The Next Part Of Session 12 Of Course 19 -- The Klein Bottle And Orbifold Differentiation

When it comes to the presence of a one-dimensional superstring of discrete energy permittivity -- as the given arbitrary string wobbles here slightly from its initial relative Njenhuis-norm-to-holomorphic positional side to its relative Njenhuis-norm-to-reverse-holomorphic positional side, during a respective iteration of BRST, it will as well have a tendency of bearing a smooth-curved and semi-sinusoidal topological sway -- that is perturbated from an initial disturbance of space that is drawn into the holomorphic direction in such a manner that is positional-wise towards its counterpart, in so as to then be perturbated from a disturbance of space that is drawn into the relative reverse-holomorphic direction in such a manner that is positional-wise away from its counterpart.  As what I have just mentioned is happening -- the directly corresponding counterpart of the said given arbitrary open-loop that acts here as a one-dimensional superstring of discrete energy permittivity, will here bear a covariance -- that is both codeterminable and codifferentiable -- in so as to work to act in the sub-Fourier-based "direction," that happens in so as to bear the capacity of forming the conditions that are necessary, in so as to cause there to be a homeomorphic field that is to be formed during the directly respective iteration of BRST -- to where this field, of which is then to be formed here, is to then exist in a semi-Laplacian-based manner, in-between the so-stated superstring and its counterpart.  As all of this is happening -- the superstring of such a said case is to then be decompactifying to the inverse scalar amplitude, as to its directly associated Lorentz-Four-Contraction that is to be considered here.  Here -- the so-eluded-to Clifford Expansion that is to here happen to the directly corresponding light-cone-gauge eigenstate that is directly associated with the kinematic activity of a one-dimensional superstring of discrete energy permittivity,  is to then bear both Real Reimmanian and Njenhuis torsional indices, -- that are to then act upon the thence formed Schwinger-Indices of such a given respective case,  in so as to here work to help to form a tense of what works to comprise part of the delineatory eigenbase of the directly corresponding gravity-waves -- that are to here be propagated by the so-eluded-to activity of the so-stated light-cone-gauge eigenstates, that are of the said given arbitrary respective one-dimensional superstring that is of such a so-stated case
To Be Continued!  I will continue with the suspense later!  Sincerely, Samuel David Roach.