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\begin{table}
\begin{tabular}{c} 
\centerline{mSUGRA : $m_h\lsim 124$ GeV, $\tan\beta \gsim 3.3$}\\ 
\end{tabular}
\begin{tabular}{|c|c|c|c|c|c|}\hline
Channel & TeV & LHC & LC & $\gamma$C & $\mu$C \\ \hline
$V^*\to Vh\to V b\bar{b}$    & $\pm$ 10\% & & $\pm$ 10\%  & & \\ \hline
$VV \to h \to b\bar{b}$ & & $\pm$ 10\% & & & \\ \hline
$V^*\to Vh\to Vc\bar{c}$ & & & 
$M_{1/2}\lsim 350$ : $\pm$ 20\% & &
\\ \hline
$V^*\to Vh\to VWW^* $ & & & $\begin{array}{c}
M_{1/2}\lsim 300 : \pm 20\%,\\ {\rm for}~ \tan\beta\lsim 30~{\rm or} \gsim 50
  \end{array}$& &
\\ \hline
$V^*\to Vh\to WW^* $ & &$\begin{array}{c}
M_{1/2}\lsim 300 : \pm 20\%,\\ {\rm for}~ \tan\beta\lsim 30~{\rm or} \gsim 50
  \end{array}$ & & & \\ \hline
$V^*\to Vh\to V\tau^+\tau^-$ & & & $\begin{array}{c}
M_{1/2}\lsim 300 : \pm 50\%,\\ {\rm for}~  \tan\beta\gsim 50 \end{array}$
& & \\ \hline
$VV\to h\to \tau^+\tau^-$  & & $\begin{array}{c}
M_{1/2}\lsim 300 : \pm 50\%,\\ {\rm for}~  \tan\beta\gsim 50 \end{array}$
& & & \\ \hline
$V^*\to Vh \to Vgg$ & & & $M_{1/2}\lsim 350$ : $\pm$ 20\% & & \\ \hline
$VV\to h \to gg$ & &  $M_{1/2}\lsim 350$ : $\pm$ 20\% & & & \\ \hline
$gg \to h\to \gamma\gamma$ & & $\begin{array}{c} M_{1/2}\lsim 300
 : \pm 20\%\\ \tan\beta\lsim 30 ~{\rm or} \gsim 50 \end{array}$ & & & \\ \hline
$t\bar{t}\to t\bar{t} h \to t\bar{t} b\bar{b} $ & & SM like & & & \\ \hline
$\gamma\gamma \to h\to b\bar{b}$ & & & &$M_{1/2}\lsim 300$ : +50\% & \\ \hline
$\gamma\gamma \to h\to WW^*$ & & & &$\begin{array}{c}M_{1/2}\lsim 350 :\\ -20\% \div +50\%\end{array}$  & 
\\ \hline
$\gamma\gamma \to h\to \tau^+\tau^-$ & & & & $\begin{array}{c} 
\tan\beta \sim 50 : \pm 50\% \\ \tan\beta < 50 : +50\% \\
{\rm for}~M_{1/2}\lsim 300 \end{array}$ & \\ \hline
$\gamma\gamma \to h\to \gamma\gamma$ & & & & 
$\begin{array}{c}M_{1/2}\lsim 350 :\\ -20\% \div +50\%\end{array}$ & \\ \hline
$\mu^+\mu^- \to h \to b\bar{b}$ &  & & & & $\begin{array}{c}
M_{1/2}\lsim 400, M_0\lsim 600
: +50\% \\ M_{1/2}\lsim 300, \tan\beta>50 : -50\% \end{array}$ \\ \hline
$\mu^+\mu^- \to h \to WW^*$ &  & & & & $\pm$ 10\% \\ \hline
$\mu^+\mu^- \to h \to \tau^+\tau^-$ &  & & & & $\begin{array}{c}
M_{1/2}\lsim 400, M_0\lsim 600
: +50\% \\ M_{1/2}\lsim 300, \tan\beta>50 : -50\% \end{array}$ \\ \hline
\end{tabular}
\end{table}


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