Part One of the Third Session of Course 16

If you will, I am going to start with the simple.  Superstrings have fields.  Superstrings kinematically differentiate in the substringular in such a manner in so that these are detectable as these are extrapolated in the manner that these are in the globally distinguishable.  When superstrings spatially differentiate in a given arbitrary trajectory that these are projected in, through the spectrum of the Ultimon, after a successive series of an iteration of instantons, the said given arbitrary superstrings work to form what may be logically deduced as world-sheets -- whose physical memory of such may be thought of as ghost anomalies.  World-Sheets often allow the first-ordered point particles -- that may often here be point commutators -- to flow within the substringular neighborhood of the directly corresponding Sterling Approximations.  This genus of extrapolation is as to the locus of where the correlative superstrings had been over the course of an integration of the Lagrangian-based extrapolation -- in such a manner in so that the harmonic scattering of the so-stated point commutators, that are in the relatively direct path of the so-stated superstrings of discrete energy, forms, to a degree, some sort of  "anatomical" mappable tracing as to the potential whereabouts and activity of the directly corresponding superstrings of discrete energy that are here under question.  The mapping of ghost anomalies tends to pull the directly corresponding point commutators, that are moved by the so-stated harmonic scattering, inward at the outer edges of the related tracing.  This happens here, while yet working to pull the directly corresponding point commutators that are moved by the so-stated harmonic scattering outward at the relatively more interior general format of locus as to those regions that ghost anomaly-based indices are formed.  This happens over the correlative sequential series of instantons in which the motion of superstrings are being delineated and redelineated into the Gliossi Ward Neumman bounds of the said point commutators.  Such a scattering -- when happening in the same time-wise directoral format of path-wise Lagrangian genus of directoral sway -- is said to happen in what may be termed of as the forward-holomorphic directoral Hamiltonian path operand, when in relation to the directly corresponding distribution format of superstrings that are not perturbated from a constant metrical direction.  So, when a superstring is reversed from what was its initial delineation of time flow, its directoral Hamiltonian path operand is said to be altered into what may be termed of as the relatively reverse-holomorphic direction.  The forward-holomorphic direction may be arbitarily chosen as the relative left and/or counterclockwise direction, and, the reverse-homorphic direction may be arbitrarily chosen as the relative right and/or clockwise direction.  Phenomena that are worked upon in the substringular at the Poincaire level are considered to be substrates.  Entities that act upon their substringular region at the Poincaire level are holonomes.  So, a holonomic substrate is a substringular phenomena that both acts upon and is also acted upon by another substringular entity at the relative Poincaire level.  I will continue with the suspense later!  Sam Roach.