Let us initially consider one given arbitrary orbifold eigenset, that is to here be basically pushed, just soely by the force of gravity, in this respective given arbitrary case -- of which is to here be moving through a discrete unitary Lagrangian, through which the said eigenset is to be translated through its directly corresponding Hamiltonian operand -- as one discrete metrical-gauge-based Hamiltonian operand, via the group-metrical constraint of a discrete set of a sequential series of group-related instantons. Let us next, consider that the directly correlative set of gauge-bosons -- of which are here to work, in so as to "pluck" the directly corresponding second-ordered light-cone-gauge eigenstates, in so as to work to form Schwinger-Indices that are to act as the holonomic substrate of gravity waves -- are to act in such an overall directoral-based manner, in so as to work to form one overall resultant genus of a holomorphic-based topological sway -- over the so-eluded-to set time constraint, that is of the said sequential series of group-related instantons, via which the resultant overall tense of those integrative Schwinger-Indices, that are to thence form by the said "plucking" of the so-stated light-cone-gauge eigenstates by the so-stated gauge-bosons, are to then form one resultant tense of a gravitational-based push, of which is to help at working to move the said orbifold eigenset into what I have so-eluded-to as its relative forward-holomorphic direction, that is of such a respective given arbitrary case scenario. Let us next say that the overall resultant directoral-based holomorphicity, that is to here be directly corresponding to the topological sway of those said gauge-bosons, that are to here be working in so as to "pluck" the said light-cone-gauge eigenstates -- is to reverse in the overall genus of its resultant direction, over an ensuing sequential series of group-related instantons. Such a reversal in the holomorphicity of the "plucking" of such light-cone-gauge eigenstates, will then often tend to work to reverse the general overall resultant holomorphicity of the flow of the resultant formed Schwinger-Indices. Such a reversal in the holomorphic wave-tug of these correlative Schwinger-Indices, may then often work to reverse the direction -- of what would here be an otherwise relatively ineffectual pulsation of a Hamiltonian-based operator -- to where this will often work to reverse the holomorphic direction of the here discussed overall so-stated orbifold eigenset. Such a reversal in the general direction of an orbifold eigenset, will then tend to work to form an antiholomorphic Kahler condition -- over the here ensuing group-metric.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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