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

When two or more cohomologies are bound -- in an orthogonal-based manner -- then, the directly affiliated  coalescing of the correlative world-sheets involves permutations at the so-eluded-to binding cite, that are formed by the holonomic substrate of one genus and format or another of a norm-state projection.  Such permutative-based holonomic substrate eigenstates may either be of a cyclic-based format of permutation, or, such permutative-based holonomic substrate eigenstates may also, instead, bear a Majorana-Weyl invariance -- to where the specific locus-based cite of the so-eluded-to permutation-bearing norm-state projection may either be of an indistinguishably different differential genus, that may vary in its Ward-Caucy conditions, or, the specific locus-based cite to the so-eluded-to permutation-bearing norm-state projection may be of a steady-state genus of spatial interconnection, that does not vary to the same so-eluded-to extent.  Either way, the binding cite, that would here work to interconnect two specific smaller-based cohomologies, into a more overall specific larger-based cohomology, will bear at least some sort of torsional-based spike -- that works to form a tense of necessary Chern-Simmons singularity -- that works to form a higher tense of a harmonically scattered genus of norm-state-projection, in so as to bear more of a viable ability for any given arbitrary reverse-mode of norm-state-projection (a compatable norm-state projection that bears an opposite kinematic basis of holomorphic topological sway) to act upon the initially stated general format of cohomological index, so that the just stated cohomology may be annharmonically scattered into that general format of substringular residue that is then pulled off of the here relative Real Reimmanian Plane -- into the correlative plane of gravitons and gravitinos.  Such residue of Gliossi-Sherk-Olive ghosts -- that is then pulled into the respective plane of gravitational particles -- is utilized, over a more broad-based sequential series of iteration of group instanton -- in so as to eventual be utilized indirectly to form Neilson-Kollosh ghosts -- in so as to form a substringular residue from the annharmonic scattering of the just mentioned ghosts, that is then pulled back into the initially mentioned relative respective Real Reimmanian Plane.  This is the general process of the exchange of cohomological residue that happens in so as to form the general holonomic substrate that the Rarita Structue eigenstates must work upon most directly, through the activity of the correlative Schwinger Indices -- in order for the Ricci Scalar to be able to take effect.  To Be Continued!  Sam.