Friday, February 22, 2019

Scalar-Related Expressions

Particularly when one is here to be dealing with the transference of energy, that is here to be directly corresponding with the Fourier-related translation of a phenomenology, that is of a Noether Flow -- one may then call the correlative directorial axes, that are here to be centered around a Hamiltonian operator as a phenomenon of wave-tug, that is here to act as an extrapolated entity of a tense of holonomic substrate -- when this centralized set of holonomic-related directorials, may then act as a function as to here to be tugged along the path in which the said Hamiltonian Operator is to be going in, in so as to act as the source of what may here be called a genus of a particular case of a metric-gauge eigenstate.  Furthermore -- when one is here to be dealing with the actual motion of the  transference of a set of one or more discrete quanta of either energy and/or zero-point energy, via a Fourier-related translation of a phenomenology that is of a Noether Flow -- one may then call the  correlative directorial axes, that are here to be centered around the Lagrangian, -- as a phenomenon of wave-tug, that is here to act as an extrapolated entity of a tense of motion -- when this so-eluded-to set of motion-related directorials may then act as a function of here, to be tugged along the path of the said actual motion or  Lagrangian of such a set of one or more discrete quanta of energy, -- in so as to then to be acting as one general genus of what may be termed of here as being a particular case of a gauge-metric eigenstate.  Such a tense of either "metric-gauge" or "gauge-metric,"  -- when one is here to be taking the directorial flow of a phenomenology -- without mathematically working to consider the correlative variables that would otherwise be included,  such phenomenology, when of Noether Flow,  may be termed of as being an example of a scalar euclidean expression.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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