Part Two About Electrons And Cohomological Generation

Let us initially consider an electron -- that is here to be accelerated through a given arbitrary conductive cable, as a metrical-gauge-related Hamiltonian operator, that is to be propagated through its respective Hamiltonian operand -- along the trajectory of its correlative Lagrangian-based path, over an evenly-gauged Hamiltonian eigenmetric.  Let us next consider, that the conductance of the material that is here to work to comprise the general magnetism, in which the said electron of this respective case is to be tugged into an electrical flow -- by the translation of the activity of its valence bands -- is to increase in its scalar magnitude, over the Fourier Transformation in which the electron is to go through the process of being transferred through the said respective Hamiltonian operand, in a manner that is Lagrangian-wise hermitian over time.  Since the said electron is here to be accelerated -- the pulse of that just mentioned electron will be amplified in a Ward-Cauchy-related manner, along the course of the propagation of the said electron across its correlative valence bands.  This will then work to indicate, that this will then involve a set of metrical-based Chern-Simons singularities.  As this is to occur, let's say that things happen, to where the acceleration of the said electron is to be maintained in its scalar translation over time, -- in spite of the added conductivity.  This will then work to cause an increase in the generation of its charge over time, -- and thus, this will then work to cause an increase in its cohomological generation over time.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.