Friday, December 4, 2015

Some Knowledge As To Light-Cone-Gauge Topologies

Let us here consider a light-cone-gauge eigenstate that is of a Kaluza-Klein topology.  We are considering what is here happening during BRST.  As the said light-cone-gauge eigenstate is here undergoing a Clifford Expansion during the Polyakov Action -- basically, the intrinsic function as to the scalar magnitude of the amount of mini-stringular segmentation that is being fed into the so-stated light-cone-gauge eigenstate of such a case -- is of the nature of only working to bear just enough core-field-density to cover the so-eluded-to euler expansion of the stretching-out of the so-stated light-cone-gauge eigenstate, during the so-stated respective given arbitrary iteration of BRST.  Yet, as the correlative gauge-bosons that work to "pluck" the correlative second-order light-cone-gauge eigenstates are in a Gliosis-based contact with the correlative topology of the said second-order eigenstates -- the activity of such a direct tangency will here work to cause the Yukawa implementation of there then being just enough "slack" in the compactification of that twined mini-stringular segmentation, that would here act as the holonomic substrate of the so-stated second-order light-cone-gauge eigenstates -- in so that the so-eluded-to fabric of the said Kaluza-Klein topology will then be able to bear the necessary peaks and troughs in its locus of spatial disturbance, in so that the said  eigenstates of the wave functionality of discrete energy impedance will be able to act in a manner that may be described of as a "pluck" -- even though a Kaluza-Klein light-cone-gauge topology tends to bear a supplemental Lagrangian wave-tug/wave-pull in its Lagrangian eigenbase during BRST (this is when not including the imbued conditions that are implied by the conditionality of a Yukawa-Based Clifford Expansion).  The situation is similar, but a little bit different -- with the case of a Yang-Mills light-cone-gauge topology.  I will continue with the suspense later!  To Be Continued! Sam Roach.

No comments: