A Little Bit About Substringular Couplings

What if a Yakawa Coupling that here existed in-between one set of superstrings had an even chirality, while the said Yakawa Coupling that also existed in-between another set of superstrings had an odd chirality, and, the two sets of superstrings that I just mentioned here in this given arbitrary case scenario were kinematically covariant?  The traits that I just described here by these two given sets of superstrings would have an assymetric J.  The compactification of the set of superstrings which had an even chirality would here propagate as a convergent series of holomorphic discharge, while, the compactification of the set of superstrings which had an odd chirality would here discharge Fock residue that would work to propagate as a divergent series holonomic eigenbasis.  As the two sets of superstrings that I just described interact as a reiterative variant operation, the assymetric-basis of their spin-orbital-interaction would here diverge as their angular momentum would simultaneously converge -- in a relativistical manner. As the spin of the two codifferentiating substringular traits that I just described work to polarize, in terms of their wave-tug delineations, the renormalization of their series output -- in terms of the consequent supplemental homotopic discharge -- this activity would here converge the local Poincaire distribution of the overall parity of the described given loci that is involved with the interaction of the two said traits.  The just mentioned two traits are here working to describe the interaction of the two said sets of superstrings that I have been describing in this given arbitrary case scenario.  The convergence that would then happen here would work to cause the given distribution of wave generators that are involved in this case to form a set of a fractal of covaliance. Such a "covaliance" would exist in-between the operational indices of those superstrings that worked to describe the two said traits.  These traits would here be eigen to the homostasis of a minimal variation of Ward-Caucy boundaries, when one is considering the desingularization of the corresponding substringular neighborhood fluctuations.  Such fluctuations would operationally allow for both the corresponding radial and transversal codifferentiation of a fixed matrical mode.  Such a mode would tend to not form critical cusps that would have a strong probablility of desolving upon an odd function of local kinematic transposition.  Once the corresponding transposition of the interactive decomposition that would result in the here mentioned case is encoded for by the substringular encoders -- while such a said transposition is iterated and reiterated in the same general process -- the corresponding Majorana-Weyl invariant anomalic substringulaar sway that would thence be formed by the related operation would spontaneously be nullified by the previous eigenaction.  The just mentioned activity would cause the corresponding Cassimer Invariant-mode to be physically integrated upon as a substringular fractal of a substrate, so that the resulting convergence of the insuing kinematic differential association may bear its correlative vibrational mode.  This would cause the creation of such a vibratory mode, of which would here produce eigenstates of Hamiltonian operation in terms of the resulting involvement.  This is so that the most directly inolved codifferentiable substringular trait that would be involved here would be able to then bear a Fourier-based condition of parametrically corresponding invariance.  I will continue with the suspence later!  Sincerley, Sam Roach.     

Course 4 On The Substringular Vs. The Globally Distinguishable, Session 15, Part One

As a string spins, rolls, and transversely moves along the ultimon, it also moves as an organization of individual points. These individual points not only move as a unit, yet these also reform many times in the process of going between any two locations. So, as a string breaks down into point particles in-between instantons, the individual point particles are constantly iterating and fading as entities in-between each locant that is in the size of a point. This started when time began, and will continue until time ends. As explained, points attempt to obey the Heisenburg Principle and the Pauli Exclusion Principles. Points also involve many waves. The density of a point may be described as condensed oscillation. When the points are pulled "forward," these will be noded out. This will make these to appear faded out. The process of points of a string in-between stringular iterations fading out, and iterating in relation to the behavior of the basis of light effects the ways in which the string iterates in terms of the related Lorentz-Four-Contractions. This is because the ways in which the waves that comprise the partial aspects of the given string differentiate in terms of where these are nodal and antinodal relative to the nodes and antinodes of all of the proximal light eigenstates in such a way so as to influence the way that the string will be measured, as a unit, relative to light, how the string will cohesively integrate relative to the measurements of an observer, and how the parameters that are measured that that given string will differ with where the string is to be localized as a phenomenon that is determined to be in a specific spot in the globally distinguishable. If this given string were to remain as simply a set of point particles that are not and will not reorganize as a string, then the ways in which the given set of points differentiate and the boundary conditions of the vacuum regions that this space will now iterate will form. I will continue with the suspense of this session later. Until then, you have a great day!
Later,
Sam.

Course 4 on The Substringular Vs. the Globally Distinguishable, Session 5, Part two

The whole "point particles" including the empty space of the points' homogeneous fields are really point particle neighborhoods. Do you remember me mentioning the Pauli Exclusion Principle and the Heisenburg Exclusion Principle? The Heisenburg Exclusion Principle basically says that you can not find or determine exactly where a very small particle is at and what it is giving off at the same time. The Pauli Exclusion Principle is basically that two things can not occupy the same spot at the same time. (Adjacent electrons must bear antisymmetric spin.) A typical point particle as its core density iterates and reiterates within a volume of roughly two to 10,000 times the volume that it would have if it was completely condensed. It does this iterating throughout the translation of its point particle neighborhood radii (consistently during iteration and Ultimon Flow). The point particle, as a density, is condensed oscillation. Condensed oscillation will tend to "want" to spring out when it is given a chance, just like a spring will spring out when it is released. The world-tube governs the Ward Conditions of the strings. Strings are the basis of the organization of point particles. So, a point particle will "want" to reiterate primarily in the relative center state of its neighborhood after the point iterates one radii of its neighborhood over the course of the substringular activity that involves the given point particle (when one considers 'the flow from iteration time to Ultimon time to be a blend of metrical activity). This is because the cross-section of the given world-tube will be holomorphically translated after during such a travel. Yet, this would leave one to 9,999 dispersed areas of locant that are not covered! No problem. After the point travels the given distance, it will iterate at all two to 10,000 states due to the majorization of the plane that the point traverses. This is because the point particle, in traveling the radii of its neighborhood, will curve in four directions besides its "0" dimensional framework. This is because the given point particle neighborhood is treated here as one of the simplest "three-dimensional" phenomenon that is curving in space to where it behaves like a "four-dimensional" phenomenon as the Ultimon cycles. Each added dimension adds a power of ten to the areas equivalently swept, since the world-tube bears 10 directly associated dimensions (explained later) and 10^0 = 1, 10^1 = 10, 10^2=100, 10^3=1,000, and 10^4=10,000. So, the point is at 10,000 different locations many times over the cycle of one iteration. (It is at one spot at a time, yet this is at a lower level of discrete. This is under regular Einsteinian motion. 1/10,000 of the condensed oscillation centered in a point particle neighborhood pulses radially after each iteration of the substringular.