –26:7:07.20 | 23.59 | 0.03 | 0.03 | 0.74 | 1.169 | 1.119 | 0.018 | 3 | 3 | 1 | 7-I | –0.03 | (low) |
Y1 | 23:52:00.157 | –26:8:30.31 | 23.35 | 0.03 | 0.03 | 0.95 | 1.028 | 1.012 | 0.003 | 1 | 1 | 2 | 4-III | 1.00 | low |
Y2 | 23:51:57.156 | –26:4:02.37 | 23.45 | 0.03 | 0.40 | 0.58 | 1.108 | 1.031 | 0.007 | 2 | 2 | 1 | 5-III | 1.19 | low |
Y3 | 23:51:43.332 | –26:8:00.89 | 23.68 | 0.04 | 0.02 | 1.24 | 1.128 | 1.059 | 0.012 | 3 | 3 | 2 | 8-I | 0.54 | high |
Y4 | 23:51:35.750 | –26:7:10.65 | 23.80 | 0.04 | 0.12 | 0.74 | 1.371 | 1.111 | 0.020 | 1 | 3 | 2 | 6-II | 0.64 | high |
Y5 | 23:51:54.448 | –26:3:13.65 | 23.98 | 0.04 | 0.03 | 0.96 | 1.149 | 1.037 | 0.007 | 2 | 2 | 2 | 6-II | 0.68 | ? |
Y6 | 23:51:53.437 | –26:4:29.94 | 24.37 | 0.08 | 0.02 | 1.81 | 1.167 | 1.067 | 0.011 | 1 | 1 | 3 | 5-III | 0.07 | low |
Y7 | 23:51:56.568 | –26:7:51.45 | 24.27 | 0.05 | 0.02 | 1.13 | 1.045 | 1.021 | 0.005 | 3 | 3 | 2 | 8-I | 0.00 | low |
Y8 | 23:51:37.151 | –26:2:30.46 | 25.40 | 0.08 | 0.97 | 0.46 | 1.183 | 1.140 | 0.018 | 1 | 2 | 3 | 6-II | 0.58 | low |
J1 | 23:51:34.855 | –26:3:32.74 | 25.21 | 0.08 | 0.97 | 0.55 | 1.299 | 1.398 | 0.033 | 3 | 3 | 2 | 8-I | 0.60 | (low) |
Notes. Information given in this table: (1) Object identification; (2, 3) α and δ J2000; (4, 5) AUTO magnitudes and error bars in H band; (6, 7) SExtractor stellarity index and maximum FWHM measured on the detection H + Ks image; (8, 9, 10) lensing magnification (high-z and low-z hypothesis) and associated uncertainty; (11, 12, 13) quality grade for high-z candidates according to three criteria: possible contamination by close neighbours (Q1), completeness and quality of photometric SED (Q2), and UV luminosity (Q3); (14) total grade Q; (15) optical χ2, and (16) tentative classification between low and high-z using a stringent prior in magnitude. In the case of z1 and J1 (in brackets), the low-z indentification is forced based on the detections in the 24 μm and z850 bands, respectively, for z1 and J1 (see Sect. 4.6).
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