Volume-Based Cohormologies

Let us here initially consider the cohomological-based tracing of a bosonic superstring of discrete energy permittivity -- as it is differentiating in a Fourier-based manner, via a Majorana-Weyl-Invariant-Mode.  The directly corresponding three-dimensional field of the so-eluded-to two-dimensional superstring that is of this case, is to then work to form a ghost-based pattern that is patterned after a relatively toroidal-based manner.  This happens at a relatively set locus, to where this will then work to form a correlative cohomology, that will here tend to form a volume-based doughnut-like resultant of a Reimman-based scattering, as the so-eluded-to cohomological-based pattern that I have here so-stated, is being generated as a holonomic substrate of physical eigenindices.  These eigenindices, that will here work to form a  physical indication as to the where, the how, and when, that the so-eluded-to closed-loop discrete quantum of energy permittivity has been active at -- after the so-stated Reimman-based scattering of the correlative relatively forward-holomorphic norm-state-projections have succeeded to form the so-mentioned physical "memory" -- as to the Poincare-based nature of the directly prior Fourier-based activity, that is of the said bosonic superstring.  This would then happen, in so as to form a relatively tightly-knit harmonic integration of the here so-eluded-to eigenindices, that have here come together in so as to work to form the so-stated conglomeration of norm-state-projections -- that will then work to form adjacent eigenstates of such a physical memory, that work to bear an even chirality.  Once that the so-stated cohomological mappable tracing has been imbued upon, the given arbitrary respective proximal locus of the said tightly-knit substringular neighborhood -- at which such an indication as to those manners by which the so-stated two-dimensional superstring of discrete energy permittivity had differentiated, in a Fourier-based manner -- will happen, to where there will spontaneously be an ensuing relatively anharmonic scattering of the said given arbitrary integration of ghost-based indices -- to where such an anharmonic scattering may be viewed of as a general genus of a Rayleigh scattering, that will work to degenerate or scramble the initial tense and Laplacian-based structure of the previously mentioned Reimman scattering.  This will happen, to where the so-eluded-to adjacent disorganized eigenindices that are of a relatively odd chirality, -- will then be re-delineated to another substringular locus, in so as work to help in the general activity of the recycling of norm-state-indices, -- to where the initial so-eluded-to GSO ghost-based cohomological mappable tracing, will then tend to be reallocated to a locus that is off of the initially so-eluded-to relative Real Reimmanian Plane.  This happens, in so as to work to form dilatons and dilatinos -- that are indirectly put together, in so as to form gravitons and gravitinos.  The residue of these ghost-based indices, work to form a set of physical memories -- that may be termed of as Neilson-Kollosh-Ghosts, that, when anharmonically scattered, are re-delineated in so as to be brought back into the initially so-stated Real Reimmanian Plane -- in the form of a recyled tense of norm-state-projections, in so as to work to form a cycle that works, in the process of physical refurbishment in the substringular, over time.  I will continue with the suspense later!  To Be Continued!  Sam Roach.