A Little Heads Up To Courses 16 and 26, Part One

Let us say that a superstring is to move thru a path in such a manner in so that it changes in four derivatives, in which that said superstring performs such a change 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 elongated in a Fourier-based pulse of metric at the same locus that the said superstring is here said to undergo the said change in four derivatives -- this said elongation of kinematically-based operation of pulse of which is conimetrically and coniaxial-based formatted at the conicenter of the just mentioned spot, to where the Ward-Caucy-based tensoric concavity that here alters in its topological curvature is here temporarily jerked out of what started as a harmonically flowing superstring that then becomes temporarily anharmonic -- at the said relatively discrete said locus of perturbation that is arbitrarily given as such in this case.  The genus of Chern-Simmons-based singularity could then be described by infinity times infinity, or, in other words, by infinity squared.  If, at a position of the trajectory of the Lagrangian-based path of the said superstring that tis further down the path of the said superstring that is further down the Fourier-based mapping of the projection of that stated superstring -- at an ensuing metrically bracketed time locus, the said superstring changes in three derivatives while it simultaneously, thru the mentioined conipoint's vantage point, jerks at this locus in an anharmonically-metrical manner in such a way that the 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 that moves as a two-dimensional field that moves thru a unitary exterialized Lagrangian, then, the genus of its Chern-Simmons singularity format may be described of as being discrete relative to 1/infinity, or, in other words, the directly related singularity here would equal 0+.  The curvature of the said one-dimensional superstring here would be hermitian when in terms of the overall Laplacian-based mapping of the trajectory of its path -- as may be denoted by the extrapolation of the field import of its Gliossi-Shirk-Olive ghost-based field indices, these indices of which here are comprised of as positive-norm-state indices that work to trace the said mapping of the mentioned path as a timeless-oriented differentiation.  I will continue with conveying the basis of this concept later!  Sincerely, Samuel David Roach.