Part Two Of The Seventeenth Session Of Course Ten

As I was discussing, as the discrete units of the directorals that here correspond to the prior eluded tensors are considered over an arbitrarily given Fourier condition that inter-relates the related superstrings that work to comprise the assoicated said traits, residue that is here delineated over a relatively brief metric works to transversally and vibrationally commute a certain degree of "tingling" that lubricates the kinematic association that covariantly binds the two said traits.  The coupling that happens over the course of the prior mentioned brief metric is an arbitrary given example of a Yakawa coupling that here involves indices that works to allow a variance that translates a tense of Weyl covariance that tends to conform to the corresponding Ward Caucy conditions that work to define the physical boundaries of the said traits in all of the Fourier-based derivatives that involve the overall dimensional scope in which the superstrings that work to define the said traits exist in.  The corresponding Cassimer Invariance that will happen here -- if the related Yang-Mills supersymmetry is to here take hold -- will then attain a spontaneous metric that here involves a parity and dual chirality that will work to even out the loci of the settings over the duration in which each associated encodement is quantized.  Yet, if the corresponding Yang-Mills supersymmetry that we are to consider were to not be attained here, then the associated holomorphic residue will flow over the duration of the brief metric that inter-relates this second possible scenario -- after each reiteration that would thence happen between the homotopic indices of the said traits.  The prior mentioned metrical condition would cause the metaphorical-based "fluid" flow that I had initially mentioned in my last post to become perturbated in terms of its displacement over a tightly-knit Fourier Transformation in which the traits mentioned earlier will, in this case, not be as superconformally invariant as these otherwise would be.  Under the conditions of such a perturbation of what would otherwise be more delineatorial-based stable, the inter-related fractal of magnetic coupling that could be extrapolated here would involve an increase in magnitude as well as an increase in terms of the corresponding fractal of charge.  The "fluid" would then snap and recoil in terms of its delineation over the course of the prior mentioned tightly-knit Fourier Transform.  If the associated holomorphic index that would then exist under the directly prior mentioned conditions were to now increase in terms of action intensity over the course of the kinematics that would involve the covariance of the related eigenstates that are comprised in part by the superstrings that work to form the prior mentioned said traits, then the recoiled sections of "amorphous" quantitative topology may -- after the coure of the proper sequence of iterations and the proper series of wave discharge -- slip in terms of its positioning of local distribution as a folded manifold to where it would go back into a connection that would here exist in-between the hyperstates of the said traits in so that the exterior counterpoise that would here be physically present, as well as the corresponding hypnostates of the related holonomic ground-states, would then differentiate through time in a singularized manner in so that the given phenomena would then act as a theoretical homotopical-based eigenbasis.  Such an eigenbasis would here be partially codifferentiable in terms of the inter-relation of the covariance of the two said traits over a related Fourier Transformation in such a manner so that the related activity would work to draw in the quanta of a re-convergent norm projection. I feel that I am burning the candle at both ends.  I will continue into course 11 when my sanity lets me.  I will continue with the suspence later!  Sincerely, Sam Roach.