Different General Formats of Ghost-Based Scattering

When any given arbitrary cohomological setting is scattered from its initial Reimman-based configuration, into a relatively annharmonic dissaray -- this so-stated condition of dissaray, of which would here be due to the activity of a Rayleigh scattering of the here just eluded-to ghost-based configuration, in which this happens to where this said general genus of a scattering of ghost anomalies -- of which annharmonically work to scatter a set physical memories of both the existence and the activity of the projection of the trajectory of either a superstring, an orbifold, and/or an orbifold eigenset into a residue of norm-based projections, this will happen to where these will here then be moved into an ensuing stage of the recycling of ghost-based indices.  The previously mentioned helicit-based torque that is applied to the motion of any given respective arbitrary orbifold eigenset -- of which is caused by the re-positioning of the correlative gauge-bosons, in the manner of a directly corresponding re-delineation of the differential angling of the so-stated gauge bosons (E(6) X E(6) stings), will here tend to be a major factor in the reason as to the why and the how as to the bringing-in of relatively reverse-holomorphic norm-state-projections upon a relatively forward-holomorphic Reimman-based configuration -- to where a respective given arbitrary cohomological setting is then scattered by a Rayleigh-based scattering, which, in effect, will here then work to form a dissaray of the initial ghost-based scattering that I have been reffering to in this post.  If the re-distribution of the angling re-delineation of the differential geometry of the correlative respective gauge-bosons that would directly apply to this case, are pulled into the here just eluded-to perturbative-based re-delineation of the said E(6) X E(6) strings, as such said gauge-bosons are altered in the differential geometry of as to the genus of their Gliossi-based wave-tug/wave-pull that these imbue upon their respective given arbitrary second-ordered light-cone-gauge eignstates -- that these "pluck" during a state of a consecutively sequential series of group-related instantons, over time, in a relatively acutely-based  Ward-Caucy-involved manner, then, the scattering of the said cohomology will then here tend to be of a relatively conical-based kinematic differentially geometric manner, yet, if the re-distribution of the angling re-delineation of the differential geometry of the correlative respective gauge-bosons that wold directly apply to this case, are pulled into the here just eluded-to perturbative-based re-delineation of the said E(6) X E(6) strings, as such said gauge-bosons are altered in the differential geometry of as to the genus of their Gliossi-based wave-tug/wave-pull that these imbue upon their respective given arbitrary second-ordered light-cone-gauge eigenstates that these "pluck" during a state of a consecutively sequential series of group-related instantons, over time, in a relatively obtusely-based Ward-Caucy-involved manner, then, the scattering of the said cohomology will then here tend to be of a relatively toroidal-based kinematic differential geometric manner.