Initially consider each individually taken discrete quantum of energy, that works here in so as to comprise one respective given arbitrary orbifold eigenset, over a proscribed gauged-metric. Consider the directly corresponding cohomology that each of these said discrete quanta of energy are here to work to form, over the so-stated gauged-metric. Next, integrate all of the extrapolated cohomological phenomenology that is here to be formed by the correlative summed orbifold eigenset -- as this is here to be the sum of all of the individually taken cohomological eigenstates that are here in reference to the additive cohomological eigenstates of the composite discrete energy quanta, that are here to work to comprise the said orbifold eigenset -- over the so-eluded-to relatively transient duration of time. Next, consider the Lagrangian-based path that each of the composite discrete energy quanta are to go through, over the course of the said gauged-metric. Now, extrapolate the summed overall Lagrangian that the so-mentioned orbifold eigenset is to go through -- when one is here to consider that this said eigenset is to act as one metrical-gauge-based Hamiltonian operator -- since it acts here as a set of discrete quanta of energy that operate in so as to perform one specific given arbitrary function, over time. This resultant cohomological stratum may then be used to help at determining the delineation-related physical memory -- as to both the where, the how, and the when that a specific respective Ward-Cauchy-related Hamiltonian operator had interacted, amongst the norm-state-projections that it had come into a Gliosis-based contact with, as this discrete energy had been distributed and re-distributed as a piecewise continuous phenomenology, over time. This will then work to help one at understanding the activity of energy, as it is interacting with its immediate environment over time.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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