Unitized Coupling

If two different distinct Hamiltonian Operators, that are to act as monopoles that are here to be of the same number of spatial dimensions, as these so-eluded-to eigenstates, that are of a discrete quantum bearing of divvied-out energy-- that are here to generate the same absolute value of a Lagrangian-related energy, at a given arbitrary conipoint in space and time -- even though these two distinct Hamiltonian Operators, are to bear their respective correlative motion, in a manner that is of a covariant antiholomorphic means of interaction, over an evenly-gauged Hamiltonian eigenmetric, -- to where there is then to be the condition that these two said Hamiltonian Operators, if coupled in such a manner as this would tend to infer, -- would then tend to act, in so as to consequently work to help to form some sort of inter-relationship of those charges or fractals of charges, that are delineated to the electrostatic or fractal of electrostatic Ward-Cauchy-related conditions, that are of such a case scenario, in so as to work to help to cause charged particles to orbit and spin, in the manner in which these do over time.  This is, in part, because -- like I have mentioned before, such a so-eluded-to Coupling is tantamount to, (-i)*i, which is equal to one (1).   This just described tense of activity --thence works to involve unitization, -- and when eigenstates act in so as to be unitized, this will tend to move phenomena into a state or condition of optimum rest. Sincerely Samuel David Roach.