\begin{table}%t4 \caption{\label{tab4}Hemispheres of maximal asymmetry from a $5^\circ$ search (in contrast to the more accurate $1^\circ$ search in Table \ref{TgaleqHoqo}). The purpose of the sparse search is to run MC simulations. The meaning of the columns is explained in the caption of Table~\ref{TgaleqHoqo}.} %\centering \par \begin{tabular}{lccccccc} \hline\hline\noalign{\smallskip} & d.o.f. & $\frac{\chi^2}{\rm d.o.f.}$ & $\frac{H_0}{H_0^*}$ & $q_0$ & MC$_{\chi^2}$ & MC$_{\frac{H_0}{H_0^*}}$ & MC$_{q_0}$ \\ & & & & & ($\Delta\chi^2$)& ($\Delta\frac{H_0}{H_0^*}$) &($\Delta q_0$) \\\noalign{\smallskip} \hline {\bf data set A} \\ $A_{\rm V} \leq 1$, $\sigma_v = 345$ km~s$^{-1}$, $z \leq 0.2$ & 137 & 1.27 & $1.02 \pm 0.02$ & $-0.78 \pm 0.90$ &&& \\ Hemispheres max. Asymmetry in $\chi^2$:& & & &&&&\\ Pole: $(l,b)=(60^{\circ},10^{\circ}) $& 53 & 0.84 &$ 0.97 \pm 0.03 $&$ -0.11 \pm 1.45$ & 0.2$\%$ & 4.0$\%$ & 48.6$\%$ \\ Pole: $(l,b)=(240^{\circ},-10^{\circ})$& 82 & 1.33 &$ 1.08 \pm 0.03 $&$ -2.05 \pm 1.28$ & (37.93) & (0.11) & (1.95) \\ \hline {\bf data set B} \\ $A_{\rm V} \leq 1$, $\sigma_v = 345$ km~s$^{-1}$, $z \leq 0.2$ & 75 & 0.84 & $1.01 \pm 0.03$ & $-1.42 \pm 1.23$ &&&\\ Hemispheres max. Asymmetry in $\chi^2$:& & & &&&&\\ Pole: $(l,b)=(60^{\circ},10^{\circ}) $& 34 & 0.57 &$ 0.98 \pm 0.05 $&$ -1.34 \pm 2.63$ & 38.6$\%$ & 50.2$\%$ & 71.4$\%$ \\ Pole: $(l,b)=(240^{\circ},-10^{\circ})$& 39 & 0.96 &$ 1.06 \pm 0.05 $&$ -2.20 \pm 1.56$ & (11.98) & (0.08 & (0.87) ) \\ \hline {\bf data set D} \\ $A_{\rm V} \leq 1$, $\sigma_v = 345$ km~s$^{-1}$, $\sigma_{\rm int}=0.016$ $z \leq 0.2$ & 117 & 1.37 & $1.01 \pm 0.03$ & $-1.39 \pm 1.35$ &&&\\ Hemispheres max. Asymmetry in $\chi^2$:& & & &&&&\\ Pole: $(l,b)=(75^{\circ},20^{\circ}) $& 53 & 1.14 &$ 0.95 \pm 0.03 $&$ 1.45 \pm 1.88$ & $<$0.2$\%$ & 0.2$\%$ & 1.8$\%$ \\ Pole: $(l,b)=(255^{\circ},-20^{\circ})$& 62 & 1.36 &$ 1.08 \pm 0.04 $&$ -4.17 \pm 1.98$ & (32.33) & (0.13) & (5.62) \\ \hline \end{tabular} \end{table}