So, what's on the other side of a dimensional entity that has no physical pretense at that general localization? :
Let's take into consideration a two-dimensional superstring of discrete energy permittivity (as an oversimplification), that propagates the presence of the holonomic substrate of a three-dimensional world-sheet. Since the correlative string is only two-dimensional, it needs the local presence of positive-neutral-ground-states -- to act as entities, that are here to work to help form partial dimensional slits -- that are here to interact with those directly corresponding point commutators, -- in order to work to form a tense of a three-dimensional-related conformal invariance, that is to act "on both sides" of the correlative superstring of discrete energy permittivity that has been eluded-to here. The corresponding Nijenhuis "fringes" of the directly pertinent partition-based discrepancies, are what may be thought of here as a fractal of a "Van-Der-Waals force", that is here to work to form a tense of a field, of what may be termed of here as being a general type of a conformal-repulsion-locality. As a Laplacian Transform, as to what may be mapped-out in-between the earlier said Nijenhuis "fringes" and the immediately adjacent superstrings, -- there is the eminent presence of the directly pertinent anti-differentiable cohomology-related globalizations -- whose Ward-Cauchy-based behavior may be defined in part, by the extrapolation of those correlative substringular entities, that are to here to display the correlative behavior that act as arc-hyperbolic-trigonometric functions, whose side-bearing couplings, will then consequently orientate the respective correlative mers of norm-based projections, in such a manner, in so as to help to guide what is here to be the present relationship between the associated Real-based entities and the directly corresponding Nijenhuis entities. This happens, in order to help to work-out the Ward-Cauchy interdependence -- that is here to exist between discrete energy and its resultant physical memory. This just stated orientation is to happen, via the commutation of a discrete world-sheet that is quantized, in part, into the overall world-sheet of its directly corresponding orbifold eigenset. This said overall world-sheet, when in relation to the topology of a substringular membrane that is of a mass-bearing nature -- will often in reality, tend to instead to be of such a metric, that is here to be of a Calabi-Yau nature. To Be Continued! Sincerely, Samuel David Roach.
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