As to Covariant Light-Cone-Gauge Quantization

Let us say that one had a large quantity of superstrings in a set specific general relative locus, that either had an abelian light-cone-gauge topology (Kaluza-Klein) or a non-abelian light-cone-gauge topology (Yang-Milles).  Let us say say that the just-eluded-to basis of general region in which either respective set of superstrings -- that would here exist in orbifolds -- existed in a  homogeneous substringular neighborhood, in terms of the format or genus of the abelian-based geometry that the first-ordered correlative light-cone-gauge eigenstates of each of the two respective given arbitrary sets of superstrings worked to bear.  Now, imagine the interaction of the core-field-densities of each of the so-stated and so-eluded to respective first-ordered light-cone-gauge eigenstates and second-ordered light-cone-gauge eigenstates, that work to comprise both respective given arbitrary case scenarios -- working to form a correlative eigenbasis of kinematic differential association over time, that has both an interdependent and an independent inter-play of field-indices that inter-relates the said light-cone-gauge eigenstates, as both a basis of holonomic substrate and as a basis of local field-generation. Such an integrable eigenbasis of field-interplay may then be described of as a covariant light-cone-gauge quantization -- since each light-cone-gauge eigenstate of each respective individual scenario acts as both itself and as the whole group at the same time.  I will continue with the suspense later!  To Be Continued!  Sam.