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

If the permutations that were to exist in such a manner, in so as to bind one or more smaller bases of cohomology -- are not of a hermitian nature, then, these so-stated permutations here do not directly involve a smooth topology.  Often, a permutation that works to bind one cohomology to another, works to pull the initially inferred cohomological projection off of the respective relative Real Reimmanian Plane -- thus forming a Njenhuis-based projection of an integration of cohomological ghost-based indices.  Such permutations here, that are off of the initial Ward-Caucy bounds of the initially stated basis of cohomological projection, are perturbative -- in a Laplacian-based manner -- to the Gaussian format of the so-stated initial cohomological projection.  No matter how hermitian both cohomological-based projections are individually, the overall insinuated binary cohomology that would thus form would not be completely hermitian, and thus such a binary cohomological stratum would never by Yau-Exact -- due to the so-eluded-to perturbative permutation that would here work to bind the two so-stated initially smaller cohomological stratum.  If such a cohomological-based stratum were to then be perturbated spontaneously into a phenomenon that would not bear Yau-Exact individually based superstrings (if the directly associated superstrings that were to work to comprise the so-stated physical stratum, that worked to form the just mentioned binary cohomological pattern, were to alter into a condition of being not Yau-Exact), then, such a phenomenon would not then work to describe the physical memory of a phenomenon of mass.  This would then mean that this phenomenon, at this point, would not directly bear the essence of any given arbitrary Calabi-Yau manifold.  This would then mean that the correlative Ricci Scalar eigenstates that are then here to interact with the so-eluded-to superstrings, that were to work to form such an altered cohomology, would then not interact with the so-stated cohomological stratum in the manner that gravity tends to interact with a mass in.  Such a net cohomological stratum is a description of either scattered energy or scattered electromagnetic energy, depending upon how the directly involved Chern-Simmons singularities vibrate -- otherwise, either harmonically or annharmonically, respectively.  If the Chern-Simmons singularities that are here of a given arbitrary case, do vibrate -- with relative harmonics, in spit of the permutations, then, the Ricci Scalar eigenstates of such a case is appertaining to a condition of scattered kinetic energy.  Yet, if the directly correlative Chern-Simmons singularities of such a case vibrate with relative annharmonics, then, the Ricci Scalar eigenstates of such a case is appertaining to a condition of scattered electromagnetic energy.  To Be Continued With 10!!!