Table 4: Hemispheres of maximal asymmetry from a $5^\circ $search (in contrast to the more accurate $1^\circ $ search in Table 3). The purpose of the sparse search is to run MC simulations. The meaning of the columns is explained in the caption of Table 3.
  d.o.f. $\frac{\chi^2}{\rm d.o.f.}$ $\frac{H_0}{H_0^*}$ q0 MC$_{\chi^2}$ MC $_{\frac{H_0}{H_0^*}}$ MCq0
          ( $\Delta \chi ^2$) ( $\Delta \frac{H_0}{H_0^*}$) ( $\Delta q_0$)

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)
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) )
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)


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