

\CTran{  Minimal SuperSymmetric Standard Model }

\vspace*{1cm}



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\centerline{
{{$
%\begin{eqnarray}
\begin{array}{|c|c|c|}\hline
 {\rm Superfields} & SU(3)_C\times SU(2)_L\times U(1)_Y &
 {\rm Components} \\ \hline \hline 
Q_r^{i,\alpha} & ({\bf 3},{\bf 2},\frac{1}{6}) & \left (\begin{array}{c}
\tilde{u} \\ \tilde{d} \end{array} \right )_L \;,\; \left (\begin{array}{c}
u \\ d \end{array} \right )_L \\[4mm] 
D^c_{r,\alpha} & (\bar{\bf 3},{\bf 1},\frac{1}{3}) & \tilde{d}^c \;,\; d^c
\\[4mm] 
U^c_{r,\alpha} & (\bar{\bf 3},{\bf 1},-\frac{2}{3}) & \tilde{u}^c \;,\; u^c
\\[4mm] 
L_r^i & ({\bf 1},{\bf 2},-\frac{1}{2}) & \left (\begin{array}{c}
\tilde{\nu}_e \\ \tilde{e} \end{array} \right )_L \;,\;
\left (\begin{array}{c} \nu_e \\ e \end{array} \right )_L \\[4mm]   
E^c_r & ({\bf 1},{\bf 1},1) & \tilde{e}^c \;,\; e^c \\[4mm] 
H_1^i & ({\bf 1},{\bf 2},-\frac{1}{2}) & \left (\begin{array}{c}
\tilde{H}_1^0 \\[1mm]\tilde{H}_1^- \end{array} \right ) \;,\;
\left (\begin{array}{c} H_1^0 \\[1mm]H_1^- \end{array} \right ) \\[4mm]
H_2^i & ({\bf 1},{\bf 2},\frac{1}{2}) & \left (\begin{array}{c}
\tilde{H}_2^+ \\[1mm]\tilde{H}_2^0 \end{array} \right ) \;,\;
\left (\begin{array}{c} H_2^+ \\[1mm]
 H_2^0 \end{array} \right ) \\[5mm]
\hline
\end{array}
%\nonumber
%\end{eqnarray}
$}}}
%\end{left}
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\vspace*{1cm}

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\centerline{
{{$
\begin{array}{|c|c|c|}\hline
{\rm Superfields} & SU(3)_C\times SU(2)_L\times U(1)_Y &
{\rm Components}\\ \hline \hline
V_3^{(R)} & ({\bf 8},{\bf 1},0) & \tilde{G}^{(R)} \;,\; G_\mu^{(R)} \\[3mm]
V_2^{(\Gamma)} & ({\bf 1},{\bf 3},0) & \tilde{W}^{(\Gamma)} \;,\;
W^{(\Gamma)}_\mu \\[3mm]
V_1 & ({\bf 1},{\bf 1},0) & \tilde{B} \;,\; B_\mu \\
\hline
\end{array}
$}}}
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