\begin{table}%t2 \caption{Point sources identified in our speckle images. For details about~IRS1 and the binary system~IRS2$a$/$b$, we refer to the text. We identify components~$a$ to~$f$ with the stars already discovered in the image by \cite{alv04}. } \label{tab:pointsources} \small%\centerline { \begin{tabular}{c c c c l} \hline\hline % & & & & \\[-8pt] Name & RA~(J2000)$^a$ & Dec~(J2000)$^a$ & $K'$ Magnitude$^b$ & Comment\\ % & & & & \\[-8pt] \hline % & & & & \\[-8pt] a & \rahm{23}{13}\ras{45}{33} & \decdm{61}{28}\decs{21}{02}& 10\fracmag94 & \\ b & \hspace{11mm}\ras{44}{81} & \hspace{10mm}\decs{10}{63} & 11\fracmag29 & \\ c & \hspace{11mm}\ras{44}{95} & \hspace{10mm}\decs{12}{33} & 11\fracmag46 & \\ d & \hspace{11mm}\ras{45}{11} & \hspace{10mm}\decs{09}{69} & 11\fracmag73 & \\ e & \hspace{11mm}\ras{45}{37} & \hspace{10mm}\decs{15}{12} & 11\fracmag77 & embedded in feature $C$\\ f & \hspace{11mm}\ras{45}{34} & \hspace{10mm}\decs{15}{93} & 11\fracmag73 & embedded in feature $C$\\ g & \hspace{11mm}\ras{45}{36} & \hspace{10mm}\decs{14}{80} & 11\fracmag73 & embedded in feature $C$\\ h & \hspace{11mm}\ras{45}{31} & \hspace{10mm}\decs{14}{72} & 11\fracmag86 & \\ i & \hspace{11mm}\ras{45}{29} & \hspace{10mm}\decs{13}{74} & 11\fracmag71 & \\ j & \hspace{11mm}\ras{45}{27} & \hspace{10mm}\decs{13}{25} & 11\fracmag73 & \\ k & \hspace{11mm}\ras{45}{25} & \hspace{10mm}\decs{13}{05} & 11\fracmag81 & \\ l & \hspace{11mm}\ras{45}{24} & \hspace{10mm}\decs{13}{28} & 11\fracmag83 & \\ m & \hspace{11mm}\ras{45}{22} & \hspace{10mm}\decs{12}{71} & 11\fracmag71 & \\ n & \hspace{11mm}\ras{45}{36} & \hspace{10mm}\decs{12}{99} & 11\fracmag75 & \\ o & \hspace{11mm}\ras{45}{50} & \hspace{10mm}\decs{10}{50} & 11\fracmag60 & \\ p & \hspace{11mm}\ras{45}{29} & \hspace{10mm}\decs{18}{42} & 11\fracmag73 & \\ q & \hspace{11mm}\ras{45}{16} & \hspace{10mm}\decs{19}{69} & 11\fracmag77 & \\ r & \hspace{11mm}\ras{45}{33} & \hspace{10mm}\decs{08}{48} & 11\fracmag71 & \\ \hline \end{tabular}} \medskip $^{a}$ For the astrometry, the relative errors are of the order of~0\farcs1. The absolute calibration using the reference position of IRS1 in 2MASS introduces further errors~(0\farcs2); $^{b}$~the photometry was done relative to IRS1 with an~uncertainty of~0\fracmag3. For the conversion to absolute photometry, we assumed a~IRS1~magnitude of~8\fracmag9 \citep{ojh04}. \end{table}