  The newly found \cite{CDFnew} dijet peak in the 120 GeV to 160 GeV mass
region produced in co-production with W IS actually a Higgs Boson in spite of
the expectation of a different decay pattern for most Higgses. Our point,
however, is that the bound state of 6t + 6$\bar{t}$, which we have put forward
already in several articles \cite{boundfirst}\cite{bound}
\cite{dark}\cite{hierarchybound}, easily could be lighter - possibly much
lighter - than half the Higgs mass. Higgs would in this case decay dominantly
to two of our bound states. If these bound states were indeed very light (say
around 10 GeV) their decay products into hadrons would like two jets, one for
each bound state. Even a very small mass for our bound state is not unexpected
isofar as it is part of our model that especially the top-quark-Yukawa coupling
is being tuned so as to make precisely this bound state of $6t + 6\bar{t}$
become (approximately) massless. This tuning is a consequence of our Multiple
Point Principle \cite{old} \cite{SIMPP} which states that the realized
parameter/coupling values correspond to having a maximal set of degenerate
vacua. Even the very recent LHC-peak in photon photon might be fitted to our
model.
