A Potentially Viable Idea

Here's a little bit of something to think of, in relation to the main influences of physical nature:

(((Discrete Metric-Gauge-Related-Field-Operator)*(Discrete i*PI(del) Action)*(Power (4.135607315*10^(-17) of one Watt))*(Discrete Inertial-Related Pulsation)*(Discrete Idea)*(Discrete Entropy)*(Discrete Charge))/(Discrete Majorana-Weyl-Invariant-Mode))
= 2.062365054*10^(-129)*(6.62607004*10^(-34)Joules*Seconds) (Zero-Point Energy).

((1.110972413*10^(-18)Kg/Coulumbs)*(8.635858*10^(-63)Coulumbs*Seconds)*(4.135607315*10^(-17) of one Watt)*(8.71563*10^(-79)Meters*Seconds)*(7.041797292*10^(-27)Inverse Meters)*(3.364124329*10^(-25)Seconds/Coulumbs)*(1.6022*10^(-19)Coulumbs))/(9.5942*10^(-80)Kilograms*Seconds)).

= 2.062365054*10^(-129)*(6.62607004*10^(-34)Joules*Seconds) (Zero-Point Energy), or, in other words, this is 2.062365054*10^(-129) of the Planck Constant!

I apologize for the mistake about this earlier!!!

I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

P.S.:  Yes Doctor Little, this is the blog of one of your patients!

One Manner Of "Looking At" The Majorana-Weyl-Invariant-Mode

What I have implied of as being the Ward-Cauchy-related holonomic substrate of "pressurized vacuum" in the substringular, is that metaphorical "ether" which both superstrings and mini-stringular segmentation are here to be encompassed within.  If one were theoretically to take some given constant as multiplied by tthat main influence which is formed by the force of pressurized vacuum (metric-gauge), while then coupling this with some constant that is here to be multiplied by the main influence that is formed by the point commutative force (i*PI(del) Action), this would then work to form the equivalence of the Majorana-Weyl-Invariant-Mode times some other given constant.  This works to imply, that the multiplicit functional coupling of the gauging of Ward-Cauchy-related field, -- With the processes of the alteration(s) in the general condition of their partition-related discrepancies, of which are here to be inherent from within the structural confines of mass-bearing orbifold eigensets, is key at working to help at forming the general superstringular process of the multiplicit Majorana-Weyl-Invariant-Mode.  Samuel David Roach.

Those General Influences That Worked At Forming Time And Space

Just as the coupling of the influence of thought energy with inertia worked at forming time, at the general instant of the "Big-Bang"; the action of such inertia over time, is what worked at forming the existence of what we call space, -- again, at the general instant of the "Big-Bang." Sam Roach.

When Gravity Is Hyperbolic In Its Translation

When gravity is hyperbolic in its translation in the relative forward-holomorphic direction, -- its topological sway tends to have a concave-down bearing.  Consequently; when anti gravity is hyperbolic in its translation in the relative forward-holomorphic direction, -- its topological sway tends to have a concave-up bearing. I will continue with the suspense later! Samuel David Roach.

General Propagation-Related Modes

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

Eminent Knotting Along The Rarita Structure

Any given arbitrary eigenindex of the Majorana-Weyl-Invariant-Mode, is formed by the resultant interaction, of a general genus of an eminent Ward-Cauchy-related knotting in the realm of the substringular, -- as this is here to be considered, when taken to be existent along the general topological stratum of the Rarita Structure. I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

When A Mass-Bearing Orbifold Eigenset Is Converted Into Pure Energy

When any given arbitrary mass-bearing orbifold eigenset, is here to be converted into pure energy -- that initially present Majorana-Weyl-Invariant-Mode, that such a said eigenset was to have, when it was of a mass-bearing nature, is here to be dissimilated (taken away).  To Be Continued!  Sincerely, Sam Roach.

Yau-Exact Condition And Piecewise Continuous Nature

The greater that the scalar amplitude is to be, of that Majorana-Weyl-Invariant-Mode -- which is here to be of a given arbitrary orbifold eigenset, -- that is hence to be of a respective given arbitrary case scenario, -- this will consequently tend to follow; that, the more stringent of a nature that its directly corresponding Yau-Exact condition, will consequently tend to be exhibited as.  The more stringent of a nature, that the directly corresponding Yau-Exact condition of an orbifold eigenset will thereby tend to be exhibited as, by such an inferred set of discrete quanta of energy that operate to perform a specific task, -- the more rapidly that such a so-stated orbifold eigenset, will consequently tend to be in the process of working to display the exhibition, that is of its directly corresponding piecewise continuous flow, which is here to be correlative to the general activity, whereby such an orbifold eigenset, is here to be working to generate as much cohomology as it is to be degenerating, over a directly corresponding evenly-gauged Hamiltonian eigenmetric. Sam.

Second-Order Light-Cone-Gauge Eigenstates And Force

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

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.

Change In Tense Of Slater-Related Propagation

Let us consider an orbifold eigenset, that is here to be moving via a Lagrangian-based path, that is of a euclidean nature, -- to where the here inferred propagation of this said orbifold eigenset, is here to be of a Slater-related nature.  This implies, that the propagation of the said eigenset -- is here to be in the process of being translated through space, via a mean Lagrangian-related Hamiltonian operand, -- to where such a said eigenset, may consequently be depicted of as a set of a discrete quanta of energy, -- that are here to be in the process of being transferred in a relatively "straight" manner, through some sort of a tense of an identity function, (F(y) = F(x)).  Furthermore; let's now say, that the ensuing nature of the motion of such a said orbifold eigenset, via its correlative Lagrangian-based path, is here to alter from its initial euclidean-related nature, -- to where even though the said orbifold eigenset is still to be propagated in a Slater-related manner, it is to instead to be of a Clifford-related nature.  Consequently; the said orbifold eigenset, is now to work to bear a hyperbolic translational flow of its spatial eigenindices, in the process of its spatial transference over time, -- to where, instead of the said respective eigenset to thence to be moving in a manner that may be depicted of as being translated in a relatively "straight" way, via some sort of an identity function, it is instead to be moving in a manner that may be depicted of as being translated in a relatively concave-up way, such as with (F(y) = F(x)^(a constant)).  Sam Roach.

Torsion And Attribute Of Metric-Related Singularity

Let us initially consider an orbifold eigenset, that is here to undergo a metric-related Chern-Simons singularity -- via the translation of this said eigenstate, over the course of its motion through space and time.  If the dimensional-related pulsation of the said orbifold eigenset is to be increased in its torsion, the directly corresponding Chern-Simons singularity that it will consequently tend to undergo, via the course of its spatial translation, (for the here inferred eigenset, as a whole), will tend to bear a tense of amplification.  However; if the dimensional-related pulsation of the said orbifold eigenset is to be decreased in its torsion, the directly corresponding Chern-Simons singularity that it will consequently tend to undergo, via the course of its spatial translation, (for the here inferred eigenset, as a whole), will tend to bear a tense of attenuation.  Sincerely, Samuel David Roach.

External Yukawa Field And The Kahler-Metric

Let us initially consider an orbifold eigenset, that is here to be reverberating at a general proximal local region.  When the immediately external Yukawa field, is to alter in its directoral-related net scalar amplitude of angular momentum, over time, as this is here to be taken, when in terms of that  attribute of the Kahler-Metric, that is of the wave-tug that is to be applied upon the topological stratum of the here stated orbifold eigenset, in a Gliosis-related manner -- this will consequently often tend to cause the initially stated orbifold eigenset to perturbate out of the here mentioned inferred tense of a reverberation-related mode.  I will continue with the suspense later!  Sincerely, Samuel David Roach.

A Little As To Gravitational Waves And Knotting Equations

Here's a relatively simple tense of "food for thought."  Since gravity is exhibited as an association of gravitational waves, those knotting equations that may be utilized to work to express the condition of gravitational fields, -- is to work to involve the attribute of non-linear differential equations. Sam.

De Rham Cohomology And Orbifold Eigenset

Let us initially consider a mass-bearing orbifold eigenset, that is here to be traveling via a mappable De Rham cohomology-related Lagrangian -- over a span of time.  If such a given arbitrary respective orbifold eigenset, were to be traveling via a course of motion, that is here to be of a  binary Lagrangian, then, the said eigenset will consequently tend to be less able to be perturbated out of the inferred course of a De Rham cohomology-related projection of trajectory, than if it were to, instead, to be traveling via a course of motion, that would otherwise be of a unitary Lagrangian.  Likewise;  if such a given arbitrary respective orbifold eigenset, were to be traveling via a course of motion, that is here to be of a tertiary Lagrangian, then, the said eigenset will consequently tend to be less able to be perturbated out of the inferred course of a De Rham cohomology-related projection of trajectory, than if it were to, instead, to be traveling via a course of motion, that would otherwise be of a binary Lagrangian.  Consequently; the more "knitted" that a De Rham cohomology is to be, that is of one general nature, through which it is here to be traveling at a constant rate over time, the more difficult that it will tend to be -- for an external source to be able to alter its general flow of motion, out of the here inferred tense of a course of a De Rham cohomology.  I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

The Quicker The Flow Of The Perturation Of Chern-Simons Invariants

The quicker that the flow of the perturbation of Chern-Simons Invariants over time happens to be for a mass-bearing orbfiold eigenset, the higher that its resultant charge will tend to be. Sincerely, Samuel Roach.

What I Perceive Of As The Cohomology-Related Template And The "Force"

Here's something that I have mathematically worked with, as I currently perceive this, as a means of working to determine a general type here of a relationship, between the general tense of a cohomology-related template, and the "force." :

Let us initially and briefly explore the consideration of a few different general concepts.  Let us consider a mass-bearing orbifold eigenset, that is of a particular general genus of a symplectic-related field, -- to where this said symplectic field is here to be transferred in a kinetic manner, over time, by a genus of a Khovanov-related field -- to where the inferred Legendre homology, that is here to be kinematically working to translate the mass-bearing orbifold eigenset through space over time, is here to be of a genus of field, that is here to act as a heuristical counter part to the implied mass-bearing symplectic field.  Next; Consider the general Union Set of eigenindices, that are here to act in common, between both the earlier implied mass-bearing field And the respective correlative kinetic-bearing field, -- and treat this as a theoretical eigenstate, via a little bit of tweaking.  Next; Consider a cohomology-related template, that may help one to mathematically translate that general type of a reverse-fractal, that is of the particular type of format, that may be present in any one given arbitrary respective case, to where one is then to consequently derive a tense of charge, to where such a charge, is here to be at a Less microscopic level. Next; consider what I have mentioned once, as the E(8)XE(8) stringular oscillation-based tendency, -- as this may here be thought of as being the source of that general type of an effect, that works to act to either form the general fortification or the general weakening of Chi-related entities in time and space.
Let's call the implied E(8)XE(8) oscillation-related tendency, "Chi.";
Let's next call the union set of eigenindices, that are here to be tweaked into an eigenstate, "U."
Let's next call the cohomology-related template mentioned here, "Gamma."

Consequently, in a non perturbative case, when the "force" is holomorphic in its delineation, then:
Chi = (((U*Gamma) + (U^2*Gamma^2 + 4*U)^.5)/2). -- to where this is the basic tendency.

Furthermore, in a non perturbative case, when the "force" is anti holomorphic in its delineation, then:
Chi = (((U*Gamma) - (U^2*Gamma^2 + 4*U)^.5)/2). -- to where this is the basic tendency.

Again, this is what I perceive in the math that I did earlier.  I thought that I would share this with you.  If one can come up with any viable changes or improvements upon this, more power to you!  Sincerely, Samuel David Roach.

The Betti Action And Smooth Asymmetric Delineation

When the Betti Action is here to work to be directly associated with an even Betti number, -- the respective given arbitrary superstring of discrete energy permittivity, that is here to directly correspond to such a correlative Betti Action, is to be orientable.  When a given arbitrary superstring is to be orientable, the said string that I have inferred here, may be said to work to bear a homeomorphic field relationship, in covariance with its directly associated counter string. When a superstring of discrete energy permittivity is to be directly associated with a counter string in such a manner, to where it is here to work to bear a homemeomorphic field in its covariance with its directly associated counter string, it may consequently be said, -- that such a said field is then to bear a smoothly homogeneous Fourier-related translation.  (This particular said Fourier-related translation, is such a condition, -- to where the said homogeneous field, is here to bear a smooth relation -- over a duration of gauge-related metric.)  When there is here to be a smoothly homogeneous Fourier-related translation of field, when this is here to be taken between a superstring of discrete energy permittivity and its counter string, -- the asymmetry that is here to exist, between the stated string and its directly corresponding counter string, is here to be smoothly delineated.  I will continue with the suspense later!  To Be Continued! Samuel Roach.

Diffeomorphic Field And The i*PI(del) Action

Let us initially consider a mass-bearing orbifold eigenset, that is here to be smoothly accelerating in time and space.  The just stated eigenset, is here to be in the process of being transferred -- over the course of a Noether-related flow.  The closer to diffeomorphic that the holonomic substrate of the directly corresponding orbifold eigenset is to be in this case, the more smoothly that the flow of the activity of the correlative i*PI(del) action will tend to be, --  to where the directly corresponding flow of the perturbation of its correlative Chern-Simons Invariants, will then tend to work to bear a smoother flow, -- than if the holonomic substrate of the said orbifold eigenset, were, instead, to be further from being diffeomorphic.  ( A diffeomorphic field, is a field-like entity, that is homogeneous in smoothness -- when this is here to be taken over a Laplacian ("snap-shot" in time)-related set of conditions.)  Sam Roach.

Gravitational Waves, Pulse, And Impedance

Gravitational waves tend to work to form the general effect of an "inertia-related pulse."  Let us initially consider a mass-bearing orbifold eigneset; that is here to be moving at an initial velocity, over an initially proscribed time. The said orbifold eigenset, is here to be initially moving in a theoretical environment, that is here to bear no gravitational influence upon the said eigenset.  After the stated initially proscribed time, the force of  gravity is then to become eminent upon the stated orbifold eigenset.  When the thus stated "inertia-related pulse," that is here to be formed, as that influence that is here to act as the effect of the motion of such gravity, is to be applied upon such an inferred Noether-based mass-bearing orbifold eigenset, in a holomorphic manner -- over an evenly-gauged Hamiltonian eigenmetric, such a general tense of a directed "inertia-related pulsation," is thence to tend to form a general genus of an impedance upon the said mass-bearing orbifold eigenset, -- to where the thus mentioned eigenset of this particular general case, will then tend to have a more difficult time at moving at its initial rate than it did -- prior to the application of the force of gravity upon it.  Sincerely, Sam Roach.

Differences, Due To Relative Change In Wobble

Let's consider two different given arbitrary covariant mass-bearing orbifold eignesets, that are here to be both parallel in their motion, -- as well as the Ward-Cauchy-related condition, that these are also to initially be traveling at the same rate, in their relationship to light.  These just mentioned orbifold eigensets, are also here to initially be of both the same construction, spin-orbital momentum, and angular momentum.  Next; there is then to be such a subsequent change in their relative covariance,-- to where one of these two stated orbifold eignesets is to rapidly change in its series of radial spatial translation -- over an evenly-gauged Hamiltonian eigenmetric -- while the other of the two said orbifold eigensets is to still remain moving and operating, in such a manner as it was inferred to be spatially translated as before.  Consequently; both the relativistic time, mass, and the relativistic length of the two said orbifold eigensets, will then Not "appear" to be exactly the same towards one another, when this is here to be taken in covariance with each other, due to their relative change in motion in relationship with the motion of light. To Be Continued!  Sam Roach.

Perturbation In Type Of Expansion, During An Acceleration

Let us initially consider an orbifold eigneset -- that is here to be traveling at a constant rate of motion, as it is here to be in the process of undergoing a general genus of a Clifford Expansion, -- to where in this particular case, such a stated eigenset is here to be diverging from a given arbitrary general locus, via a correlative hyperbolic tangential flow.  It (the orbifold eigenset) is then to spontaneously alter in its rate of motion, as this stated eigenset, at the same time (through the vantage-point of a central conipoint), is to be in the process of altering in its general type of an expansion, -- to where, the said orbifold eigenset is to now to be in the process of undergoing a euclidean expansion instead of a Clifford Expansion ( to where the general type of a divergence implied here, is then to alter -- from working to bear a hyperbolic tangential flow, Into then altering into working to bear a euclidean tangential flow).  As such a said orbifold eigneset is to be spontaneously altering into an accelerative mode -- as it is here to be be changing in its general genus or type of divergence, at the inferred respective given arbitrary proximal locus implied here, by going from working to bear a Clifford Expansion, to then working to bear a euclidean expansion, -- this will then tend to almost indefinitely, in so long as this said eigenset is here to be undergoing a general tense of a Noether-related flow, -- to tend to work to cause, at the proximal locus at which the said orbifold eigenset is to spontaneously change in both its accelerative rate And in its general genus of expansion (to where, this is a case, in which such a general tense of a divergence is here to be perturbated, at the inferred given arbitrary proximal locus in time and space, at which the inferred dual spontaneous set of changes that I have described of earlier here, are thence to occur), then consequently; this is a general type of a situation, in which there will tend to be both the formation of one or more metric-related Chern-Simons singularities, at the proximal locus at which such a dual set of general changes are here to occur, as well as the condition that there will also consequently tend to be the formation of one or more Lagrangian-related Chern-Simons singularities, at the proximal locus at which such a dual set of general changes are here to occur.  Samuel David Roach.

A Correction To Some Of My Recent Posts

I was recently studying both some of my past work, as well as looking over the math that I had done, as appertaining to a couple or so of my past posts.  It appears, that what I had termed of as being of a "tori-sector-range," is actually more succinctly -- a "dimensional-train," that is here to be of only one layer of reality, that is appertaining to one universe that is out of a set of parallel universes.  It also makes a little more sense, that if you were to consider that the "cross-sectional" thickness of the "dimensional-train," that is of the ever torsion-related windings of one overall universal setting,  is still to be at least somewhat similar to my previous estimation, that this concept; whereby, if you were to consider that a "tori-sector-range" that is to be as a "dimensional-train," that is here to work to represent the ever torsion-related windings of one particular layer of reality, that is of one specific universe; that it may be possible, that, if you were to divide the size of the so-stated "cross-sectional" region of a "dimensional-train" that I had earlier stated, by the number of layers of reality of one universe (from within a set of parallel universes), that this consequential resultant "dimensional-train," could be thought of as being or appertaining to the ever torsion-related linkage, that is here to thereby act, in so as to web together the workings of one specific layer of reality, that is part of one universal setting, -- during each successive iteration of the generally noticed duration-related activity of what I term of as being of Ultimon Flow. Sam Roach.

Theoretical Robin Boundary Condition At the Relative Norm-To Reverse-Holomorphic End Of An Orbifold Eigenset

Let us initially consider a given arbitrary orbifold eigenset, that is here to have a Robin Boundary Condition imposed upon it -- at the relative norm-to-reverse-holomorphic end of the said respective orbifold eigenset.  Let's say that the holonomic substrate, that is here to work to help in comprising this said Robin Boundary Condition, -- is to be maintained in its structure -- via the general tense of a respective homogeneous geometrical field, that is here to be relatively flush in its Gliosis-related contact, with the said relative norm-to-reverse-holomorphic topological surface of the said orbifold eigenset, at the internal-reference-frame of the so-stated eigenset, that is being discussed here.  Let us next say; that the one tightly-bound limiting surface, that was here to work to inhibit any spatial transference of the said oribifold eigenset, beyond its initially stated relative norm-to-reverse-holomorphic insulated plane  -- is to act, at a reference-frame that is External to the here stated eigenset, in such a manner, -- to where this may "teeter-totter" back-and-forth, like a see-saw, as such a said orbifold eigenset is to be translated over time and space, via a correlative Fourier Transform.
I will continue with the suspense later!  To Be Continued!  Sincerely Samuel David Roach.

My Premise, As To An Occasional Potential Inter-Meshing Amongst Different Universes

"Segments" that are of a given arbitrary "dimensional-train," that are here to work to represent part of one directly corresponding given arbitrary universal setting, in one set of parallel universes -- may occasionally potentially partially inter-mesh with "segments" that are of another given arbitrary "dimensional-train," that are here to work to represent part of another directly corresponding given arbitrary universal setting, in the same earlier stated set of parallel universes, and still Potentially maintain their initial tense of a universal setting -- under the course of the following two potentially feasible general stipulations:  P.S. What I mean by "universal setting," is as being of one type of universe.

1)  If the potentially resultant symmetry-related Ward-Cauchy boundary conditions, are to be physically obeyed -- to where such a potential partial inter-meshing would Not work to be prevented, -- by one tense or another, of something on the order of the Pauli Exclusion Principle (which could thence, otherwise work to prevent such a general inferred type of a potential partial inter-meshing).

AND;

2)  If the Ward-Cauchy norm-related conditions of the two different potentially partially inter-meshing "segments," that are here appertaining to small parts of two different inferred universal settings, are here to work to allow for both of such potentially inter-meshing "dimensional-trains," to consequently work to bear such a general tense of an orthogonal delineation -- to where these inferred segments, that are here to work to represent two different individually taken sets of Hamiltonian Operators, -- are then to be able to tend to bear a tense of a super string-related wobble, that would consequently work to signify the general type of a physical condition, to where both of these segments, that are here to be appertaining to small parts of two different respective universal settings, to still maintain the condition, as to continue to be of their originally respective inferred tense of two individually taken universal settings.

Otherwise; the initially eluded-to potential inter-meshing of two segments -- that are here to be appertaining to small parts of two different respective types of universal settings, would consequently more than likely Not be able to happen then!

I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Holomorphic Direction And Pressurized Vacuum

The relative forward-holomorphic direction of an orbifold eigenset, is the innate direction that such a stated eigenset will generally have a tendency of moving into -- if the surrounding proximal local substringular pressurized vacuum, -- is here to work to bear a relatively low scalar amplitude of impedance, upon the potential motion of such a said respective given arbitrary orbifold eigenset.  Sam Roach. (PHS 1989).

An Attempted Link Between Two Theories

First of all:  Do you remember how I had once stated to the general effect, that all of the universes of one set of parallel universes exist, -- in a such a manner, to where these were here to be inter-twined amongst each other?  Next; do you remember me stating, that all of the discrete quanta of energy of one particular universe, that is of one particular set of universes (parallel universes), are here to tend to exist along, what I had termed of here as being of a "tori-sector-range"?  Let's say, for instance, that all of the discrete energy, that are here to be of one particular universe, during those substringular iterations of the generally noticed duration-related moments of Ultimon Flow -- as this is here to be of one specific given arbitrary "tori-sector-range," when these are here to be in continuation of belonging to the same said respective inferred universe, are here to tend to exist along a "strip" of space-time-fabric (aside from those certain homotopic interconnections, that work to bind various increments of one universe in correlation to the others) -- that is here to bear a "cross-sectional slice," that I have estimated here, to be somewhere on the order of being about:

1.5808517*10^(-32) meters By 8.5613512*10^(-27) meters.

Such a said "slice," may be thought of as being an ever twisting and twisted Minkowski-related "dimensional-train," -- that is here, as a tense of being both of a multi-varied torsion of a flat space, that may, as well, be thought of as being an integrative tense of existing as a tense of a Hilbert space also.
When one is to put all 91*10^(81) universes, that are of all of one set of parallel universes together, this works to help at making a tense of a volume-related realm of reality.

I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Hamiltonian Operand And Mini-Stringular Segmentation

The general type of a Hamiltonian operand that the countless eigenstates of mini-stringular segmentation are to travel through, over the general course of time, -- is the general Ward-Cauchy-related physical stratum of substringular pressurized vacuum. Sincerely, Samuel David Roach.(1989).

Thought Waves Overcoming Impedance

The main difference between the nature of thought waves and the nature of gravitational waves -- is that thought waves are propagated in a manner that is both transversal and supplemental, whereas, gravitational waves are propagated in manner that is both transversal and perpendicular.  This works to mean, that there is a Ward-Polarizable relationship between thought waves and gravitational waves.  Gravitational waves tend to work to form a tense of impedance, upon the propagation of the countless orbifold eigensets that are existent.  Therefore, thought waves, and thereby thought energy, may sometimes work to be able to overcome at least a little bit of the impedance, that the action of gravitational force is here to work to produce. To Be Continued!  Sincerely, Samuel David Roach.

Gravity And Pressurized Vacuum

Alterations in the scalar amplitude of the gravity, that is here to be applied upon a physical phenomenon -- will tend to alter the corresponding scalar amplitude of the quantum of substringular pressurized vacuum, that is here to be impeding the flow of a respective substringular phenomenon.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Flow Of Orbifold Eigensets And Path

Orbifold eigensets tend to move in the path of "least resistance."  Such a multiplicit path of "least resistance," is the "path" that is here to work to bear the least scalar amplitude of pressurized vacuum.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.