Thursday, November 14, 2013

Part Two of the 15th Session of Course 14 About Group Action

When one-dimensional superstrings of discrete energy permittivity map out a physical memory of the projection of the trajectory of the said one-dimensional string, without the contined existence of what here would have been those ghost anomaly-based indices that existed initially in the path of the kinematic-based differentiable Lagrangian -- that would here appertain to the tracing of the prior motion of the multiplicit eluded to one-dimensional superstrings of the eluded to directly prior extistent physical memory of the said superstrings.  This would then here mean that the ghost anomalies that had been formed by the inter-relative Gliossi contact, that would here exist between the said one-dimensional superstrings of discrete energy permittivity with the directly associated relatively forward-holomorphic-based norm-states that had been immediately scattered out of their initial basis of physical memory -- in a manner that is of an anharmonic manner, by the activity of relatively respective reverse-holomorphic-based norm-states.  So, if a superstring of both a relatively forward-time-based forward-holomorphic-based Hamiltonian operation moves through a given arbitrary Lagrangian -- in so as to harmonically scatter those positive-norm-states that were in its path, there would here, in this case, be negative-norm-states that had moved upon the initial said harmonically scattered arrangement of ghost anomalies that I had eluded to, in such a manner in so that the said ghost indices that had initially formed as a physical memory as to the directly prior motion and existence of the directly associated superstrings -- of which may here, in this given case scenario, be tentatively considered as appertaining to one-dimensional superstrings of discrete energy permittivity, in this given arbitrary case, form a Gliossi interaction with the Ward-Caucy bounds of the said ghost anomalies in an anharmonic genus of scatteriing.  This is to where the resultant Hamiltonian perturbative reaction would bear both a non-linear-based Clifford-based covariant basis of Yakawa -based topological sway -- that would form interactive Njenhuis singularities that work to pull and tug the initial arrangement of positive-norm-states from the Poincaire setting of the said ghost anomaly-based traceable mapping into a covariant-based codetermiable Njenhuis sway, this of which works to take the said perturbative scrambling of the indices of the said ghosts to be redistibuted and redelineated off of the relative local Real Reimmanian plane, with enough of an amplitude to where the resultant holonomic substrate of anharmaonically scattered norm-states may be pulled into dilatons and dilatinos that convert into gravitons and gravitinos.  This is due to a dual tense of both relatively infinite and relatively infinitessimal kinematic-based singularities that are interactive, yet, without canceling -- due to the dual  multiplicit binary directoral-based Lagrangian partials that are here involved with each other in an unborne tangency over time.

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