Superconformal Invariance And Lorentz-Four-Contractions

Let us initially consider a given arbitrary individually taken orbifold eigenset, that is to be in a proximal local state of superconformal invariance -- at a reference frame that is Poincare to the externalized core-field-density of the cohomological shell, that is of the said orbifold eigenset, -- as it is to here be undergoing a Fourier Transformation, over a sequential series of group-related instantons.  The tighter that the tense of superconformal invariance is, of what is here to be of a vibrating orbifold eigenset, that is to be basically remaining in one proximal local Ward-Cauchy-based spot -- the lower that the correlative Lorentz-Four-Contractions will be, upon those superstrings of discrete energy permittivity, that work to comprise the so-stated orbifold eigenset, -- over any correlative extrapolated gauged group-metric, that is here to be of an even function of Hamiltonian operation.  Furthermore, -- the tighter that the tense of superconformal invariance is, of what is here to be of a vibrating orbifold eigenset, that is to be basically remaining in one proximal local Ward-Cauchy-based spot -- the higher that the correlative Polyakov Action eigenstate will be, upon those superstrings of discrete energy permittivity, that work to comprise the so-stated orbifold eigenset, -- over any correlative extrapolated gauged group-metric, that is here to be of an even function of Hamiltonian operation. 
I will continue with the suspense later! To Be Continued!  Sincerely, Sam Roach.

Electromagnetic Energy As A Partially Yau-Exact Phenomenology, Part One

Orbifold eigensets that are comprised, in part, by superstrings that are of discrete electromagnetic energy permittivity, that are, when individually taken, to be continuing to move through the same medium over time, tend to behave in such a manner -- to where these may here be described of as being of such a Ward-Cauchy-based state of being partially Yau-Exact.  When a beam of electromagnetic energy is continuing to travel through the same medium over time, -- the transversal-based eigenindices of any one given arbitrary respective orbifold eigenset of electromagnetic energy, -- of which are here to tend to move in the same general direction that the correlative wave-tug of the angular momentum of the composite photons, that are here to work to comprise the said given arbitrary orbifold eigenset of such a respective case, are to be directed in  -- when this is existing in a general condition of superconformal invariance -- are here to tend to generate as much cohomology as these are to degenerate, over a set extrapolated gauged group-metric.  Yet, the homotopic torsional eigenindices, that are here to move in the same general direction as the spin-orbital momentum of the said respective given arbitrary orbifold eigenset is to be directed in, are to not to tend to be of a Yau-Exact nature.  Such said torsional eigenindices, are here to tend to either generate or to degenerate significantly more cohomology than these are here to respectively degenerate or generate -- given whether or not the directly corresponding orbifold eigenset of electromagnetic energy is to either be respectively amplified or augmented Or dampened or atenuated over time, -- as this may be extrapolated over a group-related metric, that is of a Ward-Cauchy-based Kahler condition, that is here of an Even gauge-metrical functional Hamiltonian operation over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Light Intensity And Orbifold Abrasion

The higher that the intensity of electromagnetic energy is, upon the proximal locus of the topological stratum of a given arbitrary orbifold eigenset, over a set group-metric of time, -- the more that there will be the potential tendency of there then being a higher density of infrared photons, that are to likely be at the said proximal locus of the topological stratum of the respective given arbitrary orbifold eigenset, over that same said group-related metric.  As said before, the higher that the intensity is, of infrared photons upon the proximal locus of the topological stratum of a given arbitrary orbifold eigenset, the more of a chance that such a tendency alone will then work to involve the resultant causation of oscillation-based distortions upon the said respective orbifold eigenset of topological stratum.  Therefore, the higher that the intensity of electromagnetic energy is, upon the proximal locus of the holonomic substrate of an orbifold eigenset of topological stratum is, the more likely that the correlative orbifold eigenset is to then to work to bear a higher tense of substringular abrasion -- since such an individually taken factor will tend to increase the tendency of working to form oscillation-based distortions upon the topological surface of the holonomic substrate of such a said respective given arbitrary orbifold eigenset --- if over the same duration of group-related metric.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

General Genre Of Cyclic Permutations

I can immediately think of three different general genre of cyclic permutations.:  1)These may be Calabi-based. -- There may be fluctuations in any one respective given arbitrary tense of a Majorana-Weyl-Invariant-Mode, that is Poincare to the so-eluded-to internal reference frame -- that is of the correlative topological stratum of the correlative holonomic substrate.  2)These may be metrical-based. -- There may be an analogous but different relatively proximal local gauging of the directly corresponding group-metrics, that may be effectual to the Gliosis-based topological stratum, that is here of the correlative holonomic substrate at the Poincare level.  &, 3)These may be Lagrangian-based. -- There may be analogous but different relatively proximal local Lagrangian-based paths, that may be attributed to the correlative metrical-gauge-based Hamiltonian activity that may be traversed, -- over the course of a directly corresponding Fourier Transformation, that would here be happening at an internalized gauged reference frame.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Additive Schwinger-Indices

Let us initially take into consideration, two different Schwinger-Indices -- that are to here be in the process of being propagated along the topological surface of the holonomic substrate of two different respective given arbitrary segments of mini-stringular topology, -- over one directly corresponding duration of group-related metric.  Let us next consider, that the relative covariant velocity of both of the respective correlative  Schwinger-Indices is to be the same, and in the same general direction -- via the vantage-point of a central conipoint, -- over the course of that group-metric, in which the so-stated Schwinger-Indices are to be in the process of being propagated in a relative general manner, towards each other.  Let us next consider, that both of the so-stated Schwinger-Indices are to strike each other in a Gliosis-based manner, at a node that is to exist further-up in the holomorphic direction from the initially considered point of perspective, in which the initial stipulations were implied.  At this point, the behavior of the resultant Schwinger-index -- will then tend to be of an additive nature, from the nature of the two initially so-eluded-to wave-based disturbances in space, that the two initial Schwinger-Indices happened to respectively be, at the start of this case scenario.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Relative Reversal Of Gauge-Boson Plucking

Let us initially consider one given arbitrary orbifold eigenset, that is to here be basically pushed, just soely by the force of gravity, in this respective given arbitrary case -- of which is to here be moving through a discrete unitary Lagrangian, through which the said eigenset is to be translated through its directly corresponding Hamiltonian operand -- as one discrete metrical-gauge-based Hamiltonian operand, via the group-metrical constraint of a discrete set of a sequential series of group-related instantons.  Let us next, consider that the directly correlative set of gauge-bosons -- of which are here to work, in so as to "pluck" the directly corresponding second-ordered light-cone-gauge eigenstates, in so as to work to form Schwinger-Indices that are to act as the holonomic substrate of gravity waves -- are to act in such an overall directoral-based manner, in so as to work to form one overall resultant genus of a holomorphic-based topological sway -- over the so-eluded-to set time constraint, that is of the said sequential series of group-related instantons, via which the resultant overall tense of those integrative Schwinger-Indices, that are to thence form by the said "plucking" of the so-stated light-cone-gauge eigenstates by the so-stated gauge-bosons, are to then form one resultant tense of a gravitational-based push, of which is to help at working to move the said orbifold eigenset into what I have so-eluded-to as its relative forward-holomorphic direction, that is of such a respective given arbitrary case scenario.  Let us next say that the overall resultant directoral-based holomorphicity, that is to here be directly corresponding to the topological sway of those said gauge-bosons, that are to here be working in so as to "pluck" the said light-cone-gauge eigenstates -- is to reverse in the overall genus of its resultant direction, over an ensuing sequential series of group-related instantons.  Such a reversal in the holomorphicity of the "plucking" of such light-cone-gauge eigenstates, will then often tend to work to reverse the general overall resultant holomorphicity of the flow of the resultant formed Schwinger-Indices.  Such a reversal in the holomorphic wave-tug of these correlative Schwinger-Indices, may then often work to reverse the direction -- of what would here be an otherwise relatively ineffectual pulsation of a Hamiltonian-based operator -- to where this will often work to reverse the holomorphic direction of the here discussed overall so-stated orbifold eigenset.  Such a reversal in the general direction of an orbifold eigenset, will then tend to work to form an antiholomorphic Kahler condition -- over the here ensuing group-metric.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Relative Density Of Centralized Knotting Of Rarita Structure Eigenstates

The higher that the relative density is, of eigenstates that are as to the centralized knotting of the Rarita Structure is to be, the higher that the tendency of such a so-eluded-to region will be, as to being  relatively more Yukawa to Schwinger-Indices, and therefore, the higher that the tendency of such a so-eluded-to region will be -- as to being relatively more Yukawa to the presence of a gravitational-based wave-tug/wave-push, -- over a set constraint of a group-related metric.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Conformal Invariance And Transversel Velocity

Let us initially say that there are two different orbifold eigensets, that are both of the same general constitution, as well as of the same Hodge-Index as to the general quanta of energy that are to work to comprise the two so-eluded-to eigensets, as well as working to bear the same directoral-based tense of its Lagrangian-based propagation, that are then of the same general genus, that are both of a Noether-based flow, that work to bear two different radial-based velocities -- at the vantage-point of a central Lorentz-based conipoint, yet, to where, these two so-eluded-to eigensets are to bear the same relative transversal-based velocity -- at the vantage-point of a central Lorentz-based conipoint, -- over a set gauged metric, that is both covariant, codeterminable, and codifferentiable, over a sequential series of group-related instantons.  This will then work to determine the condition, that, even though both of such said orbifold eigensets are to then to tend to here be of the condition, as to working to bear the exact same general scalar amplitude as to both the degree and/or the manner as to how loose and/or how tight the transversel eigenbase of the directly correlative Majorana-Weyl-Invariant-Mode of both of such said orbifold eigensets is, during the set group-metric, yet, both of such orbifold eigensets are to then to tend here to be of the condition, as to working to bear a different general scalar amplitude as to the degree and/or the manner as to how loose and/or how tight the radial eigenbase of the directly correlative Majorana-Weyl-Invariant-Mode of both of such said orbifold eigensets is, over the set group-metric. I will continue with the suspense later! To Be Continued!
Sincerely, Samuel David Roach.

Schwinger-Indices and Gravitational Density

The higher that the scalar amplitude of the Hodge-based formation of Schwinger-Indices is, per density of overall dimensional parameterization, tends to be, given a dependent condition of a common duration of a group-related metric  --  then, the higher that the gravitational density will tend to be, of such  a so-eluded-to Ward-Caucy-based region.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Energy Density And Cohomologies, Part Two

Let us here consider two different covariant given arbitrary orbifold eigensets, that are of the same Ward-Caucy mass-based density, over the course of one respective given arbitrary group-metric.  Let us next say, that one of such orbifold eigensets is moving at a faster relative velocity -- in a terrestrial-based manner -- than the other said orbifold eigenset, over the self-same said group-metric.  The faster of the two said orbifold eigensets, will tend to eliminate its cohomologies at a faster rate than the slower of the two said orbifold eigensets.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

More As To Both Phenotypical And Recessive Bonding Cites

When a sub-atomic particle is to bear what would here amount to of as having a recessive bonding cite, during which directly associated group-metric -- the other one or more sub-atomic particles that are to bond to the initially so-stated sub-atomic particle, are to bear what would here amount to of as having a phenotypical bonding cite -- then, that holonomic substrate as to the "fitting" of the bonding cite that is recessive, will not tend to bear an adequate Hodge-Index of that mini-stringular segmentation that is immediately Yukawa to the Fourier-based activity of the bonding by which the two so-eluded-to sets of sub-atomic particles are to bond -- via that Gliosis-based inter-relation, in which what is here to be the phenotypical bonding cite, is to, instead, work to bear that adequate scalar magnitude of a Hodge-Index of that mini-stringular segmentation that is immediately Yukawa to the Fourier-based activity of the said bonding of the two so-stated sets of sub-atomic particles, that are here to work to form a less fractaled composition, as to this tending to be of a higher order of the  building blocks of the construction of a given arbitrary respective atom.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Exterior-Based Noether Currents

Let us say that one were to have a given arbitrary orbifold eigenset that was vibrating at one general spot, while it is as well remaining relatively still in a state of conformal invariance -- while, there are here to be certain individually taken orbifolds, that are to then exist from within the premises of the initially so-stated orbifold eigenset, that are definitively moving around from within the Ward-Caucy bounds of the relatively steady-stated externally-based orbifold eigenset-based reference frame of such a respective given arbitrary case scenario.  Since the externally mentioned reference frame -- being the said orbifold eigenset that is relatively stationary, is in a tense of conformal invariance, it is to here bear a Noether Current that works in such a cyclical-based manner -- to where the velocity of the so-stated reference frames as to being of the orbifold eigenset, may be equated to be at roughly zero, when in terms of the said external reference frame to here be staying from within an allotted specific zone of a vibratory tense of spatial parameters, over the directly affiliated group-metric of such a case.  Yet, since the orbifolds that are to here exist in a Fourier-based manner from within the said orbifold eigenset, are to here work to bear a definitive velocity during the so-eluded-to directly affiliated group-metric -- the individually taken orbifold eigensets that are to here be moving in both a definitive transversal and in a definitive radial-based manner over time, are to here bear a definitive Ward-based velocity, and thus, such so-stated internally-based orbifolds are to then bear such a relatively looser tense of a Majorana-Weyl-Covariance, to where such internally-based orbifolds are then to act in such a manner in so as to have a certain tense of a Noether-based current.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel Roach.

Certain Adjustments Due To Tahcyonic Flow

Let's say that a certain given arbitrary superstring of discrete energy permittivity is not orientable -- over the course of one respective correlative iteration of the Bette Action, that the said superstring is undergoing, over the course of a directly corresponding iteration of BRST. The said superstring is then to go through one iteration of its succession of the Kahler-Metric that it is to be directly associated with. Let us say, as well, that the so-stated superstring is likewise, not orientable, over the ensuing iteration of the Regge Action.  The superstring is then -- since it is here unorientable -- to go into a tacyhonic phase, for at least a relatively transient duration of group-affiliated instantons.  The said superstring is still encoded to undergo more of the process of the Kahler-Metric -- in order for the so-stated superstring to re-attain all of its fractals of discrete energy, that it needs, in order to remain as a discrete unit of energy permittivity.  So, for however long that the so-stated superstring of discrete energy permittivity is to be still undergoing its then present need for going through the Kahler-Metric that it is to be going through -- the said superstring will go through an indistinguishabley different set of substringular neighborhoods, that will then work to be able to fulfill the so-stated superstring's need for a direct affiliation with the appropriate genus of those substringular members of the Kahler-Metric that it needs to be directly in correspondence with -- in order for the said superstring to be able to re-attain its fractals of discrete energy permittiivity that it needs, in order for the said superstring to be able to both persist and exist as a discrete unit of energy permititvity --, to where the said superstring will then be in a position to where it may then be able to finish its direct correspondence with the encoded genus of the Kahler-Metric that it is needed to be in a direct association with, over the corresponding group metric of time to where this may happen.