When a topological entity vibrates harmonically in all of the Ward-Caucy-based physical dimensions that are given by the physical boundaries that are directly associated with the initially said entity, and the so-stated physical topological-based entity is hermitian in both a Lagrangian-based manner and in a metrically-based manner -- while yet also only vibrating in the relative Real Reimmanian Plane, then, this works to define the said physical topological-based entity as being Yau-Exact, under the so-eluded-to duration that works to elude to the directly affiliated group metric. Hermitian topological entities, particularly Yau-Exact ones, act in such a manner in so as to obey Chan-Patton rules -- in so long as the just stated general format of entity is moving in so as to move in accordance with a Noether-based flow, over a directly corroborative group metric. When a topological entity, that acts in so as to obey the general premis of Chan-Patton rules, bears a topological-based sway, then, the just stated "sway" moves in so as to also be Yau-Exact -- unless there are alterior viablely affectual Njenhuis tensors that act upon the holonomic substrate of the initially mentioned topological entity. Njenhuis tensors kinematically differentiate off of the directly affiliated relative Real Reimmanian Plane, although these so-stated Njenhuis tensors will still work to allow a topological entity -- that these act upon in a Yakawa manner -- to vibrate harmonically per iteration of group related instanton, and thus bear a correlative attribute of working to obey Chan-Patton rules. Any non-kinematic-based perturbation that physically bears an unsmooth Lagrangian-based topology is not completely hermitian, and thus, does not directly refer to the correlative existence of Yau-Exact substringular phenomenology in this case.
I will continue with the suspense later! To Be Continued!!! Sincerely, Sam Roach.
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