Cool 18

 The Fourier-Related-Progression, of the Lagrangian-Based Expansion, of a kinematically propagated, De Rham Calabi-Yau Manifold, will spontaneously tend to exhibit, both a relatively resolutely discrete tense, of quantum energy permittivity, &, a relatively succinctly discrete tense, of quantum energy permeability, as it is delineated spatially.

An ideal De Rham Calabi-Yau Manifold, will generally tend to be Yau-Exact, in that, a Kahler Hamiltonian Topological Manifold, that generates a smoothly traceable Lagrangian, that is here to exist in a purely hermitian manner, will tend to bear a piecewise continuity, in the general course of the propagation of its net holonomic eigenstate, causing it to spontaneously tend to be piecewise continuous, in the general process of recursively generating as much (co)homology as it is to degenerate, over a set time. 

A kinematically propagated, De Rham Kahler Hamiltonian Topological Manifold, tends to bear a relatively “pressured” metric-related quantum energy permittivity,&, a relatively aerodynamic heuristic-related quantum energy permeability. 

Kinetic De Rham Calabi-Yau Manifolds, that are Yau-Exact, tend to spontaneously behave, as being gauge-invariant. 

The greater that both the quantum energy permittivity & the quantum energy permeability are to be exhibited as expressing, over a set duration of proscribed time, the stronger that the kinematically propagated net inertial eigenstate, will consequently tend to spontaneously be, to where, the respectively latent covariant proximal local expectation value, of the probable possibility, of relatively sustained gauge-invariance, will therefore often tend, to be more plausibly permissible, in such a physical case scenario, as the restraints of impeding energies, that would otherwise make such a possible sustainable tense of developed gauge-invariance improbable, are here to not be viably effectual, upon the topological substrate, of the implicit kinematically propagated team, of discrete energy eigenstates, as Gliosis to the Poincaré level, in so as to bring on the prior insinuated physical conditions, in which a particular genus or type of gauge-invariance may occur!🤝

The space time continuum is looped, super strings tend to be looped, so, doesn’t it make sense to people, that at the pinnacle of its logical order, time is looped too?!

The longer of a relativistic duration, in which an isotropically stable inertial tense of ordered restraint, is here to have recursively iterated for a relatively long time, that it will often tend to consequently occur, that the potential tendency of a resultant spontaneous arrangement of viable gauge-invariance, will often tend to be thus enhanced. 

When the physical impetus of wave-tug, that is here to be applied, as a tense of physical restraint upon the implicit team of mass-bearing discrete energy quanta, in such a manner, to where both the relativistic direction & the scalar amplitude of the respective wave-tug are not to change, in any inordinate sense of the word, as taken at an internal reference frame, that this indicates gauge-invariance. 

Cool 17

 Not only may thoughts potentially effect the probability density; So can free-will, imagination, the yin(g) and the yang, as well as the rest of the metaphorical gauntlet of those emotion-based physical characteristics, that are here to be capable of exerting at least some form or another of physical force, upon the relative positioning of physical phenomenology, in so as to effect the potential spots, as to where various microscopic things could possibly be at. 

Hermitian frequencies, that work to bear Lagrangian-Based Nijenhuis tensors, tend to exhibit harmonically recursive fluctuations, of viably incurred topological-related sway. 

Hermitian frequencies, that work to bear Lagrangian-Based Riemann-Related tensors, tend to exhibit a perturbative topological contour of trace, causing these frequencies to thereby tend to lack, a tense of topological invariance. 

A (co)homology-based manifold, that is non perturbative in its covariant metric, and is also here to be translated physically, via the incursion of a hermitian Lagrangian, will generally tend to bear a viable tense, of topological invariance. 

The denser that the energy of heat transport (transfer) is to be, the stronger that the eminently corroborative entropy, will spontaneously tend to consequently be. 

The more erratic that infrared photons are to behave as, when in conjunctivitis covariance with a mass that is at a particular temperature, the more entropy it tends to exhibit.

The more harmonically conveyed that infrared photons are to be exhibited as, the less entropy that these will spontaneously tend to be eminently corroborative with. 

An amplified, harmonically perturbative, frequency oscillation, will tend to spontaneously work to bear, an eminently corroborative, hermitian augmentation of field pulsation, when this is here to be physically taken, in covariant retrospect, to the externalized spatial disturbance. 

An amplified, anharmonic in perturbation, frequency oscillation, will tend to spontaneously work to bear, an eminently corroborative, spurious augmentation of field pulsation, when this is here to be physically taken, in covariant retrospect, to the externalized spatial disturbance.

A diminished, harmonically perturbative, frequency oscillation, will tend to spontaneously work to bet, an eminently corroborative, hermitian attenuation of field pulsation, when this is here to be physically taken, in covariant retrospect, to the externalized spatial disturbance. 

A diminished, anharmonic in perturbation, frequency oscillation, will tend to spontaneously work to bear, an eminently corroborative, spurious attenuation of field pulsation, when this is here to be physically taken, in covariant retrospect, to the externalized spatial disturbance. 

An escalating frequency, tends to increase in recursion, and decrease in time. Whereas; A de-escalating frequency, tends to decrease in recursion  and increase in time;When kinetic. 

One discrete increment of zero point energy, I have mathematically determined lately, as far as I can tell, is:

2.06217667801*10^(-162) Cubic Joules Per Meters Squared Seconds To The Fourth. 

So; When 511,385,442,463*10^(116) discrete increments of zero point energy, are to couple in a hermitian manner, with (meters seconds squared per kinetic energy)*(meters seconds squared per kinetic energy) — while the yet being amplified by a factor of two pi, that this forms the Lagrangian of the Planck Energy; And When the Planck Energy is to couple with the exact equal and opposite direction of its Lagrangian, that this eminently tends to facilitate the creation, of a quantum of the Planck Phenomenon. 

A physical frequency oscillation, that works to bear a pressure-related Lagrangian-Based Drive, will quite often tend to bear optimum viable efficiency, when it is delineated into the direction of least distance. 

A physical frequency oscillation, that works to bear a puncture-related Lagrangian-Based Drive, will quite often tend to bear optimum viable efficiency, when it is delineated into the direction of least time. 

Cool 16

 Zero point energy is an actual phenomenon, yet, via math, I determined that, instead of coming in units of Joules, zero point energy comes in units of Joules Cubed per meters squared seconds to the fourth. Zero point energy also doesn’t go discretely into the Planck Energy, yet it Does go discretely into the Planck Bar Energy. So; If one were to couple a whole lot of discrete increments of zero point energy, With the covariant spontaneous trivial isometric coupling of a Fourier-Related-Progression (upon itself), that eminently involves unitary heuristic-gauge pulse per kinetic energy, that this may tend to form the Planck Bar Energy. When such a phenomenon of Planck Bar Energy is augmented by a factor of two pi, this then forms a phenomenon of Planck Transversal Energy. And when Planck Transversal Energy is coupled with the equal and opposite direction of its Lagrangian-Based Motion, this forms an actual thing of energy that is energy, relative to us. 

The more piecewise continuous, that the pulsation is to be, for a given arbitrary, respective, Kahler Hamiltonian Topological Manifold, the less erratic, that its eminently corroborative Fourier-Related-Progression, will tend to be.

The more erratic, that the directly corresponding kinetic energy is, for an eminently corroborative tense, of Fourier-Related-Progression, the more of a tendency, that there will consequently be, that it will bear enhanced entropy.   

The more piecewise continuous, that the frequency is to be, for a given arbitrary, respective Kahler Hamiltonian Topological Manifold, the more likely, that the eminently corroborative Kahler-Metric, that is here to be equivocally associated, will spontaneously bear the general characterization, of a Calabi-Yau Manifold, or perhaps even working to bear the characterization, of being Yau-Exact. 

Piecewise Continuous Frequencies, when individually taken, often tend to be eminently corroborative, with a hermitian general framework, of viable linear time, in so long as the eminently associated general physical situation, is here to bear a strong tense of Riemann-Based isotropic stability, in terms of having purely Gaussian Noether Symmetry, in retrospect to its eminently covariant surroundings. 

The stronger that the eminently associated pulsation is to become, for the Fourier-Related-Progression, of a directly corroborative, kinematically propagated, Kahler Hamiltonian Topological Manifold, the more amplified, that its directly related frequency, will consequently tend to spontaneously be. This is to where the period of the frequency, will tend to become shorter, and thus more recursively quick in relative duration. The weaker that the eminently associated pulsation is to become, for the Fourier-Related-Progression, of a directly corroborative, kinematically propagated, Kahler Hamiltonian Topological Manifold, the more diminished, that its directly related frequency, will consequently tend to spontaneously be. This is to where the period of the frequency, will tend to become longer, and thus more recursively slow in relative duration. 

The more amplified that the pulsation is to be, for an eminently associated Kahler Hamiltonian Topological Manifold, the more augmented, that its corroborative Fourier-Related-Progression, will spontaneously tend to be. The more diminished that the pulsation is to be, for an eminently associated Kahler Hamiltonian Topological Manifold, the more attenuated, that its corroborative Fourier-Related-Progression, will spontaneously tend to be.

 The more resolute that the resonant pulsation is to be, for an eminently associated Kahler Hamiltonian Topological Manifold, the more force, that its corroborative Fourier-Related-Progression, will consequently tend to spontaneously incur, upon its covariant surroundings. 

The more succinct that the resonant pulsation is to be, for an eminently associated Kahler Hamiltonian Topological Manifold, the more permeability, that its corroborative Fourier-Related-Progression, will consequently tend to spontaneously incur, upon its covariant surroundings. 

Resolute pulsation tends to enhance the abrasive force, that is eminently associated, with the Fourier-Related-Progression, of a resonant, kinematically propagated, Kahler Hamiltonian Topological Manifold. Whereas; Succinct pulsation tends to enhance the hermitian force, that is eminently associated, with the Fourier-Related-Progression, of a resonant, kinematically propagated, Kahler Hamiltonian Topological Manifold, over time.