Wednesday, May 20, 2015

Part One of Session 16 of Course 18 -- The Ricci Scalar and Kaeler Differentiation

The Schotky Construction is composed of the manner in which the Klein Bottle is put together.  In other words, the composition of any given arbitrary Klein Bottle eigenstate is based upon the make-up of the Schotky Construction.  The Schotky Construction bears a make-up that is based upon the consideration of those respective orientifolds, of this given arbitrary consideration -- that are physically held together by the correlative Wilson-based Ward-Caucy delineations, that work to comprise the manner in which the so-stated relative lengthwise and thickness-wise ends of the said Schotky Construction are put together, in so as to form the substringular-based attributes as to the way that any respective given arbitrary Klein Bottle eigenstate is put together.  I will describe the nature of such a construction later.  This so-mentioned Schotky Construction's general physical composition in the substringular, is always how any actual unfrayed Klein Bottle eigenstate is put together -- whenever such a said eigenstate of this so-stated genus of substringular format is of the capability of being able to act as the "key player" of what is utilized in so as to move any respective given arbitrary Higgs Boson eigenstate, that is of a correlative nature, into the general core-field-density of the activity of the directly affiliated multiplicit Kaeler-Metric eigencondition of group metrical eigenbase.  The physical tense of any given arbitrary Klein Bottle eigenstate tends to act, as much as feasible, in so as to exist in a state of optimum conformal invariance.  Often, what may work to appear as what acts, in a kinematic manner, as specific Klein Bottle eigenstates, are phenomena that are being utilized in  a tense of indistinguishable difference -- particularly, if the correlative superstrings that are here being directly involved in such a case, are of a tachyonic-based nature.  Yet, due to the manner of the activity of the multiplicit Klein Bottle eigenstate -- on account of both the manner of its Schotky Construction, and also, the general "apparatus" of the Kaeler-Metric-based eigenmatrix-based inter-relationshipts -- the motion of the said Klein Bottle, in general, is relatively situated in a tense of a Majorana-Weyl Invariant Mode.  I will continue with the suspense later!  To Be Continued!  Sam Roach.

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