Table 3: Statistics of the field-star decontamination, in magnitude bins, for representative cases.
  FSR 942 ( $R<3\hbox {$^\prime $ }$)   FSR 855 ( $R<3\hbox {$^\prime $ }$)   FSR 801 ( $R<3\hbox {$^\prime $ }$)
$\Delta\mbox{$\space J$ }$ $ N_{\rm obs}$ $ N_{\rm cl}$ $ N_{1\sigma}$ $ \sigma_{\rm FS}$ $ FS_{\rm unif}$   $ N_{\rm obs}$ $ N_{\rm cl}$ $ N_{1\sigma}$ $ \sigma_{\rm FS}$ $ FS_{\rm unif}$   $ N_{\rm obs}$ $ N_{\rm cl}$ $ N_{1\sigma}$ $ \sigma_{\rm FS}$ $ FS_{\rm unif}$
(mag) (stars) (stars)   (stars)     (stars) (stars)   (stars)     (stars) (stars)   (stars)  
7-8 - - - - -   $1\pm1.0$ 1 1.0 0.42 1.07   - - - - -
8-9 - - - - -   - - - - -   - - - - -
9-10 - - - - -   $1\pm1.0$ 1 1.0 0.99 1.42   - - - - -
10-11 $3\pm1.7$ 3 1.7 0.57 0.51   $5\pm2.2$ 1 0.4 1.12 1.02   - - - - -
11-12 $4\pm2.0$ 4 2.0 0.38 0.18   $4\pm2.0$ 2 1.0 1.70 0.49   $2\pm1.4$ 1 0.7 0.18 0.23
12-13 $7\pm2.6$ 1 0.4 0.50 0.12   $6\pm2.4$ 1 0.4 3.09 0.43   $4\pm2.0$ 2 1.0 0.30 0.20
13-14 $24\pm4.9$ 17 3.5 0.75 0.08   $20\pm4.5$ 3 0.7 2.47 0.19   $4\pm2.0$ 2 1.0 0.36 0.10
14-15 $38\pm6.2$ 21 3.4 1.61 0.09   $33\pm5.7$ 6 1.0 6.27 0.26   $9\pm3.0$ 3 1.0 0.72 0.11
15-16 $63\pm7.9$ 27 3.4 2.87 0.08   $56\pm7.5$ 12 1.6 5.31 0.11   $25\pm5.0$ 9 1.8 1.60 0.12
16-17 $45\pm6.7$ 21 3.1 4.91 0.14   $72\pm8.5$ 29 3.4 6.14 0.12   $21\pm4.6$ 8 1.7 1.78 0.09
All $184\pm13.6$ 94 6.8 3.2 0.03   $198\pm14.1$ 56 3.6 11.1 0.07   $65\pm8.1$ 25 2.9 2.8 0.06
The table provides, for each magnitude bin ( $\Delta\mbox{$\space J$ }$), the number of observed stars ( $ N_{\rm obs}$) within the spatial region sampled in the CMDs shown in the top panels of Figs. 3 and 4, the respective number of probable member stars ( $ N_{\rm cl}$) computed by the decontamination algorithm, the $ N_{1\sigma}$ parameter, the 1$\sigma $ Poisson fluctuation ( $ \sigma_{\rm FS}$) around the mean, with respect to the star counts measured in the 8 sectors of the comparison field, and the field-star uniformity parameter ( $ FS_{\rm unif}$). The statistical significance of $ N_{\rm cl}$ is reflected in its ratio with the 1$\sigma $ Poisson fluctuation of $ N_{\rm obs}$ ( $ N_{1\sigma}$) and with $ \sigma_{\rm FS}$. The bottom line corresponds to the full magnitude range.


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