Part Three of the Eleventh Session of Course 16

A Njenhuis Klein-Gordan mechanism is an interaction that happens when transversel, radial, and/or spin-orbital tensors that are off of the Real Reimmanian Plane interact with a given arbitrary superstring of discrete energy permittivity at a tangent of normalcy that is orphoganal to the extra dimensionality of the Imaginary-based subspaces that are directly correlative to any pertainent given arbitrary case scenario.  For instance, let us say that a given arbitrary superstring has just become non-orientable.  The so-stated superstring is not able to be orientable during both the directly corresponding Bette Action eigenstate and the directly corresponding Regge Action eigenstate.  Under the just stated conditions, the said given arbitrary superstring will become tachyonic over the course of the ensuing iteration of group instanton that the so-stated superstring will be flowing into -- for over the course of one or more instantons. Since the superstring is to now become at least temporarily tachyonic in this case scenario, the ensuing one or more eigenmetrics of the Regge Action eigenstates that will be directly involved with the interaction of the said given arbitrary superstring with its envronment over a sequential series of instantons will be initially scattered annharmonically at the initial stage of such a perturbation of the so-stated superstring -- due to the said superstring that is here being discussed going from a Noether-based flow into a tahchyonic-based flow.  Those tensors that act upon the said superstring -- in the form of norm-state projections -- in so as to allow for the superstring to be able to succeed at its needed path at becoming tachyonic, will bear a subtended directoral basis that is Njenhuis in nature.  When the said superstring that is here becoming at least temporarily tachyonic is also undergoing a change in norm conditions -- known of as a Gaussian Transformation -- then, the activity of that substringular scattering that is involved with the eluded-to genus of the added condition of the Kaeler Metric being introduced into the activity of the here tachyonic superstring will be of an annharmonic nature. This annharmonic nature is involved with the here local intrusion of a Klein Bottle eigenstate, along with a geometrical-based need for a perturbation of that indistinguishably different Regge Action eigenstate that will need to "fidget" in order to accomodate the altered genus -- as to the format of how the directly associated superstring will move over the ensuing increment of time that is here correlative.  It is when a tachyonic condition that is directly involved with a superstring that is also entering into an eigenstate of the Kaeler Metric that is when there are both norm-state projections that are Njenhuis that interact upon the correlative superstring, as well as that there will here be a "fidgeting" of the directly corresponding indistinguishably different Regge Action eigenstate that is to take the "brunt" of the motion of the here newly developed tachyonic nature of the so-stated superstring that has just left from being of a Noether-based nature.  Yet, when a superstring remains, instead, of a Noether-based nature, then, when a Kaeler-Metric is introduced to a superstring that is to undergo a Gaussian Transformation, the directly corresponding scattering of the correlative Regge Action eigenstate is instead of a harmonic nature, since, here, the general nature of the flow of the so-stated superstring is, in this case, not perturbated out of this here said condition.  This scattering is directly related to the nature of the flow of the correlative superstring as it is projected through a Regge Slope eigenstate.  If the kinematic projection through such a slope is hermitian, then, it is being harmonically scattered.  Yet, if the kinematic projection through such a slope is Chern-Simmons in its basic nature, then, it is being annharmonically scattered.  I will continue with the suspense later!  Sincerely, Sam Roach.