When the Fourier-Related-Progression, that is of the Lagrangian-based motion of a given arbitrary Hamiltonian Operator, that is to be initially propagated, via the workings of a hermitian Clifford Expansion, to where it is here to spontaneously bear an alteration (perturbation), into the ensuing Fourier-Related-Progression, of the Lagrangian-based motion of the respective Hamiltonian Operator, that is thence to consequently result in ending-up being propagated, via the workings of a hermitian Euclidean Expansion; It follows, that this general type of an inferred kinematic cohomology-related transformation, will often have some sort of a tendency, of being exhibited by the altered covariant field of such a stated Hamiltonian Operator, via the general mathematical workings, of the Greene Function. TO BE CONTINUED! SINCERELY, SAM.
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