More — Metric-Gauge-Related Pulsation

 When one is to mathematically couple metric-gauge, with the reciprocal of the derivative of inverse secant, one will have a mathematical expression, that is analogous to the correlative respective metric-gauge-related pulsation. (Similar representation, yet without the correlative change in corresponding units.) TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH.

As a general rule of thumb; When the discrete energy impedance, that is here to be of a given arbitrary quantum of energy, is to be non perturbative, it may be said, that the said respective given arbitrary quantum of energy, will consequently tend, to be gauge-invariant. As a corollary-based way of putting things; When the discrete energy impedance, that is here to be of a given arbitrary quantum of energy, is to be perturbative, it may be said, that the said respective given arbitrary quantum of energy, will consequently tend, to not be gauge-invariant. 

When the Majorana-Weyl-Invariant-Mode, is succinctly transferred, the eminently associated inertial-related progression, will consequently tend to be spontaneously hermitian. This often tends to occur, with a compact mass-bearing Kahler Hamiltonian Operator, that spontaneously works to exhibit, no eminently viable metric-based Chern-Simons-related spurs, when taken over the general course, in which this is here to be solely considered, as during the implicitly inferred proscribed duration, of such a tense, of an eminently associated, Lagrangian-Based progression.  

The general concept, that is inherently related, to the viably utilized incursion, of those implicit physical constraints, that are eminently associated, with the flow of chi related force per time, is metaphorically akin, to the metaphysical concept, that may be thought of, as shakra.  

A Kahler Hamiltonian Operator, that works to bear an isotropically stable Kaluza-Klein associated net light-cone-gauge eigenstate, may often tend to exhibit a unitary gauged tense, of an eminently associated display, of its inherent physical expression of angular momentum.  

A relatively strong Slater-Based Delineation, may often tend to be eminently associated, with the mapping, of a relatively strong, covariant tangentially directed Lagrangian-Based Expansion. Whereas; A relatively strong Poincare Delineation, may often tend to be eminently associated, with the mapping, of a relatively strong, covariant co-tangentially directed Lagrangian-Based Expansion.   

When a given arbitrary tangentially propagated, exponential Lagrangian-Based Expansion, is attenuated, the eminently associated Slater-Related Delineation, may often tend to be dampened.