Euclidean/Clifford Delineation Of Second-Order Light-Cone-Gauge Eigenstates

 Those second-order light-cone-gauge eigenstates, that are here to directly appertain to a Noether-Based discrete quantum of energy, tend to have a greater probability, than those second-order light-cone-gauge eigenstates, that are directly associated with a discrete quantum of energy, that is instead, to work to bear the behavior of a tachyonic-related nature, of thereby working to bear a Euclidean delineation, in the mappable-tracing of its correlative respective Laplacian-Based sub-tension, that is here to be proximal local, in its existence of iterative placement, during a given arbitrary respective iteration of group-related instanton, as this is here to be eminently spatially distributed, in such a manner, in so as to be holomorphically mappable, over the course of such a general tense, of an inferred iteration of cohomological-related displacement, as individually taken, from in-between their directly associated Fadeev-Popov-Trace eigenstate, and, their directly associated respective superstring/counter string of discrete energy permittivity. It furthermore follows; That those second-order light-cone-gauge eigenstates, that are here to directly appertain to a tachyonic-based discrete quantum of energy, tend to have a greater probability, than those second-order light-cone-gauge eigenstates, that are directly associated with a discrete quantum of energy, that is instead, to work to bear the behavior of a Noether-Based nature, of thereby working to bear a Clifford delineation, in the mappable-tracing of its correlative respective Laplacian-Based sub-tension, that is here to be proximal local, in its existence of iterative placement, during a given arbitrary respective iteration of group-related instanton, as this is here to be eminently spatially distributed, in such a manner, in so as to be holomorphically mappable, over the course of such a general tense, of an inferred iteration of cohomological-related displacement, as individually taken, from in-between their directly associated Fadeev-Popov-Trace eigenstate, and, their directly associated respective superstring/counter string of discrete energy permittivity. TO BE CONTINUED! SINCERELY, SAMUEL.