Gauge-Invariant Topological Manifold

 When a compact Hamiltonian Topological Manifold, is to be physically transmitted through a smooth Lagrangian, while yet not acting to bear any Chern-Simons-Related Spurs, when being in the general process of this, that it will consequently tend to spontaneously occur, that the discrete energy impedance, that is here to be eminently corroborative, with the reductional process of such a respective case scenario, will tend to be gauge-invariant. 

An interstellar craft, that is round at its base, when beginning in the proximal local field, of an Anti-Gravitational field, ideally wobbles at both ends, of all four Minkowski-Associated coni axions, by a subtended angling, of ~28.274334 degrees, when preparing for the spontaneous formation, of an artificial worm-hole, yet; An interstellar craft, that is round at its base, when beginning in the proximal local field, of a Heuristic-Gravitational field, on earth, ideally wobbles at both ends, of all four Minkowski-Associated coni axions, by a subtended angling, of ~29.9792458 degrees, when preparing for the spontaneous formation, of an artificial worm-hole.This is interesting, on two different accounts: 1) On a vacuum on earth, light travels at Exactly 2.99792458*10^8 meters per second. &, 2) The apex of the pyramid of Giza, from Egypt, is at a latitude, of Exactly 29.9792458 degrees North Latitude. 

The less entropic, that a given arbitrary tense, of electrodynamic circuitry, is to be, the more likely, that the eminently corroborative net charge, of which is here to be flowing through, such a respective tense of electromotive circuitry, will entail the general likings, of a gauge-invariant flow — to where the eminently associated Hamiltonian Topological Manifold, of which is here to act, as the emanating source, via which such a respective net charge, is thence to be implicitly kinematically propagated on account of, will thereby spontaneously tend to bear the general condition, of exemplifying the reductional characteristics, of the resultant demonstrative exhibition, of behaving as a gauge-invariant topological manifold. 

Decreased energy of heat transport per Kelvin Mole, as exhibited by an eminently corroborative, kinematically propagated, Hamiltonian Topological Manifold, may often tend to spontaneously increase the likelihood, of the covariant proximal local presence of gauge-invariance, to thereby be viably existent, from within the respective Ward-Cauchy Bounds, in which such an implicit team of mass-bearing discrete energy quanta, is here to be in the general process, of being kinetically transferred, over a time span. 

The greater that the number of filled energy levels, in terms of electric shells, is hereupon to be, that there are here to be spontaneously present, in the eminently associated conductor, of the implicit energy levels, of which are in covariant proximal local association, with the electromotive circuitry, when this is taken in terms of the electrodynamic charge-based holonomic substrate, that is here to be of the Hamiltonian Topological Manifold, of which is here to be of the magnetic energy that is kinetically transferred through the conductor, via electromotive current, as taken over the duration in which the net charge, of the implicit cohesive team of magnetic mass-bearing energy eigenstates, is here to be spatially transmitted along, over time, through the structural entity that it is here to be transferring physical conduction into, that it will therefore often tend to occur, that both the entropy level will consequently tend to be lowered, as well as that the electromotive resistance will also thereby also tend to be lowered. This just implied general tendency, will consequently tend to spontaneously enhance the expectation value, that is here to be eminently involved, in increasing the chance that the earlier mentioned Hamiltonian Topological Manifold, will thus be more likely to behave, as a gauge-invariant topological entity. 

The number, of what are termed of as being Landau Lines, is tantamount to being equivocal, to the number of filled energy levels, that are proximal local in covariant association, with the latent physical conditions of the conductor, of which is to bear an electrodynamic transmission, of the charges that are to be delineated, by the eminently corroborative, kinematically propagated Hamiltonian Topological Manifold, in so as to facilitate the generation of an electromotive current, of which is here to act to convey, a corroborative tense of electrical information. 

If and when a particular isotope of a material, is to innately act to bear a relatively high number of filled electrodynamic energy levels — to where the distributional delineation of the implicitly spontaneous consequential eminently corroborative conductive bands, are here to be homogeneous in its covariant electromotive assortment, then, it will often tend to consequently occur, that such a material, may therefore tend to exhibit both a relatively strong fractal modulus & a relatively strong elastic modulus, at the same time. Also as optimal; Such an implicit material, will also tend to bear relatively low electromotive resistance, — particularly at low temperatures, since low temperatures often work to involve a lowered energy of heat transport, lowering entropy. 

Highly conductive materials, that are to spontaneously have homogeneous delineated energy levels distributed within them, will often tend to have the general tendency, of exhibiting an enhanced capacity, of being able to express a relatively strong spring constant, to where, invasive phenomena that may tend to otherwise be potentially hazardous to the externalized structure of a given arbitrary construct, that is to be externally comprised of such an implicit material, will therefore spontaneously be less viably detrimental to the structural integrity of such an implied resilient material, due to not only the relatively strong fractal and elastic modulus hereby present, yet, also, since a strong spring constant, may cause incoming potentially treacherous phenomena, to have an enhanced capacity, of simply rebounding off of the externalized structure of such an implicit material, due to the mentioned strong spring constant, as taken at its outer boundary. 

Highly insulative materials, that are here to exhibit a homogeneous distributional delineation of their electron "clouds," may often tend to work to exhibit, a relatively strong tense, of an elastic modulus.

The greater that the density of electron shells is to be, as taken into consideration, for a molecular structure, the higher that its fractal modulus, will consequently tend to be. 

The more homogeneous that the distributional delineation of electron shells is to be, as taken into consideration, for a molecular structure, the higher that its elastic modulus, will consequently tend to be. 

The more homogeneous that the distributional delineation of electron shells is to be, for a molecular structure, that is to exhibit a relatively high density of such respective electron shells, the greater that its eminently corroborative spring constant, will consequently tend to be. 

I call the general tendency of potentially recursively stabilized structural integrity, that is here to be appertaining, to the reductional effectual physical attributes, of eminently corroborative materials, that work to exhibit an unusually high spring constant, “Homotopic deformation incursion counterbalance.”

The Fourier-Related-Progression, of a net phenomenology, that works to bear, a relatively strong, Homotopic deformation incursion counterbalance, will often tend to result, in thus expressing, a relatively strong, resonant pulsation. 

Miscellaneous Ideas

 The more energy of heat transfer per Kelvin Mole, that is to be proximal local to an electromotive current, that is here to be spontaneously generated in its eminently associated kinematic propagation, the more likely that such an implicit physical situation, will consequently tend to be eminently corroborative, with the likings of a Dolbeault (co)homology, since the implicit entropy that is here to be spontaneously incurred upon such an electromotive current, is thence to be relatively enhanced. 

The less energy of heat transfer per Kelvin Mole, that is to be proximal local to an electromotive current, that is here to be spontaneously generated in its eminently associated kinematic propagation, the more likely that such an implicit physical situation, will consequently tend to be eminently corroborative, with the likings of a De Rham (co)homology, since the implicit relativity lowered entropy that is here to be spontaneously incurred upon such an electromotive current, is thence to be spontaneously dampened. 

Again, implicitly; Lowered energy of heat transfer per Kelvin Mole, facilitates the spontaneous reduction of physical entropy, increasing the equivocal number of eminently corroborative Landau Lines, which thereby works to decrease the eminently associated impedance. 

The lower that the energy of heat transfer per Kelvin Mole is to spontaneously be, the more filled energy states that there will equivocally tend to be, to where there will thence spontaneously tend to thereby be a greater number of eminently corroborative Landau Lines equivocally present, in a covariant manner, from within the proximal local region of implicit electromotive current, to where this particular case scenario of physical current, will therefore tend to express less impedance and more conductivity. 

The cooler of a temperature, that a given arbitrary electromotive system of electrodynamic flow, is to be physically expressing, as taken over the covariant venture of time, the less energy of heat transfer per Kelvin Mole, that the said given electromotive system of electrodynamic flow, is to consequently tend to be physically exhibiting, over the same implicit duration of time, as taken over an eminently corroborative process, of a directly related tense, of a Fourier-Related-Progression, to where such an electromotive system of electrodynamic flow, will thereupon consequently tend to bear a relatively enhanced efficiency of conductivity, when every other viable factor is otherwise analogous, to where such a respective system of implicit current, will thereby tend to bear a relatively stronger cryogenic capacity, to bear a lowered resistance. 

When the Fourier-Related-Progression, of an eminently corroborative Kahler Hamiltonian Topological Manifold, is relatively strong in physical resolution, it will often tend to spontaneously work to bear, a relatively enhanced tense, of resonant pulsation. Whereas; When the Fourier-Related-Progression, of an eminently corroborative Kahler Hamiltonian Topological Manifold, is relatively strong in physical succinctness, it will often tend to spontaneously work to bear, a relatively enhanced tense, of resonant frequency. 

A Fourier-Related-Progression, that is eminently resolute, will often tend to move, in the direction of least distance. Whereas; A Fourier-Related-Progression, that is eminently succinct, will often tend to move, in the direction of least time. 

A Fourier-Related-Progression, that is eminently resolute, will often tend to bear an enhanced tense of angular momentum. Whereas; A Fourier-Related-Progression, that is eminently succinct, will often tend to bear an enhanced tense of angular frequency. 

A kinetically driven, recursively stable, De Rham Kahler Hamiltonian Topological Manifold, will often tend to bear, both eminence in its Fourier-Related resolution, and, eminence, as well, in its Fourier-Related succinctness. 

A viably De Rham Kahler Hamiltonian Topological Manifold, that is both strongly resolute & strongly succinct, in lieu of its general flow of eminently corroborative Fourier-Related Progression, will often tend to bear a tense of angular momentum, that is heat generative, as well as also tending to work to bear a tense of angular frequency, that is sound generative. The more efficient that such a De Rham Kahler Hamiltonian Topological Manifold is to be, the less heat and the less sound, that it will tend to generate. 

Unitary heuristic-gauge magnetic potential, is the common denominator, so to speak, between charge & entropy. Unitary heuristic-gauge magnetic potential, is what I happen to have termed of, as being the i*PI(Del)Action. When a moving team of cohesive discrete mass eigenstates, is to change in its speed and or direction, this process tends to effect the piecewise continuity and or the morphology, of the said “ teams” implicit contortion-based symmetry. This, then, works to facilitate the generation, of the respective stated i*PI(Del)Action. When such unitary heuristic-gauge magnetic potential, is to interact, in a Gliosis-Based manner, with the regionally proximal local presence, of the eminent angular momentum, this will often tend to facilitate the formation of entropy. Whereas; When such unitary heuristic-gauge magnetic potential, is to interact, in a Gliosis-Based manner, with the regionally proximal local presence, of the eminent angular frequency, this will often tend to facilitate the formation of charge. Entropy tends to scatter things, while charge often brings things together. Either way, both are big influencers of repulsion/adhesion. 

The generation of dissonant charge, often tends to bear the general physical attribute of entropy. This, thereby, is often brought into facilitation, by a re-calibrated Chern-Simons Invariant gauge-action, that works to bear, both harmonic & anharmonic ramifications. Furthermore; When the just mentioned general case scenario is to occur, this often tends to be eminently associated, with a set of one or more i*PI(Del)Action eigenstates — coupling with a directly associated set of one or more respective angular frequency eigenstates, while spontaneously, as this is to be occurring, there is to be a proximal adjutant, immediately externalized occurrence, if you can see what I’m trying to say, of an eminently corroborative coupling of another set of one or more i*PI(Del)Action eigenstates, with with a respectively different set of one or more angular momentum eigenstates. This, hereupon, tends to form a physical environment of magnetism, in which there is to be a tense of chiral-based magnetism, in the overlapping presence of physical disorder. 

The Incursion Of Electromotive "Hissing"

 The incursion of electromotive "hissing," may often be facilitated, by the interaction of spurious heat with sound. Heat is often capable of working to facilitate the presence of entropy. And; Sound is often capable of working to facilitate the presence of consonance. TO BE CONTINUED! SINCERELY, SAM ROACH.

How Cohomology Works To Help Form Electromotive Attraction

Two different covariant cohomology-related phenomena, that are here to have the opposite spin, (opposite parity), will often tend to reverse-fractal, into two different covariant charge-related phenomena, that are here to have the opposite charge (opposite chirality). Initially, Again; Electromotive charge, tends to be formed, by a tense of a kinetically symmetrical braided cohomology-related covariant structure, that is here to work to bear a directly associated hermitian Lagrangian. Now; Picture the covariant topological manifold, of two different individually taken charge-based eigenstates, that may be taken down to a fractal level, in lieu of working to consider these, at the level of behaving as two different individually taken cohomology-related structures. Let us now imagine, that both of such cohomology-related structures, are here to work to exhibit the display, of giving off the opposite directional tense of "spin." Use the right hand rule, in so as to help you to imagine this better. This will consequently work to indicate, the covariant kinematic case, of two different unique and distinct "charged" eigenstates, that are here to tend to be tugged toward each other. As basically everyone knows, two different charges that attract each other, are to work to bear the opposite chirality. This may help you to better understand, as to why I have inferred/mentioned, that such symmetrically braided cohomology-related structures, that work to bear the opposite parity, will often tend to reverse-fractal, into charge-related structures, that work to bear the opposite chirality. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! SAMUEL DAVID ROACH.

An Interesting Analogy

Even though what I term of as being the force of pressurized vacuum, the point commutative force, and also the electromotive force, -- are three different basic types of force -- here is an analogy that I think is interesting:

The force of pressurized vacuum is to "voltage," what the point commutative force is to "amperage."
I will continue with the suspense later!  To Be Continued!  Sincrely, Samuel David Roach.

The Seven Basic Physical Forces Of Nature

The seven basic physical forces of nature are:

1) The Force Of Thought.  (The harmonized articulation of which, may be called "love.")

2)  The Force Of Pressurized Vacuum.  (The force that unifies the construction of discrete energy.)

3)  The Point Commutative Force.  (The force that works to move discrete quanta of energy.)

4) The "Strong Force."  (The force that works to bind sub-atomic particles together.)

5)  The Electromotive Force.  (The force that allows for the existence of electromagnetism.)

6)  The Force Of Gravity.  (The force that works to inter-relate mass-bearing phenomena.); &,

7)  The Weak Force (The force of spontaneous radioactive decay.)

To Be Continued!  Sincerely, Samuel David Roach.  (Because, "All Minds Matter!").

Compleltion Of The Rarita Structure -- Forces

Do you remember me mentioning to you on this blog, something to the effect of (but not specifically this exactly, though) -- that the multiplicit light-cone-gauge eigenstate acts as the 'opening phenomenology' of the Rarita Structure, and that the multiplicit gauge-bosons act as the 'closing phenomenology' of the Rarita Structure?  Furthermore, it is those vibrational oscillations that are formed, by the plucking action of the multiplicit gauge-bosons upon the correlative multiplicit second-order light-cone-gauge eigenstates (which is here to form the here correlative Schwinger-Indices) -- that work to behave, in so as to work to form the exhibition of the four general forces of nature (these of which are -- the strong force, the electromotive force, the gravitational force, and the weak force).  This said plucking activity by the so-eluded-to E(6)XE(6) strings (these just mentioned strings of which act as the said gauge-bosons), works, as well, to help at making what would otherwise be a maxed-out Minkowski or holographic space (flat space), to instead, be a Hilbert or volume-based space.  (This would then work to help at making a 26 spatial dimensional world, instead, be a 32 spatial dimensional world -- for each of the three individually taken sets of parallel universes, that are here to exist in time and space.)  So -- it is the very nature, as to what helps to work to make a maxed-out flat-based space behave, instead, as a maxed-out volumed space, -- that works to form those vibrational oscillations, that are here to ripple along the Rarita Structure -- in so as to work to influence, as to what the correlative exhibitions are to be, as to the corresponding display of the four physical forces of space and time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Gauge-Bosons And Forces

Often, when gauge-bosons work to form a different general genus -- as to the manner in which these act in so as to "pluck" their directly corresponding second-order light-cone-gauge eigenstates -- this may often work to perturbate or alter the general genus of the force that may be exhibited out in the Ward-Cauchy-related bounds of the substringlar.  For instance -- one general genus of such a "plucking" may work to help at forming the strong force.  Another general genus of such a "plucking" may work to help at forming the electromotive force.  Another general genus of such a "plucking" may work to help at forming the gravitational force.  And another general genus of such a "plucking" may work to help at forming the weak force.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.