Tuesday, October 6, 2015

Part Five of the Tenth Session of Course 19 -- The Klein Bottle and Orbifold Differentiation

Any given arbitrary nucleon, is a genus of a phenomenology -- that tend to exist in what may be termed of as an F-brane.  Nucleons in an atom are generally conformally invariant at their relatively proximal locus, when this is taken at the Poincaire level -- when this is taken into consideration, at a field that is Gliossi to the core-field-density of the said multiplicit nucleon, as an index of being of a genus of an entity of holonomic substrate, that would here bear a directly corresponding Majorana-Weyl-Invariant-Mode that is thence at the locus that is Yakawa to the substringular neighborhood of such an orbifold eigenset of Ward-Caucy-based conditions.  So, in other words, let us say that a certain given arbitrary atom is moving as a Noether-based field, that is either relatively stationary or relatively kinematic, over time.  Let us then say that the respective said atom is of what may be termed of here as being of a stable nature.  This would then mean, that the nucleus of the so-stated given arbitrary atom -- would then tend to be stable, as well.  This would then mean, that the nucleon or nucleons of such a respective given arbitrary case -- as substringular member(s) of the directly corresponding atom -- are then existing, as from within the so-stated atom of this case -- in a tense of conformal invariance.  Under such a genus of the so-mentioned Ward-Caucy conditions -- such a tense of the one or more members of such an eluded-to nucleus of an atom -- is going to tend to be of a relatively optimum state of rest, whether the said respective atom is moving in and or itself in a Noether-based flow or not. This does not include the characteristic-based conditions, of as to whether or not the respective atom is moving in a tachyonic-based manner or not, though.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

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