Thursday, February 5, 2015

As to the Effect of Certain Nonabelian Norm-Projections

When a norm projection interacts with a cohomological-based index -- such as a world-sheet that is here at a relatively limited given arbitrary locus, over a transient metric that would here involve a relatively static and proximally local Lagrangian eigenbase -- that would here be a condition of such a so-stated world-sheet iterating at a tense of superconformal invariance -- to where the differential geometry of such an eluded-to Yakawa-based interaction that is here Gliossi, at the Poincaire level of the interior Ward-Neumman bounds of the holonomic substrate of the so-eluded-to topological surfaces -- that are then here in direct physical contact, is of a non abelian nature, then, the sum of the Hamiltonian-based Hodge-Indices that are acting as having more of an abelian-based interaction -- of the immediately correlative first-ordered point particles of the said norm-projection that are most Gliossi at the point of contact -- toward the immediatley correlative first-ordered point particle of the said world-sheet, that are most Gliossi at the point of contact -- when the differential trigonometric sum of the directly affiliated resultant dot-product that is most associated with the relative  Hamiltonian-based response of the activity of the said  norm-projection when struck, with the differential trigonometric sum of the directly affiliated resultant cross-product that is most associated with the relative Hamiltonian-based response of the activity of the said world-sheet when struck -- will work to help determine the manner and the degree of the resultant alteration or perturbation of the kinematic eigenbase of the ensuing activity of the so-stated world-sheet.  So, if the overall coniaxial that works to define the eigenbase of the line integral that works to form the initial stability of the Majorana-Weyl-Invariant mode of the so-state initial condition of superconformal invariance that the said world-sheet that is here being discussed, is altered from one orientation of a unified set of directoral-based axions that act as one discrete unit to another orientation of a unified set of directoral-based axions that act another discrete unit, then, the manner and the existence of the resultant activity of both the world-sheet and the directly corresponding norm-projection of this case scenario will alter -- as is according to the here respective topological sway that may be eluded-to by so-stated aleration of the directoral-based orientation -- as is according to the resultant differences that would here be most directly associated with the change in the sum of the respective said given arbitrary Hamiltonian-based Hodge-Indices that would then be of a different differential geometry that before, as I have here indicated.  To Be Continued!  Sam Roach.

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