Part One of the 12th Session of Course 18

The cohomologies that directly appertain to both the existence and the activity of orbifolds, and, the cohomologies that directly appertain to the integration of the mappable tracings of the multivarious world-sheets -- any respective world sheets, of which, are the trajectory of the physical projection of substringular phenomena of holonomic substrate -- are never of a completely static nature, over time.  Cohomologies are the integration of ghost-based indices.  Ghost-based indices are the physical memories as to the what, when, where, and how, the various substringular entities had been and moved, over time.  So, as any given arbitrary substringular entity has moved from one spot to another, the physical mappable tracing of as to where the so-stated substringular entity had been, when it had been at the said respective general locus of this specific given arbitrary case, what the integration of those indices that had come together in so as to work to form the so-stated substringular entity had been, and how the said substringular entity had moved -- over the course of the activity of that same respective given arbitrary substringular entity, is helped to be able to be extrapolatable to an observer, of whom may have worked to determine both the existence and the activity of the so-eluded-to holonomic substrate that had behaved as the so-stated substringular entity.  Due to general conditions such as the Heisenburg Principle and the Pauli-Exclusion Principle, such a general genus of extrapolatory-based detection is here to basically be mainly of a mathematical-based nature -- with our present-day modern technology.  Yet, when one is to understand the basic premises of as to how, when, where, and what a given general locus of proximal substringular entites is to behave over time, at a reasonably tightly secure locus of nature, then, it is more proportionabley viable to bear a condition of having a higher probability to be able to more accurately determine the so-mentioned conditionalities of as to the when, where, how, and what, the holonomic substrate that works to comprise any respective given arbitrary substringular entity had behaved -- in the manner that would work to help at better determining a more reliable extrapolation of the manner of activity of the said substringular phenomena, that could here be of a correlative physical scenario.  Since motion in the substringular -- for all practical purposes -- happens basically everywhere and all of the time in actual physical nature, any correlative respective set of cohomological indices is basically always going to be in some sort of motion or change, over any detectable time period in which one may be able to work to make any viable extrapolation as to the behavior of any Yakawa-based couplings of ghost-based indices.  This often holds true -- even if there are no spontaneous Gliossi-based interactions of discrete superstrings, that are to happen upon the topological stratum of the holonomic substrate of the so-eluded-to cohomologies -- for the reason of the ansantz-based fact that norm-state projections are basically constantly working to interact with the multiplicit assortment of ghost anomalies, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.