COOL 9

 A kinematically propagated, Kahler Hamiltonian Topological Manifold, that works to bear a piecewise continuous distributional delineation, while spontaneously working to bear an eminently corroborative, EUCLIDEAN-Based, Khovanov-Related (co)homology, will often tend to have a stronger Chern-Simons attribute, than an otherwise analogous, kinematically propagated, Kahler Hamiltonian Topological Manifold, that instead, works to bear, a piecewise continuous distributional delineation, that is spontaneously corroborative, with working to bear a Euclidean-Based, Symplectic (co)homology. 

A kinematically propagated, Kahler Hamiltonian Topological Manifold, that works to bear, both an eminently corroborative Symplectic-Based spin orbital momentum, in conjunction with an eminently corroborative Khovanov-Based angular momentum, will often tend to bear a significant state, of aerodynamic efficiency. 

A kinematically propagated Hamiltonian Topological Manifold, that is simply spinning, as covariant to its relative internal reference frame, is to have an enhanced Chern-Simons attribute, when its eminently corroborative (co)homology-based feature is Symplectic. Whereas; A kinematically propagated Hamiltonian Topological Manifold, that is simply moving transversely, as covariant to its relative internal reference frame, is to have an enhanced Chern-Simons attribute, when its eminently corroborative (co)homology-based feature is Khovanov. 

Proximal regional Anti Chiral magnetic states, have a general tendency, of dispersively converging. Whereas; Proximal regional chiral magnetic states, have a general tendency, of dispersively diverging. 

A spinning charge, tends to express greater magnetism, than an otherwise analogous charge, that is not spinning. 

(Co)Homology that is symplectic, tends to bear a relatively strong Chern-Simons attribute, when the eminently corroborative, kinematically propagated Hamiltonian Topological Manifold, that works to exhibit such an implicit (co)homology, is to bear the Lagrangian-Based modus of operation, of a Clifford Expansion. 

(Co)Homology that is Khovanov, tends to bear a relatively strong Chern-Simons attribute, when the eminently corroborative, kinematically propagated Hamiltonian Topological Manifold, that works to exhibit such an implicit (co)homology, is to bear the Lagrangian-Based modus of operation, of a Euclidean Expansion. 

COOL 8

 The smaller that the holes are to be, from within the physical boundary constraints, of the respective Ward-Neumann conditions, of a directly associated cohomology-related topological manifold, that is here to be generated, via the Lagrangian-Based kinematic propagation, of an eminently corroborative substringular phenomenology, the more efficient, that the spontaneous primordial effect, of its net gauge-action, will consequently tend to be incurred as. 

The more isotropically stable, that the magnetism is to be, of which is here to be radiated, by the kinetically displaced, directly associated kinematic propagation, of the Cartesian Lagrangian -Based motion, of a respectively considered Hamiltonian Topological Manifold, the more likely, that the eminently corroborative (co)homology, of which is here to be generated, by the spontaneous distributional delineation, of the implicit team of discrete energy quanta, will work to bear the likings, of a symplectic form of (co)homology. 

Since kinematically propagated, Hamiltonian Topological Manifolds, that are relatively enhanced in their compactness, when taken in a Cartesian manner, tend to be eminently corroborative, with working to bear a symplectic (co)homology, such symplectic-associated implicit teams of mass-bearing, discrete energy quanta, often tend to bear a more primordial interactive constituency, as taken in correlation between their spin orbital momentum, in lieu of their covariant eminently respective angular momentum. 

Kinematically propagated Hamiltonian Topological Manifolds, that are eminently corroborative, at working to express a symplectic (co)homology, when taken in a Cartesian manner, often tend to have a more enhanced capacity, at working to exhibit a Kahler-Metric, than otherwise analogous, kinematically propagated Hamiltonian Topological Manifolds, that instead, are eminently corroborative, to working at expressing a Khovanov tense of (co)homology. 

Khovanov cohomology-related phenomenology, that are of a Cartesian-related Manner of spatial delineation, often tend to express a less isotropically stable net gauge action, than otherwise analogous symplectic cohomology-related phenomenology does. 

Symplectic cohomology-related phenomenology, that are of a Cartesian-Related manner of distributional delineation, often tend to be more eminently corroborative, with Hamiltonian Topological Manifold-Like entities, that work to bear an enhanced charge density, than those otherwise analogous Hamiltonian Topological Manifolds, that instead, are eminently corroborative, with working to express, a Khovanov-related nature of cohomology. 

Since a symplectic cohomology tends to be eminently corroborative, with relatively stronger Chern-Simons attribute, than an otherwise analogous Khovanov-Related cohomology does, when taken in a Cartesian-Related perspective; An implicitly respective symplectic cohomology, therefore, tends to have a relatively stronger Majorana-Weyl-Invariant-Mode, than an otherwise analogous Khovanov-Related cohomology, as well. 

A symplectic cohomology, that is Cartesian, tends to work to bear, a relatively tightly knit Minkowski-Based Spin, in comparison to the general physical attribute, of the Minkowski-Based Spin, of a Khovanov-Related cohomology, which tends to be less tightly knit. 

Calabi-Yau topological manifolds, when in terms of their Cartesian attributes, tend to generally be more facilitated at spontaneously coming into fruition, when it is eminently corroborative, with the Lagrangian-Based generation of a resultant symplectic cohomology, by the kinetic differential distributional delineation, of a directly associated, kinematically propagated, Hamiltonian Topological Manifold, of which is ideally, here, to exist in a physical environment, in which the gravitational force, is viably non perturbative, at the proscribed proximal locus. 

(Co)Homology-Based topological fields, that are relatively strong in dimensional compactification, tend to bear a more Yau-Exact nature, than ulterior (co)homology-based topological fields, that are relatively less dimensionally compactified, Cartesian-Wise. 

Kinematically propagated Hamiltonian Topological Manifolds, that work to bear a relatively strong Kahler-Based Quotient, that is auspicious in working to facilitate a viably demonstrable lack of net gauge atrophy, often tend to bear a more enhanced tense of aerodynamic wave-tug, in the general process of their fractal of momentum-like permeability, than otherwise analogous, kinematically propagated Hamiltonian Topological Manifolds, that instead, do not work to bear such an implicitly gauge effective tense, of a relatively strong Kahler-Based Quotient. 

A compact Hamiltonian Topological Manifold, that is extremely succinct, in its general Ward-Based aerodynamic permeability, will often tend to work to bear a fairly resolute tense, of Ward-Based aerodynamic permittivity. 

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.