Velocity And Majorana-Weyl-Invariant-Mode

Let us initially take into consideration, a given arbitrary orbifold eigenset -- of which is to be traveling through a discrete Lagrangian, via a respective Fourier Transformation, with one given arbitrary maintained velocity, -- over one set gauged metric, that is to happen over a respective sequential series of instantons.  Let us next take into consideration, that the directly corresponding Majorana-Weyl-Invariant-Mode -- that is to here be correlative to the Hamiltonian-based operation of the delineation-based translation of the said orbifold eigenset over time, is to be of one set general genus of a tense of a relative conformal invariance -- as the so-stated orbifold eigenset is to be moving in a direction, that is to here be traveling through a relatively set directoral-based holomorphicity, with one respective given arbitrary general genus of wave-tug, that is to here be directly corresponding to the propagation of the said eigenset, over the correlative said gauged metric, over the so-eluded-to sequential series of instantons.  Let us next say, that the only Ward-Caucy condition, that is to ensue in so as to change over the then ensuing group-related metric -- is that the general genus of the tense of that conformal invariance, that is to here be directly related to the scalar amplitude of as to how tight or as to how loose that the directly correlative tense of the directly corresponding Majorana-Weyl-Invariant-Mode is, is to then spontaneously loosen by a relative factor of two.  This will then tend to mean, that the relative velocity of the said orbifold eigenset of such a given arbitrary case scenario, -- will then tend to double, -- in so long as the holomorphic means of the directoral-based wave-tug, that is to here be directly associated with the propagation of the so-stated orbifold eigenset, is to both remain as a tense of a topological stratum that is to act in a tense of Noether-Flow, as well as also as to remain as a topological stratum that is to "stay the course" of its Hamiltonian-based topological sway, as I have here so-eluded-to.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.