Friday, January 22, 2016

As To Perturbation Out Of Majorana-Weyl-Invariant-Mode

Let us say that one were to have an initial Ward-Caucy set of conditions, that is of a tense of what is here a local cite of a substringular orbifold eigenset -- that is differentiating in a Fourier-based manner, in an exhibition of a state of Majorana-Weyl-Invariance,  over a directly corresponding relatively transient sequential series of iterations of a covariant activity of group-related instantons.  Let us now say that the orbifold eigenset that we are considering here, is that of an electron that is charge-wise stable, from within the Ward-Neumman confines of a relatively charge-wise stable atom.  Let us next say that a photon is to strike the Gliosis-based field of the Yukawa-based topological setting, that is of the so-stated initially relatively stable atom -- that had worked here in so as to include the so-mentioned electron, that had acted as the Hamiltonian operator that had been eluded to earlier.  Let us say that the relatively Gliosis-based contact of the photon here in question -- with this so-stated Yukawa-based field of the said electron -- will then work to form a Calabi-Yau interaction, over the ensuing transient period of time.  Such a perturbation that is caused by the interaction of light with a quantum of mass, will initially act in so as to cause a perturbation of the said electron -- in a manner that works to move the said electron away from its initial tense of Majorana-Weyl-Invariance.  This so-eluded-to example of a Cevita interaction, will tend to settle in both the metrical and in the Lagrangian tense of optimum rest -- during the interim in which the said electron that has just been scattered is then pulled into "seeking" an upcoming ulterior tense of Majorana-Weyl-Invariant-Mode, once the so-stated electron is acted upon by those eigenindices that are of both the subatomic and the substringular level, that will subsequently work to form a Wess-Zumino interaction.  Such a general tense of a Wess-Zumino interaction, will then tend to work at bringing to the electron of this given arbitrary case, into an adjusted tense of conformal invariance with both a different delineatory index and a different metrical index -- via whatever the Fourier-based group-attractors, that work in so as to form the so-stated general tense of substringular adjustments, to then be able to bring about the needed harmonic-related perturbation that is needed, in order to work to re-establish an ensuing tense of a Majorana-Weyl-Invariant-Mode -- upon the Yukawa-based Ward-Caucy bounds of the electron that is here being discussed in such a case.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

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