Part Seven of the 12th Session of Course 18 -- The Ricci Scalar and Kaeler Differentiation

When cohomologies bend in a hermitian manner that is also of a symmetric nature, then, this is more analogous of a bosonic eigenbase of a topological-based sway -- when this is taken in terms of the directly pertinent vantage-point of the topology of such a sway, as may be taken from the Poincaire level of the correlative orbifold-based phenomenology, that is directly appertaining to the gauge-metrics of such a sway, over time.  The topological sway of any respective given arbitrary orbifolds -- as taken at the Poincaire level of the so-eluded-to superstrings that work to compise the so-stated orbifolds that may be here directly pertinent -- happens, when the wave-tug/wave-pull of the correlative spin-orbital indices that work to comprise the overall Hamiltonian-based operation of the affiliated orbifold are brought into a condition of a substringular Yakawa-based torsioning, over the directly associated successive series of iterations of group-related instanton in which such an orbifold is operational as a substringular-based holonomic substrate.  In so long as there is a viable Yakawa-based wave-tug/wave-pull upon any respective given arbitrary orbifold that is unfrayed, such a said orbifold will always be undergoing at least some sort of torsioning -- in so long as the components of such an orbifold are spontaneously contributing to the operational-based functioning of the so-stated orbifold, in any respective time-frame in which such an eluded-to  Hamiltonian operator is functional in the substringular.  The chief scalar magnitude of such a torsioning of such an orbifold of Hamiltonian operation is Gliossi to any respective given arbitrary set of superstrings of one specific substringular function -- at the successive series of the very end of each iteration of the correlative metrical activities of BRST.  The reason for this just mentioned conditionality of as to when the maximum scalar magnitude of torsioning, that is applied to any respective given arbitrary orbifold, is that the iterative effect of each ending of the successive series of BRST are the antiderivation eigenmetric that is directly correlative to when the directly affiliated light-cone-gauge eigenstates work to apply its maximum pressure upon those superstrings that operate in so as to work to comprise the affiliated orbifolds that I have been discussing here.  This maximum pressure that is applied in this case here, is due in part to the action of the Imaginary exchange of Real Reimmanian residue that is released -- over the course of the ending segments of each iteration of BRST.  Such an Imaginary Exchange that I have mentioned here, is due to the fact that the first-ordered point particles that work to comprise superstrings of discrete energy permittivity may only untwine in a back-and-forth ebbing of mini-stringular segmentation, in one set of universes, in a 32 spatial dimensional supplemental manner.