Holomorphicity Of Kinetic Energy Versus E.M.

Discrete quanta of electromagnetic energy, are comprised of bosonic superstrings of discrete energy permittivity, that work to bear their individually taken holomorphic direction -- in the general multiplicit directoral, that is of the fractal of the angular momentum that is of the individually taken direction of the relative positioning of the anuulus of its toroidal-based core-field-density, -- whereas, discrete quanta of kinetic energy, are comprised of fermionic superstrings of discrete energy permittivity, that work to bear their individually taken holomorphic direction -- in the general multiplcit directoral, that is of the fractal of the angular momentum of the individually taken direction of the relative positioning of the apex of its conical-based core-field-density.  This is the fundamental difference as to how a discrete quantum of electromagnetic energy goes about moving in its correlative holomorphic direction, as to be compared to the manner in which a discrete quantum of kinetic energy is to go about moving, in what happens to be its own correlative holomoprhic direction.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

As To "Plucking" The Light-Cone-Gauge

That general genus of eigenstates that may be termed of as "gauge-bosons," are comprised of the consistency of closed-loops of topological stratum -- that are each individually taken, as an integration of first-order point particles -- that are "beaded togehther" in a general composition, that has twice the scalar amplitude of its Lagrangian-based magnitude, as taken along its topological surface (twice the magnitude of its Laplacian-based permimeter, when taken at the Poincare level), as a fully contracted bosonic superstring of discrete energy permittivity, when taken over the course of any individually taken iteration of BRST.  Any one given arbitrary respective second-order light-cone-gauge eigenstate, is comprised of a "spindle" of mini-stringular segmentation (mini-stringular segmentation is that general genus of topological phenomenology, that works to form the holonomic substrate of the generic field-based stratum -- that works to inter-bind superstrings, via the general Ward-Caucy-based condition of homotopy), that is inter-bound over the course of BRST, in-between any respective given arbitrary Fadeev-Popov-Trace eigenstate and its directly corresponding superstring of discrete energy permittivity.  Gauge-Bosons, during the course of any one individually taken iteration of BRST, work to "pluck" those correlative second-order light-cone-gauge eigenstates that these are correlative to, like a "harp," in so as to work to produce those resultant Schwinger-Indices, that may be described of as gravity waves.  When any one gauge-boson is to work to strike any respective said second-order light-cone-gauge eigenstate -- in such a manner, to where this so-eluded-to process is, over the said individually taken iteration of BRST, to work to help to allow for the initially Gliosis-based first-order point particle of the said gauge-boson, that is to first work to strike the correlative second-order light-cone-gauge eigenstate, to remain in a direct contact with the said second-order light-cone-gauge eigenstate, over the whole iteration of BRST, then, the resultant gravity wave or gravity waves that are thus formed by such a "plucking," are to tend to work to form more of a harmonic wave pattern, -- than if the said "plucking" is to, instead, to act in so as to "jump" upon multiple first-order point particles, in the process of the formation of gravity waves, that is to happen during the Polyakov Action, over the course of any one individually taken iteration of BRST, which is over the clear majority of the beginning of any one respective given arbitrary iteration of a correlative duration of one discrete increment of instanton.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Gauge-Bosons And Photons

Let us initially consider one given arbitrary photon, that is to strike a discrete quantum of energy in a Gliosis-based manner -- at the given arbitrary respective instanton in which the so-eluded-to discrete quantum of electromagnetic energy is to be under the Ward-Caucy-based condition of then being in an eminent contact, with the externalized core-field-density of that said discrete quantum of energy that the said photon is to be striking.  Right as the so-eluded-to delineation of the multiplicit discrete quantum of energy is about to happen, -- in so as to help to work to prepare for that general activity that is to happen over the discrete increment of time, that is to be directly corresponding to the Ward-Caucy conditions of the here correlative iteration of group-related instanton, that is to be considered in this respective given arbitrary case scenario -- there will then be gauge-bosons that are to here to be in the process of being prepared to "pluck" the correlative second-order light-cone-gauge eigenstates -- at the relatively opposite side of the specific first-order light-cone-gauge eigenstate that is to soon to be struck by the holonomic substrate of the incoming photon, that is about to make a collision with the externalized core-field-density of the said light-cone-gauge eigenstate that is here to be under consideration.  At the beginning of that iteration of BRST,  in which the said discrete quantum of electromagnetic energy is to be actually coming into an eminent Gliosis-based contact with the said light-cone-gauge eigenstate, the correlative gauge-bosons that are to work to "pluck" their directly corresponding second-order light-cone-gauge eigenstates, are to work to slide along the topological surface of the so-eluded-to second-order stratum -- in so as to work to be in such a distribution, to where the said correlative gauge-bosons will be brought into a set of positions, to where these will be directed into an assymetric pattern of distribution -- in correlation to the respective given arbitrary delineation that the directly corresponding photon that is now to be in an immediate contact with the externalized core-field-density of the correlative light-cone-gauge eigenstate that is of this given arbitrary case is to be in. As the so-eluded-to discrete quantum of electromagnetic energy is to be vibrating at the proximal locus at which it is in direct contact with that discrete quantum of energy that had just been struck here, -- the correlative gauge-bosons that are of the just struck light-cone-gauge eigenstate -- are to then "pluck" the said correlative second-order light-cone-gauge eigenstates, in so as to then vibrate in an assymetric oscillation-based tense, relative to the vibrational oscillation of the here incoming photon that is to now be in the process of striking it.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Gauge-Boson Sliding

During that general activity of the decompactification that happens during the Polyakov Action -- upon any one given arbitrary discrete quantum of energy, over the course of BRST -- the correlative gauge-bosons that are to work to "pluck" the directly corresponding light-cone-gauge eigenstates, are to then be in the process of sliding along the topological surface of the hyperbollic Clifford Expansion, that is to here be Yukawa to the core-field-density of the so-eluded-to light-cone-gauge eigenstates, that are to here be directly associated with the so-eluded-to discrete quantum of energy that is to here be undergoing the so-eluded-to eigenstate of the said Polakov Action.  For the remainder of that increment of BRST, in which the said gauge-bosons are to be in the process of "plucking" the said light-cone-gauge eigenstates during the said Polyakov Action eigenstate, -- the said gauge-bosons, of which have just slid across the topological surface of the correlative light-cone-gauge eigenstates that are to have just been hyperbollically expanding in their core-field-density, -- are to then to tend to work to do what one would normally think of as the actual "plucking" action of the said gauge-bosons -- in so as to produce those Schwinger-Indices, that are to here act as the resultant gravity waves.  To Be Continued!  Sincerely, Samuel David Roach.

Dimensions Move Through

Let us consider both an f-field, a d-field, and a p-field.  Let us next say, that, over a discrete amount of time, -- both an orbifold eigenset of an f-field, an orbifold eigenset of a d-field, and an orbifold eigenset of a p-field, are to all to travel through what would otherwise be a common general Hamiltonian operand-based region.  What is here to tend to work to influence the general Ward-Caucy-based condition, in so as to help to cause both the f-field to move through a minimum of four spatial dimensions, the d-field to move through a minimum of six spatial dimensions, and the p-field to move through a minimum of ten spatial dimensions (all of these being plus the dimension of time), is that, given the general genus of the vibrations of those superstrings that are to work to make-up each of the three individually taken general genre of field-based attribute -- along with the manner by which such superstrings of such said respective given arbitrary fields are to be tugged through such a so-eluded-to Hamiltonian-based operand -- a tendency will form, in so as to have a respective minimum of four spatial dimensions (for f-fields), six spatial dimensions (for d-fields), and ten spatial dimensions (for p-fields), is to be the said case for the three different said genre of field-based attribute.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Common Holomorphicity

Let us consider the discrete quanta of energy of one given arbitrary orbifold eigenset.  As a general Ward-Caucy-based condition, -- all of the discrete quanta of energy that are immediately adjacent to any one respective given arbitrary discrete quantum of energy, are to be orphogonal to the one said discrete quantum of energy -- yet only over the course of any one specific respective given arbitrary iteration of BRST.  Over the ensuing ending of the general metric of any one respective so-eluded-to iteration of group-related instanton, (instanton after one iteration of BRST), all of the discrete quanta of energy that are of any one individually taken respective given arbitrary orbifold eigenset, are to adjust along their coniaxion-related eigenbase, -- in so as to work to allow for all of the discrete quanta of energy that are here to help to work to comprise one individual given arbitrary orbifold eigenset, to be of such a general condition in so as to move in a common specific holomorphic direction.
The between four and 32 spatial dimensions that a superstring is to move through -- over the ending of the course of one individually taken metric of group-related instanton -- is a significant contributing factor to the just described general Ward-Caucy-based condition.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Gaussian Transformations And Consecutive Kahler-Metric States

At the metrical end of one given arbitrary iteration of one respective Kahler-Metric eigenmetric -- the directly corresponding holonomic substrate-based eigenstate of the Klein Bottle, when along with its correlative Higgs Boson eigenstate, -- is to work to re-orientate by readjustment, by the metrical activity of three consecutive iterations of group-related instanton, in so as to be ready to act upon what is here to be a different Ward-Caucy-based topological substrate -- in so as to operate via the Kahler-Metric upon a different set of discrete energy quanta, that are to then undergo another eigenmetric of the Kahler-Metric.  This would then work to allow for the respective holonomic substate-based phenomenology of the said metric, to act in so as to work to help in another set of discrete quanta of energy to work to reattain their respective given arbitrary discrete energy, -- so that such discrete energy may both exist and persist.  Right after such a so-stated readjustment, -- that respective holonomic substrate-based phenomenology, that had just acted upon one set of discrete energy phenomenology -- is to then work upon another set of discrete energy phenomenology.  Such an ensuing set of phenomenology that is to be worked upon next, is not necessarily of the same universal setting as the respective given arbitrary initial set of discrete energy quanta-based phenomenology that had just been worked upon.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

More Stuff As To Calabi Spaces And The Kahler-Metric

Homotopy is the general condition, that there is -- at instanton, among all unfrayed discrete energy quanta -- an interconnection that exists, between all of the so-eluded-to quanta of discrete energy, in conjunction with every other of such discrete quanta.  What I believe that this amounts to, -- is that there is a general genus of phenomenology, that is much smaller than a superstring, as to what I call and consider to be of the nature of what may be said of as being "mini-stringular segmentation," that works to inter-bind the multiplicit-based fields of the substringular realm among each other.  The activity that is most associated with the Fourier-based mechanism of the Kahler-Metric, in general, works to cause discrete quanta of energy to re-attain their fractals of discrete energy, -- so that the building blocks of energy may both exist and persist.  This may then be considered to so-elude to the condition, that the holonomic substrate-based phenomenology, that acts in so as to help in the allowance of the activity of the Kahler-Metric, is one of the genre of the Fourier-based Hamiltonian operation -- that works to act, in so as to help in the continued maintenance of homotopy, over time.  This would then work to indicate, that the so-eluded-to multiplicit-based holonomic substrate of that phenomenology that helps to work to cause the general operation of the Kahler-Metric -- is inter-bound, via mini-stringular segmentation, in so as to bear an inter-twining with the multiplicit-based eigenstates of discrete energy that are not frayed, in so as to work to allow for the so-stated continuation of homotopy.  Furthermore, Calabi-Yau spaces are mass-related manifolds, whereas Calabi-Wilson-Gordan spaces are kinetic energy-related manifolds, whereas electromagnetic energy-related manifolds are Calabi-Calabi-related spaces.  This would then tend to mean, that individually taken manifolds of discrete energy, will always tend to exist as some sort of Calabi-based space.  This is part of the reason as to why, even when a Calabi-based space is not interacting in a Gliosis-based manner with the Kahler-Metric -- any of such Calabi-based spaces that are not frayed -- will always tend to bear a Yukawa-based interaction with the Kahler-Metric, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Some Additional Stuff About The Polyakov Action

The actual process of that decompactification, that is to be of that general tense of the activity of the Polyakov Action -- is to only to work to metrically comprise the initial (2pi-6)/2pi portion of the overall duration of instanton.  The last (2pi-6)/2pi portion of the overall duration of instanton, is when the respective Kahler-Metric (when the Kahler-Metric is to be Gliosis to the directly corresponding discrete energy of any said respective given arbitrary case) and/or the Regge Action, is to be Yukawa to the kinematic activity of any one respective given arbitrary discrete quantum of energy. So, the fully implemented scalar magnitude of the Polyakov Action eigenstate, upon one discrete quantum of energy -- that is to be Yukawa to any one given arbitrary respective superstring of discrete energy permittivity -- given what is to here to be pertinent to its scalar amplitude of the inverse of its correlative Lorentz-Four-Contraction, is to last for the relatively central ((2pi-2*((2pi-6)/2pi))/2pi) of the  metrical duration of any one respective iteration of instanton, -- during the generally noticed iteration of Ultimon Flow.  During the rest of the Polyakov Action, in general -- there is to be the ebbing of flow of that general tense of mini-stringular segmentation, -- that is to happen in order to work towards an optimum condition of homotopy during BRST.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Imaginary Exchange Of Real Residue And The Polyakov Action

Let us initially consider a discrete quantum of energy, over the course of one given arbitrary iteration of BRST.  Let us here, consider the covariant processes of both the correlative Polyakov Action eigenstate and the correlative eigenmetric, of what I call here as the Imaginary Exchange of Real Residue.  As the kinematic activity of the said Polyakov Action eigenstate, is to here to work to form the directly corresponding hyperbollic Clifford Expansion of the scalar amplitude of the coiled-up mini-stringular segmentation -- that is of the here directly pertinent light-cone-gauge eigenstate, that is of the so-stated discrete quantum of energy, -- this happens, to where the first-order point particles that are at the relative reverse-norm-to-holomorphic positioning of both the directly corresponding superstring of discrete energy permittivity and the substringular counter part of this said superstring of discrete energy permittivity, are to be brought into a topological sway -- that is to work to tug the correlative discrete quantum of energy to go from first swaying mildly into the relative forward-holomorphic direction, to then go into a mild topological sway into the relative reverse-holomorphic direction. As such a topological sway is to happen, -- the kinematic activity of the Polyakov Action eigenstate of this case, is to work to decompactify both the correlative superstring of discrete energy permittivity and its counter part, to the inverse of the scalar magnitude of its directly corresponding Lorentz-Four-Contraction.  While this is happening, both the superstring and its correlative counter string, will then work to bear both the respective first-order point particle that is at the relative norm-to-forward-holomorphic positioning of the said string and the first-order point particle that is at the relative norm-to-forward-holomorphic positioning of the directly correlative counter string, to be of the processes of an indistinguishably different replacement, -- over the directly corresponding iteration of BRST, that is to here be in the process of being iterated.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

More As To The Nature Of Fadeev-Popov-Trace Eigenstate Composition

The relative tense of the non-Lorentz-related compactification of mini-stringular segmentation, that is of any given arbitrary Fadeev-Popov-Trace eigenstate, is to bear a scalar amplitude of being of a factor of five away from being fully compactified at the beginning of BRST.  Such a lack of compactification, works to allow for the feeding-in of mini-stringular segmentation -- as is it is to ever be necessary.  Such an eigenstate of this general  genus of trace, is to be virtually closed at each endpoint.  The correlative Fadeev-Popov-Trace eigenstate, that is correlative to a one-dimensional superstring of discrete energy permittivity, is to bear five second-order light-cone-gauge eigenstates, that are here to be inter-woven with the correlative superstring, whereas, the correlative Fadeev-Popov-Trace eigenstate that is correlative to a two-dimensional superstring of discrete energy permittivity, is to bear ten second-order light-cone-gauge eigenstates, -- that are inter-woven with the correlative superstring.  This is not to be confused with the Ward-Cauchy-based condition, that any Calabi-Yau state will tend to move through between four and 32 spatial dimensions plus time -- per each ensuing successive series of group-related instanton.  A typical  superstring of discrete energy permittivity that is not of a hook-like string, will tend to iterate at BRST, -- in a tense of what is to act as being of either one or two spatial dimensions plus time.  Yet, over the course of both the ending portion of instanton, as well as during the generally unnoticed duration of Ultimon Flow, -- any respective superstring will be moving through a Hamiltonian operand, that will here work to include multiple ulterior spatial dimensions besides the generally related ones that I have just eluded to.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Mini-Stringular Segmentation Of Fadeev-Popov-Trace Eigenstates

Let us initially consider the construction of any one given arbitrary Fadeev-Popov-Trace eigenstate.  It is to here to be respectively comprised of in the following general manner.:  There is to here be a trace of 600 general respective given arbitrary increments of mini-stringular segmentation, that are to here be inter-twined upon each other in the manner of an ellongated multiplicit double-helix that bears intermittent nodes at which the two said pairs work to inter-twine -- that is here to bear two pairs of 300 helix-related phenomenology of mini-stringular Laplacian-based propagation -- at which the relative "height" of this so-stated multiplicit construction, is to be taken from the center of the norm-to-reverse-holomorphic Laplacian-based positioning (relative bottom), as taken at the start of BRST, to the center of the norm-to-forward-holomorphic Laplacian-based positioning (relative top), as taken at the start of BRST, -- is to be of the equivalence of the scalar amplitude of the length of one fully contracted one-dimensional superstring of discrete energy permittivity, or, of a relative "height" of 10^(-43) of one meter.  The shape of the said respective given arbitrary Fadeev-Popov-Trace eigenstate -- is to be of one figure-eight-based shape, that is to be inscribed inside two sets of sinusoidal dual Chi-shaped halves, that are to here to work to form the equivalence of the said figure-eight-shape in so as to be inscribed inside of the said Chi-symbol shape.  Furthermore, both the topological surface of the so-stated figure-eight partial component of the said Fadeev-Popov-Trace eigenstate, as well as the topological surface of the so-stated externalized superimposed Chi-shaped composition, are then to here each to bear the holonomic substrate of a composite Laplacian-based tense of mini-stringular segmentation, that is then to be comprised of 2 pairs of 300 relatively compactified strands of mini-stringular segmentation, -- in the process of working to form the needed said double-helix shape, -- that is of the so-eluded-to covariant tense of nature.
I will finish off with the second set of this material, in so as to help to complete the explanation that I am trying to give.  To Be Continued!  Sincerely, Samuel David Roach.

The Light-Cone-Gauge And Fed-In Mini-Stringular Segmentation

Let us initially compare two different genre of light-cone-gauge eigenstates.  One is of a Yang-Mills light-cone-gauge topology, while the other one is of a Kalutza-Klein light-cone-gauge topology.  The light-cone-gauge eigenstate that is of a Yang-Mills topology, is non-abelian in its general geometry.  Whereas, the light-cone-gauge eigenstate that is of a Kalutza-Klein topology, is abelian in its general geometry.  The light-cone-gauge eigenstate of this given arbitrary case -- that is of a non-abelian nature, works to bear second-order eigenstates that are of a relatively sinusoidal Laplacian-related composition, along the general region of the Lagrangian-based path in which these are delineated over the course of BRST. Whereas, the light-cone-gauge eigenstate of this given arbitrary case -- that is of an abelian nature, works to bear second-order eigenstates that are of a relatively supplemental Laplacian-related composition, along the general region of the Lagrangian-based path in which these are delineated over the course of BRST.  As the two so-eluded-to first-order light-cone-gauge eigenstates are to be in the process of going through an iteration of BRST that is both covariant, codifferentiable, and codeterminable, via the vantage-point of a central conipoint -- the correlative  individually taken Polyakov Action eigenstates, are to here to work to form the activity of a hyperbollic Clifford Expansion, that is to be involved with a euler-based acceleration of the directly corresponding feeding-in of mini-stringular segmentation --that is to exist for both of the correlative dually considered light-cone-gauge eigenstates, and their directly corresponding individually taken superstrings and counter strings.  The mentioned Yang-Mills-related light-cone-gauge eigenstate, during BRST, is to bear its correlative gauge-bosons -- that are to pluck each second-order light-cone-gauge eigenstate -- at those respective sinusoidal-based "troughs" at which the said gauge-bosons are to "pluck" the light-cone-gauge eigenstate like a harp.  Whereas, the mentioned Kalutza-Klein-related light-cone-gauge eigenstate, is to bear certain respective given arbitrary loci of encoded singularity -- at which their correlative and directly corresponding gauge-bosons are to "pluck" the corresponding second-order light-cone-gauge eigenstates like a harp.  Yet, as the so-eluded-to mini-stringular segmentation -- that is respective to the said Kaluza-Klein-related light-cone-gauge eigenstate -- is being fed-into the said eigenstate during BRST, -- this will work to form the equivalence of mini-troughs, at which the said respective gauge-bosons are to "pluck" the needed loci of the correlative abelian light-cone-gauge eigenstate, in so as to form Schwinger-Indices that act as gravity waves.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Gaussian Transformations And The Kahler-Metric, In General

Let us initially consider one given arbitrary orbifold eigenset, -- that is here to be eminently Yukawa to the Kahler-Metric.  Here is a brief synapsis, in both a curt and in a general manner, as to what is to happen here.:  At the onset of such a Ward-Caucy group-related metric --the so-eluded-to set of superstrings, that are to here be operating to perform one specific function, are to first here, bear an eminent Yukawa-based relationship that is not of a Gliosis-based nature, with the Kahler-Metric -- for the initial 95 iterations of group-related instanton -- in which this is happening.  For the ensuing 191 iterations of the said tense of instanton, the correlative orbifold eigenset is to be Gliosis to the so-eluded-to eigenstate of the Kahler-Metric.  For the next 95 iterations of the said tense of instanton, the correlative orbifold eigenset is to bear an eminent Yakawa-based relationship with the Kahler-Metric, yet not in a Gliosis-based manner.  For the next three iterations of group-related instanton -- the said orbifold eigenset is only mildly Yukawa in an eminent manner,  to the so-eluded-to Kahler-Metric eigenstate, -- while the directly corresponding Higgs Boson eigenstate along with the correlative holonomic substrate of the directly corresponding Klein Bottle eigenstate, are to work to re-position themselves, -- in so as to work to prepare for the activity of a slightly different proximal local Fourier-related operation, that is to involve the eminent Yukawa-based bearings of the Kahler-Metric.
I will explain this in much more detail in Course 24 -- as to conformal invariance and superconformal invariance.  I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Gauge-Tranformations And The Kahler-Metric

Once any one given arbitrary photon has worked to strike the externalized core-field-density of the light-cone-gauge of another respective given arbitrary discrete quantum of energy -- both the discrete quantum of electromagnetic energy that I have just mentioned, as well as the discrete quantum of energy that it had just scattered upon, will then proceed to become Yukawa to the Kahler-Metric in an eminent manner, -- over the course of the immediately ensuing 384 group-related instantons. The last three of such so-eluded-to 384 consecutve iterations of group-related instanton, are involved with a re-orientation -- by which the correlative Kahler-Metric eigenstate is to be re-positioned, in order to be functioning at a mildly different proximal locus.  In pretty much the central 191 consecutive iterations of group-related instanton -- that are to be from within the said 384 consecutive correlative instantons, the Kahler-Metric is to be Gliosis to both of the discrete quanta of energy that are to be undergoing the so-eluded-to gauge-transformation.  When such an eminent Yukawa-based inter-relationhip is to be of a Gliosis-based manner with the Kahler-Metric, the directly corresponding discrete fractals of energy, that are needed for the said discrete quanta of energy to both continue to exist and persist as discrete energy, are to be re-attained by both of the individually taken quanta of energy of this respective case.  Furthermore -- just as any Gaussian Transformation that is to act in an eminent Yukawa manner, when in relationship to the Kahler-Metric, is to go through its directly corresponding 384 consecutive iterations -- before such an eminent Ward-Caucy relationship is to be relaxed, -- this is as well to be true with that genus of a Gaussian Transformation that is known of as as a gauge-transformation.  I will more intensely describe the process of both the mentioned 384 consecutive iterations and the mentioned 191 consecutive iterations in Course 24 -- as to Conformally Invariant And Superconformally Invariant Phenomenology.  Please bear with me with any potential grammatical errors.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Part Two Of Heat And The Clifford Expansion Of The Kinetic Flow Of Gravity

The Ward-Cauchy-based condition, that those gauge-transformations -- that are to directly involve the formation of infrared photons, works to involve a higher scalar amplitude as to the correlative Clifford Expansion of the kinetic flow of gravity waves -- to where this is a situation that is indirectly involved with that general physical condition, that heat tends to bear a relatively high tendency of moving in the direction of spreading outward, in a manner that is optimum in homogeneity.  Furthermore, this is indirectly involved with the condition -- that any increase in the pressure upon a gas-based phenomenology, that is to tend to have its bearings in so as to move in the relative opposite state of such a spreading of infrared electromagnetic energy, will then tend to form a relative increase in either the scalar magnitude and/or in the scalar amplitude of those electromagnetic scatterings, particularly, here, of those that work to create more infrared photons per volume -- on account of the correlative and consequent gauge-transformations, -- that will tend to move in the condition of an increase in the proximal localized scalar amount of heat energy, that is here to be involved in any respective given arbitrary case.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Heat And Clifford Expansion Of Kinetic Flow Of Gravity Waves

Gauge-Transformations, that are due to the general activity that is involved with the process of electromagnetic scattering -- that work to form infrared photons, -- tend to indirectly work to form more of a Clifford Expansion of the kinetic flow of gravity waves, than other gauge-transformations do.  Such gravity waves that are to be delineated along the Rarita Structure, in the form of the directly corresponding Fourier-based euler propagated Schwinger-Indices, that are here to be delineated in such a manner, in so as to work to help at causing a general genus of a Rayleigh-based scattering of entropic photons, happens, to where such an annharmonic tense of scattering is to tend to "try" to proceed in the general Ward-Caucy-based condition of a radiation-based homogeneity.  Such a general genus of a Clifford Expansion, tends to bear such a Ward-Caucy-based condition of a radial cohomological generation -- that is to bear its central parametric coniaxion, from within the general region in which the directly corresponding Schwinger-Indices that are to here act as gravity waves, are to bear the initiation of their kinematic translation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Gauge-Bosons And Photons During BRST

Let us here, consider the tendency of a particular case.  A composite superstring of discrete electromagnetic energy permittivity, is to scatter upon the externalized core-field-density of one given arbitrary light-cone-gauge eigenstate, that is of a different quanta of discrete energy -- over the course of one iteration of BRST.  The ensuing Polyakov Action eigenstate, that is to be correlative to such a case, is to then happen to the discrete quanta of energy that had just been struck.  As mini-stringular segmentation is to be fed into the correlative mentioned light-cone-gauge eigenstate -- that the so-eluded-to photon is to be scattering upon in this case, the directly corresponding gauge-bosons of that discrete energy quanta that had just been struck, are to be pulled through a Ward-Caucy-based proximal local mini-Lagrangian, as these so-stated gauge-bosons are in the process of acting in so as to "pluck" their directly corresponding second-order light-cone-gauge eigenstates -- in so as to flow with the correlative scalar magnitude or scalar amplitude of the correlative Polyakov Action eigenstate that it is to be going through, in a manner that is most optimum and fitting.  As this is to happen, the photon that had here just struck the said alterior discrete quanta of energy -- is to bear optimum rest by keeping its bearings, pretty much at the general locus as to where it had just been delineated at, simultaneously, via the vantage-point of a central conipoint, -- in so as to perform its general metrical-gauge-based Hamiltonian operation, over the course of its functioning as a discrete quanta of energy -- over the course of the covariant, codeterminable, and codifferentiable group-related iteration of BRST.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

General Directoral-Based Drive Of Scattering Photons

When a photon acts, in so as to scatter upon any one discrete quanta of energy -- the photon may, depending upon the specific circumstances, strike the externalized core-field-density of the light-cone-gauge of the discrete quanta that it is to strike, at basically any angle that is here to take into consideration the Ward-Caucy condition, that a photon always tends to move in the direction of the holomorphic Lagrangian-based path of the annulus of the core-field-density of its composite derived superstring of discrete energy permittivity. Such a photon, that is to act in so as to strike another discrete quanta of energy over time -- is to always tend to scatter upon the externalized core-field-density of the light-cone-gauge eigenstate of the quanta of energy that it is here to strike.  This then works to mean, that, when a photon is to strike another discrete quanta of energy, in so as to scatter upon it -- the counter string of discrete energy permittivity of the incoming photon, is to be made Yukawa in a Gliosis-based manner at the Poincare level, to the externalized core-field-density of the eminent wave-based nature of the discrete quanta of energy impedance of whatever discrete quanta of energy that it is to scatter upon. Furthermore, if one photon is to "strike" another photon -- to where the correlative composite light-cone-gauge eigenstate of one discrete electromagnetic energy is to be made eminently Yukawa to the correlative composite light-cone-gauge eigenstate of another photon over time, then -- instead of the two photons to here be scattered upon each other, the two photons will become quantized into a common beam of light.  Again -- the photon is both itself and the beam of electromagnetic energy at the same time, -- just as the reverse-fractal tense of a drop of water in the ocean is to be both itself and the ocean at the same time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

General Gauge-Boson Positioning

Take into consideration the Laplacian-based angular momentum of a given arbitrary photon, that is delineated in so as to be Gliosis to the externalized core-field-density of one respective given arbitrary first-order light-cone-gauge eigenstate -- over one respective given arbitrary iteration of BRST.  Take the equal and opposite Laplaciain-based angular momentum of delineation, that is at the opposite side of the externalized core-field-density of the said first-order light-cone-gauge eigenstate, of this given arbitrary case.  The correlative respective gauge-bosons, are to then to work to "pluck" the correlative second-order light-cone-gauge eigenstates, at an overall average mean angling (as is according to a relationship to the Slater Equation) -- that is orphoganal to the just inferred equal and opposite Ward-Caucy-based positional delineation -- as such so-stated second-order light-cone-gauge eigenstates are to be "played like a harp," in so as to form those consequent Schwinger-Indices, that are to here to act as gravity waves, that are to be propagated along the Rarita Structure -- in so as to help to allow for the Hamiltonian operation of the existence of gravity to take hold.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Externalized Core-Field-Density Of Light-Cone-Gauge Eigenstates

Let us here, consider one given arbitrary discrete quanta of energy.  As one is to approach such a quanta of energy, in a Laplacian-based manner over the course of any one respective given arbitrary metric of BRST -- the Hodge-Index of mini-stringular segmentation here, works to bear a higher scalar amplitude.  Such a "mesh" of mini-stringular segmentation, that is to have its bearings just outside of any one respective given arbitrary light-cone-gauge eigenstate -- is to here be said to exist as the "externalized core-field-density" of the said light-cone-gauge eigenstate.  When a photon is to strike any one said discrete quanta of energy in a "Gliosis"-based manner -- it is actually to come into contact with the just described externalized core-field-density of the respective said given arbitrary light-cone-gauge eigenstate.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

As To Different Genre Of Gauge-Transformations

When different forms of electromagnetic energy are to strike either any given arbitrary Calabi-Yau space, Calabi-Wilson-Gordan space, or any Calabi-Calabi space manifold-type of phenomenology -- a different given arbitrary genre of a gauge-transformation is to happen.  Different genre of gauge-transformations, work to help at forming different tenses of a shimmering -- of those directly corresponding light-cone-gauge eigenstates, that are to be struck by such so-eluded-to photons in a Gliosis-based manner, over time.  Such different tenses of gauge-tranformation, tend to work to help at causing different tenses of metrical-based Chern-Simons singularities, over time.  This just mentioned tendency, tends to work at forming different genre of the consequently formed Schwinger-Indices -- by which such Schwinger-Indices are to here to act as gravity waves.  Such a unique set of gravity waves, tend to act to make the multiplicit Calabi-based spaces -- to behave in their unique correlative ways -- as such gravity waves are to here to be propagated along the directly corresponding multiplicit Rarita Structure eigenstates, over time.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Heat And Gauge-Transformations

The overall process of both the creation of heat energy, along with the Ward-Caucy-related Fourier-based activity of the vibrational oscillations of heat energy -- in the form of both the creation of infrared photons in correlation with their vibrations, over time, as well as the Ward-Caucy-related Fourier-based activity of infrared photons in correlation with their vibrations over time -- works to involve a general genus of gauge-transformation, that helps to work to allow for a plausible tense of a Hilbert-related volume, instead of bearing a Minkowski-related volume, for those directly corresponding atoms, and, at a reverse-fractaled tense, for those directly corresponding molecules, that are to here be correlative to the general tense of such a so-eluded-to manner of space-time-based activity.  Furthermore -- those gauge-transformations that are most correlative to the dual activity of both the formation and the activity of infrared photons over time, acts in part, as that general genus of gauge-tranformation -- that works as part of the process by which the directly correlative orbifolds and orbifold eigensets, that are to here be most Yukawa to such a general tense of activity, -- may then be brought into a Ward-Caucy-related condition of then being more susceptible to bearing less than a purely holographic-based manner of spatial dimensionality.  This is partially due to the general tense of that "shimmering" of those correlative light-cone-gauge eigenstates -- that is to happen, when photons are in part, to scatter upon such eigenstates, in the process of what is here is to be related to the consequent formation of that form of electromagnetic energy, that is known of as infrared photons, or, in other words, of what is known of as heat energy.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Infrared Photons And Heterotic Strings

Infrared photons help E(8)XE(8) strings to both persist and exist -- at the externalized core-field-density of the multiplicit proximal localized cite of both orbifolds and orbifold eigensets.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Gauge-Transformations And Mobiaty

That "shimmering" that is due to the Fourier-based activity of gauge-transformations, works to "harness" that Rarita Structure-based activity -- that acts in so as to help at completing "mobiaty."
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Infrared Photons And E(8)XE(8) Strings

The Fourier-based flow of the electrodynamic vibrations of infrared photons over time, tends to help to work to tug-in those group-attractors, that are thence brought into either a multiplicit taken  Calabi-Yau, Calabi-Wilson-Gordan, and/or a Calabi-Calabi-based region -- in so as to help in the fortification of both the existence and the persistence of E(8)XE(8) strings -- in their multiplicit correlative delineations.  E(8)XE(8) strings act, in so as to help in the process of inter-lacing both superstrings into orbifolds -- as well as inter-lacing orbifolds into orbifold eigensets.  E(8)XE(8) strings thus act, in so as to help in the process of working to allow for the Ward-Caucy-based multidemensional-related Hilbert-based Volume of the general substringular realm.  One could then say, that E(8)XE(8) strings are to the substringular -- what microtubules are to the reverse-fractal-based stratum of living cells.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.