Part Three of the 14th Session Of Course 14 About Group Action

Superstrings that are translocated from one spot to a totally different covariant setting kinematically differentiate spatially in a directoral set per iteration of a given arbitrary group metric -- from one relative format of setting to the next relative format of setting, over the duration of the initially mentioned group metric that I had mentioned.  This said group metric involves the said given arbitrary set of superstrings.  Superstrings often open or close in a relatively static covariant-based setting that operates in so as to work to define a tense of both a radial, orbital, and/or a transversal kinematic function of differentiation -- that is initiated at an initial locus, where the superstrings that are to either open or close may here begin to vibrate in such a manner that works to begin a projection of metrical gauge that operates in so as to bring in local zero-norm projections that function as a genus of holonomic substrate.  Such a substrate here works to pull in those corresponding topological sways that do the actual activity of respectively either opening or closing the given arbitrary superstrings, that will here either convert from a bosonic form of a superstring to a fermionic form of a superstring, or, will convert from a fermionic form of a superstring to a bosonic form of a superstring -- when in terms of the tracing of the corresponding loop amplitudes of such eluded to superstrings.  With Inverse-Fujikawa Couplings, the activity of the reversal of a relative condition of an initial given arbitary forward holomorphic basis of activity functions to form a Wick Action eigenstate, in an indirect manner, in so as to operate an inverse of a unitary Clifford Expansion that acts upon a relatively local zero-norm-state projection in so as to form a net inverse of a binary Clifford Expansion -- in so as to act upon the holonomic substrate of the binding-cite of a given arbitrary closed string, in such a manner to where the binding cite that initially worked here to keep the eluded to bosonic string as a closed-loop of integrated first-ordered point particles, may be opened at the apex point of where the said binary inverse expansion of the inverse Fujikawa Coupling is Gliossi to the point of contact -- as to where the said zero-norm-state projection integrates with the binding cite of the said closed-loop of substringular phenomenology at the Poincaire field density of the eluded to locus of inter-binding of that so stated closed-loop.  At the general region that is localized at the opposite holomorphic substringular local neighborhood from where the apex of the said binary structure eluded to, of the said inverse Fujikawa Coupling, works to loosen the binding cite of the said closed-loop phenomenology in a Gliossi manner at the Poincaire level of the exterialized twining that had initially bound the closed-loop together in the first place, there is an exterialized obtuse basis of a binary structure that here involves an inverse Clifford Expansion that acts as a "V-shape" strutural operator that is projection-wise open at both ends at in the process of opening the closed-loop of this scenario -- while yet being an apex at a further reverse-holomorphic delineation of norm-state distribution, as the said closed-loop (superstring that is here bosonic) in to be opened.  As the "V-shape" of binary inverse Clifford projection tugs in its relative holomorphic Hamiltonian gauge-metric delineatory topological sway -- over the course of the then current group instanton -- while yet compensating for the then inter-active Polyakov Action eigenmetric and the simultaneous inter-active Bette Action eigenmetric, -- the closed-loop is opened in so as to then operate as a discrete unit of plain kinetic energy.  I will continue with the suspense later!  Sincerely, Sam Roach.