Net Harmonic Schwinger-Related Vibration

 When two acutely approaching anharmonic Schwinger-Related vibrations are to converge, in which both of the initially considered respective anharmonic vibrations, are to be asymmetrically covariant, when in terms of their proximal local dispersive oscillation-based modes, there may, at times, be the consequential case scenario, in which the resultant net Schwinger-Related vibration, that is thus formed, may work to bear an eminent harmonic tense of the Fourier-Related-Progression, of a consequentially propagated oscillating wave, that is here to be transferred tangentially, along the Rarita Structure. SAM ROACH.

More About Cotangential Flow

The general cotangential flow of mini-stringular segmentation, that is here to converge upon those first-order point particles that work to comprise superstrings, during the Polyakov Action -- tends to work to bear a higher scalar amplitude of a hyperbolic approach, -- than the general cotangential flow of such mini-stringular segmentation, that is here to converge upon these same first-order point particles -- during the course of the rest of the process of BRST.  To Be Continued!  Samuel Roach.

Cotangential Flow Of Mini-Stringular Segmentation Towards First-Order Point Particles, Part Two

That general cotangential flow of mini-stringular segmenation, that works to converge upon those first-order point particles, that work to form the myriad Ward-Cauchy-related physical entities that act as norm-state-projections, tends to be of more of a euclidean nature, -- than that general cotangential flow of mini-stringular segmentation, that works to converge upon those first-order point particles, that work to form superstrings.  To Be Continued!  Sincerely, Samuel David Roach.

Cotangential Flow Towards First-Order Point Particles

That general cotangential flow of mini-stringular segmentation, that works to converge upon those first-order point particles, that work to form superstrings -- tends to be of more of a hyperbolic nature, than that general cotangential flow of mini-stringular segmentation, that works to converge upon those first-order point particles, that work to form the myriad Ward-Cauchy-related physical entities, that act as norm-state-projections. I will continue with the suspense later!  To Be Continued!  Samuel Roach.

Scattering And Cotangent Bundle

When Ward-Cauchy-related phenomenology are to scatter -- in so as to work to converge upon a substringular cotangent bundle of some given arbitrary spatial dimensionality, -- then, this is one general genus of a Reimman Scattering; Whereas, -- when Ward-Cauchy-related phenomenology are to scatter -- in so as to work to diverge from a substringular cotangent bundle of some given arbitrary spatial dimensionality, -- then, this is one general genus of a Rayleigh Scattering.  Samuel Roach.

Some Additional Stuff As To Manifolds

A smooth substringular manifold tends to be formed, when a Wess-Zumino-related gauged-action is here to converge upon the proximal locus of an orbifold eigenset, -- whereas -- a substringular manifold that is not smooth tends to be formed, when a Cevita-related gauged-action is here to converge upon the proximal locus of an orbifold eigenset.  To Be Continued!  Sincerely, Samuel David Roach.

Majorana-Weyl-Invariant-Mode And Homotopic Residue

The higher that the tense is of the correlative condition, that is appertaining to a Majorana-Weyl-Invariant-Mode -- that an individually taken superstring of discrete energy permittivity is to be of -- the more that homotopic residue is to then to tend to Converge Upon the proximal locus of the just mentioned superstring of discrete energy permittivity -- at a reference-frame that is Poincare to the topological stratum of the said individually taken string.  Consequently, the lower that the tense is of the correlative condition, that is appertaining to a Majorana-Weyl-Invariant-Mode -- that an individually taken superstring of discrete energy permittivity is to be of -- the more that homotopic residue is to then to tend to Diverge From the proximal locus of the just mentioned superstring of discrete energy permittivity -- at a reference-frame that is Poincare to the topological stratum of the said individually taken string.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Homotopic Residue And Rates Of Speed

Let us initially consider one given arbitrary orbifold eigenset.  The Slower that the said orbifold eigenset is to travel in one given direction -- the more that homotopic residue is to tend to Converge upon those individually taken superstrings, that work to comprise the said orbifold eigenset.  Consequently, the Faster that the said respective orbifold eigenet is to travel in that same one given direction -- the more that homotopic residue is to Diverge from those individually taken superstrings, that work to comprise the said orbifold eigenset.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

First Discussion As to Flow Of Partition-Related Discrepancies

The higher that the Beti number is, during a dimensional compactification, of which is to here to happen right before any one given arbitrary iteration of BRST -- the more partition-related discrepancies will tend to flow out of or diverge from a correlative superstring just before the said iteration of BRST.  Furthermore, -- the higher that the absolute value of the Beti number is, during a dimensional decompactification, which is here to happen during any one iteration of the Regge Action -- the more partition-related discrepancies will tend to flow into or converge upon a correlative superstring, during the so-stated iteration of the Regge Action.  Compactification of dimensions tends to work to involve a tangential flow of exchanged homotopic residue, whereas, decompactification of dimensions tends to work to involve a cotangent-related flow of exchanged homotopic residue. 
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach. 

Some More As To The "Truth" Tachyon

What happens to be so special about the conformal dimension of a cohomological eigenstate of a "truth" tachyon, is that one "mer" of it -- when this is taken at the Poincare level that is just external to such a so-stated "mer" -- is to have a conformal dimension of exactly 3.  This is because a typical eigenstate of the cohomology of a truth tachyon, is both metrically and Lagrangian-wise hermitian -- in each tending iteration of its Laplacian-related Transform, and such an eigenstate is to therefore to have no "imaginary discrepencies." What I mean here by this, is that there tends to be no metrical spurs that are thence distributed -- as such a said truth tachyon is delineated from one translocation of its Laplacian-based setting to the next, -- as well as the condition that, over such an "even-keel" of a correlative pulsation, that such a said truth tachyon is to change in only as many derivatives as the number of spatial dimensions that it is being transmitted through over time.  ((2+2^(0/anything)=2+2^(0)=2+1=3, since anything^(0)=1.)  This is due to the genus of the dimensional train-related wave propagation series.  (The resultant power series of both the pulsation and the field delineation of this correlative case --when this is taken as an integration of both the motion-related eigenindices and the Hodge-related eigenindices, that are here to be correlative to the said "mers" -- translocates heuristically, in so as to converge upon a set of one or more metrical and Lagrangian-based rational Njenhuis roots over time.)
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Extra Stuff About Cyclic Permutations

Let us initially consider a phenomenology that goes through a state of a Fourier-related activity,  that is repeated over and over again -- yet, to where such a so-eluded-to general tendency of a cycle is to work to bear one or more slight changes, over the course of the iterations of each of such a so-eluded-to process or processes of cyclical states.  If the pattern of the cyclical changes, is never symmetrically completed -- in such a manner to where the overall pattern of such a general condition of a cycle is not equivalently iterative, then, such a cyclical pattern is said to diverge.  Yet, if the pattern of the cyclical changes, is to instead, be symmetrically completed in such a manner -- to where the overall pattern of such a general condition of a cycle is to be equivalently iterative, then, such a cyclical pattern is said to converge.  For instance -- let us consider an elliptical pattern, that is cyclical in permutation.  Let us say -- within a here considered tendency of time constraints -- that one physical phenomenology is to orbit around another physical phenomenology, in such a manner to where the tense of such an orbit, per each adjacent iteration of orbit, is to be slightly different is its precise Lagrangian-based contour, -- yet, let us say that in this given arbitrary case scenario, that after one thousand iterations of such an elliptical tendency of orbit, that the whole overall general pattern of a cyclical tendency is to be repeated in the exact same manner again, to where the second set of one thousand iterations of such an elliptical orbital-based tendency is to be exactly the same as the first set of one thousand iterations of such an elliptical orbital-based tendency.  In this just mentioned tense of a condition of cyclical permutation, the cycle is to here be symmetrical in its behavior, and thus, such a so-stated tense of a condition of cyclical permutation is to here be convergent, -- at least over the course of the first two thousand iterations of such a pattern of a cyclical-based permutation-related tense of elliptical orbit.  Furthermore, there are three general genre of Fourier-related cyclical permutations -- of which may sometimes be combined. There are Lagrangian-based cyclical-based permutations, and/or there are metrical-based cyclical permutations, and/or there are contour-based cyclical-based permutations.  I will later discuss what is meant by a Laplacian-related state of conditions, that would work to bear a tense of cyclical permutation.

I will continued with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.