More About the Higgs Action

The Higgs Action moves through a Minkowski plane that bears a Fourier tensed Schotky Construction of non-trivially isomorphic group-metrics that involve Ward Conditions of bimorphological distribution indices due to the wobble of the Klein Bottle, that allows the associated superstrings that are to enter the physical Neumman parameters of the said Klein Bottle to obtain (reobtain) the permittivity that these said superstrings are to receive so that these superstrings may remain as the discrete energy that these are to be so that energy and reality may continue to exist. When considering the wobble of the Schotky Construction to be a Njenhuis Tensor, the given planar group-action that I described is a group integrand of the whole Schotky Interaction involved is to be considered as one Real Reimmanian integrable surface, then the Ward Conditions of the said Schotky Interaction is said to bear a Hilbert integrable surface. The Higgs Action itself, although much smaller than the whole Schotky Construction, is Diracly differentiable through the described Fourier Transformation in a majorized Hilbert Space as compared to the Real Reimmanian Surface that the Schotky Interactioin as a whole, is differentiable in only a Minkowski Plane that bears a Njenhuis wobble. When considering the raising of the Klein Bottle to be in the norm to holomorphic direction, the dot product of this directoralization acts as a Minkowki holonomity that is binarily Lagrangian. Each individual group metric directoralization of the described binary Lagrangian acts as a unitary Lagrangian. When considering the Njenhuis indices of the Real Reimmanian perturbation of the norm Fourier Translation of the said Schotky Interaction, as the Klein Bottle is transferred through the holomorphic directoralization in a norm manner relative to the raising of the Klein Bottle, the angling of the Higgs Action is a unitary Hamiltonian operation that integrates between the said binary Lagrangian Fourier Transformation of the Schotky Construction as a multiplicit Hamiltonian Operator. The subsequent antiholomorphic, and norm to antiholomorphic, redirectoralizations of the Schotky Interaction that proceed after this Schotky Interaction kinematically differentiate first norm to holomorphically, then holomorphically, through the associated binary Lagrangian Plane, acts with a non-trivially isomorphic redistribution of the angling of the Higgs Action by an initially Minkowski antiholomorphically realigning of forty-five, unperturbated in vibrational index, degrees, allows for the Klein Bottle to then move to the relative right and then to the relative downward to complete the oscillation of the said Schotky Interaction. When the Schotky Interaction moves from the relative "upward" to the relative left, the Higgs Action initially has a reallignment of its angling by a holomorphically Minkowski, unperturbated in vibrational index, degrees of 22.5. The interconnection between the Higgs Action and the Klein Bottle exists due to the "velcro-like" interactions of the mini-string (substringular field) of the Higgs Action and the mini-string (substringular field) of the bottom of the Klein Bottle's surface.