  We argue that the $125 GeV$ "Higgs" particle is unlikely to arise as a
fermion- antifermion composite if the underlying dynamics is a vectorial gauge
theory. The reason is that the lightest scalar in such theories is heavier than
the lightest pseudo-scalar with the mass difference being fixed by the scale of
the theory. LHC searches suggest that the scale of any new physics, including
that of a putative new theory dynamically generating the 125 GeV "Higgs"
particle, is relatively high $\sim{(1/2TeV-1TeV)}$. Also the LHC analysis
suggests that it is {\it scalar} namely $J^P = 0^+$ rather than pseudo-scalar.
Thus it is unlikely that the "Higgs" could arise as a composite in such
theories- though it will arise in special cases when the underlying binding
gauge group is real as a fermion-fermion bound state.
  The direct considerations of the various two point functions in the large
$N_c$ limit presented below- suggest that massless pseudo-scalars, but not any
other anomalously light meson, arise as composites of massless fermions say the
massless u and $\bar{d}$ quarks in QCD. These massless pions manifest the
spontaneous breaking of the global axial symmetry in QCD with the pions being
(pseudo) Nambu Goldstone Bosons. This offers a different insight into SXSB in
QCD and most other confining non-abelian gauge vectorial gauge theory.
Specifically we consider the euclidean two point functions $F_I|x-y|$ for
asymptotic $|x-y|$ expressed as a sum over fermionic paths. We conjecture that
for the pseudo-scalar two point function - and for that case only- self
retracing paths and closely related paths make in this limit a positive,
coherent and dominant contribution, a contribution which evades the generic
asymptotic exponential fall-off and allows the lightest pseudoscalars to be
massless. The same arguments imply that the scalars are very massive.
