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\begin{table}
\begin{tabular}{|c|c|c|c|c|c|}
\hline 
Channel & Collider & $m_h$ & mSUGRA & mGMSB & mAMSB \\[2mm] \hline \hline
$V^*\to Vh\to V b\bar{b}$ & $\begin{array}{c}{\rm Tev}\\ {\rm LC}\end{array}$
 & $\begin{array}{c}\lsim 135 \\ \lsim 0.7\sqrt{s} \end{array}$ & $\pm$ 10\% & $\pm$ 10\% &
$M_A \lsim 300 : +50$\%
\\ \hline
$VV \to h \to b\bar{b}$ & LHC & $\lsim 120$ & $\pm$ 10\% & $\pm$ 10\% &
$M_A \lsim 300 : +50$\%
\\ \hline
$V^*\to Vh\to Vc\bar{c}$ & LC & $\lsim 0.7\sqrt{s}$ & $M_A \lsim 500 : \pm 20$\% &
$\begin{array}{c} M_A\lsim 200 : \lsim -50\% \\
200\lsim M_A\lsim 400 :  -50\%  \\
400\lsim M_A \lsim 600 : -20\%  \end{array}$ &
$\begin{array}{c}500\lsim M_A\lsim 650 : -20\% \\
300\lsim M_A \lsim 500 : -50\% \\
M_A\lsim 300 : \lsim -50\%\end{array}$ 
\\ \hline
$V^*\to (V)h\to (V)WW^* $ & (LC), LHC & ($\lsim 0.7\sqrt{s}$), $\gsim 110$ & $\begin{array}{c}
M_{A}\lsim 150 : \pm 20\%,\\ {\rm for}~ \tan\beta\lsim 30~{\rm or} \gsim 50
  \end{array}$& like $Vc\bar{c}$ & like $Vc\bar{c}$
\\ \hline
$\begin{array}{c}V^*\to Vh\to V\tau^+\tau^- \\
VV\to h\to \tau^+\tau^- \end{array}$ & $\begin{array}{c}{\rm LC}
\\ {\rm LHC}\end{array}$
 & $\begin{array}{c} \lsim 0.7\sqrt{s} \\ \lsim 150 \end{array}$ &$\begin{array}{c}
M_{A}\lsim 150 : \pm 50\%,\\ {\rm for}~  \tan\beta\gsim 50 \end{array}$ &
 $\tan\beta \gsim 50$ : $\gsim$ 50\% & $M_A\lsim 500$ : +50\%
\\ \hline
$V^*\to (V)h \to (V)gg$ & (LC), LHC & ? & $M_{A}\lsim 200$ : $\pm$ 20\% &
like $Vc\bar{c}$ &$\begin{array}{c}550\lsim M_A\lsim 650 : -20\% \\
250\lsim M_A \lsim 550 : -50\% \\
M_A\lsim 250 : \lsim -50\%\end{array}$
 \\ \hline
$gg \to h\to \gamma\gamma$ & LHC & $\lsim 150$
 & $\begin{array}{c} M_{A}\lsim 150
 : \pm 20\%\\ \tan\beta\lsim 30 ~{\rm or} \gsim 50 \end{array}$ & 
like $Vc\bar{c}$  &$\begin{array}{c} 550\lsim M_A \lsim 750 : -20\% \\ 
 250\lsim M_A \lsim 550 : -50\% \\  M_A\lsim 250 : \lsim -50\% \end{array}$
 \\ \hline
$t\bar{t}\to t\bar{t} h \to t\bar{t} b\bar{b} $ & LHC & $\lsim 130$ & SM like &
$\begin{array}{c}
{\rm SM~ like}\\+50\%~{\rm for} \tan\beta\gsim 50\end{array}$  &
$M_A\lsim 300$ : +50\%
 \\ \hline
$\gamma\gamma \to h\to b\bar{b}$ & $\gamma$C & ? & 
$M_{A}\lsim 150$ : +50\% & SM like & $M_A\lsim 300$ :  +50\%
\\ \hline
$\gamma\gamma \to h\to WW^*$ & $\gamma$C & ? 
&$\begin{array}{c}M_{A}\lsim 200 :\\ -20\% \div +50\%\end{array}$ &
$\begin{array}{c} M_A\lsim 200 : \lsim -50\% \\
200\lsim M_A\lsim 400 :  -50\%  \\
400\lsim M_A \lsim 600 : -20\%  \end{array}$ &$\begin{array}{c}500\lsim M_A\lsim 650 : -20\%
\\ 250\lsim M_A \lsim 500 : -50\% \\
M_A\lsim 250 : \lsim -50\%\end{array}$ 
\\ \hline
$\gamma\gamma \to h\to \tau^+\tau^-$ &$\gamma$C & ? & $\begin{array}{c} 
\tan\beta \sim 50 : \pm 50\% \\ \tan\beta < 50 : +50\% \\
{\rm for}~M_{A}\lsim 150 \end{array}$ & $\tan\beta \gsim 50$ : $\gsim$ 50\%   &
$M_A\lsim 600$ : +50\%
\\ \hline
$\gamma\gamma \to h\to \gamma\gamma$ &$\gamma$C  & ? & 
$\begin{array}{c}M_{A}\lsim 200 :\\ -20\% \div +50\%\end{array}$ &
 like $\gamma\gamma \to h\to WW^*$  &$\begin{array}{c}500\lsim M_A\lsim 650 : -20\% \\
250\lsim M_A \lsim 500 : -50\% \\
M_A\lsim 250 : \lsim -50\%\end{array}$
\\ \hline
$\mu^+\mu^- \to h \to b\bar{b}$ & $\mu$C  & up to $\sqrt{s}<2 m_W$ &  $\begin{array}{c}
M_{A}\lsim 250
: +50\% \\ M_{A}\lsim 150, \tan\beta>50 : -50\% \end{array}$ &
$\begin{array}{c}
200\lsim M_A\lsim 600 : +50\%\\
M_A\lsim 200 : \gsim 50\%\end{array}$ &$\begin{array}{c}
450\lsim M_A\lsim 900 : +50\% \\
M_A\lsim 450 : \gsim 50\%\end{array}$
\\ \hline
$\mu^+\mu^- \to h \to WW^*$ & $\mu$C & up to $\sqrt{s}<2 m_W$ &  $\pm$ 10\% &
$\tan\beta\simeq 50$ : +50\% & $M_A\lsim 600$ : +50\% 
\\ \hline
$\mu^+\mu^- \to h \to \tau^+\tau^-$ &$\mu$C  & up to $\sqrt{s}<2 m_W$
 &  $\begin{array}{c}
M_{A}\lsim 250
: +50\% \\ M_{A}\lsim 150, \tan\beta>50 : -50\% \end{array}$ 
& like $\mu^+\mu^- \to h \to b\bar{b}$ &
like $\mu^+\mu^- \to h \to b\bar{b}$  
\\ \hline
\end{tabular}
\end{table}





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