As To The Nature of the Scattering of Ghost Anomalies

When certain given arbitrary relatively reverse-holomorphic norm-based projections act in so as to strike certain loci of cohomological-based-indices, or ghost anomalies, in a Gliossi manner -- in so that the part of the said relative reverse-holomorphic norm-projections that tend to act in so as to hit the here respective ghost-based indices -- that have been eluded-to here, are the subtended mini-stringular segmentation that  would exist here in-between the respective first-ordered point particles, that work to comprise those relatively forward-holomorphic norm-state projections -- these latter mentioned projections of which to make-up the holonomic substrate of the so-stated ghost anomalies or cohomological-based indices.  When that part of the entity of a static-based norm-state-projection -- that works to form the composition of a ghost anomaly -- that is hit by a relatively reverse-holomorphic norm-state-projection, is struck both by mini-stringular segmentation, and, at a certain general locus of its own holonomic substrate of mini-stringualr segmentation, then, the entity of the cohomological-based index -- in the form of that norm-state-projection that is here hit by a relatively reverse-holomorphic norm-state-projection -- will be torsioned in such a manner, in so that it will tend to slide in at least one tense of either a norm-to-forward-holomorphic direction or in a norm-to-reverse-holomorphic direction, away from the directoral-based Hamiltonian flow of the incoming so-stated relatively reverse-holomorphic norm-state-projection, that had here struck at the general field of a here relatively forward-holomorphic norm-state projection -- this of which had initially worked to form an index of a ghost-based cohomological structure. If, instead, the holonomic substrate of the first-ordered point particle eigenbase of one relatively reverse-holomorphic norm-state-projection -- that functions to form a Rayleigh scattering of a ghost anomaly -- works to strike the holonomic substrate of the first-ordered point particle eigenbase of one relatively forward-holomorphic norm-state-projection, that had functioned in so as to form a Reimman scattering that had initially formed the here eluded-to ghost anomaly -- the scalar amplitude of the Hamiltonian-based multiplets that would thence be formed will then tend to be higher, than if, instead, the holonomic substrate of the respective mini-stringular segmentation were to be what had collided, in this case. The Hodge-Index that is related to the density of the mini-stringular structure -- in the form of how many of certain cross-sections of mini-string segmentation per general locus are being struck, by how many of certain respective cross-sections of mini-string segmentation, per general locus, in the opposite general direction, is the general idea as to how to work to determine the resultant effect of the collision of one cohomological index by one ghost-based inhibitor.  This is based upon the condition that first-ordered point particles are formed by a balling together of mini-stringular segmentation. To Be Continued!!! Sam Roach.