Sunday, February 25, 2018

Vibrations Of Bosonic Superstrings During BRST

Let us initially consider a mass-bearing bosonic superstring of discrete energy permittivity -- that is to be undergoing the Polyakov Action, over an individual eigenmetric of an increment of BRST.  As such a said string is to be going through the Polyakov Action, via a scalar amplitude that is to the inverse of its directly corresponding Lorentz-Four-Contraction -- the directly corresponding superstring of such a given case, is to here to tend to be mildly vibrating harmonically at the locus at which it is to be basically existing at a standstill at, over the course of one individual iteration of instanton.  As such a said bosonic superstring is here to be mildly vibrating at its Relatively Laplacian-based locus -- at which point in duration, such a superstring is to be undergoing the Polyakov Action to the inverse of its Lorentz-Four-Contraction -- the activity of the interaction of the topological stratum of the so-stated superstring, with those surrounding norm-state-projections that it is coming into a Gliosis-related contact with, is to work to form a tightly-knit cohomological stratum of a Hamiltonian operand that is delineated at the core-field-density, that is proximal local to the specific unique cite of the said topological stratum of the respective bosonic superstring of this given arbitrary case.  This tightly-knit cohomological stratum, -- that is proximal to the core-field-density of the holonomic substrate of the respective string -- may here be called an eigenstate of a Gliosis-Sherk-Olive cohomology.  The manner of working to consider such a cohomological eigenstate as a relatively temporal phenomenology, may then be called a Gliosis-Sherk-Olive ghost.
 I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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