The higher that the scalar amplitude is to be, that is of the correlative Majorana-Weyl-Invariant-Mode -- the more Yau-Exact will be the tendency of the directly corresponding orbifold eigensets, that will here work to then be comprised of by the overall set of mass-bearing discrete energy quanta, to where this will then operate in so as to work to comprise a mass, that is here to be directly correlative to the respective given arbitrary Ward-Cauchy-related case scenario of this given genus of situation. The more Yau-Exact that a set of mass-bearing discrete quanta of energy will tend to be, -- the more acutely that the so-eluded-to set of discrete energy quanta will then tend to generate as much cohomology as it will tend to degenerate over time. This will then mean, that -- the more Yau-Exact that a set of orbifold eigensets will tend to behave as portraying -- the more piece-wise continuous that such a set of discrete energy quanta that operate in so as to perform one common function, will tend to generate as much cohomology as it will tend to degenerate over time. Therefore, any set of orbifold eigensets, that operate in so as to be able to bear a relatively high resonant vibration -- will tend to acutely generate as much cohomology as it will degenerate -- as a piece-wise continuous Hamiltonian operator -- as well as that such a Hamiltonian operator, will tend to bear a relatively high scalar amplitude of a Majorna-Weyl-Invariant-Mode, over any one proscribed evenly-gauged Hamiltonian eigenmetric. I will continue with the suspense later! To Be Continued!
Sincerely, Samuel David Roach.
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