As is with the Schwinger Indices that are directly affiliated with one-dimensional superstrings of discrete energy permittivity, those vibrational oscillations that act as one whole -- that are formed by those first-ordered light-cone-gauge eigenstates that directly appertain to one two-dimensional superstrings, may be termed of as one first-ordered Schwinger Index. Furthermore, the vibrational oscillations of one second-ordered light-cone-gauge eigenstate as one whole, that directly appertain to one respective given arbitrary two-dimensional superstring of discrete energy permittivity, may be termed of as one second-ordered Schwinger Index. Also, the individual vibrational oscillation that is formed by one "pluck" of one "plucking" of that which is formed at one specific locus on the general topological surface of one second-ordered light-cone-gauge eigenstate -- that directly appertains to one two-dimensional superstring -- may be termed of as one third-ordered Schwinger Index. Such just eluded-to second-ordered light-cone-gauge eigenstates, that stem off from what is here one Fadeev-Popov-Trace eigenstate -- toward what is here its directly appertaining two-dimensional superstring of discrete energy permittivity -- bears two general adjacent topological origins, that are per what would be each source of such origins -- when appertaining to the stemming at the general locus of Fadeev-Popov-Trace eigenstate, that are initially derived in a Gliossi-based manner at the Poincaire level on the relative forward-holomorphic directoral positioning of the just-eluded-to Fadeev-Popov-Trace eigenstate. Such eigenstates of the light-cone-gauge are here to bear a discrete wave-functional-based impedance -- that are interconnected with the here directly appertaining two-dimensional superstring of discrete energy permittivity of this case. The general format of the localization of the general quality of pitch that is to be formed of the condition of the holonomic substrate of the directly associated third-ordered Schwinger Indices, has similarities with that of which directly appertains to that which involves any given arbitrary one-dimensional superstring of discrete energy permittivity, yet, with the second-ordered light-cone-gauge eigenstates of the here latter case that would involve, instead, any given arbitrary two-dimensional superstring of discrete energy permittivity that is here delineating mini-string segmentation or core-field-density -- that bears the Laplacian-based alteration in relative pitch, when going from the "0 degree mark" of the so-stated respective two-dimensional string -- that is here stemming inward at the relative Poincaire level of connection at the so-eluded-to superstring, in a counterclockwise tense, that goes, in a Laplacian-based manner, back around to completion near the "2pi mark" -- when mapping-out such a pattern of the said second-ordered light-cone-gauge eigenstates, as "looking" in the vantage-point of the here relatively forward-holomorphic direction of the so-related said two-dimensional string.
To Be Continued! I will continue with the suspense later! Sam.
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