A Hamiltonian Operator, of which is to initially be expressing a De Rham cohomology, that is here to be traveling through an anti gravitational field, to where the earlier stated Hamiltonian Operator, is subsequently to be altered, into spontaneously entering the ensuing proximal local presence of a heuristic gravitational field, will often change here, into then working to express a Dolbeault cohomology. SAM. (1989).
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