Part Two As To Magnetic Flux Density

So, each wave that is of one given arbitrary phenomenology of magnetic flux density, is an eigenstate of each of the other of such waves.  The magnetic flux density of each individually taken tori-sector-range of electrodynamic energy, would then act as an individual eigenmatrix -- if the light-related cohomological-based tracing is here to be conformally invariant upon the entire oscillation of point particles of the first-order, -- that are of the Ward-Cauchy bounds of the so-eluded-to Lagrangian-related trace, in so as to work to allow for one to be able to make a Laplacian-related tracing, that is piecewise continuous along the circuit of the entire physical memory as to both the how, the when, and the where that the flux density that is given, had just differentiated in, in a Fourier-related manner.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

As An Aside: 

The matrix of a magnetic flux density eigenstate, could potentially work to involve multiple tori-sector-ranges on the substringular level. Anyways, when an eigenstate of a magnetic flux density holonomy, is to be operationally delocalized, then, the Ward-Cauchy-Related conditions, of which are here to be eminently associated, with the delineated distribution of its initially proximal local Majorana-Weyl-Invariant cohomology-related singularity, will often have the general tendency of being attributably nullified. With such inferred mass-bearing Hamiltonian Operators, this just eluded-to process of operational delocalization, will often tend to occur within the general region of the majorized plane, of the directly associated GSO cohomology-related field, of the inferred eminently corroborative proximal local Calabi-Yau Manifold, of which is here to be behaving as such an earlier stated tense of a mass-bearing Hamiltonian Operator. Each of such individually taken desingularizations, is initiated via the gauge-metric-related action, of a kinematically-based operational holonomic tensor, of which is to incur its eminent engagement upon such a stated Calabi-Yau Manifold, in so as to tend to work to effect the corroborative general physical attribute, of the net light-cone-gauge eigenstate, of which is here to be imperatively associated, with the workings of the magnetic flux density eigenstate, that is here to be eminently associated, with such an earlier implied set, of multiple tori-sector-ranges, Again; In this. particular case scenario, what I mean by "tori-sector-ranges," are here to be corroborative to the workings, of a respective set of multiple layers of reality, that are here to still be of the same universal setting.