  The QCD (tri)critical point, a genuine second-order phase transition, implies
existence of a massless scalar mode, and singular behavior near it. In this
work we however focus on the finite region around it, defined by a condition
$m_\sigma=2m_\pi$. We point out that in this region the inter-hadron
interaction should be dramatically changed. Light sigma should increase
attractive mean field potentials for baryons and non-Goldstone mesons. The same
effect can be observed in additional downward shift of the mass of vector
mesons $\rho,\omega,\phi$, accessible via dilepton experiments. For pions we
predict that the mean change due to light sigma is in fact a
  $repulsive$ mean potential. The implications of these effects for collective
pion and nucleon flows, radial directed and elliptic, are estimated. Finally,
we speculate tha unusual behavior of flows observed by NA49 at 40 GeV PbPb
collisions at SPS may be explained by location of the critical point region
nearby.
