Friday, January 22, 2016

About Antiholomorphic Divergences

Let us here consider two different orbifold eigensets, that are initially moving in a kinematic manner -- with what may be here viewed of as a supplemental line, that is not of a Wilson-based linearity, that works to inter-bind the topological index of the physical entity of their mutual condition of holonomic substrate.  Let us now say that the two so-stated orbifold eigensets have been differentiating in a Fourier-based manner, for a relatively preminent duration of time -- to where these may both be considered here to be moving in the same general directoral-based genus of holomorphicity -- over the so-eluded-to eminent sequential series of group-related instantons.  Let us now say that there is a group-inhibitor index of one general given arbitrary nature -- that acts upon the two individually taken substringular entities of holonomic substrate of Hamiltonian operation -- that acts in so as to work to prohibit the continued covariant Fourier-based activity, that is of the motion of the two so-stated orbifold eigensets that are here initially flushly moving in a common general direction, with a Ward-supplemental subtension that is to be here drawn-out between the two said eigensets of superstrings, in a Laplacian-based manner.  Let us now say that the Fourier-based operation of the Hamiltonian-based delineation of the functional index of the so-stated group-inhibitor, would here work to cause a relatively sudden Njenhuis-based Ward-supplemental motion -- that would here be enacted upon both of the said orbifold eigensets of this respective given arbitrary case -- to where the two so-eluded-to sets of superstrings will then be moving with the opposite general index of delineatory operation, over the directly ensuing sequential series of group-related instantons.  This immenent and swift perturbation in the immediate field density -- that would then exist between the two said orbifold eigensets would then work to form a hyperbolic tangential-based covariant field of divergence -- that would be exhibited here by a Cevita interaction that would be operational between the two Clifford-based Hamiltonian field operators (the two orbifolds of which would here be the two said operators).  The so-eluded-to perturbation of divergence would then be an annharmonic perturbation -- that would form both Lagrangian-based Chern-Simons singularities and metrical-based Chern-Simons singularities -- of which would then work to form an antiholomorphc Kahler condition, of which would then work to set-on an ensuing Kahler-Metric.
I will continue with the suspense later!  To Be Continued!  Samuel David Roach.

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