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. 

Cool 4

 The more hermitian that the homotopic dispersion is to be, the more hermitian that the eminently corroborative i*PI(Del)Action will consequently tend to be. 

The more spurious that the homotopic dispersion is to be, the more spurious that the eminently corroborative i*PI(Del)Action will consequently tend to be. 

Through my recent mathematical work, I discovered what should have been an epiphany to me before. By the way, an epiphany is something that should have been really obvious, but it needed to be brought to someone’s attention for clarification. Here is a general example of the basic idea, being in logical support of this epiphany: Let’s say that one were to have an initial Calabi-Yau Manifold, that is here to be differentiating kinematically, in both three different Riemann-Based differential axions & in three different Imaginary-Based differential axions. Next; It’s homotopic dispersion, in the form of a kinetically perturbative homotopic expansion, is to spontaneously have a binary dimensional compactification incurred upon its topological substrate. What this potentially involves, is a binary enhanced tense of isotropic stability, in which one is to eminently go into having both two less Riemann-Based differential axions and two less Imaginary-Based differential axions, yet to where the same general physical operational function of the respective implicit Hamiltonian Topological Manifold is to remain the same, — it’s just that the homomorphic impetus & the angular momentum, of the implicit team of discrete energy, is now to become more succinct in its directional wave-tug, and more trivial isometric in its isotropic vibrational sway. So; In some cases, a dimensional compactification is Not Necessarily directly involving a decrease in the number of present spatial dimensions, — it may often potentially mean a more succinctly aerodynamic angular momentum, that is more restricted in its topological sway, due to the proximal local presence of Kahler-Based Inhibitors, as existent in the Kahler-Based Quotient, to where the implicit team of discrete energy is now to be more of a metaphorical team, by behaving as a more homomorphic and a more isotropically stable set of cohesive energy eigenstates. 

The more isotropically stable that the homotopic expansion is to be enacted as being, the more spontaneously gauge effectual that the projected trajectory of its kinematic propagation, will consequently tend to be locally imparted. 

The general physical condition of Isotropically stable homotopic expansion, often tends to be eminently corroborative, with hermitian homotopic dispersion. 

The general physical condition of Isotropically unstable homotopic expansion, often tends to be eminently corroborative, with spurious homotopic dispersion. 

Hermitian homotopic dispersion, often tends to be eminently corroborative, with the spontaneously gauge effectual projected trajectory, of the related orbifold. 

Spurious homotopic dispersion, often tends to be eminently corroborative, with the lack of effectual gauge-invariance, in the projected trajectory, of the respective related orbifold. 

The general physical condition of Isotropically stable homotopic expansion, often tends to be eminently corroborative, with the presence of gauge-invariance. 

The general physical condition of Isotropically unstable homotopic expansion, often tends to be eminently corroborative, with the lack of gauge-invariance. 

Convergent homotopic dispersion, tends to be eminently corroborative with charge. &; Divergent homotopic dispersion, tends to be eminently corroborative with entropy. 

Hermitian homotopic expansion, tends to be eminently corroborative with convergent homotopic dispersion. Spurious homotopic expansion, tends to be eminently corroborative with divergent homotopic dispersion. 

Convergent homotopic dispersion, tends to work to bear less gauge atrophy, than an otherwise analogous tense of implicitly considered phenomenology, that instead, is to demonstrate a tense of divergent homotopic dispersion. 

Mass-Associated convergent homotopic dispersion, that is heuristically gauged, will often tend to eminently involve, a moving charged microscopic topological entity, that is here to generally be induced, to spontaneously move into the direction of least time. 

Mass-Associated convergent homotopic dispersion, that is metrically gauged, will often tend to eminently involve, a moving charged microscopic topological entity, that is here to generally be induced, to spontaneously move into the direction of least distance. 

Mass-Associated divergent homotopic dispersion, that is heuristically gauged, will often tend to bear gauge atrophy, in its metaphorical effort, to move into the direction of least time. 

Mass-Associated divergent homotopic dispersion, that is metrically gauged, will often tend to bear gauge atrophy, in its metaphorical effort, to move into the direction of least distance. 

Mass-Associated convergent homotopic dispersion, that is heuristically gauged, may often tend to be eminently corroborative, with the general workings, of a kinematically propagated, charged Non Abelian topological manifold. 

Mass-Associated convergent homotopic dispersion, that is metrically gauged, may often tend to be eminently corroborative, with the general workings, of a kinematically propagated, charged Abelian topological manifold. 

Mass-Associated divergent homotopic dispersion, that is heuristically gauged, may often tend to be eminently corroborative, with the general workings, of a kinematically propagated, entropic Non Abelian topological manifold. 

Mass-Associated divergent homotopic dispersion, that is metrically gauged, may often tend to be eminently corroborative, with the general workings, of a kinematically propagated, entropic Abelian topological manifold. 

Cool 3

 The utilization of solar panels, in which light is converted into electrical energy, has the likings of being eminently corroborative, with the general multiplicity of dealing, with a practical application, that uses the Poisson Integral. 

The utilization of electricity to form light, has the likings of being eminently corroborative, with the general multiplicity of dealing, with a practical application, that uses the Green Function. 

The utilization of solar panels, in which light is converted into electrical energy, has the likings of being eminently corroborative, with parametric dimensional compactification. 

The utilization of electricity to form light, has the likings of being eminently corroborative, with parametric dimensional de-compactification. 

Early on in the history of the multiverse, when some of the electromagnetic energy, that was generated into existence, soon after the Big Bang had occurred, was to thereupon become spontaneously converted into electrical energy, that this general occurrence, that again, happened early on in the implicit time line of space and time, was an action of parametric dimensional compactification, that worked to allow for the facilitated development of mass-bearing phenomena, when in conjunction with the primordial Higgs Field, in so as to help, in the furthered evolution of that general space time fabric, that kept being metaphorically tweaked, until physical conditions became what they eventually have become, at this current point in time. 

The photoelectric effect, may often tend to be eminently corroborative, with a given arbitrary genus, of a practical application, of the utilization of the Poisson Integral. Whereas; The Fujikawa Coupling, may often tend to be eminently corroborative, with a given arbitrary genus, of a practical application, of the Green Function. Such inverse physical operations, may often tend to be facilitated, into a tense of induced recursion, to where the presence of light, is to act to facilitate the spontaneously ensuing presence of electrical flow, that is to subsequently act, to facilitate the spontaneously ensuing presence of light, and so forth… . 

The Higgs Field inherently works to help, in the general process of the compactification, of steady state kinetic energy, converted it into mass-bearing energy phenomena. 

Parametric dimensional compactification, often tends to move in the direction of an Abelian light-cone-gauge topology. Parametric dimensional de-compactification, often tends to move in the direction of a non Abelian light-cone-gauge topology. 

Strong parametric dimensional compactification, often tends to be eminently corroborative, to being and or adjusting, to a metric-gauge based Fourier-Related System. Whereas; Strong parametric dimensional de-compactification, often tends to be eminently corroborative, to having a heuristic-gauge based Fourier-Related System.

 Strong parametric dimensional compactification, often tends to be eminently corroborative, with a “pressure-based” Lagrangian-Related Drive. Strong parametric dimensional de-compactification, often tends to be eminently corroborative, with a “puncture based” Lagrangian-Related Drive.