As to the Mode of Various Hamiltonian Operators

Let us say that there is one Hamiltonian operator -- that may be here be depicted as the holonomic substrate of the pulse of one respective given arbitrary orbifold, that would bear an eigenbase of an acceleration through a Lagrangian -- in such a manner in so that the so-stated pulsation of the said orbifold will bear Chern-Simmons singularities that are of a metrical-based format, even though this so-stated orbifold will not necessarily here bear Lagrangian-based Chern-Simmons singularities -- unless there is a Gliossi-based interaction that is not colinear, as I will explain in a little bit.  After a discrete quantum of time later (over the kinematic activity that would involve here a sequential series of group instantons), the said orbifold will alter or perturbate in the mode of its Hamiltonian-based pulse, or, in other words, the acceleration of the so-stated orbifold will change in its scalar magnitude of Hamiltonian-based momentum -- in the process of the so-eluded-to set of superstrings that bear the eluded-to given arbitrary function of operation will be either ellongated in its given arbitrary respective pulse or attenuated in its given arbitarry respective pulse, over the so-stated general consideration of time, in this respective given arbitrary scenario.  This will here mean that the initial eigenbase of the overall Hamiltonian-based momentum of the said orbifold will have here, over the course of the so-eluded-to perturbation of its pulse, been interactive, in a Yakawa-based manner, with an exterial-based substringular phenomenon or phenomena -- that will have here initiated a Gliossi-based wave-tug/wave-pull, that will have brought a spontaneous response upon the initial orbifold, to where such a response will have changed the genus of the Hamiltonian eigenbase. Such an alteration in the so-eluded-to Hamiltonian-based eigenbase of "momentum" will have directly corresponded to the Hodge-based extrapolation of the scalar magnitude of the rate of change of the so-stated initial orbifold here mentioned, in the respective directoral-based Lagrangian of that said orbifold, that may here then work to also cause a set of one or more Lagrangian-based Chern-Simmons singularities to happen to the said initial orbifold, over time.  The directoral-based addition of the Hodge-based Hamiltonian expression of the exterial-based orbifold upon the initially mentioned  directoral-based Hodge-based Hamiltonian -- that works to help define the resultant pulsation of the initial orbifold, after the so-eluded-to perturbation that I have here implied -- will work to cause both the directoral-based pull of the initially stated orbifold, and, its resultant manner of changed pulsation -- to where the additional eigenbase of Chern-Simmons singularities, in terms of both the Lagrangian-based singularities and the metrical-based singularities, will work to help indicate the resultant behavior of the initially mentioned orbifold, over time.  This will often inevitably be the case, since any corroberation of Gliossi-based interactive orbifolds -- that bear any given arbitrary Yakawa-based interaction over any definitive projection -- will be of such a remote difference from being of a Wilson-based colinearity -- to where the resultant implied Gliossi-based wave-tug/wave-pull of the interacting orbifolds will actually tend to bear at least some manner of Lagrangian-based singularity, upon impact.  I will continue with the suspense later!  Sam.