Part Three Of Session 12 Of Course 19 -- The Klein Bottle And Orbifold Differentiation

The condition that any mini-stringular Laplacian-based networking -- of what may be termed of as the mappable tracing of zero-norm-state-projections, often works to form a general condition of a Njenhuis state of substringular tension -- that is to be delineated here among the holonomic substrate of that mini-stringular segmentation, by which the Fourier-based activity of the so-stated Njenhuis tensors are to here be interactive upon certain other respective given arbitrary indices of the field-density of that homotopic residue, -- that is to here be external to the core-field-density of certain given arbitrary superstrings of discrete energy permittivity, that are to here be of a Yukawa-based nature, in a covariant manner, to the general tense of the interdependent Ward-Caucy-based conditions of the so-stated holonomic substrate of the extostential field divergence, that is of the said given arbitrary state of the so-stated zero-norm-projections of such a respective case, -- may often work upon the holonomic substrate of the directly corresponding superstrings of discrete energy permittivity that I have eluded--to in this said general codeterminable and codifferentiable sub-Fourier-based Ward-Caucy state, of what is to here be one relatively transient kinematic inter-relation of mini-stringular segementation with discrete energy, to come into the spontaneous need for the implementation of the interaction of the proximal local holonomic substrate of a respective given Higgs Boson to be brought into the so-eluded-to local substringular neighborhood, in so as to bring the Gliosis-based implementation of the Kahler-Metric upon the core-field-density of those substringular eigenmembers of which are to here be brought into what is here to be the Gliosis-based interaction of the directly associated quanta of discrete energy with the proximal localized Klein Bottle eigenstate, that is to here be brought into the said local substringular arena, in so as to bring into play those superstringular changes that are needed -- in order for there to be both the continuation and the perpetual interaction of certain discrete energy quanta among other discrete energy quanta, -- in order for energy to both persist and exist.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.