More About Yakawa Couplings

The most common Yakawa couplings are the Fujikawa and the Reverse Fujikawa couplings. The next most common couplings that are Yakawa are the cohomological bindings of M-State shells that either appertain to one-dimensional superstings' integrative fields over a relatively small group metric Laplacian which can be described as a tightly knit Fourier Series integration that defines an open string and its field over a conformal set of iterations OR two-dimensional superstrings' integrative fields over a relatively small group metric Laplacian which can be described as tightly knit Fourier Series integration that defines a closed string and its field over a conformal set of iterations. Let's say that two conformal fields of either one-dimensional superstrings or of two-dimensional superstrings that iterate taken individually in a relatively tight location so as to define either two thin Hilbert figure-eight morphologies or two toroidal morphologies taken respectively that bind at a locus that is defined by the conipoint and coniaxial norm conditions of both subspaces in conjunction with the interaction of either two norm Campbell Projections, or, two norm Hausendorf projections, that are brought together via the propagatorial norm conditions of the neighboring Schwinger Indices which form a pertinent Gaussian gauge-metric and directoralization, because the local Schwinger Indices are formed by the local vibrations of first and second-ordered light-cone-gauge eigenstates that are from either the same core region of the associated superstrings, or from proximally regional superstrings that bear the same Planck phenomena normalcy as projected in a euclidean directoralization relative to one another, (The given Hodge Projection defines the same tense of substringular impedance orphoganation.), the associated substringular M-Fields, when completely unperturbated and therefore also Noether here, when covariant upon a supplementally norm tensorism, will bind together at the designated locus or loci until these are scattered upon or made tachyonic or acted upon by a supplementally norm Chern Simmons holonomic singularity in a spontaneous manner. Such a binding is accomplished by the hyperbollically tangent tying of intermingling mini-string or substringular field integration that involve an interactive commingling due to the sub-impedance and sub-permittivity eigenstates that sway toward each other in the given manner due to the fractoring of the Gaussian Ward conditions that are present. Such a tying happens one binding cite at a time per BRST instanton as the whole cohomology is eventually bound over a relatively small group metric. In-Between each instanton, the superstrings go thru ultimon flow, and are encoded to tie and rety more and more over the course of relatively few iterations that involve Real time. Once the cohomological unit is tied and obtains a Chan-Patton or Clifford Caucy Ward conditionality, the associated structure is stable under a tense of conformal invariance, until either it is scattered upon by a holonome or by a state of Majorana-Weyl invariant tensorism to where it becomes at least partially tachyonic, or is interfered with by a Chern-Simmons singularity or set of singularities that are directorally distributed by a propagated holomorphic or antiholomorphic holonome that goes from being a Njenhuis tensor to being a tensor that is displayed on the Real Reimmanian plane.