When one is to have a mass-bearing cohesive set of discrete energy quanta, that is here to be behaving in a tachyon-related manner, — the more spatial dimensions that such a said set of discrete energy quanta is to be exhibiting, over a set duration of time, the more acute that the angling of its directly corresponding Nijenhuis impedance will tend to be, that is here to be imparted upon the correlative gauge-action, of the proximal local angular momentum field eigenstate, that is related to the co-differentiable permeability of the said mass-bearing cohesive set of discrete energy quanta. For example: Let us consider two different cases of such inferred sets of mass-bearing discrete energy quanta. One of such sets is to be of a three spatial dimensional nature, while the other of such sets is to be of a six spatial dimensional nature. Both of such sets of discrete energy quanta, are here to be behaving as tachyons; as well, as that both of such sets of discrete energy quanta, are otherwise to be behaving in basically the same general manner of a covariant spatial translation — over a discrete quantum of relativistic time, — as taken over the vantage-point of a central coni-point, that is here to be translated through space, over an evenly-gauged Hamiltonian eigen-metric. The just mentioned mass-bearing set of discrete energy quanta, that is here to be exhibiting the nature of behaving as a superstring-related entity, involving six spatial dimensions, will consequently tend to bear a smaller subtended angle of a Nijenhuis impedance, that is here to be imparted upon the correlative gauge-action, of the proximal local angular momentum field eigenstate, that is related to the co-differentiable permeability of the said mass- bearing cohesive set of discrete energy quanta. (1989). To Be Continued! Sincerely, Samuel David Roach.
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