Thursday, May 22, 2014

Substringular Reiterations

May we look at substringular reiterations as a convergent sequence of slices in the space-time fabric -- whose bases are exact and linear differential associations of physical point particles, the convergent series of wave reiteration being the summed wave interconnections which work to differentiate all neighboring semi-groups as a covariant platitude -- in which the superstrings that code for a given globally distinguishable homotopy remain unchanged, when relative to the directly corresponding parity attributions, these attributions of which are delineated by the overall eluded-to system of phenomenology?  Well, this mean that the so-stated superstrings may change, yet, does this mean that the directly associated particular supersymmetry will here work to cause the net apprehendable condition of the said superstrings to then remain unchanged?  Any given arbitrary superstring of discrete energy permittivity will iterate, during group instanton, at a slice locant.  It works to orientate with its directly covariant Fock Space counterpart.  Once that the first-ordered point particle neighborhoods of the affiliated superstring are working to exchange the output of their wave-based indices, a quaternion is formed among all of the superstrings of discrete energy permittivity of the directly corresponding tori-sector-range.  This leads to the reiteration of group instanton.  After group instanton, the given superstring that I have eluded to will bear a relative dissociation -- scattering as a mildly cohesive set of first-ordered point particles that are more annharmonically delineated than these are during the directly prior conditions that existed at instanton.  The mappable tracing of where and how the superstring had behaved during the directly previous iteration of instanton will then be imbued upon the "turf'" of the substringular as a set of ghost-based indices.  Once that the so-stated first-ordered point particles that appertain to an indistinguishably different superstring, that is here moving in a relatively conformally invariant setting, have moved along the Ultimon -- in so as to be brought to virtually the same spot at which these had iterated during the prior stage of group instanton, the so-stated first-ordered point particles that had worked to form the so-eluded to superstring of discrete energy permittivity will then work to form a superstring that will be distributed at the ensuing iteration of istanton, since such a superstring is here obeying Noether Flow.  This would here mean that the so-stated superstring that is reformated to reiterate at an adjacent delineation from where it had previously iterated, will be distributed at the ensuing instanton at the same general substringular neighborhood, and thus, at a very similar basis of slice locant.  This process will then continue, following a variation of parameters localization -- in which the coefficients that would here work to describe the specific delineation of the first-ordered point particles that comprised the formation of the directly corresponding superstring, will integrate in such a manner in so that the individual Poincaire-based cites -- as to the bringing together of the so-stated point particles -- will bear a Hamiltonian-based eigenset that will work to determine the basis of that group attribution that will most fascillitate the Gaussian eigenbasis of the wholeistic set of antiderivatives that would here work to form the foundation of the so-stated ensuing local substringular delineation of superstrings that are to come together at the said given arbitrary cite.

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