Saturday, July 18, 2015

Part Two of Session Four of Course 19 -- The Klein Bottle and Orbifold Differentiation

The interior of the cohomological-based pattern that is formed by any respective given arbitrary Klein Bottle --is like a limited contorted "toroid" that contains both forward-holomormphic and reverse-holomorphic-based norm-states.  These multivarious norm-states of which tend to differentiate in a Fourier-based manner that is of a relatively harmonic manner, over time.  Yet, when the interaction of the norm-states, that exist from within the Ward-Neumman boundaries of the interior of the holonomic substrate of any respective given arbitrary Klein Bottle eigenstate, act in so as to differentiate kinematically in a relatively rigorous  annharmonic manner over time, the cohomological-based pattern that is formed by both the existence and the activity of the so-stated given arbitrary Klein Bottle eigenstate, eventually is perturbated into a Rayleigh-based scattering of those norm-state indices that had previously existed within the Ward-Caucy bounds of the said Kliein Bottle eigenstate.  This just mentioned general genus of activity of which may often cause the composition of the specific respective given arbitrary Klein Bottle eigenstate to be indistinguishably replaced, via those immediately surrounding eigenindices that may here work to both antiderivate the previous Klein Bottle eigenstate, while yet re-constructing a newly established Klein Bottle-based construction -- in a manner that works to bear a tendency of an indistinguishable difference.  This just-eluded-to recycling-based tendency of a "worn-out" Klein Bottle eigenstate into a newly established so-stated Klein Bottle eigenstate, works to conform to the overall tendency -- that is directly affiliated with the recycling of norm-state-projections, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

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