Let us initially consider a given arbitrary bosonic superstring of discrete energy permittivity -- that is here to be increasing in the scalar amplitude, as to the general amount of cohomology, that it is here to be generating over a set duration of time. This will then work to mean, that the general amount of cohomology-related eigenstates, that the said discrete quantum of energy permittivity will tend to be producing (to where this so-eluded-to set of cohomology-related eigenstates, of which are here to be produced by the process of the vibrational oscillations, that are of the here given arbitrary bosonic superstring), over the course of one evenly-gauged Hamiltonian eigenmetric --, will then be increased to a greater general amount of cohomology-related eigenstates, over the course of an ensuing but equal scalar amplitude of an evenly-gauged Hamiltonian eigenmetric. The more cohomology that is to be generated by a given arbitrary bosonic superstring of discrete energy permittivity over time, the more that physically-based norm-state-projections will tend to be drawn-in or convergent upon the correlative cotangent bundle -- that is here to be directly corresponding to the internal reference-frame of the kinematic-related covariant Lagrangian, that is to be of the proximal locus, that is here to be adjacent to the core-field-density of the moving overall vibrational oscillation of the directly corresponding superstring of discrete energy permittivity -- that is here to work to be directly involving the mappable-tracing, that is of the said discrete quantum of energy permittivity, as it is here to be transferred through its correlative Hamiltonian operand over time.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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