Other Cool Ideas 1

 The wave-based motion of a heuristically-gauged Kahler Hamiltonian Topological Manifold, tends to bear a general permeability, in the process of its kinematic propagation, through the general venue of space-time-fabric, that is here to work to bear, a lower entropic abrasion per Fourier-Related-Progression, than the wave-based motion, of an otherwise analogous Kahler Hamiltonian Topological Manifold, that instead, is here to work to be exhibiting, a metrically-gauged tense, of transferred kinematic propagation. 

Cool Stuff

 The coupling of the i*PI(Del)Action with angular momentum, may often tend to be eminently associated, with the facilitation of the scattering of infrared photons. Furthermore; The coupling of the i*PI(Del)Action with angular frequency, may often tend to be eminently associated, with the facilitation of the formation of chiral-based magnetism. In other words; The coupling of unitary heuristic-gauged magnetic potential with angular momentum, may often tend to work to form the scattering of infrared photons. While the coupling of unitary heuristic-gauged magnetic potential with angular frequency, may often tend to work to form chiral-based magnetism. 

The covariant proximal local presence of imaginary charge, often tends to be eminently associated, with the alteration of spatial dimensionality. The greater that the eminently corroborative positive ordering of Nijenhuis (imaginary) physical impartation is to be, that is here to be directly associated with the action of a particular incurred imaginary charge, the more that the respectively associated spatial dimensionality, will tend to be decreased. Furthermore; The greater that the eminently corroborative negative ordering of Nijenhuis (imaginary) physical impartation is to be, that is here to be directly associated, with the action of a particular incurred imaginary charge, the more that the respectively associated spatial dimensionality, will tend to be increased. 

Free-Will often tends to be more eminently corroborative with heat than with sound, whereas, Imagination often tends to be more eminently corroborative with sound than with heat. 

Free-Will often tends to be more potentially corroborative with entropy than with charge, whereas, Imagination often tends to be more potentially corroborative with charge than with entropy. 

Free-Will tends to be more restrained in a metric-based manner than in a time-wise-related manner, whereas, Imagination tends to be more restrained in a time-wise-related manner than in a metric-based manner. 

A holomorphic driven chiral-based magnetic eigenstate, tends to be eminently associated, with a negative charge. Whereas; An anti-holomorphic driven chiral-based magnetic eigenstate, tends to be eminently associated, with a positive charge. 

Adjacent Holomorphic driven chiral-based magnetic eigenstates, tend to spin asymmetrically, relative to each other, due to the ramifications of mirrored symmetry. 

Holomorphic driven chiral-based magnetic eigenstates, tend to bear the opposite charge than what is expressed from the likes of antiholomorphic driven chiral-based magnetic eigenstates. Anti chiral charges, or, in other words, opposite charges, attract. 

Holomorphic driven chiral-based magnetic eigenstates, when individually taken, tend to be comprised of, by a more dimensionally compact Hamiltonian topological manifold, than their eminently corroborative anti holomorphic driven chiral-based magnetic eigenstate counterparts, when individually taken, in a respectively considered manner. 

Chern-Simons Invariant gauge-action recalibration due to the kinetic interplay of fractional spin, tends to spontaneously work to form the covariant proximal local presence, of holomorphic driven chiral-based magnetic eigenstates. Whereas; Chern-Simons Invariant gauge-action recalibration due to the kinetic interplay of whole spin, tends to spontaneously work to form the covariant proximal local presence, of anti holomorphic driven chiral-based magnetic eigenstates. 

When a mass-bearing Hamiltonian Topological Manifold, is to work to bear a fractional spin, the  corroborative equal and opposite reaction to the general likings of this, of which is here to be eminently associated, with the directly related harmonic re-calibration of Chern-Simons Invariant gauge-action, is thence to work to facilitate the formation, of a holomorphic driven chiral-based magnetic eigenstate, of which is here to spontaneously generate, the covariant proximal local presence, of a negative charge.

When a mass-bearing Hamiltonian Topological Manifold, is to work to bear a whole spin, the corroborative equal and opposite reaction to the general likings of this, of which is here to be eminently associated, with the directly related harmonic re-calibration of Chern-Simons Invariant gauge-action, is thence to work to facilitate the formation, of an anti holomorphic driven chiral-based magnetic eigenstate, of which is here to spontaneously generate the covariant proximal local presence, of a positive charge.

Let’s say that one is to consider, here, in a given arbitrary case scenario, two different and distinct commutations of wave-based transference. Both of which, here, are to express the same piecewise continuous quantum, of net physical energy. One of such commutations of wave-based energy, is here, in this particular case scenario, to express a relatively stronger pulse, than the other of the two. That commutation of wave-based transference of the two, that exhibited the stronger pulsation, is here to be exhibiting the greater scalar magnitude, of Fourier-Related-Progression. 

Let’s say that one is here to consider, two different and distinct commutative wave-based transferences. One is to be binary metric-gauged, while the other is to be unitary metric-gauged. Otherwise, these two different respective commutative wave-based transferences, are to be viably analogous. That implicit transference of wave-related phenomenology, that is here to be binary metric-gauged, will thereupon tend to spontaneously work to exhibit, a stronger Fourier-Related-Progression, than the other one. 

More Nifty Physics Ideas

 Closed loop super strings, that are not eminently electromagnetic by nature, will tend to bear a viable tense of metric-gauge incursion. Furthermore; Open loop super strings, will often tend to bear a viable tense of heuristic-gauge incursion. 

When Fadeev-Popov-Trace eigenstates are eminently efficient, via their spatial translation, this will often tend to be eminently corroborative, with the physical venue, of metric-gauge. Whereas; When Fadeev-Popov-Trace eigenstates are eminently efficient, via their time wise translation, this will often tend to be eminently corroborative, with the physical venue, of heuristic-gauge.

Discrete energy quanta, that work to bear an abelian light-cone-gauge topology, tend to bear Fadeev-Popov-Trace eigenstates, that are eminently efficient, in lieu of the general venue, of there directly associated spatial translation. Furthermore; Discrete energy quanta, that work to bear a non abelian light-cone-gauge topology, tend to bear Fadeev-Popov-Trace eigenstates, that are eminently efficient, in lieu of the general venue, of their directly time-wise translation. Abelian light-cone-gauge phenomena, tend to move in the general direction of metric efficiency. Whereas; Non Abelian light-cone-gauge phenomena, tend to move in the general direction of durational efficiency. 

Abelian light-cone-gauge eigenstates, often tend to exhibit an enhancement of entropic physical characteristics, when the eminently corroborative Fadeev-Popov Trace eigenstates, are metrically perturbative. Whereas; Non Abelian light-cone-gauge eigenstates, often tend to exhibit an enhancement of entropic physical characteristics, when the eminently corroborative Fadeev-Popov Trace eigenstates, are time-wise perturbative.  

Discrete energy quanta, that tend to move in the direction of least distance, often tend to bear the corroborative presence of Fadeev-Popov Trace eigenstates, that are eminently efficient, metric-wise. Whereas; Discrete energy quanta, that tend to move in the direction of least time, often tend to bear the corroborative presence of Fadeev-Popov Trace eigenstates, that are eminently efficient, time-wise. 

The stronger that the internal gauge-action is to be, that is here to be incurred upon a discrete quantum of energy, as a tense of pseudo electromotive impedance excitation, the greater that the spontaneous restraining force is to consequently be, of which is here to tend to metaphorically harness a tense of viable control, over the direction and the other factors of motion, of which are here to be imparted, over the general implicit Lagrangian -Based motion of this. 

The quicker that the harmonic attribute of the i*PI(Del)Action is to spontaneously happen, of which is thence to be eminently physically imparted upon its externalized environment, the more charge generation, that will often tend to be proximal local in covariant occurrence, as taken over time. Whereas; The quicker that the anharmonic attribute of the i*PI(Del)Action is to spontaneously happen, of which is thence to be eminently physically imparted upon its externalized environment, the more of a generation of entropy, that will often tend to be proximal local in covariant occurrence, as taken over time. 

The more kinetic that the infrared energy of a region tends to be, the more entropic that such a region will consequently tend to be. 

Let’s say that the kinetic infrared energy of two different equally heated regions, is to be behaving in the same general manner. One of such regions is to have a lower molar mass than the other. The region of relatively lower molar mass, here, will tend to bear a greater entropy, than the other of such regions. 

Anharmonic Chern-Simons Invariant gauge-action re-calibration, tends to facilitate at working to make the regionally proximal local infrared energy more kinetic. 

The coupling of the i*PI(Del)Action with angular momentum, often tends to enhance an added kinetic effect, upon the regionally proximal local infrared energy. 

The more spurious that local discrete quanta of infrared energy are to behave as, the spontaneously greater that the consequential entropy will tend to be. Furthermore; The more hermitian that local discrete quanta of infrared energy are to behave as, the spontaneously lower that the consequential entropy will tend to be. 

An enhanced kinetic effect, upon the local discrete quanta of infrared energy, tends to be equivocal, to an enhanced scattering, of such stated infrared energy quanta. Therefore; The stronger that the kinetic attribute of infrared energy quanta is to be, the more spurious, and thereby the more scattered, that it will consequently tend to be. Adjacent infrared photons may be said to be scattered, relative to one another, when they are here to exhibit an uneven parity, when this is here to be considered, corroboratively taken. 

Just as physical momentum often tends to be corroborative with heat, and frequency often tends to be corroborative with sound, — entropy often tends to be eminently associated with heat, and charge often tends to be eminently associated with sound. Furthermore; Heat often is associated with a spurious tense, of adhesion/cohesion/repulsion. ;&; Sound often is associated with a hermitian tense, of adhesion/cohesion/repulsion. 

Harmonic sound, often tends to facilitate the generation, of a tense of cohesion. Dissonant sound, often tends to facilitate the generation, of a tense of repulsion. 

Cohesive heat, often tends to facilitate the generation, of a tense of adhesion. Dispersive heat, often tends to facilitate the generation, of a tense of repulsion. 

Charge often tends to facilitate the generation, of an ordered tense, of cohesion/repulsion. Entropy often tends to facilitate the generation, of an unordered tense, of cohesion/repulsion. 

The generation of Dissonant charge, often tends to be eminently associated, with the initially incurred induction facilitation, of the incursion of dissonant sound.