COOL 7

 The more convergent that the homotopic dispersion is to be, for an eminently corroborative, kinematically propagated, Hamiltonian Topological Manifold, the more hermitian that the delineation, of the directly associated i*PI(Del)Action, will consequently tend to be. 

Harmonic electromotive pulsation per energy, tends to facilitate an eminently corroborative Fourier-Related-Progression, that is potentially conducive to charge. Anharmonic electromotive pulsation per energy, tends to facilitate an eminently corroborative Fourier-Related-Progression, that is potentially conducive to entropy. 

In terms of the (co)homology, of a discrete increment of energy quanta, a hole, or a set of holes, when individually taken, is hereupon the regional locus, from within the Ward-Neumann bounds, of the respective (co)homology, at which the net gauge-action, of the eminently corroborative, kinematically propagated, Hamiltonian Topological Manifold, of which works to spontaneously generate, the respective (co)homology at hand, is not viably effectual, in the general kinetic process, of its covariant delineation. 

Electromagnetic pulsation per kinetic energy, of which is the Fourier-Related-Progression, of light-like phenomenology, if it is amplified enough, and of a strong enough resonant frequency, may often tend to have the spontaneous capacity, to potentially short-out, the covariant functional ability, of relatively adjacent, electromechanical systems. 

A symplectic substringular homology-based structure, as taken at a Laplacian, generally has more of a tendency, of working to bear multiple holes, than an otherwise analogous substringular homology-based structure, that instead, works to innately bear a Khovanov-Based nature. 

A symplectic substringular homology-based structure, as taken at a Laplacian, generally has more of a tendency, of working to bear multiple regional loci, from within the dimensional scope of its covariant metric Ward-Neumann bounds, at which the net eminently corroborative gauge-action, of which the eminently associated, kinematically propagated, Kahler Hamiltonian Topological Manifold, of which is here to be spontaneously generating, the respective homology-based structure, is to be viably ineffectual. 

With a symplectic (co)homology-based structure, the gauge-effectual region, surrounding each individually taken hole, that is to be distributed, from within the dimensional scope, of its Ward-Neumann bounds, is to tend to bear a polarized concave up contour, in retrospect to the vantage-point, of the internal reference frame, of each respective hole. 

Since a symplectic cohomology tends to be more compact, in a Cartesian-Related manner, than an otherwise analogous Khovanov cohomology, then it logically follows, that a symplectic cohomology, will often spontaneously tend to bear a stronger Chern-Simons attribute, than an otherwise analogous Khovanov-Related cohomology will exhibit. 

The propagated generation, of a symplectic cohomology, when its eminently corroborative i*PI(Del)Action, is to physically couple, with a viable tense of angular frequency, will generally tend to form, a stronger tense of electromotive charge, than an otherwise analogous tense, of the propagated generation of a Khovanov cohomology, will tend to orchestrate. Furthermore; The propagated generation, of a symplectic cohomology, when its eminently corroborative i*PI(Del)Action, is to physically couple, with a viable tense of angular momentum, will generally tend to form, a stronger tense of electromotive entropy, than an otherwise analogous tense, of the propagated generation of a Khovanov cohomology, will tend to orchestrate. 

Cool 6

 The more enhanced that the Kahler-Metric is to be, for a respective, given arbitrary, kinematically propagated,  eminently corroborative Hamiltonian Topological Manifold, the more likely, that such an implicit team of discrete energy eigenstates, will consequently tend to be gauge-invariant. 

A Yau-Exact, kinematically propagated, Kahler Hamiltonian Topological Manifold, will often tend to be gauge-invariant. 

A kinematically propagated, Kahler Hamiltonian Topological Manifold, that is here to be proximal local, to a non perturbative gravitational field, will often tend to be gauge-invariant. 

A non perturbative anti gravitational field, often tends to be more conducive to gauge-invariance, than an otherwise analogous, non perturbative heuristic gravitational field. 

A non perturbative anti gravitational field, often tends to have a greater affinity for Yau-Exact conditions, than an otherwise analogous, non perturbative heuristic gravitational field. 

A non perturbative anti gravitational field, often tends have a more enhanced tense of Kahler stability, and therefore spontaneously having a greater affinity, for working to exhibit a viable tense of extremal metrics, than an otherwise analogous, non perturbative gravitational field, that instead, is of an eminently corroborative, heuristic nature. 

A kinematically propagated, Hamiltonian Topological Manifold, that works to bear a viable tense, of eminently corroborative Yau-Exact physical conditions, will often tend to bear a relative lack of gauge atrophy, in the directional wave-tug of its Lagrangian-Based Drive, as taken in the relative forward holomorphic direction. 

Cool 5

 A Khovanov (co)homology, often tends to be eminently corroborative, with the likings, of a non Abelian light cone-gauge topology; To where, a Khovanov (co)homology, often tends to be eminently corroborative, with the likings, of a heuristically gauged, kinematically propagated, Hamiltonian Topological Manifold. 

A Symplectic (co)homology, often tends to be eminently corroborative, with the likings, of an Abelian light cone gauge topology; To where a Symplectic (co) homology, often tends to be eminently corroborative, with the likings, of a metrically gauged, kinematically propagated, Hamiltonian Topological Manifold. 

The more hermitian, that a kinematically propagated, Hamiltonian Topological Manifold, is to behave as, the more likely, that its cohomology-related structure, of which its eminently corroborative Lagrangian-Based motion, is to spontaneously generate, will thereby have an enhanced probability, of working to exhibit, a De Rham nature. 

The less hermitian, that a kinematically propagated, Hamiltonian Topological Manifold, is to behave as, the more likely, that its cohomology-related structure, of which its eminently corroborative Lagrangian-Based motion, is to spontaneously generate, will thereby have an enhanced probability, of working to exhibit, a Dolbeault nature. 

The more resolutely charged, that a kinematically propagated Hamiltonian Topological Manifold, is to behave as, the more likely, that its eminently associated motion, will be hermitian, to where it will thereby consequently be more likely, that its cohomology-related structure, of which its eminently corroborative Lagrangian-Based motion, is to spontaneously generate, will therefore have an enhanced probability, of working to exhibit, a De Rham nature. 

The more resolutely spurious, that a kinematically propagated Hamiltonian Topological Manifold, is to behave as, the more likely, that its eminently associated motion, will be entropic, to where it will thereby consequently be more likely, that its cohomology-related structure, of which its eminently corroborative Lagrangian-Based motion, is to spontaneously generate, will therefore have an enhanced probability, of working to exhibit, a Dolbeault nature. 

The more resolutely spurious, that a kinematically propagated Hamiltonian Topological Manifold, is to behave as, the more likely, that its eminently associated motion, will consequently tend to work to exhibit, an enhanced tense, of energy of heat transfer per Kelvin Mole. 

Phenomenology of kinematically propagated, Hamiltonian Topological Manifold, that is to be eminently corroborative, with a viable tense, of divergent homotopic dispersion, will often tend to exhibit, an enhanced tense, of energy of heat transfer per Kelvin Mole. 

Phenomenology of kinematically propagated, Hamiltonian Topological Manifold, that is to be eminently corroborative, with a viable tense, of convergent homotopic dispersion, will often tend to exhibit, an enhanced tense, of charge. 

The more piecewise continuous, that the Yau-Exact behavior is to be, for a charged, kinematically propagated, Hamiltonian Topological Manifold, the more efficient and effective, that the wave-tug, of the eminently associated electromotive charge, will often tend to be. 

The more piecewise continuous, that the Yau-Exact behavior is to be, for a charged, kinematically propagated, Hamiltonian Topological Manifold, the more likely, that the implicit team of mass-bearing discrete energy quanta, will tend to be gauge-invariant. 

Kinematically propagated, Calabi-Yau, Hamiltonian Topological Manifolds, tend to bear a more piecewise continuous Lagrangian-Based Flow, than otherwise analogous, kinematically propagated, Hamiltonian Topological Manifolds, that instead, are not Calabi-Yau. 

A Calabi-Yau Manifold, has a greater tendency of being gauge-invariant, than an otherwise analogous, implicit Hamiltonian Topological Manifold, that instead, is not Calabi-Yau. 

Kinematically propagated, Hamiltonian Topological Manifolds, have a greater probability of being gauge-invariant, if the proximal local gravitational force is non perturbative, than if, under otherwise analogous conditions, it were proximal local to a perturbative gravitational field, instead.