Monday, October 16, 2017

Conical lnternal Fields Of Light-Cone-Guage Eigenstates

Whenever any one given arbitrary first-ordered light-cone-gauge eigenstate, is here to be made Yukawa as a general genus of holonomic substrate, in-between any one respective given arbitrary Fadeev-Popov-Trace eigenstate and its correlative superstring of discrete energy permittivity, over the course of any one iteration of the Polyakov Action during BRST -- then, that tense of an immediate topological field, that is to here be made internal to the kinematic positioning of the said light-cone-gauge eigenstate -- is then here to be of a relatively conical nature in a hyperbolic-based manner, as the so-eluded-to discrete energy is to here be going through the so-inferred Lorentz-Four-Contraction, that is to be happening to the said quantum of energy.  The larger that the relative scalar amplitude of that Lorentz-Four-Contraction is, that is here to be happening to the said discrete energy quantum that is to here to be  occurring over the course of one specific instanton -- the less conical that the internal field will tend to be, of the topological interior of the kinematic stratum in which the so-eluded-to first-ordered light-cone-gauge eigenstate  will be of, in this said given arbitrary case.  Furthermore -- the smaller that the relative scalar amplitude of that Lorentz-Four-Contraction, that is here to be happening to the said discrete energy quantum that is here to be occurring over one discrete instanton -- the more conical that the internal field will tend to be, of the topological interior of the kinematic stratum in which the so-eluded-to first-ordered light-cone-gauge eigenstate will be of, in this given arbitrary case.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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