More As To The General Interactions Related To Cohomology

The general condition, as to the interactions of point commutators with superstrings -- consequently works to form the general condition, -- as to the multiplicit stratum of cohomology.  Point commutators exist as a set of one or more first-order point particles, that are generally interconnected, in one manner or another, by that holonomic substrate of mini-stringular segmentation, in which the multiplicit homotopic field (which is, as well, to be comprised of by a general tense of mini-stringular segmentation), that is here to be external to the core-field-density of such said point commutators, is here to tend to typically bear a relatively euclidean approach, in its convergence upon the topological surface of the here holonomic substrate, of such inferred point particle eigenstates.  Superstrings exist as a set of one or more first-order point particles, that are generally interconnected, in one manner or another, by that holonomic substrate of mini-stringular segmentation, in which the multiplicit homotopic field (which is, as well, to be comprised of by a general tense of mini-stringular segmentation), that is here to be external to the core-field-density of such said point particles, is here to tend to typically bear a relatively hyperbolic approach, in its convergence upon the topological surface of the here holonomic substrate of such inferred point particle eigenstates.  Point commutators tend to bear more of a "jointal" tense of topological stratum; whereas, superstrings tend to bear more of a "smooth-curved" tense of topological stratum.  Consequently -- the general condition,  as taken at a Ward-Cauchy-related level, -- as to the interactions of relatively "jointal" phenomenology in the substringular -- that are here to work to bear an externalized field, that is to bear a relatively euclidean approach of those directly corresponding mini-stringular eigenstates, that are here to converge upon such mentioned "jointal" phenomenology, -- upon the topological stratum of relatively "smooth-curved" phenomenology in the substringular -- that are here to work to bear an externalized field, that is to bear a relatively hyperbolic approach of those directly corresponding mini-stringular eigenstates, that are here to converge upon such mentioned "smooth-curved" phenomenology -- consequently works to form the general condition, -- as to the multiplicit stratum of cohomology.  I will continue with the suspense later!  To Be Continued! Samuel David Roach.