Del Of The Ricci Flow And Metric-Gauge-Related Pulsation

Let us initially consider a covariant relationship, that is here to exist between two different orbifold eigensets. Let us think, more specifically, about the relationship between the Del of the Ricci Flow, and the directly related resultant covariant metric-gauge-related pulsation -- that is here to exist (or "co-exist"), between (or among) the given arbitrary field, -- that is here to help at working to link the interaction, that is here to occur between the two different but interdependent inferred cohesive sets of discrete energy quanta, that are to be considered in this particular case scenario. :

When the Del of the covariant Ricci Flow is to be of a positive fractional value, that is here to be relatively closer to "0," then, the resultant metric-gauge-related pulsation will consequentially tend to be of a larger scalar magnitude/amplitude -- than if the correlative Del of the covariant Ricci Flow were, instead, to bear a positive fractional value, that would otherwise be relatively closer to "1."

Furthermore; when the Del of the covariant Ricci Flow is to be of a negative fractional value, that is here to be relatively closer to "-1," then, the resultant metric-gauge-related pulsation will consequently tend to be of a larger scalar magnitude/amplitude -- than if the correlative Del of the covariant Ricci Flow were, instead, to bear a negative fractional value, that would otherwise be relatively closer to "0."

To Be Continued! Sincerely, Samuel David Roach.

Fields And Chern-Simons Singularities

When there is to be an alteration in that fractal of the electric field, that is here to be directly associated with that motion of the Noether Current, that is here to be of a given arbitrary orbifold eigenset, this will often tend to be caused by a spontaneous alteration in the angular momentum, that is here to be directly corresponding to such a here stated orbifold eigenset, over time, -- to where this will consequently tend to result in the formation of a correlative set of one or more Lagrangian-based Chern-Simons singularities, that are thence to be formed at the moment of such a spontaneous alteration in the angular momentum of such a here mentioned orbifold eigenset.  Furthermore; when there is to be an alteration in that fractal of the magnetic field, that is here to be directly associated with the motion of the Noether Current, that is here to be of a given arbitrary orbifold eigenset, this will often tend to be caused by a spontaneous alteration in the spin-orbital momentum, that is here to be directly corresponding to such a here stated orbifold eigenset, over time, -- to where this will consequently tend to result in the formation of a correlative set of one ore more metric-based Chern-Simons singularities, that are thence to be formed at the moment of such a spontaneous alteration in the spin-orbital momentum of such a here mentioned orbifold eigenset.  To Be Continued!  Sincerely, Samuel David Roach.

Anti Gravity And Decrease In Substringular Impedance

The more anti gravity, that is here to be applied to the boundary conditions of a mass-bearing orbifold eigenset, in the substringular -- the less impeded that the said orbifold eigenset will consequently tend to be, in the process of its motion along the general path of its directly corresponding Hamiltonian operand, -- over the course of time.  The less impedance that is thereby to be applied to the general motion of an orbifold eigenset, the less inhibited that such a said eigenset will consequently tend to be, -- by the general force of the Ward-Cauchy-related substrate of the correlative substringular pressurized vacuum, that it is here to come into contact with, as well, over the course of such an inferred evenly-gauged Hamiltonian eigenmetric.  The less inhibited that such an orbifold eigneset will tend to be, at moving along the general course of its directly corresponding Hamiltonian operand over time, -- the higher that its superstringular permittivity will consequently tend to be.  Furthermore; the higher that the superstringular permittivity of an orbifold eigenset will tend to be, the faster that such a said orbifold eigenset will consequently tend to be able to be moving at.  Consequently; the more of an increase in the presence of anti gravity, that is thereby to be directly associated with the covariant motion of a mass-bearing orbifold eigenset (that is here to tend to be, of a Noether-based nature), when this is here to be taken over an evenly-gauged Hamiltonian eigenmetric, the faster rate that such a said eigenset will consequently tend be able to accelerate at, over time.  As mentioned many times before; the faster that a mass-bearing orbifold eigenset is to accelerate, the quicker that its  directly corresponding i*PI(del) Action will then tend to be.  Therefore; the more that there is to be an increase in the anti gravity, that is here to be applied to the covariant Fourier-related proximal local kinematic presence of a mass-bearing orbifold eigenset, over time, -- the quicker that its directly corresponding respective i*PI(del) Action will therefore tend to be.  The quicker that the i*PI(del) Action is thence to occur for a mass-bearing orbifold eigenset, the more charge that will consequently tend to be present at that varied proximal locus, that is here to be positioned at the directly corresponding region, that is existent at the covariant Fourier-related kinematically altering substringular neighborhood, that is here to be directly appertaining to such a respective eigenset.  Therefore; the more anti gravity that is here to be fed into a system, that is thence to be directly associated with a mass-bearing Noether-related orbifold eigenset, -- the more charge that will consequently tend to be associated with such a here stated orbifold eigenset per time, over the course of that duration in which such an inferred impartation of anti gravity is here to be brought into the Ward-Cauchy-related bounds, that is of the motion of such a respective mentioned mass-bearing orbifold eigneset.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Chern-Simons Invariant-Related Action And The i*PI(del) Action

Let's initially consider two different orbifold eigensets, that are here to work to bear a covariant-related motion in relationship to one another.  Both are here to be similar but different, except for one main factor, -- even though both of these said orbifold eigensets, are here to work to bear the same transversal change in motion, -- when in respect to the motion of electromagnetic energy.  Here is the one main difference between the two so-inferred eigensets; one of these said orbifold eigensets, is to work to bear a greater scalar amplitude of a tense of spin-orbital momentum than the other said orbifold eigenset.  The said eigenset of the two, that is here to work to bear a greater scalar amplitude of a tense of spin-orbital momentum than the other inferred eigenset -- is then to consequently work to tend to bear a greater scalar amplitude of torsion, that is here to be applied to the topological stratum of its directly corresponding entity of holonomic substrate, -- than the amount of a scalar amplitude of torsion that is here to be applied to the other mentioned orbifold eigenset of this particular case.  The here inferred Ward-Cauchy-related Hamiltonian Operator, that is here to tend to work to bear a greater torsional force that is here to be applied to the topological stratum of its directly corresponding entity of its holonomic substrate, -- will then consequently tend to bear a greater plateau of a change in motion, than the other here mentioned inferred Ward-Cauchy-related Hamiltonian Operator.  This will thus work to help in causing there to tend to be more of an applied tense of an i*PI(del) Action, that is here to be "geared" upon this said orbifold eigenset, which is also here to work to bear a greater tense of a torsion of which is here to be applied to its topological stratum, than what is here to be applied to the other said eigenset of the two.  This will thence tend to work to cause the so-inferred orbifold eigneset, that is here to work to bear a greater tense of torsion -- that is here to be applied upon it, to work, as well, to bear a greater scalar amplitude of a Chern-Simons Invariant-Related Gauge-Action, that is here to be applied upon it.  Furthermore; in this particular case, the orbifold eigenset that is here to bear the greater tense of a Chern-Simons-Invariant operation, will then tend to work to be associated with a greater charge, than the other said orbifold eigenset will tend to be associated with, -- over an evenly-gauged Hamiltonian eigenmetric.  To Be Continued!  Sincerely, Samuel David Roach.

Gauge-Metric-Related Pulsation And Its Correlative Tree-Amplitude Attribute

Let's initially consider an orbifold eigenset, -- that is here to be exhibiting a behavior that is to be tantamount to a gauge-metric, that is here to be pulsating through time and space, via a directly corresponding Hamiltonian operand, that is here to act as a binary Lagrangian-based path in time and space. Next, let's say that the relative velocity of such a said orbifold eigenset, is here to be maintained.  Let's next say that a Hamiltonian operator that is here to be exhibiting a tense of a holonomic substrate, that is here to make such a said operator to be tantamount to be acting as a phenomenology of metric-gauge, to where such a said Hamiltonian operator is to spontaneously couple in a Yukawa-related manner with the initially stated orbifold eigenset, in a manner that is here to subsequently work to help in causing the initially stated orbifold eigenset to alter in its Kahler-related quotient, in such a manner to where its directly corresponding Lagrangian-based path, is to alter into a resultant tense of acting as a tertiary Lagrangian-based path, -- to where the tree-amplitude-related tense of the motion of the initially stated orbifold eigenset, is to now to tend to work to bear an increase in its genus of knotted interaction with its immediate environment -- over an evenly-gauged Hamiltonian eigenmetric.  Such a perturbation in the Lagrangian of the motion of the initially inferred set of discrete energy quanta, that are here to operate in so as to perform one specific function, will then tend to work to cause the so-eluded-to orbifold eigenset, that has here to have increased in its genus of tree-based Lagrangian scalar, to become of more of a Yukawa-based influence upon the motion of the general region in which the said orbifold is here to be moving through, as it is here to have gone from acting as a metric-gauge that is here to have been traveling via a binary Lagrangian-based path, Into acting as a metric-gauge that is here to result in consequently to be traveling via a tertiary Lagrangian-based path.  I will continue with the suspense later! To Be Continued!Samuel Roach.

Added Torque Towards Cohomology-Related Generation

Let us consider two different mass-bearing orbifold eigensets -- of which are then to work to bear a Majorana-Weyl-Invariant-Mode, which is thereby super conformally invariant at an internal reference-frame. Each of these said given arbitrary orbifold eigensets, are here to be in the process of being translated through a Lagrangian, at an external reference-frame,  by a Legendre homology -- at a relatively high rate of speed.  Both of said such orbifold eigensets are here to work to bear both the same relativistic mass, as well as the Ward-Cauchy-related condition -- that both of such said orbifold eigensets are here to work to bear the same relativistic transversal velocity, when this inferred transversal velocity is here to be considered, as relative to the motion of electromagnetic energy.  Next, let's say that both of these respective given arbitrary eigensets, are to be transferred at such a so-eluded-to velocity -- over the same duration of an evenly-gauged Hamiltonian eigenmetric, -- in a manner that is simultaneous, via the vantage-point of a central conipoint.  One of these just mentioned mass-bearing orbifold eigensets, is to simply be in the process of being translated in a transversal manner, over the proscribed time that is being implied here; whereas -- the other mentioned mass-bearing orbifold eigensets, is to be in the process of being translated in a manner that is both of a transversal nature and of a radial nature, over the proscribed time that is being implied here.  That orbifold eigenset of the two, that has been discussed in this case, that is here to bear both a radial and a transveral motion -- over the course of its projected trajectory, which is over the same duration of time, -- will then tend to work to bear an added tense of torque, than the other said orbifold eigenset.  This will then work to help at tending to cause this said respective eigenset -- that is here to work to bear a greater tense of torque than the other of the two said respective eigensets, to then act, in so as to work to generate more cohomology over time, than the other orbifold eigenset that is being discussed here.  When one is then to consider a reverse-fractaled-out condition, of the just mentioned cohomology being translated into a tense of charge, -- this will then mean, that this may then elude to the condition, that the said orbifold eigenset of such a respective given arbitrary case, that is here to bear an added tense of torque, than the other of such inferred eigensets, to where this will then tend to potentially work to help at forming a greater scalar magnitude of charge generation over time, at a relatively speaking more macroscopic level than the subatomic level, than the other of the two different said orbifold eigensets.  To Be Continued!  Sam Roach.

Assembled Into A Tense Of Majorana-Weyl-Invariant-Mode

When a discrete set of superstringular phenomenology of kinetic energy -- is here to become assembled into a tense of a multiplicit Majorana-Weyl-Invariant-Mode, this will then work to convert such a said set of discrete kinetic energy, to transform into a tense of one or more mass-bearing orbifold eigensets.

Kahler-Based Quotients And Substringular Structural Integrity

The greater the scalar amplitude of the correlative Kahler-based quotient of an orbifold eigenset -- the more fortified the E(8)XE(8) oscillation-based tendency is.  The more fortified the E(8)XE(8) oscillation-based tendency is, -- the greater the structural integrity is, of the directly corresponding orbifold eigenset.  Samuel David Roach.

Majorana-Weyl-Invariant-Mode And Pulse

Let's say that one were to  have two different mass-bearing orbifold eigensets, that are here to be traveling with the same velocity.  Let's say that both of such orbifold eigensets, were to have the same Hodge-Index of discrete energy quanta.  The orbifold eigenset of such a case, that is here to work to bear a greater Majorana-Weyl-Invariant-Mode, will then tend to have a higher scalar amplitude of a pulse -- than the other comparative orbifold eigenset, that is of such a given case.  I will continue with the suspense later!  Sam Roach.

Some General Genre Of Interactions

When a set of individually taken superstrings of discrete energy permittivity, that are initially to not be eminent in interdependence, are here to be brought together -- in so as to help at working to form an orbifold eigenset, then, this said just mentioned process, is one general genus, of what may here to be thought of as being a tense of a Wess-Zumino interaction, as this is here to be taken at a relatively small level.
Consequently -- when an orbifold eigenset, is to be scattered into a tense of individually taken discrete quanta of energy, -- that are to no more to be working together, in so as to otherwise be operating as a group to perform one specific function -- then, this said process is one general genus, of what may here to be thought of, as being a tense of a Cevita interaction, as this is here to be taken at a relatively small level.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Scalar Amplitude Of Chern-Simons Attribute

Let us initially consider an orbifold eigenset -- that is here to be traveling, in the relative holomorphic direction -- over time.  The motion of the said given arbitrary orbifold eigenset -- that is here to be traveling in the respective holomorphic direction -- will tend to be propagated, with somewhat of a direct correlation, in so as to work to be relatively lined-up -- with the direction of that directly corresponding respective Laplacian-related bearings of a wave-tug potential, that is here to be most appertaining to the proximal local positioning, that is of the angular momentum of the so-stated orbifold eigenset.  Since an orbifold eigenset is a set of one or more discrete quanta of energy -- that operate, in so as to perform one specific function -- those superstrings of the said general genus of an eigenset, that are most proximal local to the relative Laplacian-related positioning of its directly corresponding angular momentum, that are of the said cohesive set of discrete energy quanta, -- will then tend to work to bear a relatively higher probability of advancing into their ensuing spatial delineations -- in such a manner, that is here to be of more of a hermtian-related nature.  This is then to consequently cause the physical Ward-Cauchy-related condition, -- to where, those superstrings, that are most proximal local to the respective cite, at which the angular momentum of its eminently correlative orbifold eigenset is to be tugged at towards -- will then tend to bear a relatively lower scalar amplitude of a Lagrangian-related Chern-Simons attribute, -- than those superstrings, that are, instead, to be external to that proximal local cite-based region, at which the respective Laplacian-based angular momentum of such a said orbifold eigenset is to eminently to be tugging towards, in so as to work to allow for the holomorphic translation of the said orbifold eigenset, over time.
I will continue with the suspense later!  To Be Continued!  Samuel David Roach.

Attraction Of Orbifold Eigenstates

Let us initially say, that one were to be considering two different orbifold eigensets.  Both of such said orbifold eigensets -- are here to be propagated at the same covariant-related velocity, over the course of some given arbitrary evenly-gauge Hamiltonian eigenmetric -- via some general genus of a Fourer Transformation.  Both of such so-stated orbifold eigensets, are here to be comprised of, by mass-bearing superstrings of discrete energy permittivity.  Since both of such just stated eigensets, are to work to bear a mass-bearing nature -- these two said orbifold eigensets, are here to both, individually taken, to bear the Ward-Cauchy-related physical condition -- as to be of a Majorana-Weyl-Invariant-Mode.  This will then work to mean, that both of such said eigensets, are here to be superconformally invariant -- at an internal reference-frame.  Whichever orbifold eigneset, is here to work to bear a higher scalar amplitude of a Majorana-Weyl-Invariant-Mode -- the more magnetism that such a said orbifold eigenset will then tend to display, over the course of the earlier mentioned duration, that is to happen over an evenly-gauge Hamiltonian eigenmetric.  To Be Continued!  Sincerely, Sam Roach.

Metric-Related Pulsation And Dimensional Compactification

Metric-Related singularity, is here to be directly involved with the dimensional-related pulsation -- that is of a set of one or more discrete quanta of energy, over time.  So, if an orbifold eigenset is to change in either the number of spatial dimensions that it is here to be exhibiting, Or, in its rate of pulsation over time, -- then, such a said orbifold eigenset is to then to be indicating, that it is here to be working to bear a metric-related tense of one or more Chern-Simons singularities.  Furthermore, -- if an orbifold eigenset is to be of the nature, as to here to be having what may be described of as being of a flat Ricci Curvature -- then, such a said orbifold eigenset is to here to be in the process of maintaining the same number of spatial dimensions over time.  Consequently, in so long as an orbifold eigenset, that is to here to be working to bear a flat Ricci curvature, -- is to here to be consistent in maintaining a constant rate of pulsation in the substringular, over time, -- then such a said orbifold eigenset, will then tend to work to bear no metric-related Chern-Simons singularities.
I will continue wth the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Mini-Stringular Segmentation And The i*PI(del) Action

Here's some metaphorical "food for thought."
What the "action" of the said i*PI(del) action is to be, is the multiplcit and multivarious interactions, that are of those directly corresponding loci of mini-stringular segmentations, that are to act or exhibit here -- a set of gauge-metric eigenstates, that are here to work to tend to result in, -- the correlative conditions, by which the multiplicit discrete quanta of energy permittivity are to then to have a Laplacian-related delineation of those "partition-based discrepancies," that are here to be distributed as inferred, -- as is to be proportional to the directly corresponding eminent Polyakov Action.  This "action" of increments, of what may be thought of as being "quanta" of zero-point-energy -- works to not only help-out in delineating the appropriate number of partition-based discrepancies per superstring and its correlative counterstring, as is as accordling to the scalar amplitude of the Polyakov Action, -- it also tends to work to follow the same general "trend" of attribution, to all of the superstrings, that are of one given arbitrary respective orbifold eigenset.  To Be Continued!  Sincerely, Samuel David Roach.

A Basic Example Of Ward-Polarization

Here is a basic general example, of what may be termed of as a phenomenon -- in which there is to be the Ward-Cauchy-based condition of Ward-Polarization:

Let us initially say that one is to have an orbifold eigenset, that is to be undergoing a tense of conformal invariance at its internal reference-frame, that is here to work to bear a tense of what would here be at least the equivalence -- of a tense of angular momentum, that is subtended in what would here be the relative forward-holomorphic direction.  Let's next say, that over the translation of a relatively small distance, as taken in the earlier mentioned forward-holomorphic direction, from where the initially stated orbifold eigenset is to be bearing its so-eluded-to tightly-knit location of vibrational oscillation,  -- there is to be the bearings of a tense of a quantum of electromagnetic energy to be present.  However, there is here, in this general case, an orbifold eigenset, that is placed in-between the direction of the angular momentum that is of the initially stated orbifold eigenset and the so-stated quantum of electromagnetic energy -- that is here to be placed in such a manner, to where the relative holomorphic direction of the orbifold eigenset that is here to get in the way, is to be orthogonal to the holomorphic direction of the initially stated orbifold eigenset.  Such a substringular condition of such a case, may then work to partially, if not completely, block any otherwise eminent Yukawa Coupling to then to be able to be achieved, between the initially said orbifold eigenset and the so-eluded-to electromagnetic energy-based orbifold eigenset.  This general genus of a Ward-Cauchy-related condition,  is one of basically countless types of situations -- in which there is to be the phenomenon, of what may be termed of as Ward-Polarization.  Samuel David Roach.

Evenly-Smooth Application Of i*Pi(del) Action

Whenever one is to have a given arbitrary orbifold eigenset -- that is here to work to maintain its genus of spatial dimensionality, in which the directly corresponding homotopic residue is to be conserved, over a given evenly-gauged Hamiltonian eigenmetric -- from the vantage-point of the internal reference-frame of such a said respective orbifold eigenset -- there is then to tend to be an evenly-smooth application of the directly corresponding given arbitrary i*PI(del) Action. This will then tend to mean, -- that the respective given arbitrary orbifold eigenset of such a case, will then tend to maintain the tense of its rate of the acceleration of its pulsation, over the course of the duration of such a respective evenly-gauged Hamiltonian eigenmetric.  This will then tend to mean, that the so-eluded-to set of discrete energy quanta, that are here to operate to perform one specific Ward-Cauchy-related function -- will then tend to bear no metrical-related "spurs" in its so-eluded-to acceleration. This will then work to tend to mean -- that, over the so-mentioned Hamiltonian eigenmetric, -- that the said eigenset will, over the course of the so-eluded-to duration that is here to be extrapolated, tend to work to bear no spurs in its metric-based Chern-Simons singularities, -- since there is here to be no alteration in the acceleration of its dimensional-related pulsation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Increasing Relative Velocity And Rarita Structure Eigenstates

Let us initially consider an orbifold eigenset, that is here in this case to consist of at least in part -- the presence of mass-bearing superstrings of discrete energy permittivity.  Let us next say -- that the said orbifold eigenset, is to be accelerating up to nearly the rate of light speed.  As the said orbifold eigenset is to be increasing in its relative velocity, over an evenly-gauged Hamiltonian eigenmetric -- it is then to bear increasingly more mass, -- even though the overall specific Ward-Neumman constraints of the said eigenset's physical bounds are to if anything decrease.  This then works to indicate, that, as the so-eluded-to set of superstrings that are here to operate to perform a specific function, is to move at a relatively increasing rate, when this is in comparison to light that is here to go even faster -- that the density of the mass of the said orbifold eigenset is then to increase as well.  This will then work to indicate the physical conditions of an increased density, as to what are here to be the correlative centralized knotting of the proximal local Rarita Structure eigenstates.  It is the Rarita Structure, that works to convey both the vibrations of gravity, as well as the multivarious inflections in the conveyance of the ever changing forms of the four main physical forces of nature.
I will continue with the suspense later!  To Be Continued!  Sincerely Samuel David Roach.

Depth Of Vibration And Majorana-Weyl-Invariant-Mode

The higher that the tense is, that the correlative Majorana-Weyl-Invariant-Mode is to be of -- for any one given arbitrary orbifold eigenset -- the Deeper that the vibrational mode will tend to be (although slower), for those individually taken superstrings of discrete energy permittivity, that work to comprise the said respective orbifold eigenset.  Consequently -- the lower that the tense is, that the correlative Majorana-Weyl-Invariant-Mode is to be of -- for any one given arbitrary orbifold eigenset -- the Less Deep that the vibrational mode will tend to be (although faster),  of those individually taken superstrings of discrete energy permittivity, that work to comprise the said respective orbifold eigenset.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Conditioned Substringular Orientation

Whenever an orbifold eigenset is conditioned to be of an unorientable nature, both its correlative composite superstrings of discrete energy permittivity as well as its correlative composite gauge-bosons -- will be put into such a Ward-Cauchy-related set of conditions, to have thus been made unorientable.  Yet, whenever the superstrings of discrete energy permittivity, that are here to be of an orbifold eigenset, are instead, to have been conditioned to be made orientable -- then its correlative composite superstrings as well as its correlative composite gauge-bosons, will then be of such a nature -- to where these will ensue to have been made orientable.  Gauge-Bosons will always tend to display the spatial dimensionality, that is of the correlative field of discrete energy permittivity that these indirectly help at working to form, via the nature of their kinematic Hamiltonian function -- yet, in such a manner to where such a general genus of heterotic superstrings -- such as the just mentioned gauge-bosons -- will always be of a symplectic homology, when this is to here to be taken simply in and of itself.  You see -- gauge-bosons are a certain form of heterotic stringular phenomenology, that are here to exist from within the multiplicit Ward-Neumman bounds of the core-field-density of any one individually taken discrete quantum of energy, which act in my particular string theory model -- in so as to pluck the correlative second-order light-cone-gauge eigenstates, that directly correspond to the wave-functionality of the discrete energy impedance of any one discrete quantum of energy, -- in so as to multiplicitly work to form that general genus of Schwinger-Indices, that are necessary, in so as to be able to help in the process of then to be working to form the general physical forces, that are to be exhibited by the said multiplicit discrete energy (such as either the strong force, the electrostatic force, the gravitational force, and/or the weak force).  Metaphorically think of this biological example.  Animals have mitochondria in their cells. Mitochondria are certain organisms that exist in all animal cells -- that act, in so as to help-out in the process of working to form most of the chemical energy of any one said animal.  Likewise -- gauge-bosons exist from within the confines of discrete energy quanta, -- in so as to help-out in the perpetuity of the existence of those said discrete energy quanta.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Velocity And Flow Of Homotopic Residue

Let us initially consider an orbifold eigenset -- that is to here to work to bear one specific theoretical rest mass.  The faster that the velocity of the said orbifold eigenset is to be -- the less partition-based discrepancies that will then exist from within the confines of the individually taken superstrings of discrete energy permittivity that work to comprise the said eigenset, yet, there will tend to here be, as well, a proportional increase in the number of mass-bearing strings that will then be existent from within the confines of the said orbifold eigenset -- so, as the said orbifold eigenset is to increase in its relative speed over a set duration, -- the said eigenset is then to become denser in discrete energy, since mass tends to increase as such a said mass is to increase in its velocity relative to light.  So, even though homotopic residue tends to flow out of the individually taken superstrings of an orbifold eigenset as it approaches light speed -- homotopic residue still tends to be conserved for the said orbifold eigenset, -- since there is here to be a proportional increase in the number of superstrings that work to comprise such a said eigenset.  (Mass increases as speed increases.  Mass is a form of energy.  Therefore, as an orbifold eigenset is to increase in its velocity relative to light -- the number of strings that work to comprise such a said eigenset is to increase in number.)
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.