Monday, July 10, 2017

Electrons And Holomorphic Direction

Let us initially consider an electron.  Furthermore, let us consider the mass-bearing superstrings of an electron, -- as such Calabi-Yau-based superstrings of discrete energy permittivity are to exist here, in so as to work to come together as part of the said electron, -- to where the electron, as a unit, is to act here as an orbifold eigenset.  Let us next consider an individual mass-bearing superstring of discrete energy permittivity, that works to help at forming the said electron, to where that electron of this case is here to act as an orbifold eigenset.  The Calabi-Yau field of such mass-bearing states, is to here to bear a proximal local shell-like toroidal-shaped cohomological-based surface, at the Poincare level to its external core-field-density.  The so-eluded-to Calabi-Yau eigenstate, that is here to act as a mass-bearing eigenindex, that is of the said electron, is to theoretically act in such a manner -- in so as to work to bear a tendency of tugging to bear its relatively forward-holomorphic direction in the mean Lagrangian path, that is to exist right in-between both the directoral-based delineation of the angular momentum that is in the direction of its edge, as well as also existing right in-between the directoral-based delineation of the angular momentum that is in the direction of its anuulus.  Next, consider the integration of all of the so-eluded-to mass-bearing superstrings of discrete energy permittivity, that are to theoretically comprise the "rest mass" of the so-stated electron.  Each of such Calabi-Yau-based strings is to tend to behave in such a way, to where these are to heuristically lean-in towards the multiplicit-based earlier mentioned mean Lagrangian path -- that lies in-between the multiplicit edge and the multiplicit anuulus of the so-eluded-to Gliosis-Sherk-Olive (GSO) toroidal-based cohomological-based field.  The resultant of such a tendency, is to then to work in part, to help influence, along with the main influences of its charge and its magnetic field in relation to the general protonic field that it is attracted to, -- the Ward-Cauchy-based conditions that are related to the general manner of the spin-orbital momentum of the said electron, over time.  I will discuss more later, -- the more prominent influences of charge upon the magnetic field of sub-atomic particles, -- which happens in so as to work more at helping at producing the spin-orbital momentum of an electron.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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