As I was eluding to before, this "disappearing act" works to help form the basis, of what may here be considered as an association with both the minimum distance and the minimum time that a superstringular entity may travel, to where the discrete values that are to here be relative to a direct correlation -- with either the Planck Length and/or the Planck Radius -- may then be established, based upon a directly correlative extrapolation of such a so-eluded-to scenario. Now, you may wonder -- how does the homeostasis of the bearings of a superstring of discrete energy permittivity, actually work together, -- when this is taken in our initial consideration of relativity, to where this will consequently work-out in the real world, in so as to come into play with any given arbitrary set, that is of that general sequential substringular iterations of group-related instanton, that come together in so as to work to help to form the Fourier-based translation of energy, that is being conveyed over time? The following may help to start to explain this generic type of question: Certain first-ordered point particles will end-up at about roughly the same spot over a sequential series of instantons, on account of such a directly related set of superstrings -- that are here to be comprised of such so-stated first-ordered point particles, that are to here be in the process of what may here be called a tense of superconformal invariance. When a set of superstrings of discrete energy permittivity, are to here be undergoing a tense of superconformal invariance -- at what is to here be at the Poincare level to the proximal localized tense of static equilibrium, that is to here be involved with such a tense of a relatively stable framework that may be then considered to be of a relatively non-kinematic tense, over time, to where then, such a said set of superstrings that are to be conformally invariant in such a so-stated manner, are to here be undergoing a relatively tightly-knit tense of a Majorana-Weyl-Invariant-Mode. Thus, the directly associated sequential series of group-related instantons of such a tightly-knit tense of conformal invariance, are then said to converge upon the directly corresponding Hamiltonian operand -- by which these are to be in a steady-state with, -- over the directly associated time by which such a static-based framework is to not be kinematically perturbated from the said proximal localized locus of field operators. Such a tense of a framework, that is to here be in a relatively tightly-knit tense of conformal invariance, is to then, during such a relative tense of invariance, to tend to be in the process of being kept from perturbating as a divergent metrical-gauge-based Hamiltonian operator, by the Fourier-based influence of a set of one or more group-attractors -- that will as well, tend to act in so as to help to keep the said convergent covariant set of operators in tact, as a relatively static Hamiltoniain operation, by the Fourier-based activity that is translated by the activity of the self-same entities that I have just described of as being a directly influential tense of group-attractors, that are to then be Yukawa to the eigenstates of the field generators of the so-eluded-to convergent eigenindices -- that are here to be in the said tense of superconformal invariance. Now if the so-eluded-to tendency of the so-stated activity of the directly associated group-attractors is to susequently diverge from being Yukawa to the topological substrate of the so-eluded-to superconformally invariant field -- this will often work to cause the initially stated static-based field, to go into the process of a Rayleigh-based scatttering of its correlative eigeninidces, -- which will consequetly tend to work to form an annharmonic wave-tug upon the homotopic residue of the initially static set of superstrings. This will then tend to form an odd chirality among the adjacent superstrings that were intially of an even chirality -- which will consequently work to disorient any immediately ensuing extrapolation of the point particles that will have here worked to initially help to form the so-eluded-to superstrings of discrete energy permititivty that we were initially discussing.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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