A Tad Bit More as to Some Stuff As To Schwinger Indices

With one-dimensionanl superstrings, the second-ordered light-cone-gauge eigenstates go from starting from the relative right of the reverse-norm-to holomorphic end of the Fadeev-Popov-Trace eigenstate -- when one takes the vantage-point of consideration in the relative forward-holomorphic direction from the so-stated Fadeev-Popov-Trace eigenstate --, to the here considered relative left of the reverse-norm-to-holomorphic end of the same so-stated Fadeev-Popov-Trace eigenstate, again, when one takes the vantage-point of the consideration that is in the relative forward-holomorphic direction from the same so-stated Fadeev-Popov-Trace eigenstate, -- to the next so-eluded-to second-ordered light-cone-gauge eigenstate stemming from the center of the same so-stated Fadeev-Popov-Trace eigenstates, to the conditionality of the next two here considered second-ordered light-cone-gauge eigenstates respectively stemming from the relative right-based norm-to-holomorphic positions up to the relatiev left-based norm-to-holomorphic positions -- again, this being in consideration as to when going in a vantage-point that is in the relative forward-holomorphic direction, as is when going from the so-stated Fadeev-Popov-Trace eigenstate towards the directly corresponding one-dimensional superstring of this respective given arbitrary case.
Next, I will explain a little bit as to the nature of the Schwinger Indices that directly appertain to the correlative two-dimensional superstrings of any given arbitrary case.  To Be Continued!  Sam.