Remember back at the condition that I have mentioned in the past -- that the projection of the trajectory of a substringular phenomenology is a world-sheet. The mappable-tracing of a world-sheet is a cohomology. That manner of considering a cohomology -- to where this may be viewed of as a relatively transient phenomenology, that is generally not to be apprehended -- is a ghost anomaly. Cohomologies are initially harmonically scattered into place, via a correlative Reimmanian scattering, into a set of norm-state-projections -- that work in so as to help at indicating the physical memory of both the where, the how, and the when, that any particular given arbitrary respective substringular phenomenon had physically differentiated -- over any correlative proscribed sequential series of instantons. The initiation of such a general genus of Reimmanian-based scattering, works to form a harmonic perturbation of those norm-state-projections, that had just been in the Lagrangian-based path of that Ward-Cauchy-related phenomenology, that is here to be forming an integrable set of cohomological eigenindices, as a set of Hamiltonian operand-related eigenstates, -- in so as to work to form a Wess-Zumino distortion of those point commutators that had eminently been in the path of the said substringular phenomenology, that had just formed the said cohomology. Such a general genus of a Wess-Zumino distortion, is here to be formed by a set of relatively forward-holomorphic tending norm-state-projections -- that are here to have come into contact with that Ward-Cauchy-based phenomenology, that is here to form the so-eluded-to set of the so-stated physical memories. I will get to the topic, as to the conditions that are related to those Cevita distortions of point particle-related motion -- soon.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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