Part Two Of Light-Cone-Gauge Quantization And Gravity

Let us initially consider one given arbitrary orbifold eigenset.  Let us now consider more specifically, the basically wave-based functional Hamiltonian operator, that is of the discrete energy impedance, that is to here work to help in the formation of the discrete quantum of the wave-based energy impedance of the said orbifold eigenset -- of which is to here be the physical overall light-cone-gauge eigenstate of the so-stated orbifold eigenset, as a whole.  let us now say, that there are to here be a relatively small set of such orbifold eigensets -- of which are to here work to bear a quantized metrical-gauge-based Hamiltonian operation of light-cone-gauge eigenstates.  Let us next consider, that such a set of the so-eluded-to Ward-Caucy-based conditions, will work to tend to help allow for a relatively quantized set of Schwinger-Indices, -- of which are to here act as a relatively quantized set of gravity waves.  Let us next consider, that such a quantized tense of gravity waves, will here work to form an initially steady-state tense of a conformally invariant gravitational field -- as is appertaining to the general Ward-Caucy set of conditions that I had basically mentioned in the last post.  Now -- what if there was to be a Cevita-based metrical-gauge-based Hamiltonian operator, that was to act as a general ghost-based inhibitor -- that was to here bear a Yukawa-related wave-tug, upon the cohomological-based mappable-tracing of the topological stratum of the world-sheet-related holonomic substrate, that is of the inter-play of the said relatively small set of orbifold eigensets, that are to here to be of a relatively eigen nature to the so-stated Hamiltonian operation of the given correlative steady-state-based proximal Fourier-related locus, by which the relatively limited Hodge-Index of the relevant sets of discrete energy quantum of this case, are to here be initially of a gravitational mode -- that is of a relatively tight tense of a Majorana-Weyl-Invariant-Mode?  If such a kinematic-based presence, that is of such a ghost-based-inhibitor -- were to be of an effectual Yukawa-based nature to the so-eluded-to initial set of a relatively limited Hodge-Index of orbifold eigensets, over a sequential series of group-related instantons, by such a so-stated inhibitor, is to here be of a Gaussian-based nature to the sequential gauge-metrical Hamiltonian operator, that is of the translation of the correlative cohomological mappable-tracing -- then, in this physical case, this situation will tend to help to form a Rayleigh scattering of the proximal local gravitational force, that was initially of a steady-state nature, -- which will thereby act in so as to scatter, in an anharmonic manner, the so-eluded-to gravitational force, that was initially under a tense of conformal invariance.  Such a resultant anharmonic scattering, will cause the correlative adjacent eigenindices that had just been scattered -- to bear an odd chirality.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.