Holographic Relations To Construction of Space-Time Fabric

Let us say that a superstring is to move through a path in such a manner in so that it changes in four derivatives in a three-dimensional-based Minkowski plane, in such a manner that it jerks -- kinematically -- in what was initially a harmonic rhythm that is made anharmonically ellongated in a time-interdependant-based pulse of metric at the same general locus that the said superstring undergoes the said change in four derivatives -- this ellongation of kinematically-based pulse of which is conimetrically and coniaxial-based in format, at the relative conicenter of the just mentioned spot where the Ward-Caucy-based tensoric concavity is temporarily jerked out of what started out as a harmonically flowing superstring.  This happens in such a manner that the eluded to motion of the said superstring here becomes temporarily anharmonic at the said relatively discrete general said locus of the given eluded to perturbation.  The genus of Chern-Simmons-based singularity would here then be described by infinity times infinity, or, in other words, infinity squared.  (The directly associated singularity at the said locus of perturbation over the eluded to eigenmetric of the directly associated activity would be of a higher genus of singularity than may be described of as just infinity.  This is because one here has a singularity of a Lagrangian-based perturbation that is coupled by a singularity of a spurious-based perturbation.)  If, at a position of the trajectory of the Lagrangian-based path of the said superstring, that is, in this case, further down the time-interdependant-based mapping of the projection of that stated superstring -- at an ensuing metrically bracketed time eigenlocus of metrical delineation -- the said superstring will then here change in three derivatives.  This is while the motion of the said given arbitrary superstring jerks at this locus in an anharmonically-metrical-based manner.  This happens in such a manner in so that the thus formed pulse of the just mentioned superstring is sped-up at the conicenter of the coniaxial at where the said superstring was at, when it here changed in three derivatives as a plane of a one-dimensional superstring of holonomic substrate -- that is moving through a multiplicit spatial range over time.  The just mentioned one-dimensional superstring will then move as an entity in a manner that exhibits a directly corresponding two-dimensional field that bears a Lagrangian that is multiplicit in directoral covariance over time.  I will continue with the suspense later!  To Be Continued.  Sincerely, Sam Roach.