Part One of Session Three of Course 19 -- The Klein Bottle and Orbifold Differentiation

Did you ever wonder how any given arbitrary Klein Bottle eigenstate -- as being put together in the manner of a Schotky Construction -- could be physically maintained in the substringular, without bearing any significant substringular perturbation acting upon it, in such a manner in so that a Njenhuis-based Klein-Gordan-Mechanism could spontaneously here be working upon it in a viabley perturbative manner, over time?  The Klein Bottle -- as being put together as I have described in my blog, as in the manner of the Schotky Construction -- differentiates in a Fourier-based manner per each succeeding iteration of group-related instanton.  Such a so-mentioned Fourier-based differentiation happens in both a transversel-based manner, a radial-based manner, and also in a spin-orbital-based manner -- via those Ward-based coniaxials, of which here work to define the spatial structure of any respective given arbitrary Klein Bottle eigenstate, over a successive series of instantons in which the said eigenstate is moving through what is known of as the Kaeler Metric.  In so long as the correlative discrete energy that is involved here, is only of a Noether-based flow over a successive series of group-related instantons, both those superstrings of discrete energy permittivity and also those Fadeev-Popov-Trace eigenstates of discrete energy impedance, that enter any respective specific given arbitrary Klein Bottle eigenstate, through each succeeding iteration of the directly corresponding Kaeler Metric -- in which such quantum eigenstates of discrete energy are here re-attaining their fractals of discrete respective permittivity and impedance, are pulled into the here directly associated given arbitrary Klein Bottle, in a methodical-based manner -- in so as to undergo the re-attainment of all of their fractals of discrete energy that these need, in order to be fulfilled as being the respective discrete energy permittivity and discrete energy impedance, after the succession of the directly corresponding individually taken eigenmetric of the said proximal Kaeler Metric.  This activity of the Kaeler Metric, as well, works to cause both the wave-functionabiltiy of discrete energy permittivity as is in counterstrings -- and also causing the wave-functionabililty of discrete energy impedance as in light-cone-gauge eigenstates, to re-attain their discrete fractals of their intrinsic entity -- in so that both the particle-based nature and the wave-based nature of discrete energy -- may remain as a continual existence of energy, over time.
Later, I will discuss as to how the so-eluded-to motion of any respective given arbitrary Klein Bottle eigenstate works to cause such a said re-attainment.
To Be Continued!  I will continue with the suspense later! Sincerely, Sam Roach.