Part Three of the Third Session of Course 16

The norm-state indices that work to comprise the given arbitrary ghost anomaly one may consider here is both a specific case of a physical phenomenon that works upon its immediate environment, and also a specific case of a physical phenomenon that is worked upon by its immediate environment.  This would make the norm-state indices that here integrate to form the so-stated ghost anomaly index both a holonomy and a substrate that is Yakawa to its physical environment of substringular neighborhood -- in a Gliossi manner at the Poincaire level, that atones a bearing at the genus of substringular region that is tantamount to the here adjoining integration of superstrings of discrete energy permittivity -- that work to form a locus of the immediate locus of directly interacting orbifold eigensets.  This is here a situation in which the eluded to orbifold eigensets are behaving in a kinematic environment that is prone to vear in the relative forward-holomormphic directoral wave-tug/wave-pull over time.  So, as the so-stated given arbitrary orbifold eigensets of the said scenario are pulled into the genearal directoral Hamiltonian operand -- that bears a path of Lagrangian that is unimetrical over the course of a successive series of group instantons, in such a manner in so that the mappable tracing of their physical memories works form a cohomology-based build-up that effects the concertive directly adjacent orbifolds -- that bear a local import of adjacent operations that perform different discrete functions that act within the premises of a local substringular neighborhood, both the activity of the eluded to orbifolds and the activity of the eluded to adjacent orbifolds forms a respective set of kinematic delineation that act as a holonomy.  This being of the initially mentioned orbifold eigenset -- that is acted upon as a substrate -- due to the so-stated activity that the said adjacent orbifold eigensets bear upon the initially stated orbifold eigensets. This may work to form an assymetric chirality of a consideration as to what the given arbitrary holonomy and substrate are, when the given arbitrary holonomy and substrate are acting via an eluded to Hamiltonian Fourier Transformation that bears a kinematic-based mappable tracing that is extrapolated respectivitly inward.  (The holomorphically dot-product-wise condition versus the holomorphically cross-product-wise condition, in this case.)  The basis of the here eluded to interaction is actually meant as the interaction of the physical memories of the so-stated orbifold eigenset.
P.S.:  Actually, what I meant by "holonomy" is "holonome."  A holonomy is the condition of a physical phenomenon being a holonome.  I will continue with the suspense later!  Sincerely, Sam Roach.