Inverted Energy-Charge

 The proximal local presence of metric-gauge holonomy Per Sub-Cohomology-Related eigenstate, tends to work to form the consequentially accelerated proximal local presence, of a fractal of “inverted energy-charge.”  I will continue with the suspense later! To Be Continued! Sincerely, SAM ROACH. (1989).

Sub-Cohomology

 Let me soon introduce to you, a new concept that I have been thinking of lately. This concept appertains, to the Ward-Cauchy presence, of a fractal of Cohomology. Just as Cohomology appertains to the “physical memory” of the general interaction, of super strings With point particle-related physical norm-state-projections (such as zero-norm-state-projections, Campbell norm-state-projections, Hausendorf norm-state-projections, And Campbell-Hausendorf norm-state-projections); — That inferred fractal of Cohomology, of which I am to name of here, as being on the order of acting as Sub-Cohomology eigenstates, — may more aptly be described of as being, the “physical memory” of the general interaction, of first-order point particles With zero-point-energy. The higher that the directly corresponding Beti number is to be, — that is here to be directly associated with the metric-related gauging of the spatial dimensionality, of the respective corroborative super strings, — the greater that the scalar magnitude will consequently tend to be, of the proximal local presence, of the directly appertaining Sub-Cohomology eigenstates, that are thence formed. Consequentially; the lower that the directly corresponding Beti number is to be, — that is here to be directly associated with the metric-gauging of the spatial dimensionality of the respective corroborative super strings, — the smaller that the scalar magnitude will consequently tend to be, of the proximal local presence, of the directly appertaining Sub-Cohomology eigenstates, that are thence formed. SAM (1989). 

Reverse-Fractal Into Highly Conductive Phenomenology

 Mass-Bearing Noether-based superstrings of discrete energy permittivity, that bear a strong tense of isotropic stability, have the general tendency, of being able to reverse-fractal towards the general attribute, of directly associating with phenomenology, that are to work to exhibit a high tense of magnetism. Furthermore; phenomenology that are to exhibit a high tense of magnetism, tend to reverse-fractal, towards the general attribute, of directly associating with phenomenology, that are to work to exhibit a high tense of conductivity. Consequently; mass-bearing Noether-based superstrings of discrete energy permittivity, that bear a strong tense of isotropic stability, often tend to have the general tendency, of being able to reverse-fractal towards the general attribute, of directly associating with phenomenology, that are to work to exhibit a high tense of conductivity. To Be Continued! Sincerely, SAMUEL DAVID ROACH.

Regional Swipe Inhabitation

 Let us say that one were to have two different Noether-based mass-bearing super strings of discrete energy permittivity. Over a given arbitrary Laplacian condition, both of such said strings, are to work to bear the same Lorentz-Four-Contraction; as well as that both of such said strings, are also to work to bear the same general tense of a swivel-like contour. However; one of such super strings of discrete energy permittivity, is to have a higher spatial dimensionality than the other one. Due, in part, to the increase in the tensor-related set of attributes, that are here to be directly corresponding, to the manner by which the correlative partition-based discrepancies, that are here to be appertaining to the string that is exhibiting a higher number of spatial dimensions, is to be delineated — this situation will thereby consequently tend to result, in the general physical Ward-Neumann-related condition, by which both of such said strings, will thereby tend to exhibit basically the same scalar magnitude of “regional-swipe-inhabitation” as each other, — over the thus inferred Laplacian-based physical condition, in which both super strings of discrete energy permittivity, are to be compared, in a manner that is both covariant, co-determinable, and co-differentiable, via the “perspective” of a central coni-point, during the same venue of iteration of the inferred group-related instanton. I will continue with the suspense later! (1989). Sincerely, SAM ROACH.

Operations That A Cohesive Set Of Discrete Energy Quanta May Perform

 A given arbitrary mass-bearing cohesive set of discrete energy quanta, that is gauged in an isotropically stable manner — in so as to exhibit a group action — may perform between one to four different specific “impelling” tasks, over the durational span of a relatively transient sequential series of group-related instantons. (As this is here to be considered to be taken, over an evenly-gauged Hamiltonian eigenmetric.) I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach. (PHS 1989).

Unilateral Direction-Related Wave-Tug

 Let us initially consider two different tachyon-related mass-bearing cohesive sets of discrete energy quanta. One is to work to bear a Fourier-related gauged-action, that is here to be acting as the holonomic substrate of a monomial group action; whereas, the other implied set of cohesive discrete energy quanta, is to work to bear the Fourier-related gauged-action, that is here to be acting as the holonomic substrate of a quadranomial  group action. That set of discrete energy quanta of the two, that is here to be of the nature of acting as an entity, that is here to be exhibiting the behavior of a monomial group action, will tend to work to bear a tachyon-related Nijenhuis impedance, that is to exhibit a direction-related wave-tug, that is here to be delineated in a Li-antichiral-related manner, when in relation to the directly corresponding spatial translation, that is of the correlative angular momentum eigenstate, that is of its covariant co-differentiation with the correlative adjutant proximal local tachyon-related holomorphic permittivity, that is here to be most directly associated with the innate superstring-related directional “drive,” that is of the proximal local discrete energy permittivity, of such a given arbitrary case scenario. However; that set of discrete energy quanta of the two, that is here to be of the nature of acting as an entity, that is to be exhibiting a quadranomial group action, will tend to work to bear a tachyon-related Nijenhuis impedance, that is to exhibit a direction-related wave-tug, that is here to be delineated in a manner, that is of both a Real Riemannian and of a positively chiral nature, when in relation to the directly corresponding spatial translation of the correlative angular momentum eigenstate, that is of its covariant co-differentiation with the correlative adjutant proximal local tachyon-related holomorphic permittivity, that is here to be most directly associated with the innate superstring-related directional “drive,” that is of the proximal local discrete energy permittivity, of such a given arbitrary case scenario. This consequently tends to work to make the said tachyon-related holomorphic permittivity — that is, in the particular case, of the superstring-related set of discrete energy quanta, that is here to be acting as a quadranomial group action, to consequently tend to result, in working to bear a unilateral direction-related wave-tug, with the directly corresponding metric-gauge eigenstate, that is most proximal local to the eminent spur in the covariant co-differentiation, that is of the kinematic activity of its correlative tachyon-related Nijenhuis impedance. (1989). To Be Continued! Sincerely, SAM ROACH.

Tachyon-Related Nijenhuis Impedance

 When one is to have a mass-bearing cohesive set of discrete energy quanta, that is here to be behaving in a tachyon-related manner, — the more spatial dimensions that such a said set of discrete energy quanta is to be exhibiting, over a set duration of time, the more acute that the angling of its directly corresponding Nijenhuis impedance will tend to be, that is here to be imparted upon the correlative gauge-action, of the proximal local angular momentum field eigenstate, that is related to the co-differentiable permeability of the said mass-bearing cohesive set of discrete energy quanta. For example: Let us consider two different cases of such inferred sets of mass-bearing discrete energy quanta. One of such sets is to be of a three spatial dimensional nature, while the other of such sets is to be of a six spatial dimensional nature. Both of such sets of discrete energy quanta, are here to be behaving as tachyons; as well, as that both of such sets of discrete energy quanta, are otherwise to be behaving in basically the same general manner of a covariant spatial translation — over a discrete quantum of relativistic time, — as taken over the vantage-point of a central coni-point, that is here to be translated through space, over an evenly-gauged Hamiltonian eigen-metric. The just mentioned mass-bearing set of discrete energy quanta, that is here to be exhibiting the nature of behaving as a superstring-related entity, involving six spatial dimensions, will consequently tend to bear a smaller subtended angle of a Nijenhuis impedance, that is here to be imparted upon the correlative gauge-action, of the proximal local angular momentum field eigenstate, that is related to the co-differentiable permeability of the said mass- bearing cohesive set of discrete energy quanta. (1989). To Be Continued! Sincerely, Samuel David Roach.  

Centripetal Force And Charged Particle

 Let’s consider a mass-bearing cohesive set of discrete energy quanta, that is to be rotating, via a parabolic path, that is here to also be simultaneously tugged into one specific transversal direction, over a given arbitrary discrete duration of time. Let us now consider, that there is here to be a designated group action, of which is to work to involve a cohesive operation of many individually taken inferred sets of cohesive energy quanta. The greater that the correlative centripetal force, that is here to be applied to an overall set of the multiplicity of a charged mass-bearing cohesive set of discrete energy quanta, over the earlier implied duration of time, the stronger that the angular momentum will tend to be, — as this is here to be taken, in lieu of the implied transversal direction in which such a herein stated set of discrete energy, that is here to be operating to perform one common function, is to be tugged through (upon), to where the just implied act of torsion, will consequently tend to work to increase the resultant aerodynamics of the said overall set of composite individually taken mass-bearing sets of cohesive energy quanta. SAM ROACH.

Magnetism Directly Associated With Charge

 Let us initially consider a charged mass-bearing cohesive set of discrete energy quanta, that is here to be transferred from one given arbitrary locus to another given arbitrary locus. The quicker that the correlative Chern-Simons Invariants are to perturbate, that are here to be of the said respective mass-bearing cohesive set of discrete energy quanta, to where these are here to be most directly associated with the general process of the flow of the charged motion, of such an inferred set of interdependent discrete energy, to where this will consequently tend to reverse-fractal into bearing the result, of such a general kinematic tense of an inferred type of a procedure, of which is here to be directly corresponding to the Lagrangian-based motion of a superstring-related Fourier Transformation of a charged particle, that is being transferred through space over time, to where this particular scenario of a charged mass-bearing cohesive set of discrete energy quanta, is thence to tend to work to bear a heightened scalar amplitude of magnetism associated with its charge, as when compared to an ulterior superstring-related situation, in which the correlative Chern-Simons Invariants are to alter in the exhibition of their delineation in a slower manner, of a covariant-related tense of change over time.To Be Continued! I will continue with the suspense later! Sincerely, Samuel David Roach. (PHS1989).

Nijenhuis Direction Of Magnetic Thrust

 Mass-Bearing cohesive sets of discrete energy quanta, that are here to work to bear a tense of a fractal of magnetic thrust, — that is here to work to bear a Nijenhuis tense of delineation, — tend to have a greater probability of potentially bearing an effect upon phenomenology that is of other universal settings, than other mass-bearing cohesive sets of discrete energy quanta, that are to have the bearings of a fractal of  magnetic thrust, that is instead, to only work to bear a Riemannian tense of delineation. To Be Continued! Sincerely, SAM ROACH.

As To Why Fermions Tend To Have A Greater Charge Density

 One of the reasons — as to why mass-bearing cohesive sets of discrete energy quanta, that operate, in so as to work to bear a fractional spin (super small particles that work to bear a fractional spin, are commonly  named of as being fermions), tend to work to bear a greater charge density, than mass-bearing cohesive sets of discrete energy quanta, that instead, operate, in so as to work to bear a whole spin (super small particles that work to bear a whole spin, are commonly named of as being bosons), — is to basically be of the herein mentioned reason: mass-bearing cohesive sets of discrete energy quanta, that are here to exhibit a fractional spin, — tend to exhibit a more spurious alteration in their Chern-Simons Invariants, during the process in which such a set of particles, that are here to work to bear a fractional spin (the respective fermions), are to alter in their direction and/or in their rate of motion, when this is here to be considered, in their relationship to the motion of electromagnetic energy. To Be Continued! Sincerely, SAM ROACH. (PHS 1989).

Charge Density

 Cohesive sets of discrete energy quanta, that are here to work to bear a fractional spin, tend to reverse-fractal into exhibiting a greater charge density, than cohesive sets of discrete energy quanta, that are, instead, to work to bear a whole spin. To Be Continued Later! Sincerely, Samuel David Roach. (PHS,1989).

Magnetic-Related Thrust

 The more that a given arbitrary mass-bearing cohesive set of discrete energy quanta, is capable of tending  to be able to exhibit a greater attribute of tensor-related metric displacement over time, — the more that such a said respective mass-bearing cohesive set of discrete energy quanta, is thence to consequently tend  to be capable of achieving a greater magnetic-related thrust in the process. To Be Continued! SAM ROACH.

Affinity To Responding To Anti Gravity

 The higher that the Kahler-based quotient is to be, for a given arbitrary mass-bearing cohesive set of discrete energy quanta, the greater that the directly corresponding Majorana-Weyl-Invariant is consequently to tend to be.  The greater that the correlative Majorana-Weyl-Invariant mode is to be, the deeper that the directly corresponding resonant vibration, that the respective given arbitrary mass-bearing cohesive set of discrete energy quanta, is consequently to tend to be. The deeper that the correlative resonant vibration is to be — when this is here to be taken in terms of the respective directly corresponding mass-bearing cohesive set of discrete energy quanta, the more that such a herein stated set of discrete energy quanta, is consequentially to have a stronger affinity of responding in an effectual manner, to the proximal local presence of anti gravity. Therefore; the higher that the Kahler-based quotient is to be, for a given arbitrary respective mass-bearing cohesive set of discrete energy quanta, the greater that such an inferred  discrete set of inter-related energy quanta, that are here to be operating, in so as to perform a group-related function over time, will consequently tend to result, in working to bear a greater affinity of responding in an effectual manner, to the proximal local presence of anti gravity. To Be Continued! Sincerely, SAM ROACH.

Some Potentially Viable Thoughts AsTo Cohomology-Related Eisenstate Of An F-Field

 Here is a mathematical idea, as to my present perception is to be, in regards to how to help in describing — what the cohomology-related eigenstate of an f-field is:

Initially; take the knotting equation, for whatever the dimensionality of the given arbitrary respective cotangent bundle, for what the directly associated field is to be — as this is here to be taken, in terms of “gamma-knot” — while then multiplying this by the mathematical expression for the product of the Planck Constant, as this is here to be coupled with the applicable square of the directly associated discrete increment of time. Next; Divide this whole just mentioned or inferred expression, by the following, — Take the value of “8*PI^2.”  Multiply this by the following type of a general series of Hamiltonian Operators — ((The Hamiltonian Operator that is most associated with the correlative respective Knot Divided by the square-root of two) + (The Square of The Hamiltonian Operator that is most associated with the correlative respective Knot Divided by two) + (The Cube of The Hamiltonian Operator that is most associated with the correlative respective Knot Divided by two times the square-root of two) + (The Fourth Power of the Hamiltonian Operator that is most associated with the correlative respective Knot Divided by four)).  The consequential resultant of this just inferred mathematical process, is what I perceive to be, as a means of working to describe the entity of a cohomology-related eigenstate. Please feel free to indicate to me, whether or not this idea is reasonably decent! Sincerely, SAM ROACH.

Proximal Local Presence Of Kahler-based Quotients

 The proximal local presence, of what works to form that general holonomic substrate, that may be mathematically described by the conceptualization of Kahler-based quotients, as this is here to be appertaining to the multiplicity of the metric-related condition of discrete energy phenomenology, helps to work to form a basis, for the existence of magnetism. I will continue with the suspense later! Sincerely, SAM ROACH.

Legendre Homology And De Rham Cohomology

 Let us consider two different scenarios, of conveyed discrete mass-bearing energy quanta. One of such respective given arbitrary “scenarios,” is to work to bear a tense of a directly corresponding mass-bearing cohesive set of discrete energy quanta, of which is to be conveyed by an isotropically stable Legendre (co)homology; whereas, the other inferred respective given arbitrary “scenario,” is to work to bear a directly corresponding mass-bearing cohesive set of discrete energy quanta, of which is to be conveyed by an isotropically unstable Legendre (co)homology. Otherwise, both of these two scenarios, as to the conveyance of a set of mass-bearing discrete energy quanta, — are basically of the same nature. That given respective scenario of the two, that is to involve a mass-bearing cohesive set of discrete energy quanta — that is here to involve its directly corresponding conveyance, via the kinematic spatial translation of an isotropically stable Legendre (co)homology, via a correlative Fourier Transformation, will consequently tend to have a greater probability of working to involve a resultant De Rham cohomology, than the other given respective case scenario, — of which is here, instead, to tend to have a greater probability of working to involve its conveyance of a mass-bearing cohesive set of discrete energy quanta, via the kinematic spatial translation of an isotropically unstable Legendre (co)homology — in so as to be more likely to tend to work to form a Dubeault cohomology . TO BE CONTINUED! Sincerely, SAMUEL DAVID ROACH. (1989)!

Tense of Legendre Homology

 Let us initially consider two different tenses, of the conveyance of a mass-bearing cohesive set of discrete energy quanta. Let us say, that both of the two different mass-bearing cohesive sets of discrete energy quanta, are basically of the same type of a nature. However; one of such sets of discrete energy quanta, is here to be conveyed by an isotropically stable Legendre (co)homology, whereas, the other of such sets of discrete energy quanta, is here to be conveyed by an isotropically unstable Legendre (co)homology. That conveyance of a mass-bearing set of discrete energy, that is here to be conveyed by an isotropically stable (co)homology, will consequently tend to bear a greater susceptibility towards a tense of magnetism, than the other of such mass-bearing sets of discrete energy. (This is to where, that mass-bearing cohesive set of discrete energy quanta, that is here to have been conveyed by an isotropically unstable (co)homology, is less likely to bear as strong of an affinity, towards any holonomic substrate of magnetism). SAM ROACH.

Synchronous Superstrings

 When all of those superstrings of discrete energy permittivity, that are here to work to comprise a given arbitrary respective mass-bearing cohesive set of discrete energy quanta, — are to work to bear a synchronous tense of motion, as this is here to be considered, over an evenly-gauged Hamiltonian eigen-metric — this general type of a physical Ward-related condition, will thereby result, in working to cause the directly corresponding herein stated set of discrete energy quanta, to tend to consequently result, in having a tense of isotropic stability. Isotropically stable cohesive sets of discrete energy quanta, tend to have more of a probability of working to bear a tense of group action, — than other cohesive sets of discrete energy quanta, that are, instead, to bear a tense of isotropic instability. To Be Continued! Sincerely, SAMUEL DAVID ROACH.

Group Action And Magnetism

 Let us initially consider two different unique mass-bearing cohesive sets of discrete energy quanta.  Both of which are here to be of the same quantum of mass; as well as the given arbitrary physical condition, that both of such said sets of discrete energy quanta, are, as well, to work to bear the same innate tendency of working to exhibit a De Rham cohomology.  Furthermore; both of such respective mass-bearing cohesive sets of discrete energy quanta,  are also to tend to work to bear both the same charge, as well as working to bear the same basic means, of translating the exhibition of the externalized transversal component of their Fourier-related spatial delineation, over a fairly transient covariant relativistic duration of time, that is here to be simultaneous in comparison to one another — as this is to occur, via the vantage-point of a central coni-point.  The main difference in the behavior of these two said cohesive sets of discrete energy quanta, is that one of such sets of cohesive discrete energy, is to bear a reductional tense of group action — by working to bear a tense of isotropic stability; whereas, the other of such said respective given arbitrary mass-bearing cohesive sets of discrete energy quanta, is to work to bear a tense of isotropic instability. That stated set of discrete energy quanta (mass-bearing cohesive set), that is here to be of a tense of isotropic stability, will tend to result in working to display a relatively higher scalar amplitude of a fractal of magnetism, than the other of such said mass-bearing cohesive sets of discrete energy quanta, — of which, instead, is consequently to result in working to bear a lower scalar amplitude of a fractal of magnetism. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.

Legendre Conveyance Of Mass-Bearing Discrete Energy

 The more that the Legendre conveyance of a mass-bearing cohesive set of discrete energy quanta, is here to be of a De Rham cohomology-related nature, — the quicker that the stated mass-bearing set of discrete energy quanta, will tend to be transversally transferred through space. Sincerely, SAM ROACH. (1989).

Kahler-Based Quotients And Metric-Gauge-Related Pulsation

 The greater the Kahler-Based Quotient is to be, for a given arbitrary mass-bearing cohesive set of discrete energy quanta, — the greater the resultant Majorana-Weyl-Mode is to tend to be. The greater that the Majorana-Weyl-Invariant-Mode is to be, for a given arbitrary mass-bearing cohesive set of discrete energy quanta , — the deeper that the resultant metric-gauge-related pulsation is consequently to tend to be. Therefore; the greater the Kahler-based Quotient is to be, for a given arbitrary mass-bearing cohesive set of discrete energy quanta, the deeper that the resultant metric-gauge-related pulsation is consequently to tend to be. I will continue with the suspense later! To Be Continued! Sincerely, SAM ROACH. (1989).

Kahler-Based Quotients And Moment Of Inertia

 The higher that the Kahler-based quotient is to be, for a mass-bearing cohesive set of discrete energy quanta, -- the greater that its fractal of Moment of Inertia, will consequently tend to be. Furthermore; the lower that the Kahler-based quotient is to be, for a mass-bearing cohesive set of discrete energy quanta, -- the less that its fractal of Moment of Inertia, will consequently tend to be. Therefore; the greater that the fractal of Moment of Inertia is to be, for a mass-bearing cohesive set of discrete energy quanta, the less often that it will tend to act as being Gliosis to the Kahler-Metric. Furthermore; the less that the fractal of Moment of Inertia is to be, for a mass-bearing cohesive set of discrete energy quanta, the more often that it will tend to act as being Glisos to the Kahler-Metric. To Be Continued! Sincerely, SAM ROACH.

Less Or More Often Gliosis To The Kahler-Metric

The greater that the scalar amplitude of the Kahler-based quotient is to be, for a mass-bearing cohesive set of discrete energy quanta -- the less often that such a mentioned set of discrete energy quanta, is to tend to need to be Gliosis to the Kahelr-Metric. Thereby; the less that the  scalar amplitude of the Kahler-based quotient is to be, for a mass-bearing cohesive set of discrete energy quanta -- the more often that such a mentioned set of discrete energy quanta, is to tend to need to be Gliosis to the Kahler-Metric. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach. (PHS 1989).

Torsion-Related Tensors

 The more torsion-related tensors, that are here to be directly associated, with the spatial transference of a mass-bearing cohesive set of discrete energy quanta, over a correlative Fourier Transform, the greater that its Kahler-based quotient will consequently tend to be. This will consequently tend to result, in a decrease in the inhibition of the directly corresponding motion, of the said mass-bearing cohesive set of discrete energy quanta. I will continue with the suspense later! To Be  Continued! Sincerely, Samuel David Roach.

Kahler-Based Quotient, And Superstring-Related Fractal Of Momentum

 The greater that the Kahler-based quotient is to be, for a mass-bearing superstring-related phenomenon, that is here to be traveling through a space-related vacuum, -- the more of a superstring-related fractal of momentum, that such a said mass-bearing phenomenology is to consequently tend to exhibit -- in the process by which it is here to be transferred, though the earlier mentioned space-related vacuum. SAM ROACH.(1989).

Torsion Upon Space-Related Vacuum And Dimensionality

 Let us initially consider two different space-related vacuums, of the same three-dimensional volume. Both are to have the same amount of torsion applied to them. One of such space-related vacuums, is to work to bear a higher number of innate spatial dimensions than the other one. That space-related vacuum of the two, of which is here to work to bear a higher number of innate spatial dimensions, will consequently tend to result in working to bear a greater viscosity -- than the other of the two stated space-related vacuums.  Consequently; that space-related vacuum of the two earlier stated ones mentioned, of which is here to work to bear a higher number of innate spatial dimensions, will consequently tend to result in working to bear a greater impedance -- than the other of the two stated space-related vacuums. Samuel David Roach.

Kinematic Torsion Upon Space-Related Vacuum

 The more of a kinematic torsion, that is here to be exhibited upon a space-related vacuum, -- the more viscous that such a space-related vacuum will consequently tend to be. A more viscous space-related vacuum, will tend to work to bear a greater physical attribute of impedance. Therefore; the more of a kinematic torsion, that is here to be exhibited upon a space-related vacuum, -- the more likely that such a said vacuum, will tend to work to bear a greater physical attribute of impedance. Furthermore; the less of a kinematic torsion, that is here to be exhibited upon a space-related vacuum, -- the less viscous that such a space-related vacuum, will consequently tend to be. A less viscous space-related vacuum, will tend to work to bear a lower tense of a physical attribute of impedance. Therefore; the less of a kinematic torsion, that is here to be exhibited upon a space-related vacuum, -- the more likely that such a said vacuum, will tend to work to bear a lower tense of a physical attribute of impedance. To Be Continued! Sincerely, SAM (1989).

Viscosity Of A Vacuum

 The more viscous that a vacuum in space is to be -- the more impedance that such a said vacuum will tend to exhibit. Consequently; the less viscous that a vacuum in space is to be -- the less impedance that such a said vacuum will tend to exhibit. I will continue with the suspense later! Sincerely, Samuel David Roach.

As To Nature Of i*PI(del) Action

 Any change in either the scalar quantum and/or in the differential geometry, of those partition-based discrepancies, that help to work to comprise the topological manifold of those individually taken correlative superstrings of discrete energy permittivity, that are here to help to work to comprise a cohesive set of discrete energy quanta, will consequently tend to result, in the eminent proximal local presence of the i*PI(del) Action. I will continue with the suspense later1 To Be Continued! Sincerely, SAM ROACH. 

As To Intensity Of Vibrational Delineation

Let us initially consider those given arbitrary superstrings of discrete energy permittivity, that are to work to comprise a directly corresponding given arbitrary mass-bearing cohesive set of discrete energy quanta.  The more intense that the flow of the vibrational delineation of the correlative i*PI(del) Action is to be, for the composite summation of the earlier inferred individually taken respective superstrings, that are here to work to form the said cohesive set of discrete energy quanta, -- the greater that such a kinematic attribute, will tend to reverse-fractal into consequently resulting, in working to form a higher scalar amplitude of magnetism. This is to where, such a general attribute of tendency -- will consequently tend to work to form a greater charge per time (or, in other  words, this stated characteristic of attribution, will consequently tend to work to reverse-fractal, into a superstring-related scenario, to where the eminent external environment of the earlier stated mass-bearing cohesive set of discrete energy quanta, will then tend to work to bear a greater amperage.) To Be Continued! Sincerely, Samuel David Roach. (1989).

As To The Inverse Of A Certain Wavelength

 The flow of the multiplicity of the general process, in which there is here to be an inversion of the kinematic delineation-related tense, of the vibrational wavelength of a thought wave, is a key factor, in the reductional process, in which a given arbitrary thought wave, is thereby to be able to convert into the general topological substrate of ideas. I will continue with the suspense later! To Be Continued!  Sincerely, SAMUEL ROACH.  (1989).

More As To Noether Current, In Relation To Current

 The flow of the vibrational delineation of the i*PI(del) Action, is key at helping to work to form the Noether Current -- and the reverse-fractal of the Noether Current, is the flow of charge (current). SAM.

Flow Of Ebbing -- Discrete Energy

 The flow of the ebbing between discrete energy-related impedance and discrete energy-related permittivity, is key at working to form the general tense of Ward-Cauchy-related pulsation; (pulsation, as taken at the superstring-related level). When the substrate of inverted distance (as in the form of the substrate of physical ideas), is to interact in a Gliossis-related manner, with such an ebbing between discrete energy-related impedance and discrete energy-related permittivity, this helps at working to propagate the general flow of discrete time. To Be Continued! Sincerely, Samuel David Roach.