Thursday, April 2, 2015

Part Five of Session 12 of Course 18 -- The Ricci Scalar and Kaeler Differentiation

A Calabi-Yau Action is that activity of a Calabi-Yau Manifold -- in which the existence of the presnece of the said Calabi-Yau Manifold works to express the membrane-based characteristics of the so-eluded-to manifold.  Again, a Calabi-Yau Manifold is the locus of any given arbitrary mass-based orbifold, in which the Gliossi-Sherk-Olive cohomological pattern of one specific membrane will here work to form the mappable tracing of the behavior of the projection of the trajectory, of those superstrings that operate in so as to perform the specific function -- of that set of superstrings of discrete energy permittivity, that will have here come together in so as to form the so-stated orbifold of any related respective given arbitrary orbifold that is mass-based.  The space of a Calabi-Yau Action may be termed of as a conifold point.  This so-mentioned "point" that I have here just mentioned is the holonomic substrate of the physical phenomenology of a Calabi-Yau-Manifold, that behaves in so as to be the directoral center of the activity -- that the directly related respective given arbitrary Calabi-Yau Manifold is based at.  This is the case, as such a manifold works to act as the here mentioned membrane-based phenomenology of a mass-based mappable tracing, that I have here described.  Cohomologies vary in both the scalar magnitude and the manner of their correlative spatial differentiation -- as such a multiplicit integration of the multivarious ghost-based indices, that come together in so as to work to form any respective given arbitrary mass-based membrane-based mappable tracing -- which is of the transient history of the what, where, when, and why, as to both the existence and the motion of superstrings of discrete energy permittiivty, of which has the bearing of its physical memory, over time.  Such a physical indication of both the existence and the activity of superstirngs of discrete energy permittivity, is mapped-out, as the directly corresponding superstrings are kinematically interwoven amongst each other -- over the immediately previous sequential series of group-related instantons.  Such an eluded-to cohomological pattern comes together in so as to show the Ward-Caucy conditions of the directly correlative superstrings -- that act in so as to form the directly corresponding orbifold of any respective given arbitrary manifold of spatial operation, that may act as the Hamiltonian Operator of the composition of a correlative Calabi-Yau-Manifold, over time.  Such a Manifold -- in the process of working to bear a conifold-based point -- works to act through a tightly-knit Lagrangian, over the transient period of time in which the said Calabi-Yau-Manifold is superconformally invariant, at a level that is Poincaire to the immediate mappable tracing of the so-eluded-to orbifold, that acts as the so-stated directly correlative Hamiltonian Operator of any directly pertinent scenario. Such a scenario is one in which the correlative  orbifold of such a case, works to form the eigenbase of the directly affiliated membrane-based cohomological setting.  Such a general format of activity works to form the eigenbase of the modulus of such a Calabi-Yau-Manifold.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

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