Thursday, March 19, 2015

Part Three of Session 11 of Course 18 -- The Ricci Scalar and Kaeler Differentiation

The norm-conditions of any given arbitrary eigenstate of the Bette Manifold -- as is exhibited by the Ward-Caucy boundary conditions of the so-stated respective given arbitrary eigenstate of the Bette Manifold -- work to be defined by both the tangential and the orthogonal Yakawa-based couplings that exist, as any directly corresponding Bette Action eigenmetric is underway, during the directly affiliated metrical duration of BRST.  As the light-cone-gauge initially coils (as I eluded-to before), the Gliossi-based region that is most directly affiliated with any respective given arbitrary Bette Action eigenmetric is "tightened."  As the light-cone-gauge then recoils, the Gliossi-based region that is most directly affliliated with any respective given arbitrary Bette Action eigenmetric is "loosened."  The just mentioned recoiling activity of the light-cone-gauge -- in a multiplicit manner -- helps to pull superstrings into the ensuing increments of the Kaeler-Metric and/or into the Regge Action.  The manner in which such a torsion happens -- as is here exhibited by the said recoiling -- helps to work at pulling superstrings into the start of the generally unnoticed duration-based gauge-metrical activity of Ultimon Flow.  The manner of the so-eluded-to coiling and recoiling may often vary in the genus of its physical differentiability.  The genus of the differentiability of such a torsioning, is the factor of which is able to work at controlling the manner in which the Regge Action specifically happens, in any respective given arbitrary scenario -- in so as to produce whatever the genus of the directly affiliated Regge Slope is to be.
I will continue with the suspense later!  To Be Continued!  Sam Roach.

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