The field density of a substringular field is the locus of region where the mini-string that most directly subtends from a given arbitrary superstring is so filled with topological holonomic Hodge-substrate that it is impossible -- for all practical purposes -- for another superstring to intersect that density of mini-string that forms the phenomenological entity of the said field density of the given initially so stated superstring unless there is a Gliossi-based cohomological interconnection that binds the two here mentioned superstrings. Such a field density is two-dimensionally-based in relation to one-dimensional superstrings, and, such a field density is three-dimensionally-based in relation to two-dimensional superstrings. A cohomology is the touch-based binding of topologically-based entities. Cohomologies may be either in refference to: the binding of superstrings, the binding of first-ordered-point-particles, the binding of mini-string, or, for that matter, the binding of any phenomena that involves a topological holonomic entitiy. Cohomologies may often be in refference to world-sheets. World-Sheets that form a Ward-linear delineation are named Rham cohomologies, while world-sheets that form singularities in terms of the associated Laplacian-Based changes in norm-translation are named Doubolt cohomologies. Cohomologies, in general, reffer to a Gliossi-Based form of binding via a touch-based coupling that allows more of a direct inter-relation between different substringular phenomena. I will go back to the third part of session two later. You have a phenonomenal day!
Sincerely, Sam Roach.
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