Wess-Zumino Action -- Jacobean Manifold Harmonization

 In certain cases; When a Wess-Zumino Action, is to be incurred upon a group of two or more initially adjutant Noether-Based mass-bearing cohesive sets of discrete energy quanta, this may sometimes tend to work to facilitate the general process, of what I happen to term of, as being, a tense of the Jacobean Manifold Harmonization (JMH). TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. (1989).

Back To Basics: Covariant Cohesive Sets Of Mass-Bearing Discrete Energy Quanta -- Covariant Cohomological Structures -- Covariant Lagrangian-Based Paths

 Kinematic Fourier-Related covariant Noether-Based mass-bearing cohesive sets of discrete energy quanta, are often to tend to work to bear respective covariant cohomological structures, to where these will, as well, often tend to bear covariant Lagrangian-Based paths. TO BE CONTINUED! SAM ROACH.

Sound/Heat -- Group-Attractors/"Ghost-Based Inhibitors"

 The phenomenology of sound, as incurred upon a group of Noether-Based mass-bearing cohesive sets of discrete energy quanta, when done in the right manner, may often have the general potential tendency, of having the capability, of working to form a set of one or more, of what I have termed of as being, the general phenomenology, of "group-attractors." Whereas; The phenomenology of heat, as incurred upon a group of Noether-Based mass-bearing cohesive sets of discrete energy quanta, when done in the right manner, may often have the general potential tendency, of having the capability, of working to form a set of one or more, of what I have termed of as being, the general phenomenology, of "ghost-based inhibitors." I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, Samuel David Roach.

Perturbation In The Tense Of The Dispersion Of Local Homotopic Residue

 Often, when there is to be a spontaneous perturbation, in the relative tense of the dispersion of a local superstring-related set of homotopic eigenstates, that are here to be eminently related, to the course of the kinematic activity, of a directly corresponding Noether-Based mass-bearing cohesive set of discrete energy quanta, this will often work to alter the relative course of motion, of which such a directly associated gauged-action, that the just eluded-to "team" of mass-bearing energy, was here to have initially been interdependently acting in conjunction with, to where both the del of the gauged-action appertaining most eminently with the Hamiltonian, as well as the del of the gauged-action appertaining most eminently with the Lagrangian, is thence to be enacted upon as well, to where, this will thereby often have the general tendency, of working to alter the dimensional-related-pulsation of the earlier said Noether-Based mass-bearing cohesive set of discrete energy quanta, to where, this will often tend to work to help form, a consequentially resultant set of metric-based Chern-Simons singularities, of which are here to often tend to be produced, when there is to become the existence, of a definitive viable proximal local presence, of such an inferred genus of perturbation, as incurred upon the initially stated superstring-related correlative respective set of homotopic eigenstates. TO BE CONTINUED! SINCERELY, SAMUEL ROACH. (1989).

Coupled Braided Cohomology

 When two different given arbitrary covariant sets of braided cohomology, are to be coupled in an electrodynamic manner, the net force modulus of the resultant net structural integrity, that is thus to be formed, in lieu of this, will thereby often tend to be enhanced. TO BE CONTINUED! SAMUEL ROACH. (1989). I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED!

Yau-Exact Mass-Bearing Cohesive Sets Of Discrete Energy Quanta

 Heuristically Yau-Exact Noether-Based mass-bearing cohesive sets of discrete energy quanta, tend to work to have a greater capability of conserving homotopic residue more efficiently, than other Noether-Based mass-bearing cohesive sets of discrete energy quanta do. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. (1989).

Perturbation Of Chern-Simons Invariants -- Efficiency Of Electrical Circuitry

 In a given arbitrary electrical circuitry, those Metric-Gauge-Related Eigenstates, that are Anharmonic in vibration, that are here to be emitted, via the perturbation of those Chern-Simons Invariants, that are here to be exhibited, by the motion of those composite charged mass-bearing cohesive sets of discrete energy quanta, that are here to work to form the individually taken electrons, that are here to work to comprise the electricity, of such a respective given arbitrary electrical circuitry, will often have the tendency, of working to Increase The Inefficiency, of such a stated respective electrical circuitry; Whereas -- In a given arbitrary electrical circuitry, those Metric-Gauge-Related Eigenstates, that are Harmonic in vibration, that are here to be emitted, via the perturbation of those Chern-Simons Invariants, that are here to be exhibited, by the motion of those composite charged mass-bearing cohesive sets of discrete energy quanta, that are here to work to form the individually taken electrons, that are here to work to comprise the electricity, of such a respective given arbitrary electrical circuitry, will often have the tendency, of working to Increase The Efficiency, of such a stated respective electrical circuitry.TO BE CONTINUED LATER! SINCERELY, SAMUEL DAVID ROACH.

Scalar Amplitude Of Torsional Wave-Tug

 Let us initially consider two different given arbitrary covariant mass-bering cohesive sets of discrete energy quanta (as in a "team"of mass-bearing superstring), that are here to both be isotropically spinning at the same relativistic rotational rate, when this is here to be taken, in relation to the correlative motion of electromagnetic energy, as well as that both of such respective mass-bearing cohesive sets of discrete energy, of such a given arbitrary case scenario, are also to be traveling transversally at the same relativistic rate, when this is here to be taken in relation to the motion of electromagnetic energy. Both of such cohesive mass-bearing sets of discrete energy, are here to work to be exhibiting the general nature, of displaying a tense of a Noether-Based Flow. Next; One of such stated covariant mass-bearing cohesive sets of discrete energy quanta, is here to be working to exhibit the display, of a larger number of spatial dimensions, than the other of such stated covariant mass-bearing cohesive sets of discrete energy quanta. Otherwise, both of such inferred "teams" of discrete energy, are here to behave in a relatively similar manner. That mass-bearing cohesive set of discrete energy quanta of the two, that is here to be exhibiting the display of a larger number of spatial dimensions than the other one, will consequently quite often tend to result, in working to exhibit the display, of a higher scalar amplitude of torsional wave-tug, upon its immediately external environment, than the other of such stated mass-bearing cohesive sets of discrete energy quanta, that are of such a respective given arbitrary case scenario. I WILL CONTINUE LATER! SAM ROACH.

Homomorphic Field -- Acting In Unison

 When two different mass-bearing cohesive sets of discrete energy quanta, are to work to bear a homomorphic field amongst each other, these two different said mass-bearing cohesive sets of discrete energy quanta,will thereby consequently tend to act in unison with one another, over time. Sam Roach.

The Jacobean Manifold Harmonization (JMH)

 When two or more initially different and distinct covariant mass-bearing cohesive sets of discrete energy quanta, are to be spontaneously brought into an interdependent tense of static equilibrium, -- I call this general type of a Ward-Cauchy-related "behavior," the Jacobean Manifold Harmonization (JMH). SAM ROACH.

Indices Of Eminent Dispensation Of Energy Quanta (My Take)

 Let us consider the following perception: Initially: Let's first stipulate, that we will here treat the individually taken physical forces of nature, as respective "causes"; and that we will also treat the main influences, that are here to be formed by such implied forces, as the respective "effects." Let us next say; arbitrarily, that the multiplicity of the individually taken physical forces of nature, are here to act, upon the topological manifolds, of that physical stratum, which is of the correlative respective cohesive sets of each of such inferred discrete energy quanta. That general phenomenology, which is here to be appertaining to those continually expended indices, that are of the eminent dispensation of the metrical Lagrangian-Based flow, that is of the multiplicity of the respective individually taken cohesive sets of discrete energy quanta, works to help at forming those earlier mentioned "main influences," that are here to work to display the exhibition of those physical attributes, that are here to work to appertain to the demonstrable expression of such said "forces," as taken over the course, of a given arbitrary duration of correlative time. Sam Roach.

As To Altering The Initial Polarization-Related Effect, Of Two Different Physical Li-Based Groups

 Let us say, one were initially to have two different and distinct Li-Based groups, that were here, to initially be adjacent to one another, at a level that was here to be Poincare to the eminently inferred region, at which these two different and distinct inferred cohesive sets of discrete energy quanta, were here to be iterating at -- at a virtual metaphorical "snapshot" of duration, to where such a said "snapshot" in "time," was here to be taken, over the course of a respective given arbitrary iteration of BRST. Let us next stipulate, that these two different and distinct cohesive sets of discrete energy quanta, during such an iteration of BRST -- are to be delineated at such a general given arbitrary distribution-related manner -- to where such inferred sets of discrete energy quanta, are here to bear a covariant tense of a Nijenhuis Orthogonal nature (which is here to bear a relatively strong manner of conformal invariance, at a vantage-point, that is Poincare to that internal reference-frame, that is here to be of the eminent field-density, of the so-inferred region), at which the said sets of energy quanta, are to be both co-determinable and co-differentiable, as those composite superstrings of discrete energy permittivity, that are here to be working to make-up the external structure of such inferred "teams" of discrete energy quanta, are to be working to display the general gauge-metric-related exhibition, by which the general virtual standstill of the kinematic activity at BRST, is thence to occur. Let us next stipulate, that these two respective distinctly different "teams" of energy, are here to be Polarized -- the one from the other, -- due to the general Noether-related norm-based physical condition, that the covariant tense of the dual orthogonal projection, that is here to be existent between/amongst these two said "teams" of discrete energy, is here to be of a Nijenhuis dual state of norm-related projection  -- by which these two different Li-Based groups, that are here to be working to bear a tense of a Ward-Cauchy-related manner of norm-related projection -- are thence to be "encoded for," as belonging to two different universal settings. (Each of such individually taken Li-Based groups, is to be of a parallel universe from one another, when this is here to be taken, in correlation of the one to the other, and vice-versa), -- while all the more, this given arbitrary case scenario is to be considered, As this is here to be taken, over a basically "Laplacian" general format of stipulation. Now here's the "catcher." What If one were to alter the inferred covariant norm-conditions of each of such cohesive sets of discrete energy quanta -- the one towards the other, and vice-versa, to where the general initially considered Nijenhuis tense of orthogonal behavior, that we were just starting to discuss here, -- were now to bear a kinematic perturbation, into spontaneously and consequentially, ensuing to change into a set of two different and distinct geometric groups (groupings), that are thence to result, into working to form a case scenario, by which one is now to have two different and distinct cohesive sets of discrete energy quanta, that are now to work to bear a norm-related geometry, in which the inferred physical spaces discussed here, will now work to bear a covariant Riemann-Related geometry, that is here to be of a Real Riemann tense of norm-related projection. If and when this is here to happen in such a given arbitrary case scenario, these two different initially inferred unique "teams" of physical spaces, will then tend to end-up resulting, in working to display the exhibition, of two different and distinct sets of energy quanta, that are, at this point in duration, to be of the same universal setting. To Be Continued1 Sincerely, SAMUEL DAVID ROACH. (1989).

Legendre Homology, And Energy As Motion

 The general phenomenology of Legendre (co)homology, is directly eminent to the multiplicity of the mappable-tracing of the kinetic wave-tug -- that is here to be applied to the multiplicity of mass-bearing cohesive sets of discrete energy quanta, in so as to allow for matter to be in motion. SAMUEL ROACH.

Hermitian Wave-Tug And Correlative Fractal Modulus

 Let us initially consider two different covariant mass-bearing cohesive sets of discrete energy quanta, of which are here to be in the process of being conveyed, by the kinetic transfer of a correlative Legendre (co)homology, via a unitary Lagrangian; to where these inferred mass-bearing sets of discrete energy quanta, are here to both be exhibiting the same relativistic scalar amplitude of a Majorana-Weyl-Invariant-Mode. That mass-bearing cohesive set of discrete energy quanta of the two, that is here to be working to exhibit a stronger holomorphic hermitian wave-tug, as it is here to be in the process of being conveyed through the workings of a De Rham cohomology, over a discrete duration of time (via a directly corresponding Fourier Transformation), will tend to bear a greater probability, of working to bear a greater scalar amplitude of a fractal modulus, than the other of the two mentioned mass-bearing cohesive sets of discrete energy quanta. To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).

The Majorana-Weyl-Invariant-Mode, And The Rest State Of Mass-Bearing Sets Of Discrete Energy Quanta

 It is the multiplicity of the general exhibition of the Majorana-Weyl-Invariant-Mode, that works to be the primary type of an influence, -- that is here to work to help in allowing, for mass-bearing cohesive sets of discrete energy quanta, to have the general capacity, of being able to be brought into a "state of rest." SAMUEL DAVID ROACH.

Recursively Smooth Ricci Flow -- Anti Gravity

A Recursively smooth Ricci Flow, that is here to be due to the application of anti gravity, upon the topological manifold of a spinning interconnected conglomeration of mass-bearing cohesive sets of discrete energy quanta, tends to work to decrease the inhibition of the spatial transference of such an inferred general genus of a topological manifold, in so as to be able to tend to free-up the potentially ensuing transversal motion, of such a said spinning interconnected conglomeration of mass-bearing cohesive sets of discrete energy quanta. I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL.

Isotropic Stability And Magnetism

 Molecular lattices that are here to be comprised of, by many cohesive sets of isotropically stable mass-bearing discrete energy quanta -- tend to bear a greater scalar amplitude of magnetism, than other types of molecular lattices, that are not to be comprised of as such. To Be Continued! Sincerely, SAM ROACH.

Homeomorphic Isotropic Stability — High Tense Of Majorana-Weyl-Invariant-Mode

 Isotropically stable mass-bearing cohesive sets of discrete energy quanta, that are here to be spatially transferred in a homeomorphic manner, — by the kinetic assistance of a Legendre tense of (co)homology, tend to work to bear a relatively higher scalar amplitude of a Majorana-Weyl-Invariant-Mode — to where this will often tend to be associated in one manner or another, with a charged particle, that is here to be in the process of being spatially conveyed, with a relatively low scalar magnitude of electrical resistance. SAM.

Isotropic Flow And Capacitance/Conductance

 A banded group of isotropically stable cohesive sets of discrete energy quanta, tends to be more facilitated  at working to form a homeomorphic flow; than a banded group of isotropically unstable cohesive sets of discrete energy quanta does. Furthermore; the homeomorphic flow of a banded group of isotropically stable cohesive sets of discrete energy quanta, tends to bear both a greater capacitance and a greater conductance; than the homeomorphic flow of a banded group of isotropically unstable cohesive sets of discrete energy quanta does. I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL.

Homeomorphic Flow Of Isotropically Stable Phenomenology

 A homeomorphic flow, that is of a banded group of isotropically stable cohesive sets of discrete energy quanta, tends to work to display, both a relatively higher capacitance and a relatively higher conductance; than a heteromorphic flow, that is of an otherwise similar banded group of isotropically stable cohesive sets of discrete energy quanta. I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).