Monday, June 6, 2016

A Preliminary To What's Coming Up

Let us initially consider a given arbitrary orbifold eigenset -- that is, in this respective case, comprised of a group of many discrete quanta of energy.  This would then work to determine the condition, that this respective orbifold eigenset would then consist of both several superstrings of discrete energy permittivity, their correlative superstringular counterparts, their correlative Fadeev-Popov-Trace eigenstates, and their correlative light-cone-gauge eigenstates.  Since an orbifold eigenset is the discrete quantum of energy that is directly affiliated with one set of superstrings, that operate in so as to work to perform one specific function -- all of the discrete quanta of energy that work to comprise the so-stated orbifold eigenset, are to be traveling at basically the exact same velocity, -- when this is to be taken in relation to both the existence and the motion of electromagnetic energy.  This would then mean, that all of the superstrings of discrete energy permittivity and their correlative superstringular counterparts -- that would here to then work to comprise any one specific respective given arbitrary orbifold eigenset, will tend to bear basically an identical scalar magnitude or scalar amplitude of their directly pertinent Lorentz-Four-Contraction.  This would then mean, that all of the superstrings of discrete energy permittivity and their correlative superstringular counterparts -- that would here to then work to comprise any one specific respective given arbitrary orbifold eigenset, will tend to bear basically an identical scalar magnitude or scalar amplitude of their directly pertinent Polyakov Action-based substringular-based effect, over the course of any one given arbitrary set of iteration of BRST in which such an extrapolation may be considered at, at one specific instant under consideration.

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