Part Four Of Light-Cone-Gauge Quantization And Gravity

When a Rham-based cohomology is to work to bear the spontaneous Ward-Caucy-based conditions of any respective given arbitrary case of perturbation, via an antiholomorphic Kahler condition, then, thereupon as to the respective and viable alteration in the initial relative holomorphic direction of the correlative cohomological flow of those eigenindices -- that had just worked to form the initial mappable-tracing of the discrete physical memory of the trajectory, of what would here be the proximal local immediate effect of the motion of the so-eluded-to Fourier differentiable orbifold eigenset, that was initially of the kinematic transference of a Rham-based cohomology, is to now be of the kinematic transference of a Doubolt-based cohomology.  Now, if the directly corresponding gravitational field that is Yukawa to the holomorphic flow of an initially Rham cohomology, is to bear an isomorphic core-field-density from right before the so-eluded-to Lagrangian-based Chern-Simons singularity had happened, that had helped to work to reverse what was here to be the relative forward-holomorphic direction, -- to right after the just mentoined genus of perturbation that had happened to the propagation of the Lagrangian-based eigenindices, that were involved with the respective initial Rham-based cohomology that had then transformed into a Doubolt cohomology, then, those gravitational-based eigenindices -- that had acted as the respective Schwinger-Indices that had acted as the respective gravity waves, will as well, tend to bear at least some sort of alteration in the Lagrangian-based propagation of the quantific wave-modulae, that is to here be directly related to a perturbation in the directoral-based translation of the cohomological-based mappable-tracing of the correlative Rarita Structure-based eigenstates, that are to here be proximal local to the cite of the here rebounding metrical-gauge-based Hamiltonian operator, that had been in the form of an orbifold eigenset that had basically made a reversal in the general direction of the flow of its correlative Hamiltonian operand.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.