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

A worm-hole works to bear a set of orbifold eigensets, that differentiate in a Fourier-based manner in so  as to being a group-associated metrical-gauge-based Hamiltonian operator -- in so as to act, as well, as one overall Hamiltonian operand -- that behaves as one overall general genus of what may here be considered as the equivalece of a field-based transmitter, that also works to pull those phenomenology of a holonomic substrate that are to initially enter the depth of the semi-anuulus-based region of the said worm-hole, through a controrsioning or in other words throgh a bending of space-time-fabric, that works to translate the so-eluded-to Gaussian indices of the said entering holonomic substrate, in a kinematic manner, that pulls these said individually taken spaces through a mappable Lagrangian-based path, in a kinematic manner, into what would here tend to end-up being a completely different spatial region as to the destination-based volumed region where the so-stated holonomic substrate of entry is to end-up exiting the said worm-hole at.  This happens, in so as to make a projection of a Njenhuis tense of a Doubolt cohomological-based mappable tracing -- as to the physical mapping of the trace of one entity that is to then be transferred from one physical locality to another -- to happen, via what would mainly be due to the Fourier-based differentiation of a Minkowski-based bending of space, that is to here convey a directly corresponding Gaussian set of physical indices that are to here be translated from one spot to another -- in what would tend to be a difference of the equivalence of practically zero terrestrial-based time.  The spatial complexity of the Njenhuis tensorism of such a spatial contorsioning, would tend to involve two more sets of complex roots per eigenpulse of the self-same given arbitrary worm-hole, than the Real Reimmanian-based translation for a p-field would otherwise tend to bear, when this is taken under its directly corresponding Ward-Caucy-based conditions (this being that of the respective given worm-hole) -- which would here tend to make such a general state of a worm-hole to act as the equivalence of a heuristically majorized Hilbert Space.  To Be Continued!  I will continue with the suspense later!  Sincerely, Samuel David Roach.