\begin{table}%t2
  \caption{Statistical flow properties in the saturated, turbulent state.}\label{t:results}
\par
\small%\centerline
    \begin{tabular}{lcccccccc}
      \hline \hline
 \multicolumn{9}{c}{$|z|<2 H$ (85\% of the mass)}\\
        Run & ${\rm rms}(u_x)$ &
              ${\rm rms}(u_y)$ &
              ${\rm rms}(u_z)$ &
              ${\rm mean}(u_x u_y)$ &
              ${\rm rms}(B_x)$ &
              ${\rm rms}(B_y)$ &
              ${\rm rms}(B_z)$ &
              ${\rm mean}(B_x B_y)$  \\
      \hline
        S3D\_256 &
        $ 0.346 \pm 0.020$ & $ 0.261 \pm 0.020$ & $ 0.344 \pm 0.016$ & 
        $ 0.017 \pm 0.005$ & $ 0.189 \pm 0.009$ & $ 1.227 \pm 0.028$ & 
        $ 0.172 \pm 0.005$ & $-0.055 \pm 0.006$ \\
        S3D\_512 &
        $ 0.366 \pm 0.017$ & $ 0.331 \pm 0.009$ & $ 0.338 \pm 0.025$ & 
        $ 0.031 \pm 0.003$ & $ 0.287 \pm 0.015$ & $ 1.143 \pm 0.027$ & 
        $ 0.230 \pm 0.012$ & $-0.087 \pm 0.016$ \\
        S3D\_256\_b3 &
        $ 0.341 \pm 0.017$ & $ 0.232 \pm 0.009$ & $ 0.359 \pm 0.021$ & 
        $ 0.011 \pm 0.001$ & $ 0.142 \pm 0.009$ & $ 0.801 \pm 0.016$ & 
        $ 0.128 \pm 0.006$ & $-0.040 \pm 0.005$ \\
        S3D\_256\_Lz18 &
        $ 0.400 \pm 0.028$ & $ 0.314 \pm 0.013$ & $ 0.370 \pm 0.030$ & 
        $ 0.025 \pm 0.003$ & $ 0.208 \pm 0.011$ & $ 1.240 \pm 0.043$ & 
        $ 0.187 \pm 0.013$ & $-0.058 \pm 0.010$ \\
        S3D\_256\_Bz0.03 &
        $ 0.395 \pm 0.024$ & $ 0.292 \pm 0.013$ & $ 0.408 \pm 0.012$ & 
        $ 0.021 \pm 0.002$ & $ 0.216 \pm 0.011$ & $ 1.347 \pm 0.018$ & 
        $ 0.207 \pm 0.003$ & $-0.084 \pm 0.012$ \\
      \hline
   \multicolumn{9}{c}{$|z|>2 H$ (15\% of the mass)}\\
        Run & ${\rm rms}(u_x)$ &
              ${\rm rms}(u_y)$ &
              ${\rm rms}(u_z)$ &
              ${\rm mean}(u_x u_y)$ &
              ${\rm rms}(B_x)$ &
              ${\rm rms}(B_y)$ &
              ${\rm rms}(B_z)$ &
              ${\rm mean}(B_x B_y)$  \\
      \hline
        S3D\_256 &
        $ 1.108 \pm 0.084$ & $ 0.696 \pm 0.042$ & $ 0.635 \pm 0.016$ & 
        $ 0.059 \pm 0.066$ & $ 0.116 \pm 0.007$ & $ 0.486 \pm 0.015$ & 
        $ 0.100 \pm 0.005$ & $-0.016 \pm 0.004$ \\
        S3D\_512 &
        $ 1.072 \pm 0.086$ & $ 0.793 \pm 0.036$ & $ 0.665 \pm 0.035$ & 
        $ 0.096 \pm 0.026$ & $ 0.163 \pm 0.004$ & $ 0.547 \pm 0.016$ & 
        $ 0.138 \pm 0.006$ & $-0.025 \pm 0.004$ \\
        S3D\_256\_b3 &
        $ 1.159 \pm 0.125$ & $ 0.634 \pm 0.075$ & $ 0.597 \pm 0.067$ & 
        $ 0.022 \pm 0.065$ & $ 0.059 \pm 0.005$ & $ 0.194 \pm 0.010$ & 
        $ 0.044 \pm 0.003$ & $-0.004 \pm 0.001$ \\
        S3D\_256\_Lz18   &
        $ 1.439 \pm 0.092$ & $ 0.956 \pm 0.029$ & $ 0.897 \pm 0.077$ & 
        $ 0.130 \pm 0.054$ & $ 0.100 \pm 0.005$ & $ 0.390 \pm 0.017$ & 
        $ 0.085 \pm 0.006$ & $-0.012 \pm 0.002$ \\
        S3D\_256\_Bz0.03 &
        $ 1.403 \pm 0.101$ & $ 0.832 \pm 0.058$ & $ 0.735 \pm 0.033$ & 
        $ 0.192 \pm 0.099$ & $ 0.135 \pm 0.009$ & $ 0.448 \pm 0.027$ & 
        $ 0.107 \pm 0.006$ & $-0.016 \pm 0.004$ \\
      \hline
    \end{tabular}
  \medskip
  The two tables indicate the root-mean-square (and its temporal fluctuation
  interval) of the velocity field and the magnetic field, and the mean product
  of the radial and azimuthal components of velocity field and magnetic field.
  The top table shows the values within two scale heights of the midplane,
  while the bottom table shows the values measured above two scale heights.
  \end{table}