Scalar Amplitude Of Kahler-Based Quotients -- Correlative Intensity Of Wave-Tug

 Let us initially consider two different Noether-Based mass-bearing cohesive sets of discrete energy quanta, that are here to be of basically the same general nature. Both of these two different inferred individually taken "teams" of discrete energy, are here to be exhibiting the mappable-tracing, of a "congruent" tense of a Lagrangian-Based path, as this is here to be taken into consideration, over the durational course of a relatively brief covariant Fourier-Transformation, that is here to work to bear the span of the same sequential series of group-related instantons. (As the inferred covariant duration that is to be considered here, in which these two different inferred "teams" of energy, are here to have had worked to map-out their correlative Lagrangian-Based paths, is to be indicated by a monomial tense, of an evenly-gauged relativistic Hamiltonian eigenmetric.) Next; The kinematic motion of one of these two said cohesive sets of discrete energy quanta, is here to work to mathematically bear a greater scalar amplitude of a Kahler-Based quotient, than the other indicated cohesive set of discrete energy quanta, as this is here to be taken, over the covariant span of time, in which these two earlier inferred sets of discrete energy quanta, have worked to map-out their "congruent" individually taken Lagrangian-Based traces. As a result; that cohesive set of discrete energy quanta of the two, that is here to have worked to mathematically bear a greater scalar amplitude of a Kahler-Based quotient, -- in the process of working to map-out its correlative Lagrangian-based path, -- will consequently tend to work to bear a higher relativistic intensity of a wave-tug, upon its immediately external environment, than that other cohesive set of discrete energy quanta of the two, that was instead, to mathematically bear a lower scalar amplitude of a Kahler-Based quotient. I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL DAVID ROACH.

As To Discrete Quanta Entering Holonomic Substrate Of Klein Bottle Eigenstate

As The Kahler-Metric is Yukawa to the topological stratum of an orbifold eigenset of discrete energy quanta, the directly associated discrete quanta of energy that are to work to inter-mingle with the Ward-Caucy-based bounds of the holonomic substrate of the correlative Klein Bottle eigenstate -- immediately after each individually taken iteration of BRST -- fall into the Ward-Neumman bounds of the said respective given arbitrary Klein Bottle eigenstate, in so as to then shake back-and-forth eight overall times (primarily from the relative holomorphic direction to the relative reverse-holomorphic direction and back again, a total of eight times until the completion of such a "shaking"), in so as to work to help the so-eluded-to discrete quanta of energy, to reattain one fractal of the cross between both discrete energy permittivity and discrete energy impedance, -- right before finishing up in the process of one iteration of group-related instanton, by then participating in the gauge-metric of the directly affiliated correlative iteration of the Regge Action. As discrete energy quanta work to enter the "shuffleing," so-to-speak, upon the Ward-Neumman bounds of the said holonomic substrate, that is of the respective Klein Bottle eigenstate -- then, those individually taken norm-state-projections, that had initially worked to bear what would have tended to be a purely harmonic Reimman-based distribution, will then be pushed into a resultant Rayleigh-based scattering, -- at the Poinare level to the Gliosis-based topological stratum of those norm-state-projections, that had initially been in what would have started out as bearing both a homeomorphic and a homogeneous distribution. The activity of both the shaking of the discrete quanta of energy, that had just entered into the Ward-Neumman bounds of the so-stated holonomic substrate of the respective Klein Bottle eigenstate, along with the process of the said discrete quanta of energy being temporarily scattered in an annharmonic manner, -- works to imbue the needed individually taken fractal of discrete energy quanta, upon the topological substrate of those "packets" of energy that need to go into the process of both persisting and existing, in the ensuing Ultimon Flow.  Once that discrete energy quanta leave the Ward-Neumman bounds of the so-stated holonomic substrate of the respective eigenstate of the Klein Bottle, the general motion that the substringular realm bears, during the then eminent Regge Action -- will then work to cause the eigenindices of the said Klein Bottle eigenstate, to then perform a Reimman-based scattering, -- in so as to bring these said eigenstates back into a condition of being both of a homeomorphic and of a homogeneous nature, at the Poincare level to the topological surface of the so-eluded-to Kahler-based eigenstate.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.