
\CTran{ Supersymmetry }

\vspace*{1cm}

\Green{$\bullet$}
\Blue{\Red{Supersymmetry} is a symmetry which relates particles of different 
spins. It has a virtue of allowing non trivial interactions
between fermions and bosons.}

\vspace*{1cm}

\Green{$\bullet$}
\Blue {It is possible for the quadratic divergences to cancel between
the bosonic and fermionic loops. To insure that this cancellation
persists to all orders we need \Red{Supersymmetry}.}

\vspace*{1cm}


\centerline{\psfig{figure=higgs2.eps,height=1in}}
\centerline{\Green{---}}
\vspace*{0.5cm}
\centerline{\psfig{figure=higgs1.eps,height=1in}}

\Green{$\bullet$}
\Blue {\Red{Supersymmetry} is certainly not a symmetry in nature: for
example, there is certainly no bosonic particle with the mass and charge
of the electron. {\Red{Supersymmetry} } {\it must} be broken at a scale
of the electroweak symmetry breaking in order to keep in touch with the
solution of the hierarchy problem.}