\begin{table}%t1
%\begin{center}
\par
\caption {The ``$\chi^2$ Championship''.} \label{tab:khi2}
\begin{tiny}
\begin{tabular}{c|ccc|cccc|cccc} \hline\hline
Template $\rightarrow$ & \multicolumn{3}{|c|}{ASS} &
\multicolumn{4}{|c|}{BSS} & \multicolumn{4}{|c}{QSS} \\
 model $\downarrow$   & $p'$ & $B'$ & $\chi^2$ & $p'$ &
$\phi_0'$ & $B'$ & $\chi^2$  & $p'$ & $\phi_0'$ & $B'$ & $\chi^2$
 \\ \hline
 {ASS} & {20~$\pm$~2} & {5.0~$\pm$~0.3} & {\bf  1.1~$\pm$~0.4} & {7~$\pm$~18} & {2~$\pm$~96} & {4.6~$\pm$~1.8} & {21~$\pm$~6} & 
   {23~$\pm$~48} & {--6~$\pm$~41} & {5.2~$\pm$~0.8} & {13~$\pm$~3} \\
 {BSS} & {--22~$\pm$~47} & {0.6~$\pm$~0.7} & {13~$\pm$~3} & {21~$\pm$~2} & {14~$\pm$~32} & {5.1~$\pm$~0.4} & { \bf 1.1~$\pm$~0.3} &
   {8~$\pm$~14} & {10~$\pm$~52} & {4.0~$\pm$~1.9} & {11~$\pm$~3} \\
 {QSS} & {--25~$\pm$~39} & {0.7~$\pm$~0.6} & {12~$\pm$~3} & {8~$\pm$~23} & {--8~$\pm$~95} & {3.5~$\pm$~1.3} & {9~$\pm$~3} &
   {20~$\pm$~1} & {--3~$\pm$~16} & {4.9~$\pm$~0.5} & {\bf  1.3~$\pm$~0.3} \\
 {ASS+BSS} & {19~$\pm$~6} & {2.5~$\pm$~0.4} & {3.8~$\pm$~1} & {19~$\pm$~16} & {13~$\pm$~107} & {3.2~$\pm$~1.1} & {6~$\pm$~2} &
   {24~$\pm$~47} & {2~$\pm$~37} & {2.9~$\pm$~0.7} & {6~$\pm$~2} \\
 {ASS+QSS} & {18~$\pm$~6} & {2.6~$\pm$~0.4} & {3.4~$\pm$~1} & {4~$\pm$~14} & {16~$\pm$~95} & {3.0~$\pm$~1.5} & {8~$\pm$~3} &
   {10~$\pm$~35} & {10~$\pm$~33} & {3.3~$\pm$~1.2} & {6~$\pm$~2}
\\   \hline
\end{tabular}
\par
\begin{tabular}{c|ccccc|ccccc} \hline
Template $\rightarrow$ & \multicolumn{5}{|c|}{ASS+BSS} & \multicolumn{5}{|c}{ASS+QSS} \\
  model $\downarrow$ & $p'$ & $q'$ & $\phi_0'$ & $B'$ & $\chi^2$  & $p'$ & $q'$ & $\phi_0'$ & $B'$ & $\chi^2$
 \\ \hline
 {ASS} & {20~$\pm$~2} & {0.9~$\pm$~0.1} & {--3~$\pm$~98} & {5.6~$\pm$~0.3} & {\bf  1.2~$\pm$~0.4} & {20~$\pm$~3} & {0.9~$\pm$~0.1} & 
   {7~$\pm$~52} & {5.7~$\pm$~0.4} & {\bf  1.2~$\pm$~0.3} \\  
 {BSS} & {21~$\pm$~2} & {0.0~$\pm$~0.1} & {9~$\pm$~26} & {5.0~$\pm$~0.4} & {\bf  1.2~$\pm$~0.4} & {8~$\pm$~14} & {0.1~$\pm$~0.1} & {2$\pm
   $50} & {5~$\pm$~2} & {10~$\pm$~3} \\ 
 {QSS} & {2~$\pm$~19} & {0.1~$\pm$~0.1} & {--21~$\pm$~95} & {3.7~$\pm$~1.2} & {10~$\pm$~4} & {20~$\pm$~1} & {0.0~$\pm$~0.1} &
   {0~$\pm$~6} & {5.1~$\pm$~0.3} & {\bf  1.2~$\pm$~0.3} \\ 
 {ASS+BSS} & {22~$\pm$~3} & {0.5~$\pm$~0.1} & {18~$\pm$~46} & {5.1~$\pm$~0.4} & {\bf  1.2~$\pm$~0.4} & {18~$\pm$~10} & {0.6~$\pm$~0.1} &
   {6~$\pm$~50} & {4.0~$\pm$~0.8} & {3.7~$\pm$~0.9} \\
 {ASS+QSS} & {15~$\pm$~10} & {0.7~$\pm$~0.1} & {--3~$\pm$~96} & {4.1~$\pm$~0.8} & {3.3~$\pm$~1.3} & {21~$\pm$~2} & {0.5~$\pm$~0.1} &
   {6~$\pm$~27} & {4.9~$\pm$~0.5} & {\bf  1.2~$\pm$~0.3}
\\   \hline
\par
\end{tabular}
\end{tiny}
%\end{center}
\par
%\medskip
{Parameters of fitted pitch angles $p'$ and field amplitudes $B'$,
azimuthal phases $\phi_0'$, and $\chi^2$ values of the best-fit
template (first row). The models of field structures are given in
the first column. For the superposition templates (second part of
the table), $q'$ is the relative amplitudes of the ASS mode, with
$q=0.5$ assumed in the model. The models with $\chi^2<1.7$ which
cannot be statistically rejected are marked in bold.}
\end{table}