\begin{table}%tB.1%tB.2 \caption{\label{tab:cardpsb}Polarization efficiencies and orientations for \textit{Planck}-HFI PSBs.} %\centering \par \begin{tabular}{ccc} \hline\hline \noalign{\smallskip} Bolometer (PSB) \T\B & Polarization efficiency [\%] & Polarization angle \\ \hline\noalign{\smallskip} 100-1a & 94.7 $\pm$ 0.2 & *21\pdeg1 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 100-1b & 94.3 $\pm$ 0.3 & 109\pdeg9 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 100-2a & 96.2 $\pm$ 0.2 & *44\pdeg3 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 100-2b & 90.2 $\pm$ 0.2 & 133\pdeg5 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 100-3a & 90.1 $\pm$ 0.3 & **0\pdeg7 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 100-3b & 93.4 $\pm$ 0.2 & *90\pdeg6 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 100-4a & 95.7 $\pm$ 0.3 & 158\pdeg5 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 100-4b & 92.3 $\pm$ 0.2 & *70\pdeg0 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 143-1a & 83.3 $\pm$ 0.2 & *42\pdeg9 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 143-1b & 84.6 $\pm$ 0.2 & 135\pdeg2 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 143-2a & 87.5 $\pm$ 0.3 & *44\pdeg2 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 143-2b & 89.3 $\pm$ 0.3 & 134\pdeg0 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 143-3a & 83.9 $\pm$ 0.2 & **0\pdeg4 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 143-3b & 89.9 $\pm$ 0.2 & *93\pdeg7 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 143-4a & 93.1 $\pm$ 0.2 & **3\pdeg1 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 143-4b & 92.8 $\pm$ 0.2 & *91\pdeg5 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 217-5a & 95.0 $\pm$ 0.1 & *44\pdeg7 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 217-5b & 95.2 $\pm$ 0.2 & 133\pdeg9 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 217-6a & 94.9 $\pm$ 0.2 & *45\pdeg0 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 217-6b & 95.4 $\pm$ 0.2 & 134\pdeg8 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 217-7a & 94.0 $\pm$ 0.2 & **0\pdeg3 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 217-7b & 93.7 $\pm$ 0.1 & *91\pdeg2 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 217-8a & 94.2 $\pm$ 0.1 & **2\pdeg2 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 217-8b & 94.1 $\pm$ 0.1 & *92\pdeg5 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 353-3a & 88.7 $\pm$ 0.1 & *44\pdeg1 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 353-3b & 92.0 $\pm$ 0.1 & 132\pdeg4 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 353-4a & 87.0 $\pm$ 0.1 & *45\pdeg3 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 353-4b & 91.4 $\pm$ 0.1 & 135\pdeg2 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 353-5a & 84.4 $\pm$ 0.1 & 178\pdeg4 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 353-5b & 87.4 $\pm$ 0.1 & *90\pdeg3 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 353-6a & 87.3 $\pm$ 0.1 & **1\pdeg3 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ 353-6b & 88.5 $\pm$ 0.1 & *91\pdeg2 $\pm$ 0\pdeg9 [rel] $\pm$ 0\pdeg3 [abs]\\ \hline \end{tabular} \tablefoot {Ideal PSBs should have a 100\% polarization efficiency. The error on polarization efficiency is only statistical. Error on polarization orientation is due to systematics: the absolute error is due to the error on the measurement of the reference position; the relative error is due to an optical systematic effect in the Saturne cryostat. The statistical errors are negligible and therefore not shown in this table.} \end{table}