Certain Manners Of Norm-State-Projection Interactions

Let us consider a cohomological setting -- a set of ghost-based indices, that have here integrated into a certain pattern of a physical memory as to the where, how, and when certain superstrings of discrete energy permittivity have been interacting amongst each other -- over enough of a time period in so as to work at forming the so-eluded-to matrix of re-distributed point commutators.  Such a said cohomological-based setting will here be of a Reimman scattering of relatively forward-holomorphic norm-state-projections, that have harmonically been brought together in so as to form the so-stated physical memory as to the said where, how, and when the directly corresponding superstrings of discrete energy permittivity of such a case have interacted -- over a relatively transient period of time.  Such a Reimman scattering is of a harmonic-based nature -- each of the adjacent eigenmembers of the set of eigenstates that work to comprise such a cohomological setting work to bear an even chirality, when such a so-eluded-to symmetry is taken amongst the other eigenstates of the same overall structure of eigenmembers of such a ghost-based setting.  Let us now say that there is a relatively reverse-holomorphic set of norm-state-projections that work to strike the just mentioned cohomological setting that I have initially stated in this post.  Let us say that the interaction of the Laplacian-based initially mentioned cohomological-based setting with the Fourier-based set of what are here an egienset of a relatively reverse-holomorphic flow of norm-state-projectoins, is of a relatively small scalar magnitude of impact -- to where the initially stated Reimman structure of such an integration of ghost-based eigenindices is not moved enough, in so as to form an annharmonic scattering or Rayleigh scattering, right after it works to bear a Gliosis-based tangency with the second mentioned set of norm-state-projections of this case.  Such an interaction will then tend to form a repositioning or a readjustment of the initial Reimman-based delineation of ghost-based indices -- to where the initially stated cohomological setting will then work to bear an eigenbase of a secondary Ward-Caucy involed bounds, at which the eigenstructure of the overall initially mentioned cohomology will then bear a different set of angular momentum indices, until it is brought into another physical interaction with another set of substringular holonomic substrate -- over an ensuing Fourier-based kinematic interaction with other alterior substringular physical phenomena.  I will continue with the suspense later!  To Be Continued!  Sam.