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Table 1:

NIR and optical photometry of the single counterpart.
Date 2007-03-05T01:27-02:00
Filters J H $K_{{\rm S}}$
Mag.$^\diamond$ $15.2 \pm0.1$ $13.66\pm0.03$ $12.3 \pm0.2$
$Z_{{\rm p}}$ $2.0\pm0.1$ $2.12\pm0.03$ $2.9\pm0.2$
$AM^\dagger$ 1.10 1.09 1.08
SMA $[~\hbox{$^{\prime\prime}$ }]$ 3.3 4.0 4.9
PA $[~\hbox{$^\circ$ }]$ $-50\pm11$ $-60\pm3$ $-51\pm2$
Ecc. $0.51\pm0.09$ $0.75\pm0.03$ $0.78\pm0.02$
Date 2007-03-10T00:21-00:41
Filters J H $K_{{\rm S}}$
Mag.$^\diamond$ $15.24\pm0.02$ $13.63\pm0.02$ $12.53\pm0.08$
$Z_{{\rm p}}$ $1.929\pm0.002$ $2.07\pm0.02$ $2.62\pm0.07$
$AM^\dagger$ 1.20 1.18 1.16
SMA $[~\hbox{$^{\prime\prime}$ }]$ 3.3 4.0 4.9
PA $[~\hbox{$^\circ$ }]$ $-64\pm7$ $-62\pm3$ $-50\pm 2$
Ecc. $0.68\pm0.06$ $0.71\pm0.03$ $0.74\pm0.02$
Date 2007-03-14T00:26-00:36
Filters V R I
Mag. > $23.3\pm0.2$ $20.8\pm0.2$ $19.3\pm0.2$
$Z_{{\rm p}}$ $-0.50\pm0.01$ $-0.39\pm0.01$ $0.47\pm0.02$
AM 1.14 1.14 1.13
ext 0.13 0.09 0.05
$^\diamond$ Total NIR magnitudes were extracted within ellipses centred on the source and defined with the semi-major axis (SMA), the position angle (PA, relative to west axis and counter clockwise), and the eccentricity (Ecc.); $^\dagger$ The NIR extinction parameters were fixed to $JHK_{{\rm S}} = 0.07,0.03,$ 0.03 with an error of $\Delta ext/ext=0.2$.

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