Norm-State-Projection Eigensets

Let us initially consider a set of norm-states, that work to perform one set of functional operation.  Such a Hamiltonian operator that is to here to consist of a group of cohesive norm-states, may here be called a norm-state-projection.  Furthermore, a set of norm-state-projections that operate as a group, in so as to work to perform one specific general function, may be called a norm-state-projection eigenset.  Let us next consider, in general, the array of gauge-metrics, that are here to be most directly pertinent to those sub-Fourier-based kinematic activities, that take place from a scope that takes place in less than one discrete increment of time.  None of such gauge-metrics are to here to be able to go an exact integer number into one discrete increment of instanton, to where, although any duration that is of a viable import to any living being, will tend to bear a discrete number of instantons, yet, any of such so-eluded-to gauge metrics that are here of a sub-Fourier-based tense, will tend to never bear an exact integer number of those said gauge-metrical-based durations into any viable time, to where these are here to occur at a level that takes place in less than one discrete increment of time.  Let's now consider a superstring, as it is eminent in its Yukawa-based inter-relationship with the Kahler-Metric, in a Gliosis-based manner.  Let us next consider the four general stages that such a directly affiliated discrete quantum of energy is to be involved with, over the course of one correlative individual instanton.  There will tend to be one norm-state-projection eigenset -- that is to be involved with that decompactification that is involved with the Polyakov Action.  There will tend, as well, to be one norm-state-projection eigenset -- that is to be involved with the main part of BRST, during the remainder of that said iteration of the respective proximal local Polyakov Action egienstate.  There will also tend to be one norm-state-projection eigenset -- that is to be directly associated with the eminent Yukawa-based inter-relation, that the said discrete quantum of energy is to bear with the holonomic substrate of the correlative Klein Bottle eigenstate, in a Gliosis-based manner, with the correlative increment of the Kahler-Metric -- right after the respective so-eluded-to iteration of the proximal local increment of BRST.  And, there will also tend to be one norm-state-projection eigenset -- that is to be directly involved with the directly associated discrete quantum of energy, that has been in the process of being in a Gliosis-based relationship to the Kahler-Metric, as the said discrete quantum of energy is to be going through the ensuing correlative Regge Action eigenstate -- at the relative ending part of instanton.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.