Harmonics Of Schwinger-Indices -- General Types Of Scattering

 Harmonic propagated Schwinger-Indices, often have the general tendency, of having an enhanced capability, of working to help influence, the multiplicity of the formation of a Riemann Scattering, Whereas; Anharmonic propagated Schwinger-Indices, often have the general tendency, of having an enhanced capability, of working to help influence, the multiplicity of the formation of a Rayleigh Scattering. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. (1989).

More, As To Pulse Of Schwinger-Indices

 The quicker and/or deeper the wave-tug that is here to be incurred upon a set of one or more second-order light-cone-gauge eigenstates, by their directly corresponding respective gauge-bosons, -- the stronger that the consequentially formed pulsation of Schwinger-Indices that will often tend to result in being formed, as such said Schwinger-Indices are thence to result in being propagated out tangentially, From their initial locus of formation. I WILL CONTINIUE WITH THE SUSPENSE LATER! SINCERELY, SAM ROACH.

Pulse Of Schwinger-Indices

 Often, there is the general tendency, -- that the stronger the pulse of those vibrational oscillations, that are here to be propagated along the Rarita Structure, of which are here to be directly related to those Schwinger-Indices, that are formed by the "plucking" of second-order light-cone-gauge eigenstates by their directly correlative gauge-bosons, the more eminent that the directly associated force will tend to be, that is here to consequently tend to be transferred through the general medium of space-time-fabric. Sincerely, SAM.

Gauge-Bosons -- Schwinger-Indices -- Conveyance Of Forces Of Nature

 It is the multiplicity of gauge-bosons, that work to pluck their correlative second-order light-cone-gauge eigenstates, -- in so as to form that general genus of Schwinger-Indices, of which work to propagate along the Rarita Structure, in so as to work to help convey the multiplicity of those attributes, that are here to work to exemplify the reductional forces of nature. Therefore -- based upon my particular model of string theory: It is the gauge-bosons that work to help convey the reductional forces of nature -- in basically a particle-related manner; Whereas -- it is that earlier implied general genus of Schwinger-Indices, that I had eluded-to earlier in this particular post (as I have also mentioned such "indices," in many of my much earlier posts), that help to convey the reductional forces of nature -- in basically a wave-related manner. SAM ROACH. (1989).

A Little As to When A Discrete Quantum Of Energy Is Gauge-Invariant

 In the general procedural course of "events," in which a given arbitrary discrete quantum of energy is to remain gauge-invariant, -- there is thereby to be the eminent resultant given arbitrary physical tendency, in which the directly associated kinematic flow of the respective local sequential series, in which one is here to be considering the "plucking" action of those directly applicable gauge-bosons, as these are here to be made Gliosis upon the topological surface of those directly corresponding second-order light-cone-gauge eigenstates, to where these said second-order eigenstates, that are here to work to make-up the holonomic substrate, of what basically amounts to being the proximal local presence of the wave-based nature of discrete energy impedance, -- will thence tend to occur in such a general manner, to where this inferred flow of a resultant formation of a set of Schwinger-Indices, that are here to externally propagate, in so as to interact with their infringed upon environment, in such a manner, to be able to form the forces of nature, to where this will therefore tend to work to form, in this particular genus of a case, a homeomorphic flow of force-related eigenstates, over a directly corresponding period of time. Sincerely, Samuel David Roach. (1989).

As To A Different Nature Of Schwinger-Indices That Is Produced

 Let us consider two different covariant superstrings of discrete energy permittivity, that are here to both be working to exhibit basically the same nature of behavior, -- except, that one of such superstrings is to be vibrating in a slightly different manner, than the other of such inferred strings is to be exhibiting. This will consequently tend to result, among other things, that these two different distinct covariant superstrings of discrete energy permittivity, will consequently tend to have a strong probability, of tending to form two different distinct respective genre of Schwinger-Indices, -- as such said "Schwinger-Indices" are thence to be produced, by the correlative "plucking" of the correlative gauge-bosons  -- that are here to be directly corresponding to each of the two said respective individually taken superstrings of discrete energy permittivity -- Upon the topological substrate of their directly corresponding second-order light-cone-gauge eigenstates, -- in the process of working to form those vibrational oscillations, that are to be propagated along the general Rarita Structure, in so as to work to facilitate the conveyance of the existence of the reductional forces of physical nature. I will continue with the suspense later! To Be Continued! Sincerely, SAM. (1989).

As To The Torsion Applied To The Light-Cone-Gauge

 The more torsion that is to be applied to an eigenstate of the light-cone-gauge, -- the more likely that this factor, in and of itself, will influence such an inferred wave-related quantum of discrete energy impedance, to tend to consequently result in working to form anharmonic Schwinger-Indices, as these are here to thereby be formed, at the general proximal local region, at which such an earlier mentioned light-cone-gauge eigenstate, is here to be "plucked" like a harp, by its directly corresponding set of gauge-bosons. Sincerely, SAM ROACH.(1989).

Schwinger-Indices And Interactions

The general propagation of those harmonic Schwinger-Indices, that are here to be produced by the plucking action of gauge-bosons upon the topological stratum of their correlative light-cone-gauge eigenstates, -- often leads into the direction of tending to work to form a set of one or more Wess-Zumino interactions; Whereas -- the general propagation of those anharmonic Schwinger-Indices, that are here to be produced by the plucking action of gauge-bosons upon the topological stratum of their correlative light-cone-gauge eigenstates, -- often leads into the direction of tending to work to form a set of one ore more Civita interactions. To Be Continued! Sincerely, Samuel David Roach.

Harmonics Of Schwinger-Indices

When those particular Schwinger-Indices, that are here to be produced by any given arbitrary set of light-cone-gauge eigenstates -- that are here to be relatively proximal local to any one given arbitrary proscribed super string-related region, -- are to work to bear a vibrational propagation that is of a harmonic nature, this general tense of an occurrence will tend to "move into the direction" of attributing to the consequential Fourier-related activity, of a set of one or more relatively local Riemann scatterings of cohomology-related generation, that will tend to occur at a region that is here to be relatively adjacent to the earlier mentioned initially formed harmonic Schwinger-Indices, that are here to tend to have just been formed by that general plucking activity of gauge-bosons upon the topological surface of their correlative light-cone-gauge eigenstates.  Consequentially; when those particular Schwinger-Indices, that are here to be produced by any given arbitrary set of light-cone-gauge eigenstates -- that are here to be relatively proximal local to any one given arbitrary proscribed super string-related region, -- are to work to bear a vibrational propagation that is of an anharmonic nature, this general tense of an occurrence will tend to "move into the direction" of attributing to the consequential Fourier-related activity, of a set of one or more relatively local Rayleigh scatterings of cohomology-related generation, that will tend to occur at a region that is here to be relatively adjacent to the earlier mentioned initially formed Schwinger-Indices, that are to tend to have just been formed by that general plucking activity of gauge-bosons upon the topological surface of their correlate light-cone-gauge eigenstates. Sincerely, Samuel D. Roach.

Some Stuff About Change In Gravitational Mode

When the mode of gravity, that is here to be applied upon a Ward-Cauchy-related region, -- is to convert from a tense of a gravity to a tense of anti gravity or vice-versa -- this will tend to invert a tense of the sinusoidal conditions of those "quantized" gravity-related Schwinger-Indices, that are here to work to form such an altered mode of gravitational influence, that is here to have been changed from within such a stated Ward-Cauchy-related region in time and space. Samuel Roach.

General Propagation-Related Modes

Gravity is formed by that general orthogonal propagation-related mode, that is here to be directly associated with the flow of a general tense of those Ward-Cauchy-based Schwinger-Indices -- that are formed by the general transversal propagation, of the vibration of the holonomic substrate of light-cone-gauge eigenstates.  Anti Gravity is formed by that general orthogonal propagation-related mode, that is here to be directly associated with the flow of a general resultant tense of those Ward-Cauchy-based Schwinger-Indices -- that are formed by the general inverted transversal propagation, of the vibration of the holonomic substrate of light-cone-gauge eigenstates.  Thought waves are formed by that general supplemental propagation-related mode, that is here to be directly associated with the flow of a general tense of those Ward-Cauchy-based Schwinger-Indices -- that are formed by the general transversal propagation, of the vibration of the holonomic substrate of light-cone-gauge eigenstates.  To Be Continued!  Sincerely, Samuel David Roach.

Second-Order Light-Cone-Gauge Eigenstates And Force

The more pronounced that the vibration of those second-order light-cone-gauge eigenstates, that are  here to be appertaining to one given arbitrary discrete quantum of energy -- to where such an inferred set of second-order light-cone-gauge eigenstates, are here to work together to comprise one specific correlative first-order light-cone-gauge eigenstate, to where the course of such a general tense of a vibrational mode, is here to be over the duration of an evenly-gauged Hamiltonian eigenmetric, -- this will thereby consequently tend to follow, that the higher that the scalar amplitude will then tend to be, of the directly corresponding intensity of those wave-like Schwinger-Indices, that are here to consequently to tend to be formed by the inferred "plucking" of these said second-order light-cone-gauge eigenstates, by their directly corresponding gauge-bosons.  The higher that the scalar amplitude will then tend to be, of the directly corresponding intensity of those wave-like Schwinger-Indices, that are here to be formed by the inferred "plucking" of the correlative second-order light-cone-gauge eigenstates of a certain case, by their directly corresponding gauge-bosons, the more of a general attribute of force, -- that will thereby tend to be exhibited, at least in part, by the here inferred discrete quantum of energy, that may be appertaining to such a given arbitrary respective case scenario. Samuel David Roach.

Stringular Spatial Dimensionality And Schwinger-Indices

The higher that the spatial dimensionality that is here to be exhibited, that is of any one given arbitrary superstring of discrete energy, the greater the potential variety of resultant Schwinger-Indices, that may tend to possibly be formed by the consequential "plucking" of the correlative second-order light-cone-gauge eigenstates, that are here to be of such a respective case, By the directly corresponding gauge-boson eigenstates, that are of such a respective correlative said inferred superstring of discrete energy permittivity. Samuel David Roach.  (PHS1989).

A Certain Tense Of A Perturbation Series

What type of a perturbation series would propagate, if certain superstrings of covariant traits were to acquire a certain general genus of topological sway -- and how would this work to alter the angular momentum of that homotopy, whose phenomenology is defined, in part, by the interaction of those covariant traits with one another, as such super strings that work to form the inferred traits, -- are here to act in an eigen-related manner, to the inferred directly pertinent differentiable semi-groups, that are correlative to the said covariant traits?  (These semi-groups here, are physical entities that act as norm-state-projections, -- that act as catalysts to the formation of those strings, which work to encode for the mentioned covariant traits.)  As an arbitrary example: A superstring of discrete energy permittivity is reiterated within the same general substringular neighborhood, over a relatively brief evenly-gauged Hamiltonian eigenmetric.  Quadrillions of related strings perform such a general tense of a reiteration, at this general superstringular region as well.  A minority of the closed-looped strings that are related here, work to iterate and reiterate side-to-side, on a slightly differentiable coniaxial-related basis.  These strings are here to maintain an even function of polar shift, in order to not get "kicked-out" of their association with the other strings, to where these strings, are to work to help to define the basis of their respective covariant traits. The change in the holomorphic index, thus caused, will consequently work to commute a change of phase, when this is in terms of the nodation of the anharmonic oscillation of these strings, that are here to be altering int their intrinsic directional tendency.  This consequently causes a general change in both the correlative wave-tug and in the correlative wave connection, of both the directly involved superstrings,  as well as with the immediately adjacent Schwinger-Indices.  This phase alteration will then work to reposition the parallax of homotopic differentiation, by setting-up a substringular buffer in the related semi-groups.
I will continue with the suspense later! To Be Continued!  Sincerely, Sam Roach.

Relative Harmonics Of Fields

When harmonic Schwinger-Indices are to ripple along the topological surface, that is of a specific region of mini-stringular segmentation -- this will then tend to form a harmonic substringular field, at the proximal locus of the said region of mini-stringular segmentation.  Consequently, when anharmonic Schwinger-Indices are to ripple along the topological surface, that is of a specific region of mini-stringular segmentation -- this will then tend to form an anharmonic substringular field, at the proximal locus of the said region of mini-stringular segmentation.  I will continue with the suspense later! To Be Continued! Samuel David Roach.

Pulse Of Resultant Schwinger-Indices

The quicker that the rate is -- as to how fast that the correlative "plucking" is, of that action, in which those gauge-bosons, that are here to be of a local quantum of discrete energy, that are here to bear their course of a Gliosis-related contact, that is to be effectual upon their directly corresponding second-order light-cone-gauge eigenstates, in such a manner,  in so as to work to form those Schwinger-Indices, that act, in so as to help in the process of working to perpetuate the continued vibrational oscillation of the Rarita Structure, -- then, this will tend to work to bear the resultant of a higher pulsation of force, than it otherwise would, at that proximal locus, in which such so-stated Schwinger-Indices are here to be formed.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Metaphorical "Heartbeat" Of The Substringular

The activity of the "plucking" of second-order light-cone-gauge eigenstates, by gauge-bosons -- in so as to form those Schwinger-Indices, that act, in so as to ripple along the Rarita Structure, in order to allow for the vibrational oscillations of that mini-stringular fabric, that is here to work to form the various superstringular forces, to where the vibration of this said fabric, is to work to form the kinematic multiplicit field of the said substringular realm, over time -- works to act as the metaphorical "heartbeat" of the substringular.  To Be Continued!  Sincerely, Samuel David Roach.

Resulting Veering Schwinger-Indices

Often, an orbifold eigenset -- that is here to be moving in a hermitian manner -- will interact with a set of one or more Schwinger-Indices, in such a manner, to where this said interaction, will thence work to veer or scatter these said Schwinger-Indices, into a direction that is of a relative resultant Nijenhuis manner.  Such a Nijenhuis veering of this said set of one or more Schwinger-Indices, will thus tend to each, when individually taken, work to form a tense of causing a bearing of Lagrangian-related Chern-Simons singularity, -- since these waves that are here to be veering out into a relatively resultant Nijenhuis direction, when this is here to be taken in relationship to the said hermitian wave-tug of such a general case of an orbifold eigenset, that is here to tend to be propagating in a manner that is of a De Rham-related nature -- will then, in the process of such a said "veering-off" of the said scattered Schwinger-Indices, work to cause these said individually taken indices, to be changing in more derivatives, than the number of spatial dimensions that these are each to be traveling through, -- over the course of the directly corresponding evenly-gauged Hamiltonian eigenmetric, in which the said orbifold eigenset is to be traveling through, in a manner that is of a hermitian nature of cohomological translation, over time.  I will continue with the suspense later!  To Be Continued!  Sincerely, Sam.

E(6)XE(6) Oscillation-Based Tendencies That Tend To Be More Yukawa Towards Each Other

Let us initially consider a said Ward-Cauchy-related condition, in which there is here to be a set of orbifold eigensets, that are to each, when individually taken, to work to bear an E(8)XE(8) string oscillation-based tendency --  that is here to multiplicitly to be of an eminent Yukawa-related nature, -- when this is here to be based upon their correlative covariant relationship towards one another, over an evenly-gauged Hamiltonian eigenmetric.  This will then, as well, to be of such a nature, in so as to tend to work to cause such a set of orbifold eigensets, to then bear a respective covariant nature, in which these will also tend to bear their directly corresponding individually taken E(6)XE(6) string oscillation-based tendency, to then to be of an eminent Yukawa nature, when this is here to be based upon such a said general tense of a relationship towards one another, over an evenly-gauged Hamiltonian eigenmetric.  This will then work to mean, that such orbifold eigensets that are here to tend to work to bear such a said eminent Yukawa nature towards one another, will as well, to then bear a tendency of bearing a higher potential of working to bear more of an inter-relationship of their directly corresponding Schwinger-Indices, -- than orbifold eigensets that are to, instead, to bear a relatively Nijenhuis relationship -- when this in terms of such a so-eluded-to tense of covariance of  each of such so-eluded-to oscillation-related tendencies, towards the rest of such a so-inferred set of orbifolds that are of this second so-eluded-to general case scenario.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David  Roach.

More As To The Recycling Of Relativistic Cohomology

Mass-Bearing superstrings of discrete energy permittivity, tend to form what I term of as being Gliosis-Sherk-Olive cohomology.  As eigenstates of such so-eluded-to GSO cohomology, are to be scattered in an anharmonic manner -- these eigenstates then work, to be changed into what I term of as being the holonomic substrate of particles called dilatons and dilatinos.  This just mentioned general genus of activity, is here to be happening on the relative Real Reimmanain Plane -- whereupon discrete energy permittivity, is here to continue to be both iterated and reiterated over time.  The thence formed dilatons and dilatinos, are to then to be pushed off of the said relative Real Reimmanian Plane, in the process of working to help at recycling the local presence of norm-state-projections, in so as to refurbish the holonomic substrate of those so-eluded-to point commutators, to where, such a recycling of cohomology is here to be necessary as well, for the formation of cohomology to be able to occur off of the Real Reimmanian Plane.  Without such recycling, this situation would otherwise amount to, as well, an excessive build-up of localized Hamiltonian operators, that would no longer be able to commute -- which would end-up stopping the existence of energy.  Such a relative wave-tug, that is here to push such said dilatons and dilatinos off of the relative Real Reimmanian Plane, happens, on account of the resultant Ward-Cauchy-based angling, in which the earlier inferred Rayleigh scattering of the said GSO cohomology-related eigenstates -- which was here to be scattered in such an anharmonic manner, in so as to work to form a tense of cohomology, that may be described of as being of the nature of what I term of as being Neilson-Kolosh cohomology-related eigenstates.  As these said eigenstates of a Neilson-Kolosh cohomology, are to come together at a general locus that is off of the relative Real Reimmanian Plane, the holonomic substrate of such gathered cohomology-related eigenstates, are to come together -- in so as to work to form the indistinguishably different eigenindices, that work to comprise what I term of here as being "gravitons" and "gravitinos."  The motion of the cohomological eigenstates of "gravitons" and "gravitinos," is to then to work to indirectly induce the gauge-bosons (the E(6)XE(6) strings), of which are on the relative Real Reimmanian Plane, to act in so as to pluck the directly corresponding second-order light-cone-gauge eigenstates like a harp -- in so as to work to form Schwinger-Indices.  Such a general genus of Schwinger-Indices will then act, in so as to work to influence both the general formation and the general activity of the four fundamental forces of nature, -- such as gravity.  In the meanwhile, that general cohomology of both the said "gravitons" and "gravitinos," that was here to be scattered in an anharmonic manner, due to the resultant Ward-Cauchy-based angling, in which the earlier inferred Rayleigh scattering is to occur, -- is to be recycled back into the relative Real Reimmanian Plane, -- in so as to refurbish the holonomic substrate of those norm-state-projections, that are necessary for both the formation of cohomology to occur at this said relativistic Plane, as well as to work to allow for the commutation of the multiplicit discrete quanta of energy.  My model of string theory is becoming clearer in my mind.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.