  A Bell inequality violation (BIQV) allowed by the two-mode squeezed state
(TMSS), whose Wigner function is nonnegative, is shown to hold only for
correlations among dynamical variables (DV) that cannot be interpreted via a
local hidden variable (LHV) theory. Explicit calculations and interpretation
are given for Bell's suggestion that the EPR (Einstein, Podolsky and Rosen)
state will not allow for BIQV in conjuction with its Wigner representative
state being nonnegative.
  It is argued that Bell's theorem disallowing the violation of Bell's
inequality within a local hidden-variable theory depends on the DV's having a
definite value --assigned by the LHV-- even when they cannot be simultaneously
measured. The analysis leads us to conclude that BIQV is to be associated with
endowing these definite values to the DV's and {\it not} with their locality
attributes.
