  Triplet-mediated proton decay in Grand Unified Theories (GUTs) is usually
suppressed by arranging a large triplet mass. Here we explore instead a
mechanism for suppressing the couplings of the triplets to the first and second
generations compared to the Yukawa couplings, so that the triplets' mass can be
below the GUT scale. This mechanism is based on a ``triplet symmetry'' in the
context of product-group GUTs. We study two possibilities. One, which requires
the top Yukawa to arise from a non-renormalizable operator at the GUT scale, is
that all triplet couplings to matter are negligible, so that the triplets can
be at the weak scale. The second is that some triplet couplings, and in
particular $T t b$ and $T \bar{t} \bar{l}$, are equal to the corresponding
Yukawa couplings. This would give a distinct signature of grand unification if
the triplets were sufficiently light. However, we derive a model-independent
bound on the triplet mass in this case, which is at least 10$^6$GeV. Finally,
we construct a GUT model based on Yukawa splitting, with the triplets at
10$^{14}$GeV, as required for coupling unification to work.
