Compactification Formats of Ghost Anomalies

When a Gliossi-Sherk-Olive-based genus of ghost anomaly is formed, the directly corresponding set of point commutators that are harmonically redistributed -- in so as to form the associated traceable mapping of the just eluded to format of ghost anomaly -- in such a manner in so that the so-stated first-ordered point particles that work to form the said anomaly are brought relatively toward each other.  This forms a manner of compactification at the Poincaire level of each local cite in which the corresponding ghost anomalies are thus formed.  This genus of compactification forms a cite, in which the striking of relatively reverse-holomorphic norm-states upon the general locus of a ghost anomaly of such a format -- in what would here be an anharmonic Gliossi wave-tug/wave-pull upon the holonomic substrate that is here comprised of redistributed first-ordered point particles -- works to more readily be scattered by the eluded to Yakawa push of the here so-stated reverse-holomorphic norm-states upon the Poincaire region in which the mentioned ghost anomaly had originally occupied, in this given arbitrary genus of mappable tracing.  The thence caused anharmonic scattering of the initially stated ghost anomaly, that is here pulled apart at the indices at the Poincaire level, is here more likely to be spontaneous -- in the process of the just mentioned eliminiation of the eluded to condition of ghost-based indices, that here had initially comprised a condition of bearing a physical memory as to both the activity and the existence of the directoral Hamiltonian path-operand of a set of superstrings that operated -- in so as to perform a specific physical function.  The just eluded to anharmonic scattering thus acts in so as to form a decompactification of the directly corresponding first-ordered point particles that had existed as sets of norm-states.  Norm-States that work to comprise a ghost anomaly may either be a composition of zero-norm-states that were relatively forward-holomorphic, Campbell-norm-states that were relatively forward-holomorphic , Hausendorf-norm-states that were relatively forward-holomorphic , and/or Campbell-Hausendorf-norm-states that were relatively forward-holomorphic.  The initial harmonic scattering that works to form a set of ghost-based indices -- that work to form a ghost anomaly -- works to "steady-out" the initial kinematic motion of the directly corresponding eluded to set of norm-states, into a more static phenomena of holonomic substrate.  So, when a ghost anomaly is scattered by reverse-holomorphic norm-states, the ghost anomaly is spread outward, in a multivaried  basis of Lagrangian, that ends what was initially a ghost anomaly.  So, the initial physical condition of compacitfication that I had described works to allow for the multiplicit Clifford Expansion that happens when a ghost anomaly is struck by a reverse-holomorphic set of norm-states and/or norm-state projections.  Another wary of putting it is that the act of the formation of a ghost anomaly bears a dot-product Jacobian eigenbasis, that, when struck by a relatively reverse-holomorphic set of norm-states, works to form  a cross-product of Jacobian eigenbasis.  This works to allow for both the spontaneous and the perpetual existence of a continued tendency of Hamiltonian-based path operands -- so that both the physical memory of superstrings, as well as plenty of region for superstrings to be able to move, may be thus facilitated.  I will continue with the suspense later!
Sincerely, Samuel David Roach.