\begin{table}%t3 \caption{\label{tvlapar}Parameters of the continuum sources detected in the IRAS 00213+6530 region.} %\centerline {\begin{tabular}{lccccc} \hline\hline &\multicolumn{2}{c}{Position$^{\rm a}$}& Flux Density& Flux Density& Spectral\\ \cline{2-3} &$\alpha$ (J2000) &$\delta$ (J2000) &at 6~cm &at 3.6~cm &Index\\ Source& (h m s)& ($\degr$ $'$ $''$)& (mJy)& (mJy)& 6~cm--3.6~cm \\ \hline\noalign{\smallskip} 1& 00 23 21.01& $+$65 43 46.5& 0.87~$\pm$~0.07& \ldots$^{b}$& \ldots\\ 2& 00 23 45.65& $+$65 48 36.1& 0.17~$\pm$~0.03& $<$0.18$^{c}$& $<$0.10\\ 3& 00 23 46.41& $+$65 49 12.7& 1.66~$\pm$~0.04& 0.38~$\pm$~0.07$^{d}$& $-$2.7~$\pm$~0.3\\ 4& 00 23 49.01& $+$65 46 14.7& 0.69~$\pm$~0.03& 0.42~$\pm$~0.02& $-$0.9~$\pm$~0.1\\ 5& 00 23 52.06& $+$65 39 58.9& 4.20~$\pm$~0.60& \ldots$^{b}$& \ldots\\ 6& 00 23 53.70& $+$65 49 41.6& 0.86~$\pm$~0.03& $<$0.25$^{c, d}$& $<$$-2.1$\\ 7& 00 24 09.11& $+$65 46 58.0& 0.57~$\pm$~0.03& 0.24~$\pm$~0.02& $-$1.6~$\pm$~0.2\\ 8& 00 24 11.39& $+$65 47 09.6& 0.16~$\pm$~0.03& 0.21~$\pm$~0.02& \phb0.5~$\pm$~0.4\\ 9& 00 24 24.46& $+$65 49 05.9& 0.13~$\pm$~0.03& 0.27~$\pm$~0.02& \phb1.3~$\pm$~0.4\\ 10& 00 24 36.71& $+$65 48 27.5& 0.55~$\pm$~0.03& 0.22~$\pm$~0.03& $-$1.7~$\pm$~0.3\\ 11& 00 24 56.70& $+$65 49 10.3& 0.63~$\pm$~0.05& \ldots$^{b}$& \ldots\\ 12& 00 25 24.75& $+$65 45 48.3& 4.90~$\pm$~1.10& \ldots$^{b}$& \ldots\\ \hline \end{tabular}} \medskip $^a$~Positions taken from the 3.6~cm map, except for non-detected sources at this band, for which positions correspond to the 6~cm map. $^b$~Source well outside the primary beam at this wavelength. Primary beam correction greater than 12, and the uncertainty in the corrected flux is very large. $^c$~The upper limit for non-detected sources is 4$\sigma$. $^d$~Flux density measured in 2000 September 23. Source highly variable, so to compute the spectral index we used observations carried out at the same epoch. \end{table}