Two Different Propagating Convergent Covariant Inversely Isometric Hamiltonian Operators -- Dolbeault/De Rham Cohomology

 When two different propagating convergent covariant inversely isometric Hamiltonian Operators, of which are here to each work to bear a different rate of escalation-related spatial transference, as these inferred systems of energy are here to work to bear a Noether-Based projection of transversal/radial trajectory, over time, to where such inferred "teams" of converging energy, are here to also work to bear the general physical condition, in which these convergent "teams" of energy, are here to bear a relatively Nijenhuis nature, in regards to one another, in the projection of the directoral-based wave-tug of their correlative topological sway, of their kinematic coni-axial eigen metric, when taken over their directly associated Fourier-Related-Progression, that it may often tend to be the case, that as these two different cohesive sets of energy, when these are here to intersect, may often convert their inferred initial Dolbeault cohomology, that these had started out here to be expressing, into a spontaneously formed De Rham cohomology, over the course of an organized correlative spatial translation of cohomological deformation, as taken over the course of a correlative perturbation of gauge-metric-based permittivity. Sam Roach.