Rate Of i*PI(del) Action And Rate Of Superstringular Vibration During BRST

The quicker that any one given arbitrary mass-bearing orbifold eigenset is to accelerate, when this is here to be taken in its relationship to both the motion and the existence of electromagnetic energy, -- the faster that the directly corresponding i*PI(del) action will tend to work to happen, to those composite superstrings of discrete energy permittivity that work to comprise the said respective orbifold eigenset of such a here stated case scenario, -- when this is here to be taken in respect to a lower Hodge Index as to the number of partition-based discrepancies, that are here to be proximal local to the general topological surface of the here stated superstrings, that are here to work to comprise the earlier mentioned orbifold eigenset.  Since homotopic residue is to be conserved; the less partition-based discrepancies that work to be directly affiliated with the general topological surface of those superstrings of discrete energy permittivity that work to comprise any one said given arbitrary mass-bearing orbifold eigengeset, the more of such mass-bearing strings that it will consequently take to comprise such a said eigenset.  The denser that any one given arbitrary orbifold eigenset is to be, the quicker that those composite strings -- that work to comprise such a said eigenset -- are consequently to need to vibrate, during each successive iteration of BRST, in which such a said mass-bearing orbifold eigenset is to be accelerating in its relationship to both the motion and the existence of electromagnetic energy.  This works to produce that general Hamiltonian operation, that is here to act as a fractal of momentum, -- that works to allow for the added thrust of accelerated mass-bearing phenomenology.  Again; it is the multiplicit Legendre homology, that works to allow for the kinematic motion of mass-bearing orbifold eigensets. Samuel David Roach.