About Benign Tadpoles and Cyclic Permutations

Zero-Norm-States are benign tadpoles, in the context of what is termed of as "tadpoles" in stringular physics.                                  
Zero-Norm-States operate to help close open strings and to open closed strings.
Although theoretically point particles are parabollic and spherical, the torsion that occurs to these makes these exist in a condition of having a relatively elliptical shape over the course of the Fourier Transformations that happen in multiplicit directoralizations to first, second, and third ordered point particles over any framework that involves gauge-metrics and/or time.  Since point particles are multiplicitly bound by many wave-tug holonomic field eigenstates, the torsion that occurs here involves sets of permutations upon the Gliossi structure of point particles.  When such permutations occur over a Fourier Transformation that tends to converge the sequential series as to the morphology and topologically hermitiatn and/or Chern Simmons Neumman Ward boundaries that work to define the construction of the general locus of a superstring, then, one may describe such a convergent series of the pattern of delineations that happen to such an arbitrary point particle over the Translaton of metrics and/or time that describes the torsioned motion of the said strings through an arbitrary Lagrangian as a cyclic permuatation. When a superstring exists in a relative state of conformal invariance, then the sequential series of the topological holonomic permutation pattern -- in terms of the pattern as to the convergent alterations in the topological surface of the point particles that comprise such a superstring -- is more likely to have hermitian cyclic permutations that tend to kinematically differentiate on the relative Real Reimmanian Plane.  Yet, whenever there is a Chern Simmons perturbation in the relatve directoralization of a superstring through a Lagrangian via a Fourier Series that involves a spurious Rham associated and/or a spurious Doubolt cohomoligical covariant integrable kinematic differentiation, then the permutations that operate upon the point particles that comprise the said superstrings tends to not converge with any Yau-Exact basis into what would otherwise be a definitive cyclic permuatation.  When the permutations that operate upon a point particle are not spontaneously cyclic, then, over the course of the neighboring Gaussian Transformations that differentiate through time in a relatively local region near such a spurious alteration in the pattern of the wave-tug delineations that occur upon the point particles that comprise a given superstrings will eventually bring the superstring back into a conditon to where the point particles that comprise such a string will rgain a convergent pattern as to the metrical and Lagrangian based kinematic delineation of its permutations.  Such a condition of regaining a convergent pattern of cyclic permutations is more likely under the conditions of a relatively conformal invariant operation.  So, all point particles bear permutations on account of the wave-tug applied to these, yet, such permutations are only cyclic in a convergent tense in terms of a smooth translation of an even metrical function that transpires over a discrete set of instantons when the associated superstirngs bear at least some sort of conformal invariance.  From a broader perspective, there is generally a tense of convergent to divergent and back to convergent pattern involved with the topological delineation of the permutations that are distibuted upon the outer Gliossi surface of point particls.  In this broader perspective, the pattern of the operation of permutations is, in a reverse-fractored way, always based on an even metrical function whose Hamiltonian operation defines such permutations as relatively cyclic.    I will continue with the suspense later.  Sincerely, Sam.