A dynamically broken hadron supersymmetry appears to exist as a consequence
of QCD. The reasons for the supersymmetry appear most transparently in the
framework of the constitute quark model with a diquark approximation to two
quarks.
SUSY appears for hadrons as a result of the diquark structure believed to
exist in nucleons which each Diquark being the superpatrner of an antiquark.
This symmetry is also seen in high density matter states where color flavor
locking occurs.
Normally this symmetry relates to the three lightest quark flavors which
have an approximate SU(3) symmetry (Broken by mass splitting) However, given
the two space charge structure of the Fitzpatrick model this symmetry can be
extended to all six quark flavors which might suggest a SUSY QCD Baryongenesis
process.