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Table 2:

List of possible additional faint counterparts to CMaX sources.

CMaX
RA Dec $R_{\rm int}$ R V-R R-I $J_{\rm int}$ J J-Hd H-Kd Age Mass
  J2000 J2000 (mag) (mag) (mag) (mag) (mag) (mag) (mag) (mag) (Myr) ($M_{\odot }$)

15-1
7 00 13.364 -11 18 53.43 16.5e 17.1a 0.29 1.08b 14.4e 14.77 0.70 $\pm$ 0.06 0.19 $\pm$ 0.07 10-20 0.5-1.0
15-2 7 00 13.509 -11 19 11.14   18.3 0.70 0.78   16.84 0.66 $\pm$ 0.28 0.81 $\pm$ 0.28c ?? ??
15-3 7 00 15.325 -11 18 58.56   18.6 0.73 0.79   16.71 0.38 $\pm$ 0.29 0.68 $\pm$ 0.34c ?? ??
15-4 7 00 15.378 -11 19 3.78   19.7 1.6 1.56b   16.45 0.76 $\pm$ 0.19 0.29 $\pm$ 0.24 10-20 0.1-0.5

17N
7 00 18.724 -11 22 24.02   18.8 0.89 0.90b   16.59 0.50$\pm$ 0.25 0.58$\pm$ 0.30c ?? ??
17S1 7 00 18.806 -11 23 16.10 16.9e 17.1 0.9 0.79b 15.4e 15.58 0.77 $\pm$ 0.1 0.14 $\pm$ 0.14 20-50 0.5-1.0
17S2 7 00 18.886 -11 23 23.67   19.2 1.22 1.15b   16.71 0.89 $\pm$ 0.22 0.14 $\pm$ 0.29 20-50 0.1-0.5

37-1
7 01 22.297 -11 09 9.29   17.7 0.9 0.97b   16.18 0.65 $\pm$ 0.15 -0.1 $\pm$ 0.24 10-20 0.5-1.0
37-2 7 01 23.560 -11 08 26.77   18.2 1.61 1.67b   15.71 0.73 $\pm$ 0.12 0.07 $\pm$ 0.16 1-2 0.5-1.0
37-3 7 01 24.356 -11 09 03.00 15.9e 16.3a -0.3 0.88b 14.3e 14.78 0.55 $\pm$ 0.06 0.11 $\pm$ 0.08 5-10 0.5-1.0

42-1
7 01 35.313 -11 10 12.23   17.2 0.73 0.73b         20-50 0.5-1.0
42-2 7 01 35.437 -11 10 44.07 15.6e 15.7a -0.08 0.86b 13.9e 14.44 0.35 $\pm$ 0.06 0.08 $\pm$ 0.08 2-5 0.5-1.0
42-3 7 01 35.473 -11 10 14.46   16.4 0.74 0.71b   14.70 0.73 $\pm$ 0.08 0.21 $\pm$ 0.08 10-20 0.5-1.0

55N
7 02 8.021 -11 16 17.65 18.2e 18.2a 0.98 1.08b 15.6e 15.67 0.64 $\pm$ 0.1 0.35 $\pm$ 0.13 10-20 0.1-0.5
55S 7 02 8.139 -11 17 35.46   18.9 0.6 0.74   16.46 0.73 $\pm$ 0.2 0.58 $\pm$ 0.22c ?? ??

Notes: (a) Magnitudes adopted from the NOMAD and/or USNO catalogues, when the estimation from Gemini images are unavailable, due to saturation; (b) counterparts selected according to the R-I excess; (c) counterparts having H-K excess; (d) the 2MASS catalogue was used to obtain the JHK magnitudes, for which error bars are provided; (e) $R_{\rm int}$ and $J_{\rm int}$ represent the ``integrated'' magnitudes (see Sect. 4.2), which are shown together with the brightest object of each group.


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