\begin{table}%t6
  \caption{As for Table~\ref{hornFluctTab}, but for the cryo-stage of the SPOrt~radiometers.
  As a worst case, we assume 
  $A_{\rm p} = 0.1$~dB and $A_{\rm omt} = 0.2$~dB the attenuations of
  polarizer and~OMT, respectively. Anyway, the offset fluctuations are
  marginally dependent on their values, $S\!P_{\rm pol}$ being
  the dominant term.} \label{cryoFluctTab}
%\centering
\par
  \begin{tabular}{@{}lcccccccccc@{}}
     \hline \hline
     Configuration     & $\Delta T_{\rm ph}^{\rm cryo}$ & 
     $A_{\rm h}$  & $|S_{B1}|^2$  & 
     $A_{\perp}-A_{\parallel}$  & $S\!P_{\rm omt}$  &
     $S\!P_{\rm pol}$ & $H_{\rm p}$ & $H_{\rm omt}$ & 
     $\Delta(Q+jU)$  \\
             &  [K] & 
      [dB] &  [dB] & 
      [dB] &    &    &    &    &
      [$\mu$K]  \\
     \hline
     22 GHz       &  $\pm$$0.1$  & 0.05 & --65 & --33 
      & $1.15\times 10^{-3}$  & $2.45\times 10^{-4}$ & 
      $3.21\times 10^{-4}$ & $8.62\times 10^{-5}$ & 
     40.7\\
     90 GHz       &  $\pm$$0.1$  & 0.1 & --60 & --30 
      & $2.05\times 10^{-3}$  & $4.89\times 10^{-4}$ & 
      $6.46\times 10^{-4}$ & $1.56\times 10^{-4}$ &
     80.2\\
     \hline
\end{tabular}
\end{table}