Part Two of Chern-Simons Singularities And Ghost-Inhibitors

Let us say that one is to have an orbifold eigenset -- that is to initially be moving in what may here be thought of as the relative forward-holomorphic direction.  Let us next say that one is to here be observing the said orbifold eigenset -- as a topological substrate, that is to here be in the process of being translated as a metrical-gauge-based Hamiltonian operator, that is to here be propagated via a unitary Fourier Trasformation of a relatively cohesive set of eigenindices, that will work to help form the kinematic activity of being propagated through an elementary mean Lagrangian path -- that is of a relatively "straight" directoral-based wave-tug -- as the resultant cohomological-based mappable-tracing, is to here be propagated as a tense of the here resultant generation of a set of harmonically scattered Reimman spaces.  Let us then consider that the resultant general cohomological eigenbase, that is to here be thus formed by the physical memory of the projection of the trajectory of the so-stated kinematic-based activity that is of the so-stated orbifold eigenset, is to be of a Rham-associated nature -- since the homotopic-based torsional eigenindices, that are to here be formed by the propagation of the said orbifold eigenset through space-time-fabric, that is proximal localized at the Yukawa-based range-related cite of the functioning of the eluded-to Hamiltonian operation -- are to here bend in as many changes in derivatives as the number of spatial dimensions that the so-eluded-to set of superstrings that are to here be operating in so as to perform one specific function, are to be translated through.  All of the sudden, there is to here be a Lagrangian-based Chern-Simons singularity, that is to be formed by the initial general Fourier-related activity of the said orbifold eigenset, that was initially working to form a Rham cohomology, is to act in a directoral-based flow, that is to be propagated in so as to form a Rayleigh scattering of the cohomological eigenbase that is of the ghost-based pattern of the initially said Rham cohomology.  This will often be the result of a relatively forward-holomorphic-directed ghost-based inhibitor. This will then tend to cause a spontaneous turn of the Lagrangian-based pattern, that is of the said orbifold eigenset -- to the relative Njenhuis-to-reverse-holomorphic direction.  I will continue with the suspense later! To Be Continued!  Samuel David Roach.