The phase space of a particle or a mechanical system contains an intrinsic symplectic
structure, and hence, it is a symplectic manifold. Recently, new invariants
for symplectic manifolds in terms of cohomologies of differential forms have
been introduced by Tseng and Yau. Here, we discuss the physical motivation behind
the new symplectic invariants and analyze these invariants for phase space,
i.e., the non-compact cotangent bundle.