Isotropically Stable Second-Order Light-Cone-Gauge Eigenstates, Working To Result In Isotropically Stable First-Order Light-Cone-Gauge Eigenstate

 When a cohesive set of covariant second-order light-cone-gauge eigenstates, are here to vibrate in their propagational mode, in unison, this will often tend to facilitate the general physical attribute, of isotropic stability, from among the inferred constituency of such a cohesive set of eigenstates, to where, this will often, in turn, tend to consequently result, in increasing the general tendency of isotropic stability, in the eminently associated respective first-order light-cone-gauge eigenstate, of which such an earlier inferred set of second-order light-cone-gauge eigenstates, are here to have worked to comprise. This will thereby often tend to work to increase the probability, that the eminently associated discrete quantum of energy, of which is here to be expressing such an inferred tense of a gauged-action, will thus be more likely to be gauge-invariant, as this is here to be taken, over a respectively taken Fourier-Related-Progression. SINCERELY, SAM ROACH, 

Perturbative Light-Cone-Gauge Eigenstates -- Spurious Cohomology

 Perturbative light-cone-gauge eigenstates, tend to be eminently associated with spurious cohomology. 

The Fourier-Related-Progression Of The Homotopic Translation Of Component Light-Cone-Gauge Eigenstates

 When electromagnetic energy scatters, the Fourier-Related-Progression, of the homotopic translation, of the associated proximal local respective component light-cone-gauge eigenstates, is to tend to work to bear, an anharmonic perturbation. TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH.

Adjacent Quantized Light-Cone-Gauge Eigenstates

 Adjacent quantized light-cone-gauge eigenstates, often tend to bear a homeomorphic nature in relation to one another. 'TILL NEXT TIME! TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. 

Noether-Based Mass-Bearing Light-Cone-Gauge Eigenstates That Are Distributed Adjacently

 Noether-Based mass-bearing light-cone-gauge eigenstates that are distributed adjacently, often tend to be gauged asymmetrically. TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. 

Isotropically Stable Light-Cone-Gauge Eigenstates -- Harmonic/Anharmonic Schwinger-Related Vibrations

 Isotropically stable light-cone-gauge eigenstates, often tend to have a greater tendency, of working to form harmonic Schwinger-Related vibrations than anharmonic Schwinger-Related vibrations. It follows, then, that isotropically unstable light-cone-gauge eigenstates, often tend to have a greater tendency, of working to form anharmonic Schwinger-Related vibrations than harmonic Schwinger-Related vibrations. 

'TILL NEXT TIME, AT THIS BLOG CITE! TO BE CONTINUED! SINCERELY, SAM ROACH.

Forces Of Nature -- Adhesion/Cohesion

 The consequential resultant of the holonomic propagation of the vibrations of light-cone-gauge eigenstates, helps work to initiate the multiplicity of the forces of nature; Whereas, the consequential resultant of the holonomic propagation of the vibrations of cohomology-related eigenstates, helps work to form the respective adhesion/cohesion of such initiated forces of nature. SINCERELY, SAM ROACH.

Hyperbolic Curvature Of Directly Corresponding Second-Order Light-Cone-Gauge Eigenstates

 For one distinct mass-bearing discrete quantum of energy: 

The greater the Polyakov Action -- The Lesser the Lorentz-Four-Contraction -- the more pronounced the hyperbolic curvature, of the directly corresponding second-order light-cone-gauge eigenstates. (As the motion of such a mass-bearing discrete quantum of energy, is to be Decreasing in its relative speed.)

Furthermore:

The lesser the Polyakov Action -- The greater the Lorentz-Four-Contraction -- the less pronounced the hyperbolic curvature, of the directly corresponding second-order light-cone-gauge eigenstates. (As the motion of such a mass-bearing discrete quantum of energy, is to be Increasing in its relative speed.) (SAM).

Gauge-Bosons -- Main Type Of Phenomenology --- Incites The Reductional Forces Of Physical Nature

 Gauge-Bosons are the main general type of phenomenology, that work to "incite" the presence of the reductional forces of physical nature. It is the "plucking" of the second-order light-cone-gauge eigenstates BY gauge-boson eigenstates -- over the durational course of each individually taken group-related instanton -- that consequentially works to form those resultant vibrational eigenstates, that are thence to propagate relatively outward, in so as to work to influence those general activities of the Rarita Structure, in such a general manner, in so as to play a major role in the formation of those basic forces of physical nature, that are necessary to exist, so that there may be any sort of a  prolonged existence of the general presence, of what is perceived to be space-time-fabric. TO BE CONTINUED! SINCERELY, SAMUEL.

Abelian Wave-Tug -- Light-Cone-Gauge Eigenstate -- Inertia

 When a given arbitrary light-cone-gauge eigenstate, is here to work to apply an abelian wave-tug, upon the respective directly associated discrete energy quantum, that it is here to be physically operating upon, this general tense of a gauged-action, will consequently often tend to have the affinity, of working to form an inertial tense of impedance. Inertia is heuristically associated with the general characteristic of mass. Noether-Based mass-bearing discrete energy quanta, tend to always work to bear an abelian light-cone-gauge topology. This is part of the reason, as to why mass tends to have such an affinity, for working to display the general characteristic of "inertia." I will continue with the suspense later! SAM ROACH. (1989).

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).

The Light-Cone-Gauge And Electrodynamic Permeability

The more well-fitted that the "aerodynamic" nature is to be, (as in being able to more readily travel through the general medium of superstring-related "pressurized vacuum"), that is here to be of any given arbitrary (first-order) light-cone-gauge eigenstate, that is being displayed, -- the more electrodynamic permeability that the directly corresponding discrete energy (that is here to be proximal local to the composition of the respective stated light-cone-gauge eigenstate), is to tend to be. I will continue with the suspense later! Sincerely, SAMUEL ROACH.

Analogous Light-Cone-Gauge Eigenstates

 All of the first-order light-cone-gauge eigenstates, that are here to work to comprise a specific given arbitrary cohesive set of discrete energy quanta, will tend to work to perform an analogous exhibition of a delineation-related display, that is of its covariant morphological contour -- as this is here to be taken, over a respective Laplacian setting, -- during the course of a respective iteration of group-related instanton. SAM.

Direction Of Time And Light-Cone-Gauge Holomorphicity

 Forward-Moving time-related phenomenology, tends to work to involve the multiplicity of light-cone-gauge eigenstates, that are here to tend to work to bear the directional drive, of a relativistic forward-holomorphic wave-tug. Whereas; backward-moving time-related phenomenology, tends to work to involve the multiplicity of light-cone-gauge eigenstates, that are here to tend to work to bear the directional drive, of a  relativistic reverse-holomorphic wave-tug. Sincerely, SAMUEL DAVID ROACH.

A Perception About The Light-Cone-Gauge

 Here is a current perception that I have, about the light-cone-gauge:

The multiplicity of the interactive interconnections, that are here to exist, both between and amongst the multifarious light-cone-gauge eigenstates -- that are here to exist in time and space -- work to help, in controlling the respective multiplicity of the covariant flow of time. To Be Continued! Sincerely, SAMUEL ROACH.

Ebbing Flow Of Alterations -- Behavior Of Light-Cone-Gauge Eigenstates

 When the ebbing flow of the alterations in the kinematic behavior, that is here to be of those individually taken given arbitrary light-cone-gauge eigenstates, in which this stated "ebbing flow," is here to work to reiterate in a sequentially repetitive tense, of a Lagrangian/metric-related manner -- to where the cohesive set of such a general tense of these just stated eigenstates, is here to work to comprise the wave-based nature of the discrete energy impedance, that is here to be of a respective given arbitrary cohesive set of discrete energy quanta, -- this just inferred recursive pattern, that is here to be appertaining to the behavior of a respective set of cohesive light-cone-gauge eigenstates, will consequently often tend to result, in helping to cause the herein stated cohesive set of discrete energy quanta, of which such mentioned light-cone-gauge eigenstates are here to work to comprise, to work to bear a recursively smooth Ricci Flow. SAM.

Fadeev-Popov-Trace Eigenstates And Gauge-Invaraince

 When a Fadeev-Popov-Trace eigenstate is to work to maintain its same manner of behavior, when in relation to the motion of electromagnetic energy, over a directly corresponding sequential series of group-related instantons, then, the directly corresponding light-cone-gauge eigenstate, that such a said Fadeev-Popov-Trace eigenstate is here to be holomorphically acting upon, over the earlier mentioned respective sequential series of group-related instantons, will consequently tend to have a relatively heigtened probability, of also working to maintain its same manner of behavior, when in its relation to the motion of electromagnetic energy. When a light-cone-gauge eigenstates is to maintain its same manner of behavior, over a correlative sequential series of group-related instantons, it may consequently be said, that the directly corresponding discrete quantum of energy, that is here to be most associated with the kinematic exhibition of such a said light-cone-gauge eigenstate, is here to be "gauge-invariant." Therefore; when a Fadeev-Popov-Trace eigenstate is to work to maintain its name manner of behavior, when in relation to the motion of electromagnetic energy, one may then say, that the directly corresponding discrete quantum of energy, that is here to be most directly associated with the said Fadeev-Popov-Trace eigenstate of such a respective given arbitrary case, is here to tend to be "gauge-invariant." Sincerely, SAMUEL ROACH.

In General -- The "Gauging" Of The Light-Cone-Gauge

 Light-Cone-Gauge Eigenstates work to gauge the modification of certain attribute-related characteristics, that are here to be appertaining to certain aspects, of the the construction of the topological contour of superstrings of discrete energy permittivity, as in conjunction with their directly corresponding inferred counter strings, -- as such strings and counter strings of discrete energy permittivity, are here to be altering in their motion-related behavior, when in relation to the motion and presence of electromagnetic energy. SAM.

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.