Let us consider a given arbitrary initial case of an orbifold eigenset -- that is moving through what is to here work to form an initial Rham cohomological mappable tracing -- in such a manner, to where the actual path of the said orbifold eigenset in question is to here be moving through its directly corresponding Hamiltonian operand -- via the so-eluded-to initial tense of what is to here be the mappable tracing of a discrete unitary Lagrangian path, in which the so-eluded-to set of superstrings that are to here operate in so as to perform one specific function, is to be moving through -- as the so-stated orbifold is to here be differentiating in a Fourier-based manner, as it is being kinematically propagated as a metrical-gauge-based Hamiltonian operator, that is being delineated across what is to here be a relatively limited field transmitance, a group metric that is here to be over a relatively transient sequential series of iterations of group-related instantons. As the said orbifold eigenset is to then collide with a relatively steady-state tense of a codifferentiable set of orbifold eigensets -- this set of codeterminable orbifold eigensets, of which are to here exist in a relatively higher scalar amplitude of a Majorarna-Weyl-Invariant-Mode, -- when this is taken in terms of the field-density of superstrings that are to be collided into by the initially stated orbifold eigenset -- to be of a relatively more stable tense or genus of a conformally invariant mode -- to where the initial Fourier-based activity of the Gliosis-based contact of the initially said orbifold eigenset with the second so-stated set of orbifold eigensets, will tend to work to form a relatively mild amount of heat energy, due to the frictional force that is exhibited by the manner of the so-eluded-to Yukawa-based interdependent contact that is to here occur amongst the two so-eluded-to metrical-gauge-based Hamiltonian operators that have been infringed each other, at the externally-based Poincare level of the dual interaction of the so-eluded-to core-field-density of their relatively outer Ward-Neumman-based field indices. This mild scalar magnitude of infrared energy, that is to formed by the said collision of the two so-stated Hamiltonian operators -- will then tend to scatter upon the proximal localized field indices -- in such a manner in so as to form a tense or a genus of a Calabi-Yau interaction, -- since the so-stated interaction is to here be a scattering of a form of electromagnetic energy with the holonomic substrate of certain given arbitrary set of mass-bearing superstrings of discrete energy permittivity. Any given arbitrary Gaussian Transformation, that is to be involved with any respective given arbitrary genus of a Calabi-based interaction -- will be of a tense of what may be termed of here as a gauge-transformation. In a gauge-transformation -- this general tense of the directly corresponding Kahler-Metric, will be one in which the directly corresponding Klein Bottle eigenstates that are here to be involved, will work to bear a tensoric-affliliated state of a Njenhuis topological sway -- that will be more touched upon in course 20 (as to Calabi-Yau, Calabi-Wilson-Gordan, and Calabi-Calabi Interactions). Just as this respective given arbitrary collision of this given case scenario, will here cause the initially so-stated orbifold eigenset to bounce into the relatively opposite tense of holomorphicity -- this will then tend to form an antiholomorphic Kahler condition, that will then indirectly work to form an ensuing Kahler-Metric. This tense of a scattering, is of an annharmonic-based genus. This will then be a general genus of what may be here described of as tense of a Rayleigh-based scattering of those so-stated infrared-based photons, that are to here be made entropic -- in the course of striking the directly associated mass-bearing superstrings that are to here be associated with the so-stated Gliosis-based contact that is of this respective given arbitrary case scenario. Since the so-eluded-to tense of this said case in point is of an annharmonic-based perturbation -- this general case scenario is a given arbitrary genus of what may be termed of as a Cevita Interaction. I will continue with the suspense later!
To Be Continued! Sincerely, Sam Roach.
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