Orbifolds work to form many of the basic cohomological settings. World-Sheets always form a type of cohomological setting which depends upon the given contour that the given arbitrary world-sheet propagates in, over time. An orbifold has a topology as well -- this being the Gliossi-based contour of the core-field-density of the so-stated orbifolds, at the Poincaire level. Orbifolds often exists as D-Branes. D-Branes are manifolds of superstrings that work here to comprise electrons (mainly), in so as to act as operators, that work to perform a specific function in the substringular. D-Branes are substringular manifolds that exist in a minimum of six spatial dimensions plus time, over any given arbitrary duration -- in which one is able to extrapolate any given arbitrary corresponding Fourier Transformation. Such a manifold often exists as a Calabi-Yau manifold, since electrons bear mass, and, any mass that is struck by a photon acts -- over that group metric in which such a mass is struck at its core-field density in a Gliossi manner by a discrete unit of electromagnetic energy -- as a manifold, that would then be described of as a Calabi-Yau manifold. Orbifolds, if these are basically of a Majorana-Weyl nature, bear at least one Njenhuis tensor -- in order to allow its magnetism to actually exist. This is because substringular phenomena, that are of the general size of the nucleus or smaller, exist in a minimum of four spatial dimensions plus time, in any directly corresponding Fourier Transformation -- in which such phenomena exist in, and, when one includes the existence of more than three general formats of spatial dimensions plus time, then, one is dealing -- in one manner or another -- with at least some Njenhuis tensors, that are then here inter-mingling with the correlative Real Reimmanian tensors that would be pertainent here over any given arbitrary discrete time period that could be applicable here.
I will continue with the suspense later! To Be Continued! Sincerely, Sam Roach.
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