Cohomologies Of Orbifolds

When any given arbitrary orbifold eigenset works at moving through space, over an ensuing sequential series of iterations of group-related instanton, the ghost-based cohomological mappable tracing of such a so-stated kinematic-based motion, will work to form a Laplacian-based physical memory as to the what, how, and when of the Fourier-based motion of the said respective given arbitrary orbifold eigenset.  Some time in the transient future from when an integration of ghost-based indices of a cohomological-based mappable tracing is formed -- by the interdependent interaction of norm-state-projections with the kinematic motion of the directly corresponding superstrings of discrete energy permittivity, there will inevitably be certain various relatively reverse-holomorphic-moving norm-state-projections -- that will take what was the initial Reimman structure of the initially said cohomological-based mappable tracing, that worked to form the initial so-eluded-to harmonic-based scattering of the correlative relatively forward-holomorphic norm-state-projections that worked to form here the initially so-eluded-to cohomological-based mappable tracing -- and scatter it in an annharmonic manner, via a correlative Rayleigh-based scattering, to where the said initial integration of ghost-based indices will then break down into certain various phenomenology, that will then ensue to veer off of the relative Real Reimmanian plane, into its composite substringular phenomena, that will then come together in so as to act as discrete gravitational-based phenomenology, over time.  So, when any respective given arbitrary set of ghost-based indices -- that are formed as the physical memory of the motion of one whole discrete orbifold eigenset, is annharmonically scattered in a tense of a Rayleigh scattering -- the tendency is that the whole cohomological-based structure of the so-eludedt-to initial Reimman-based cohomological structure -- will be broken down into its component substringular discrete parts, at what would be for all intensive purposes, over basically the exact same general gauge-metric or "time."
I will continue withe the suspense later!  To Be Continued!  Sincerely, Sam Roach.