Scattering of Gliossi-Sherk-Olive Ghosts

When either an f-field, a d-field, or a p-field, is formed -- in a tense of superconformal invariance -- the resulting Calabi-Yau manifolds will then here work to bear a cohomological-based index of a mappable tracing, of which may be thought of here as their respective Gliossi-Sherk-Olive ghosts.  The formation of such respective Gliossi-Sherk-Olive ghosts happens as a Reimman scattering, of which will here work to form an even eigenbase of a chirality of scattered eigenmembers -- as a state of what may be here rendered as a relatively harmonic scattering.  Yet, when one or more photons work to interact with the said respective Calabi-Yau manifolds, the resulting cohomological-based indices will be scattered, via a tense or a genus of a form of a Rayleigh scattering -- this so-stated Rayleigh scattering of which may be thought of as an annharmonic scattering.  The annharmonic scattering of any respective given arbitrary Gliossi-Sherk-Olive ghost-based pattern is formed by the result of an interaction of a directly affiliated ghost-inhibitor with the holonomic substrate of a cohomological-based setting -- this said ghost-inhibitor of which works to act as a group attractor, that works to bring-in relatively reverse-holomorphic norm-state-projections -- to where the initially formed physical memories that are thus formed by the projected trajectory of the here directly corresponding superstrings, that will have here initially moved in any of such respective given arbitrary loci of a respective tense of superconformal invariance, will then be annharmonically scattered out of the so-stated general tense of such a given arbitrary loci of static equilibrium -- in so as to scatter the directly corresponding physical memories of both the motion and the existence of the correlative superstrings.  This happens in such a manner in so that the reverse-chiral adjacent eigenmembers of the here former integrative cohomological indices, will then be brought out of the so-stated initial ghost-based structure -- in so as to these said indices then being brought off of the relative Real Reimmanian Plane, into the relatively Njenhuis Plane.  This so-stated relative Njenhuis Plane, in general, is where the relatively correlative gravitational particles, that work to form a subtension to the correlative superstrings of discrete energy permittivity -- via the activity of the correlative local Rarita Structure eigenstate(s), through the existence of the local Ricci Scalar, are present.  This general inter-relationship between Calabi-Yau manifolds and the Rarita Structure, via both gravitons and gravitinos -- due to the existence of the Ricci Scalar -- is the general format of what is to occur, so that gravity is then here able to act upon superstrings of discrete energy permittivity in a viable way, so that there may be a cohesion among discrete energy, so that energy and thus reality may bear at least some form of direct relationship -- so that there may be any sort of viable energy at all.
To Be Continued!  I will continue with the suspense later!!!  Sam Roach.