Let us consider two different sets of orbifold eigensets -- that are to interact here, in a manner that is to be both covariant, codeterminable, and codifferentiable, -- as the two said given arbitrary orbifold eigensets are to act as two tenses of energy, that are to interact in an interdependent manner, over a relatively transient duration of time. Let us next consider one of the two mentioned orbifold eigensets as being of a vector-based bundle, whereas, the other of the two mentioned orbifold eigensets is as being of a tensor-based bundle. The orbifold eigenset that is to work to bear a vector-based bundle of cohomology, is to act in so as to exist in a tense of superconformal invariance -- to where the so-eluded-to cohomology that is thus formed by the Fourier-related differentiation of the said orbifold eigenset -- is to be of a Rham-based cohomology. The orbifold eigenset that is to work to bear a tensoric-based bundle of cohomology, is to act in so as to exist in a tense of bearing a relative lack of superconformal invariance -- to where the so-eluded-to cohomology that is thus formed by the Fourier-related differntiation of the said orbifold eigenset, is to be of a Doubolt cohomology. Such a dual state of the resultant activity that is here to happen, due to the interaction of the two said orbifold eigensets -- as these two sets of superstrings are to traverse through their correlative Fourier-related transforms -- may then be said to bear a tense of tending to bear a state of behaving in manner that is partially Yau-Exact, over time. I will continue with the suspense later! To Be Continued!
Sincerely, Samuel David Roach.
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