  Renormalization effects of large baryon-nonconserving Yukawa couplings
$\lambda^{\prime\prime}_{ijk} \overline{U_i} \overline{D_j} \overline{D_k}$
lower the right handed squark masses keeping the left-handed squark masses
virtually untouched at the lowest order. At low energy they enhance the
mass-splitting between left and right handed squarks of the same generation as
well as intergenerational mass splitting among squarks, potentially detectable
in future colliders or in rare decays. The predicted mass of the lightest stop
squark becomes lower than the experimental bound for larger ranges of parameter
space than that of the Baryon-conserving case, hence, further constraining the
parameter space of a supersymmetric theory when baryon violation is included.
