When a Fadeev-Popov-Trace eigenstate is to work to maintain its same manner of behavior, when in relation to the motion of electromagnetic energy, over a directly corresponding sequential series of group-related instantons, then, the directly corresponding light-cone-gauge eigenstate, that such a said Fadeev-Popov-Trace eigenstate is here to be holomorphically acting upon, over the earlier mentioned respective sequential series of group-related instantons, will consequently tend to have a relatively heigtened probability, of also working to maintain its same manner of behavior, when in its relation to the motion of electromagnetic energy. When a light-cone-gauge eigenstates is to maintain its same manner of behavior, over a correlative sequential series of group-related instantons, it may consequently be said, that the directly corresponding discrete quantum of energy, that is here to be most associated with the kinematic exhibition of such a said light-cone-gauge eigenstate, is here to be "gauge-invariant." Therefore; when a Fadeev-Popov-Trace eigenstate is to work to maintain its name manner of behavior, when in relation to the motion of electromagnetic energy, one may then say, that the directly corresponding discrete quantum of energy, that is here to be most directly associated with the said Fadeev-Popov-Trace eigenstate of such a respective given arbitrary case, is here to tend to be "gauge-invariant." Sincerely, SAMUEL ROACH.
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