Friday, August 22, 2014

Part Two of the Ninth Session of Course 17 About the Ricci Scalar

A Rham cohomology is a cohomology that is completely hermitian.  This means, then, that the singularities of a Rham-based cohomology are Yau-Exact.  This also means that either a superstring, an orbifold, or an orbifold eigenset, that is working to form a Rham-based cohomology, is Yau-Exact -- as such a respective given arbitrary superstring, orbifold, or orbifold eigenset is operating in such a manner -- in so as to form a Rham-based cohomology.   Although a Doubolt cohomology is often of a hermitian-based nature -- if a Doubolt cohomology is ever Yau-Exact, then, the projection of at least part of such a cohomological-based nature bears Njenhuis-based projections, that are part of the so-eluded-to cohomology -- under the just mentioned general substringular situation.  Yet, if a Doubolt cohomology bears no Njenhuis attenuations that work to comprise such an integration of ghost-based indices, then, the so-eluded-to general format of such a cohomology will then not be Yau-Exact.  This then means, that, a purely Real Reimmanian-based Doubolt cohomology will either bear Lagrangian-based Chern-Simmons singularities, and/or, such a general genus of cohomological stratum will bear metrical-based Chern-Simmons singularities.  So, if two world-sheets that work to form a ghost-based cohomological pattern work to form two orthogonal ghost-based stratum -- to where one end of either a Real Reimmanian-based projection of cohomological-based stratum and/or a Njenhuis-based projection of cohomological-based stratum is normal to the other respective end of either a Real Reimmanian-based projection of cohomological-based stratum and/or a Njenhuis-based projection of cohomological-based stratum, then, such an overall cohomological-based pattern -- that is put together, via a linking that may be formed by the activation of a norm-state projection, that puts the two initially stated cohomological-based projections together into an overall ghost-based stratum, will always work to form some sort of Doubolt cohomological pattern.  This is because, the activity of two cohomological-based projections -- being tied together in a 90 degree-like manner, works to form at least some sort of spurious and/or spike-like torsioning at the linkage, that works to put the two so-stated general formats of cohomological-based stratum together.  This is partially due to the condition that adjacent superstrings that are of the same universe, iterate in such a manner in so that these are differentially geometric -- the relative one to the other -- in a 90 degree manner.  Ghost-based indices are the mapped-out tracing of world-sheets.  World-Sheets are the trajectory of the projection of superstrings.  Cohomologies are ghost-based indices that are put together, in one manner or another.  Cohomologies are thus the physical memory of the where, how, and what -- that superstrings had just done, in any given arbitrary case.  Therefore, any binding of one or more orthogonal projections of cohomological-based stratum -- whether one or more of such cohomological-based patterns are Yau-Exact or not, in and of themselves, will always work to form an overall cohomological-based pattern that will then be of a Doubolt nature.  This is why all norm-based interconnections of one or more cohomological-based stratum will always work to form some sort of Chern-Simmons singularities.  This does not, however, work to discredit the condition that all superstrings that bear Yau-Exact singularities -- in any one individual ghost-based projection, that is considered in a unitary-based manner -- work to form the condition of the directly corresponding superstrings that had worked to form such singularities -- as being Yau-Exact.  Such Yau-Exact superstrings work to form manifolds, as to their conformally invariant base of iterating over a sequential series of instantons, that are known of as Calabi-Yau manifolds.  Calabi-Yau manifolds are the multiplicit Gliossi-Sherk-Olive stratum, that directly appertains to the existence of a superstring of mass, that  is to then here exist, in one manner or another, in a tense of Majorana-Weyl covariance.
I will continue with the suspense later!  To Be Continued!!! Sincerely, Sam Roach.

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