Thursday, June 12, 2014

An Addendum Before Starting Course 17, Part One

Did you ever wonder what happens to a "leg" of any given arbitrary eigenstate of the space-hole -- while the intrinsic physical points from a Real Reimmanian-Fock-String-Orientation is in a state of transition?  Let us first consider a certain given arbitrary two-dimesional superstring of discrete energy permittivity.  Directly to its forward-holomorphic side is a Fock-Space counterpart that ebbs the residue of certain initialized norm-state quantifies -- that works to form as a direct result of the delineation of the directly correlative ground-space.  The so-stated two-dimensional superstring is an approximation of a vibrating circular topological field that acts as a vibrating hoop of discrete energy.  The same goes with the correlative Fock-Space -- except, the said Fock-Space basically acts as an equal and opposite reaction to the directly associated ground space, that works to act in the opposite direction to the said ground-space.  This is not to be confused with the correlative Fadeev-Popov-Trace eigenstate, that is, instead, directly to the reverse-holomorphic side of the so-stated given arbitrary superstring.  The Fadeev-Popov-Trace eigenstate just mentioned acts as a discrete unit of energy impedance.  Also, a Fadeev-Popov-Trace is shaped, instead, as a topological holonomic substrate that consists of a Chi-shaped structure that is integrated, in a Laplacian manner, with a central figrure-eight structure, when one is Gliossi to the topological entity of the said Fadeev-Popov-Trace eigenstate at the Poincaire level. The counterpart of any given arbitrary Fadeev-Popov-Trace eigenstate is the operational indices of the correlative light-cone-gauge. The said two-dimensional string's intrinsic physical first-ordered point particles, that operate in so as to comprise the so-stated superstring, are compactified at half the maximum capacity -- in terms of what the maximum compactifiation of mini-string segmentation is possible in the region of the general topological field that is Gliossi to the locus of any given arbitrary first-ordered point particle of any given arbitrary superstring -- as taken at the relative Poincaire level.  The individual first-ordered point particles that work to comprise any given arbitrary superstring -- during the duration of any given arbitrary of group metric of BRST, only emit one mini-string segment that is level from the said specific superstring of discrete energy permittivity -- besides the mini-string segments that extend from the superstring towards both itself, the superstrings counterpart, and towards the superstring's correlative Fadeev-Popov-Trace eigenstate.  Yet, the holonomic substrate of the physical structure of any given arbitrary directly corresponding counterpart of a Real Reimmanian substringular entity will bear an offshoot of very many mini-string segments at the Gliossi topological extrapolation that would here be at the Poincaire level.  This is, although the compactification of the first-ordered point particles that work to comprise the individual "mers" of the so-stated superstring's counterpart are also at half the maximum compactification, than what is termed of as mini-string has the capacity of having -- when given the Ward-Neumman bounds of the Laplacian-based fractal and elastic modulae that is possible for the entity of the holonomic substrate of the composition of the described mini-string segmentation.  Again, mini-string is that general genus of entity that operates in so as to  function as the topological phenomena that both comes together in so as to form first-ordered point particles, and, it also is that holonomoic substrate that links both first-ordered point particles, superstrings, and other miscilaneous substringular phenomena -- so that topology is able to exist at all.
I will continue with the second part of this addendum later!  To Be Continued!  Sam Roach.

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