Saturday, December 26, 2015

Topological Sway Of Cohomologies

Let us first consider a given arbitrary Gliosis-Sherk-Olive ghost-based pattern -- a cohomological mappable tracing -- of what would here be a physical memory of an orbifold eigenset, that is undergoing a tense of conformal invariance at a general respective set locus -- over a relatively transient duration of time.  Let us say that the so-eluded-to set of superstrings of discrete energy permittivity, that have here operated in so as to perform one specific function -- have just been perturbated-out of the initially so-stated tense of conformal invariance -- to where the so-eluded-to tense of the respective given arbitrary Majorana-Weyl-Invariant-Mode had just been ended by an external force, that had readjusted the general relative locus of as to where the said orbifold eigenset is to be iterating at, in a Fourier-based manner.  Let us now say that the re-adjustment was of a direct correspondence to a reversal of the general holomorphic flow of the adjutant field -- that was Gliosis to the outer bounds of the Ward-Neumman field that is Yukawa to the core-field-density of the so-stated orbifold eigenset.  The said reversal in the general holomorphic flow of the Yukawa-based field of the said orbifold eigenset would then work to form an antiholomorphic Kahler condition.  Often, when there is a perturbation that happens to the Gliosis-based field of an orbifold eigenset -- that had just previously been in a state of conformal invariance,  to where the said perturbation is of the general manner of an antiholomorphic Kahler condition -- the Gliosis-Sherk-Olive cohomology that had been both formed and iterated at the general locus of the Majrorana-Weyl-based delineation, will be pulled out of its initially relatively stagnant tense of a Laplacian-based format, into what may be here described of as a topological "drifting" of the ghost-based pattern's ghost-based indices, to where the cohomology that had been formed at the so-eluded-to general locus of cohomological-based setting, will be pulled in a kinematic manner into the immediate surroundings of the initially said Majorana-based field that is proximal to the general locus of as to where the directly corresponding orbifold eigenset had worked to form its initially so-eluded-to physical memory.  This will tend to work at effecting the manner in which the correlative integration of ghost-based indices will be able to scatter in the resulting genus of its Rayleigh-based scattering -- given both the scalar magnitude of the Hodge-Index of its eigenmembers & the quantum characteristics of its antiderivative-based Hamiltonian fractals of discrete momentum, as the so-eluded-to cohomology is drifting amongst its relatively reverse-holomorphic adjutant norm-state-projections.  To Be Continued!  Sam Roach.

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