The more dimensional compactification that any given arbitrary superstring of discrete energy permittivity is to tend to bear, the less topological sway that its directly corresponding second-order light-cone-gauge eigenstates will tend to exhibit, -- consequently, the less dimensional compactification that any given arbitrary superstring of discrete energy permittivity is to tend to bear, the more topological sway that its directly corresponding second-order light-cone-gauge eigenstates will then tend to exhibit. Furthermore; the more dimensional compactification that any given arbitrary superstring of discrete energy permittivity is to tend to bear, the less that its directly corresponding discrete energy permeability eigenstates will tend to exhibit a tense of spatial perturbation. Consequently; the less dimensional compactification that any given arbitrary superstring of discrete energy permittivity tends to bear, the more that its directly corresponding discrete energy permeability eigenstates will then tend to bear a tense of spatial perturbation. Next; it consequently takes less of a perturbation of topological sway, for a lower spatial dimensional phenomenon to permeate through space, -- whereas; it takes more of a perturbation of topological sway, for a higher spatial dimensional phenomenon to permeate through space. To Be Continued! Sincerely, Sam Roach.
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