Some More As To Tenses of Singularities

Let us say that one had a substringular scenario in which a set of superstrings moved through a unitary Lagrangian, to where the genus of the directly corresponding Chern-Simmons singularity that would here appertain to the said scenario would bear a format that could be described of as being discrete relative to (1/infinity), or, in other words, the directly related singularity here would be equal to "0+".  The curvature of the said trajectoral path of the eluded to orbifold, or, set of superstrings -- that operate to perform a specific substringular function -- would then not be completely hermitian, when in terms of the overall Laplacian-based mapping of the projection of its path.  Such an attribute of a Chern-Simmons genus may be denoted by the extrapolation of the corresponding field network that could be traced by the corelative Gliossi-Sherk-Olive indices -- the said indices of which would here be physically comprised by discrete units of ghost anomaly-based residue that are left as a physical memory of the directly previous substringular motion and existence of the orbifold that is here under question.  The eluded to ghost-based indices here of which are comprised of harmonically scattered positive-norm-states, if the given arbitrary orbifold that is being considered here is moving in forward-moving time. These just eluded to indices here work to trace the said mapping as a timeless oriented differentiaion that works to show a prior-based time-oriented kinematic displacement of discrete units of energy delineation.  Yet, the said perturbation of time-oriented substringular pulse -- the scattering of ghost anomalies -- that is here the anharmonic scattering of the eluded to ghost anomalies, as a relatively transient acceleration of the oscillation of relatively reverse-holomorphic norm-states upon relatively forward-holomorphic norm-states, happens at a singularized locus at a metrical gauge that here works to produce a change in an additive derivative of the given arbitrary projection of the directly corresponding orbifold.  Such an alteration of the physical projection of the said orbifold works to form an integrative singularity that would here bear a Chern-Simmons singularity that bears -- in and of itself -- a kinematic locus as to where the limit of the mapped-out tracing of the said orbifold is not discrete, when going from one side of the eluded to locus of singularity to the other side of the eluded to locus of singularity.  This would make this latter example of a path of an orbifold, over time, to be able to be described of as a partially Chern-Simmons field trajectory.  This is because, although the orbifold would here change in more Ward-Caucy-based derivatives than the dimensionality of its trajectory, the said orbifold is at least not spurious in terms of the pulsation of its vibratorial oscillation over time here.  Any field trajectory that bears any genus of Chern-Simmons singularity-founded-basis -- whether such a genus of perturbation were to bear a whole basis of singularity that is not discrete OR even if there is a partial condition of a singularity that is not discrete, even though such a singularity may be offset by a countering bases that works to unitize the Jacobian eigencondition, then, the otherwise considered Chern-Simmons genus is here considered to be a given arbitrary example of a Cevita interaction.  I will continue with the suspense later.
Wess Zumino and Cevita Interactions will be discussed further in course 26!  Sam Roach.