Monday, April 4, 2016

Part Two Of Session 12 Of Course 19 -- The Klein Bottle And Orbifold Differentiation

As is often the case -- the Gaussian Ward-based conditions of a Yang-Mills-based light-cone-gauge topology may have a habbit of being both antiholomrphic and orphoganal to the Gaussian Ward-based conditions of an adjacent Kaluza-Klein-based light-cone-gauge topology, from within the holononmic substrate of many substringular phenomenology that are to here consist of both orbifolds that are respectively of a non abelian light-cone-gauge topology as well as orbifolds that are of an abelian light-cone-gauge topology.  For instance, let us take a metaphorical look at the composition of an electron, when this may be taken in a Laplacian-based manner of extrapolation.  The mass-bearing superstrings of an electron, such as is the case for any Noether-based mass-bearing superstrings, are of a Kaluza-Klein or of an abelian light-cone-gauge topology.  The Noether-based superstrings of an electron that are purely of a tense of kinetic energy, such as is the case for any superstrings that are purely of a tense of kinetic energy from within the framework of the Ward-Caucy-based constraints of any substringular case scenario -- are of a Yang-Mills or of a non abelian light-cone-gauge topology.  The orbifolds of an electron that are of a mass-bearing nature, work to bear a Gaussian tense that is both antiholomorphic and orphoganal to the Gaussian tense of those orbifolds of an electron, that are purely of a kinetic energy-based nature.  The resultant tendency of a lack of both mini-stringular tension and the lack of both elastic and fractal-based torsion -- that often exists among the substringular eigenmembers that are of a Yang-Mills light-cone-gauge topology -- may often tend to produce a lack of entropy in the framework of the respective orbifold eigenset, of which may often here work to allow for less of a need for what would otherwise be the imminent need for the Kahler-Metric to be interactive among the substringular eigenmembers, that are of the directly correlative substringular region of such a case.  This occasional tendency may often tend to cause a lack of the so-eluded-to imminent substringular local region, that is proximal localized with such a Laplacian-based locus -- to then bear less of a need for the utilization of the holonomic substrate of the correlative Klein Bottle eigenstate with the proxmal localized manifold, that is of the so-eluded-to orbifold eigenset of such a case, that is here of a Yang--Mills light-cone-gauge topology.  I will continue with the suspense later! To Be Continued!
Sincerely, Sam Roach.

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