COOL 20

 A covariant system of waves, that is isotropically Unstable, at a Gaussian-Related premise, as taken at the Poincaré level, to the eminently corroborative generation of oscillatory spatial disturbance, will generally tend to bear, the likings of a Dolbeault (co)homology, as taken over time. 

The greater the assortment of covariant Del Pezzo Spaces is to be, for a directly associated super string-related field, even if this is here to be taken primordially, at an internal reference frame to the implicit anti canonical spacings, that this general implied type of a general physical situation, will thereupon often tend, to enhance the thence co-differentiable proximal local probability, of the stately holonomic presence, of an eminently corroborative generation, of a co-determinable Dolbeault (co)homology. 

Theoretically it often tends to be the case, that if one were to have a set of Del Pezzo Spaces, as taken in a net harmonically interlaced manner, from within the Ward-Neumann bounds, of a covariant generated (co)homology-based holonomic structure, of a kinematically propagated premise, as this, here, is to be considered to be taken, at an immediately externalized reference frame, from the Gliosis-Based surface of the general (co)homology-based substrate, that such an implicit general genus of a (co)homology-related phenomenon, will often tend to have a more enhanced tendency of potentially being of a De Rham-Based nature, than if it were situated otherwise. 

Cool 19

 A tense of Fourier-Related-Progression, may be said to tend to be optimally effective, when its eminently corroborative pulsation is relatively resolute, and, its eminently corroborative kinetic energy is relatively succinct. 

The piecewise continuous flow, of the net wave-based condition, of a kinematically propagated, Hamiltonian Topological Manifold, will often tend to work to describe, a harmonically delineated, Fourier-Related-Progression. 

The staggered flow, of the net wave-based condition, of a kinematically propagated, Hamiltonian Topological Manifold, will often tend to work to describe, an anharmonic delineated, Fourier-Related-Progression. 

A harmonically delineated Fourier-Related-Progression, often tends to bear magnetic charge. 

An anharmonic delineated Fourier-Related-Progression, often tends to be relatively entropic. 

An anharmonic delineated magnetic charge, may often tend to be eminently corroborative, with Tesla Energy. 

A given arbitrary tense of Fourier-Related-Progression, may be said to be optimal in  

A relatively fairly harmonic conveyed entropic state, may often tend to be eminently corroborative, with the physical melting, of a particular given arbitrary solid, into its given arbitrary eminently associated liquid state.

A extremely spuriously conveyed entropic state, may often tend to be eminently corroborative, with a nuclear reaction. 

A given arbitrary tense of Fourier-Related-Progression, may often tend to be said, to be optimal in physical operation, when its directly associated tense of pulsation, is eminently corroborative with a tense of metric-gauge, while its directly associated tense of kinetic energy flow, is eminently corroborative with a tense of heuristic-gauge. 

A given arbitrary tense of Fourier-Related-Progression, may often tend to be said, to be optimal in physical operation,  when it’s directly associated tense of pulsation, is eminently corroborative with a pressure-related Lagrangian-Based Drive, while its directly associated tense of kinetic energy flow, is eminently corroborative with a puncture-related Lagrangian-Based Drive. 

A non perturbative anti gravitational field, tends to bear a more overtly flat Ricci Curvature, than an otherwise analogous, non perturbative heuristic gravitational field, tends to bear. 

A non perturbative anti gravitational field, tends to be more auspicious, for the general bearings, of an optimal Calabi-Yau Manifold, than an otherwise analogous non perturbative gravitational field, that is fundamentally heuristic, instead. 

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, is to happen in such a manner, to where both the respective relativistic direction & the respective scalar amplitude, that is here to be corroborative with the respective wave-tug, are not to change in their overt arrangement, in any inordinate sense of the word, as taken at an internal reference frame of the actual gauging, that this thus indicates gauge-invariance. 

When there is to inextricably be a recursively smooth alteration in the direction of gauge action flow, that this works to help indicate, a particular case of the general tendency of harmonic gauge perturbation. 

However; When there is to inextricably be a recursively spurious alteration in the direction of gauge action flow, that this works to indicate, a particular case of the general tendency of anharmonic gauge perturbation.   

When there is to inextricably be a recursively smooth reverberation, in the implicitly steady changes in gauge action flow, that this works to indicate, another particular case, in the general tendency, of harmonic gauge perturbation. 

The firmer the gauge action flow, the more resolutely steady that the Moment of Inertia is to spontaneously be. 

The more gauge invariant that the angular momentum is to be, the more steady state that the eminently corroborative directional drive will tend to spontaneously be, when in terms of the resolution of wave tug, that is here to be taken, at an internal reference frame, that is Poincaré to the gauge. 

The more gauge invariant that the angular frequency is to be, for a smoothly accelerating, eminently corroborative, kinematically propagated, Kahler Hamiltonian Topological Manifold, the more spontaneously steady state, that the likely, implicitly formed magnetic charge, will consequently tend to be demonstrably expressed as being.