More About Fujikawa Couplings

A two-dimensional superstring is formed when a one-dimensional superstring hermitianly bends via the Green Function to go from being a vibrating strand to being a vibrating hoop of discrete energy permittivity. When a one-dimensional superstring closes to form the discussed two-dimensional superstring, the relative "top" and "bottom" parts of the associated one-dimensional superstring loop their ends around each other in a holonomically homogeneous spatial manner 120 times while the given superstringular phenomenon has an equally added mini-string, or substringular field, holonomic gauge-action in terms of added condensed oscillation The added condensed oscillation that is brought to the closing one-dimensional superstring via the networking of Cassimer Invariance is equal to the minute decrease in the circumference of the associated two-dimensional superstring due to the tying of the two ends of the given one-dimensional superstring that is converting into a two-dimensional superstring via the hermitian bending and lacing together that may be partially described by the Green Function. The lacing together of the two ends of the associated one-dimensional superstring is due to the condition that the given hermitian bending bears a conipoint and a coniaxial at the center of the given one-dimensional superstring, and cos 120 degrees = .5, and that, at 120 degrees both sine and cosine are positive. So, the mini-string at both ends of the associated one-dimensional superstring in a hyperbollicaly tangent manner wrap themselves around each other for 120 looped Laplacian metrical delineations. This is also due to the fact that a Yang-Mills light-cone-gauge topological field is sinusoidal for a Laplacian delineation of 120 complete waves when during the core of BRST in-between a Fadeev-Popov-Trace and its associated superstring. When a two-dimensional superstring, the potential increase in wave homotopy is compensated by the holonomic decrease in the Hodge Index of the phenomenology of the given superstring via the networking of Cassimer Invariance in the locus of the associated substringular neighborhood. This aspect of Cassimer Invariance is due to the equal and opposite reaction in the opposite direction of the local Chern Simmons perturbations in terms of the Clifford expansion, and to the contraction of the kinematic differentiation of the local Campbell and Hausendorf projections that act upon the conicenter and coniaxial of the hermitian activity of the opening two-dimensional superstring. This is due to the local Calabi-Calabi, Calabi-Wilson-Gordan, and the local Calabi-Yau interactions that are defined by electrodynamic scattering that happens in the locus of the region of the given superstring that is changing morphology.