\begin{table}%t5
\caption{\label{tab:Kxx_diff_cases}$K(E)$ and $K_{\rm pp}$ for different schemes.}
%\centering
\par
\begin{tabular}{llcc} \hline\hline\noalign{\smallskip} 
\multicolumn{2}{l}{Type of turbulence}&    $\eta_{\rm T}$    &   $\frac{K_{\rm pp} K_{\rm xx}}{4/3~ p^2V_{\rm a}^2}$ \vspace{0.10cm}   \\\hline
& \multicolumn{1}{c}{} \vspace{-0.20cm} \\
LBI&Leaky Box Inspired                &       0        &  $\frac{1}{\delta~(4-\delta^2)~(4-\delta)}$  \vspace{0.15cm} \\
{\it SA}&{\it Slab Alfv\'en}          &     {\it 1}    &  $\frac{1}{\delta~(4-\delta^2)~(4-\delta)}$  \vspace{0.15cm} \\ 
IFM&Isotropic fast magnetosonic       &  ${2-\delta}$  &  $\beta^{1-\delta} \ln (\frac{v}{V_{\rm a}})$   \vspace{0.15cm} \\
Mix& Mixture SA and IFM               &  ${1-\delta}$  &  $\beta^{1-\delta} \ln (\frac{v}{V_{\rm a}})$  \vspace{0.1cm} \\
\hline
\end{tabular}
\tablefoot{The spatial diffusion coefficient is $K_{\rm xx}= \beta^{\eta_{\rm T}} \cdot K_0 \cdot {\cal R}^\delta$.\vspace{-0.25cm}}
\end{table}