Monday, July 24, 2017

Lorentz Invariance

Let us consider one given arbitrary orbifold eigenset -- that is to here to be undergoing a respective proximal local relative state of Majorana-Weyl-Invariance.  Such an orbifold eigenset is to here to be existent under a tense of conformal invariance, that, let us here presume -- is to here to be translated via a Fourier-based Transformation, that is to here to be moving, at least transiently, at a relatively constant rate, over time.  At the Poincare level to the Gliosis-based topology of the external shell of such a said orbifold eigenset -- one may say that such an eigenset, as an eigenstate, may at least be exhibiting some sort of a transient tense of a state of Lorentz Invariance.  Next -- let us consider what is to here to be going on at the Poincare level to the Gliosis-based topology of those individually taken superstrings of discrete energy permittivity, that are to here to work to comprise the overall discrete energy quantum of the so-stated orbifold eigenset -- over that gauged group-metric, in which the said orbifold eigenset is, in and of itself, to be at least transiently Lorentz Invariant. Since such individually taken superstrings of discrete energy permittivity are to constantly to be moving the scalar magnitude of either both the Planck Length and/or the Planck Radius, per each succeeding iteration of group-related instanton -- the so-stated individually taken respective strings are to constantly be perturbating in their relative rate of Fourier-related Transform -- when this is taken in a general relation to both the existence and the motion of electromagnetic energy, per each succeeding so-stated iteration of group-related instanton.  Therefore -- at the Poincare level to the Gliosis-based topology of the holonomic substrate of any individually taken superstrings of discrete energy permittivity, -- such discrete increments of energy quanta are not to act here as being Lorentz Invariant, as such eigenindices that work here in so as to help at comprising the said orbifold eigenset, are to here to act as metrical-gauge-based Hamiltonian operators, that work together as a group, in so as to perform that specific respective given arbitrary function, that its so-eluded-to reverse-fractal-based orbifold eigenset is to operate in so as to do, as a Ward-Cauchy-based eigenstate, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

No comments: