When one given arbitrary source of Ward-Cauchy-related phenomenology, is either to add and/or to detract -- from the energy of any one external given arbitrary Hamiltonian Operator, that is here to exist in time and space, -- then, this initially said given arbitrary source of Ward-Cauchy-related phenomenology, may then be said to bear a Yukawa Coupling upon the holonomic substrate, that is of the so-stated respective external given arbitrary Hamiltonian Operator, over a respective given arbitrary evenly-gauged Hamiltonian eigenmetric. Two or more different Ward-Cauchy-related sources, that are to bear an eminent effect upon one another -- are then said to be Yukawa towards each other, in one manner or another.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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