Part Three of the 14th Session of Course 17 About the Ricci Scalar

Those singularities that are formed by the kinematic interplay of world-sheet-based cohomologies that are rooted in the time-bearing differentiation of plain kinetic energy, are capable of being electrodynamically extrapolated as being off of the respective correlative Real Reimmanian Plane, relative to whatever happens to be the directly associated respective given arbitrary Njenhuis-based region -- that would here tie-in to the corroberative Real Reimmanian Plane, in so as to act as a Doubolt-cohomology, in this tense, in and of itself.  This does not completely rule out, however, the condition that certain unscattered plain kinetic energy may often bear a relatively smooth traceable cohomological pattern.  So, the general pattern of the mappable tracing of those singularities that exist in the world-sheet-based cohomology of plain kinetic energy, tends to display a physical memory that is partially perturbative and non-hermitian, in its directly pertainent general format of ghost-based indices.  When plain kinetic energy is scattered, though, it turns into a general format of physical substringular phenomena that is directly appertaining -- at least to a degree -- to an eigenbase of entropic holonomic substrate.  Entropy always involves the kinematic perturbation of the singularities of the topology of energy that is not in static equilibrium.  So, scattered plain kinetic energy is always of a Chern-Simmons eigenbase, in terms of the general genus of the directly affiliated singularities -- and not of a hermitian eigenbase, in terms of the general genus of the directly affiliated singularities.  So, the scattered plain kinetic energy that exists in the substringular, is always both non-hermitian and perturbative.  Plain energy is effected by gravity to less of a degree than either mass or electromagnetic energy, since it is so different in its general physical construction than the genus of manifolds that may be described of, instead, by the term of being of a Calabi-Yau genus.  In other words, scattered plain energy is Anything But Yau-Exact.  So, although the directly affiliated Ricci Scalar eigenstates are not primarily effected by plain scattered energy, the just stated Ricci Scalar eigenstates may be partially derived by, in extrapolation, the correlative Ward-conditions of the specific given arbitrary Hamiltonian operands that are trespassed by the mappable tracing of the trajectory of the Hamiltonian operators that may be tied to the existence of scattered plain kinetic energy.