In Fig. 
we show our final results for the dependence of the
integrated autocorrelation time on the anisotropy of the lattice for the six
lattice observables. We find small variation of the amplitude of the integrated
autocorrelation time 
for the temporal loops. The error bars
for these observables are small. It is apparent that the modes are strongly
suppressed because they effectively propagate in the spatial domain with
characteristic correlation length 
, which is small. In
contrast, the integrated autocorrelation times for the spatial loops increase
as 
increases.
Figure: Scaling behavior of 
on anisotropy.