Saturday, June 18, 2016

Cyclic Perturbations Of Noether Current

Let us initially consider an orbifold eigenset that goes from a tense of acceleration to a tense of deceleration, back to a tense of acceleration, and so on -- in such a manner to where the then apparent tendency of one going from a tense of acceleration to a tense of deceleration and back, is to be cyclical as well -- when this is taken in terms of the gradual process of going from an increase in the scalar amplitude of the velocity of the said arbitrary eigenset, into the gradual decrease in the scalar amplitude of the velocity of the said orbifold eigenset, and back.  So, the initial Ward-Caucy condition of the so-stated orbifold eigenset is in a state, to where the said eigenset is traveling at a respective given arbitrary rate.  The respective direction of the so-stated orbifold eigenset is through a constant unitary Lagrangian, via a Hamiltonian operand -- that works to bear no abrasion of tensoric-affiliated topological sway.  The  so-mentioned eigenset is to then accelerate relatively smoothly, up to a specific given arbitrary maximum velocity, while then decelerating relatively smoothly back down to the initially extrapolated velocity that works to bear its directoral-based translation -- as a disturbance in space-time-fabric that is being pushed ahead further and further through the so-stated progressive unitary Lagrangian.  As the so-stated cyclical-based perturbative-related tense of a Fourier differentiation, works to push the so-stated orbifold eigenset further and further along the same directoral-based Lagrangian -- both the Hodge-Indices of the holonomic substrate of the here given arbitrary retentive metrical-gauge-based Hamiltonian resultant -- that is successively indistinguishably different, and also the tense of the kinematic behavior of those eigenindices that work to comprise the so-eluded-to composite of the said resultant Hodge-Indices, is to here work to bear a constant succession of gauge-metrical cyclical operational functioning -- to where the chain of activities that is to here, be of the kinematic translation as to the qualitative functioning that works to form the cyclical tense of that behavior that is directly associated with the cyclical perturbation of the tense of the Majorana-Weyl-Covariance, that is of the so-stated orbifold eigenset, to where this is to repeat back-and-forth in this case, as if it were an eigenstate that is to repeat in a relatively deep Njenhuis quantum-associated "well."  (The relative "sides" of the orbifold egienset's flow is contained.)  As the tense of the said Majorana-Weyl-Covariance  is to fluctuate relatively smoothly, the correlative tense of the directly related Noether Current is to fluctuate relatively smoothly as well.  As this is happening, the tense of the related covariance is to then go form a relative loosening upon the eigenindices of its Hodge-Indices, into a relative tightening upon the eigenindices of its Hodge-Indices. I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

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