Let us here, consider the motion of a given arbitrary mass-bearing superstring of discrete energy permittivity -- that is of an electron. The individually taken mass-bearing superstrings of an electron, exist in what may be termed of as a d-field. A d-field, over any respective given arbitrary Fourier Transformation, exists in a minimum of six spatial dimensions, plus time. The mass-bearing superstrings of an electron tend to be Yau-Exact, to where such individually taken superstrings of discrete energy permittivity, are to here be an eigenstate of a Calabi-Yau manifold. Over the course of any respective given arbitrary iteration of BRST, that involves the individually taken mass-bearing superstring of an electron, the drive of the angular momentum of the topological stratum of the holonomic substrate of such eigenstates of a Calabi-Yau manifold, are to here be of the general genus of the directorial-based Hamiltonian operand, -- of what amounts to as being of the mean Lagrangian path, that may be subtended from being basically right in-between the direction that is in the path in which the correlative annulus of that superstring's core-field-density is pointing in, &, the direction that the topological substrate of the external fringes of the core-field-density of the said superstring is pointing in. This general genus of the motion of a mass-bearing superstring, along such a so-stated mean Lagrangian path, works to help at forming a harmonic tendency of a homotopic-based torsion, of which is to here help at working to help cause the respective torsional eigenindices of such a general genus of discrete energy permittivity, to tend to bear a hermitian wave-tug, that is again, of a Yau-Exact nature.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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