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. 

Cool 15

 The stronger that the Kahler-Based conditions are to be, for an eminently associated Hamiltonian Topological Manifold, the more likely that it will consequently tend to have the general capacity, of potentially becoming Yau-Exact, particularly if it is proximal local, to a non perturbative gravitational environment. 

Anti gravitational force, often has more of a potential, of facilitating the generation of less entropy, than an otherwise analogous physical situation, that instead, works to viably involve, a heuristic gravitational tense of force. 

A non perturbative anti gravitational field, that is proximal local, to an eminently corroborative, Kahler Hamiltonian Topological Manifold, will often tend to foster, a heightened tense of Yau-Exact physical conditions, in contrast to an otherwise analogous physical situation, that instead, works to involve, the proximal local presence, of a non perturbative, heuristic gravitational force. 

Strong Yau-Exact physical conditions, often tend to be auspicious, for potentially facilitating wormhole formation.

Calabi-Yau conditions are optimized, when the implicit eminently corroborative Hamiltonian Topological Manifold in question, is proximal, to a non perturbative gravitational field. When this is to occur, such a respective Hamiltonian Topological Manifold, is said, to be Yau-Exact.

A Hamiltonian Topological Manifold, is Yau-Exact, when it generates as much (co)homology as it degenerates, in a piecewise continuous manner. 

A Hamiltonian Topological Manifold, is said to bear a flat Ricci Curvature, when it is proximal local, to the eminent presence, of a non perturbative gravitational field. 

A Kahler Hamiltonian Topological Manifold, that is proximal local, to the eminent presence, of a non perturbative gravitational field, will often tend to be, of the general nature, of being a Calabi-Yau Manifold. 

Calabi-Yau Manifolds, tend to often eminently bear up to a nine spatial dimensional structure — since this assists these, at working to bear a minimal vanishing point, of tangential residue.

 

Cool 14

 When the i*PI(Del)Action, in the form of unitary heuristic -gauged magnetic potential, is tugged into the eminent flow, of the disturbance of space, that is corroborative, to the directly associated Hamiltonian Topological Manifold, that is here to have just spontaneously generated such a respective i*PI(Del)Action, that this may often tend to be a directly adherent physical situation, in which charge is to be generated instead of entropy. Yet; if the respective i*PI(Del)Action, is, instead, to be tugged into the eminent abrasion, that is corroborative with the disturbance of space, that is directly associated with the kinematic propagation, of the related Hamiltonian Topological Manifold, than it is more likely to tend to generate entropy than charge. 

The interaction of homotopic residue with angular frequency, that is of a discrete quantum of energy, as it is physically translated through its Lagrangian, is often eminently corroborative, with the Fourier-Related Flow, of the given arbitrary discrete Hamiltonian Topological Manifold in question, that is here to be exhibiting discrete energy. 

The interaction of homotopic residue with angular momentum, that is of a discrete quantum of energy, as it is physically translated through its Lagrangian, is often eminently corroborative, with the Fourier-Related Abrasion, of the given arbitrary discrete Hamiltonian Topological Manifold in question, that is here to be exhibiting discrete energy. 

When the general hermitian interaction, of the i*PI(Del)Action with angular frequency, works to involve an eminently corroborative co-tangential covariant incursion, that this will often tend to form a magnetic charge, that works to bear a negative chirality (a negative charge). 

When the general hermitian interaction, of the i*PI(Del)Action with angular frequency, works to involve an eminently corroborative tangential covariant incursion, that this will often tend to form a magnetic charge, that works to bear a positive chirality ( a positive charge). 

Just to make myself clear, just in case I make any typos: The phenomenology of the i*PI(Del)Action, is basically tantamount, to being, Unitary Heuristic-Gauge Magnetic Potential. 

The stronger that the interaction is to be, between unitary heuristic-gauge magnetic potential & angular momentum, the greater that the consequential spontaneously generated energy of heat transfer, will therefore tend to be. 

The stronger that the interaction is to be, between unitary heuristic-gauge magnetic potential & angular frequency, the greater that the consequential spontaneously generated magnetic charge, will therefore tend to be. 

Hermitian charge tends to be generated, by harmonically accelerating Hamiltonian Topological Manifolds of energy. 

Entropic features, tend to be generated, by anharmonic accelerating Hamiltonian Topological Manifolds of energy. 

The generation of enhanced heat transfer (transport), may often tend to be facilitated, by the anharmonic acceleration, of a Hamiltonian Topological Manifold of energy.  

Isotropically stable generation of hermitian charge, may often tend to be eminently corroborative, with the super symmetrical Lagrangian-Based delineation, of a piecewise continuous accelerating Hamiltonian Topological Manifold.

Unitary Heuristic-Gauge Magnetic Potential, is the reductional metaphorical common denominator, between charge — which works to represent, the physical tendency towards order, &, entropy — which works to represent, the physical tendency towards disorder. 

Unitary Heuristic-Gauge Magnetic Potential, tends to be generated, when an implicit team of mass-bearing discrete energy, is to alter, in its speed and or in its direction. 

The more compact, that a given arbitrary, kinematically propagated, Kahler Hamiltonian Topological Manifold, is to be situated as, the more likely, that it will potentially be physically conditioned, to have the general capacity, of working to be facilitated, into working to bear a covariant physical tense, relative to its surroundings, of isotropic stability — as it is here to be implicitly conveyed. 

The more facilitated that a given arbitrary Kahler Hamiltonian Topological Manifold is to be, at exhibiting a viable tense of conditioned compactification, the greater that the spontaneous probability will consequently be, that such an implicit team of net discrete energy quanta, will work to physically express, a tense of Yau-Exact behavior.