More About The Njenhuis Characteristics of Point Commutators

As to various given arbitrary point commutators that associate with each other, the different tenses of imagination that is associated with one set of point commutators relative to another -- in terms of two respective sets of point commutators that exist in two different respective universes -- works to allow these point commutators to be oriented in what tends to be an indirect manner, via both any arbitrary given Laplacian manner, as well as via any arbitrary given Fourier Transform that these may be associated with.  This is true in either a respective "snapshot" as to what is going on as well as any consideration of the mentioned point commutators over a transient period of time.  Such a covariant codifferentiation, when in terms of the respective tenses of imagination, being the basis as to why conformal repulsion localities exist in the manner that these exist in.  This works to help cause the general locus of the corresponding tori-sector-ranges that the said sets of point commutators belong to during a relatively limited number of covariant simultaneous instantons, via a Laplacian-based mapping through a centrally-based conipoint, to bear what I term of as an Imaginary Discrepancy.
Any free points -- known of as zero-norm-states -- whose conformal based dimension is zero -- work to allow these point commutators to terminate the what would here be a local tense of superconformal invariance.  This termination works to allow the said point commutators to always -- during the self-same set of group instantons that involve these, to bear condensed oscillation, as the zero-norm-states that these are here existant as -- during the said group metric -- bear inexact and non-linear differential associations both via a Laplacian setting during the individually related instantons as well as over the directly associated relatively very limited Fourier Transformtion that I have here been discussing.  The mentioned conformal repulsion locality recently mentioned works to flush the two mentioned sets of point commutators through different parallel universes aptly, once the said superconformal invariance is spontaneously ended in the mentioned case. This will happen more abruptly when regular magnetism is applied to these, whereas, if reverse magnetism is applied fairly directly to the two covariantly codifferentiable sets of respecitve point commutators that have been mentioned here, then, the general locus of the two sets of said point commutators that are here of two sets of universes will more likely remain in a tense of superconformal invariance for a longer time, and thus, will here tend to remain in their two respective different -- yet relatively close in the substringular -- universes.  The format of the applied magnetism, as well as how it is directed, works to effect the outcome of the delineation and also the re-delineation of the mentioned covariant codifferentiable sets of point commutators that have here worked to allow for the continuation of the static equilibrium of their most directly associated superstrings,these points of which  have here worked to allow superstrings to be continuous at moving through a certain given arbitrary sequential series of instantons.
I will continue with the suspense later!
Sincerely,
Samuel David Roach.