Part One To An Aside To Course Ten

Here is more as to how to determine if the tense of a parallel universe that you are searching to be in is of a particular tori-sector-range -- or, in other words, how to determine this if the tense of a particular universe that you are searching to be in is of a particular "layer of reality."  Each Basis of Light that is unfrayed that is of a particular "layer of reality" is based on seven general solution modes that also incorporate the three-dimensional Laplacian placements of each Basis of Light relative to one another, based on the condition that electrons exist in D-fields that are of a Fourier minimum of six spacial placements plus time.  This is why there are six types of heterotic vibration modes.  The six general solution modes that I just mentioned bear a 36 membered particular solution that bears three overlapping -- or redundant modes, not including the member that is associated with a constant.  The corresponding tori-sector-ranges that are relative to one another here, which multiply by a fractal of six, causes the potential determination of the number of "layers of reality."  Now, if you consider the ten tenses of topological sways that exist per sub-dimension that corresponds here, taken individually, that form an overall substrate of 1,000 different multiplicitly arranged topological sways, one may be fascillitated to determine which of the (36+1+6)*3*1,000 types of tori-sector-ranges one wishes to enter.  Or, in other words, this will help to determine which of the types of "layers of reality" are appllicable to the tense of the parallel universe that you wish to enter.  I will continue later!  Sam.    

A Little Bit About Spurious Eigenbases

What type of a perturbation series would propagate if certain superstrings of covariant traits were to aquire topological sways, and how would this alter the angular momentum of the thus related homotopy -- whose phenomenology is defined by the interaction of those covariant traits which act eigen to the pertainent differentiable semi-groups (The semi-groups here are norm-states that act as catylists to the formation of those superstrings which encode for the mentioned covariant traits)?  As an arbitrary example:  A superstring is reiterated within the same neighborhood.  Quadrillions of related superstrings do too.  A miniority of the two-dimensional strings here iterate and reiterate side to side on a slightly differentiable coaxial basis.  These superstrings maintain an even function of polar shift in order to not get "kicked-out" of their association with the other superstrings which help define the basis of their respective covariant traits.  The change in the holomorphic index, thus caused, commutes phase change in the nodation of anharmonic oscillation.  This kinematic activity causes a change in wave connection and wave-tug between the other corresponding superstrings and the initially stated ones that are associated with the mentioned norm-states . This phase alteration repositions the parallax of the related homotopic Fourier differentiation by setting up a buffer in the prior mentioned related semi-groups.  This activity localizes as a supplement in the Imaginary tense to the change of angular homotopy caused by the coaxial twists that the said superstrings are kinematically undergoing.  The buffer is produced by the harmonic sway of those wave connections which were relocalized by the propagation of axions.  Such axions, under the course of such an arbitrary scenario, were generated by the tensors that in this case caused a euclidean repositioning during each time that the related superstirngs were spontaneously torqued.  This angular momentum change would, by intereacting with the mentioned buffer, cause a divergence in the local invariance of the set interactive traits, yet, it would converge the kinematic differentiatiion of the given covariance that is happening when the said metrics that were just mentioned are undergoing the described Fourier Transformation.  This is since the co-differentiation with the "buffer" would act as a "check and balance" to the inertial Dirac of the given homotopic configuration that has been described here.  If, after a discrete series accumulation of differenial variance, and if the homotopy has undergone global kinematics in the process of such a related Fourier Transformation, then, the series here would converge upon a local basis of a fractal of static equilibrium that may be described as a tense of conformal invariance.  It is then that the given "buffer" is said to be a member of a potentially spurious eigenbasis that may be physically denoted by an orbifold that bears a relatively strong tendancy for Chern-Simmons Laplacian-based and Chern-Simmons Fourier-based singularities over a metric that would involve a relatively brief number of instantons per duration of cyclic permutation.  I will continue with the suspence later!  Sincerley, Samuel Roach.           

More About P-R-P Modes

Here is more as to how to determine if the tense of a parallel universe that you are searaching to be in is of a particulaar tori-sector-range -- or, in other words, if the tense of a particular universe that you are searching to be in is of a particular "layer of realilty."        
Each Basis of Light that is unfrayed is of a particular "layer of reality", of which is based on seven general solution modes that also incorporate the three-dimensional Laplacian placements that the mentioned arbitrary Basis of Ligh,t relative to the other Bases of Light, that one is considering, is in during the duration of an arbitrary metric of what I call the "space-hole."  Based on the condition that electrons exist in D-fields that are of a Fourier minimum of six spatial dimensions plus time is why there are six types of heterotic vibration modes of the tori-sector-ranges relative to one another, which multiplies by a factor of six the potential determination of the number of "layers of reality" in and of itself.  The seven general solution modes that I have mentioned bear a 49 membered particular solution that bears three overlapping or redundant modes -- not including the member of the described solution that is associated with a constant.  Now, if you consider the ten tenses of topological sways that exist per sub-dimension (that is, what would appear as a three-dimensional setting when one detects the arbitrarily given Planck-Based phenomenon up close), taken individually, that form an overall substrate of 1,000 different multiplicitly arranged topological sways, one may be fascillitated to determine which of the (46+1+6)*3*1,000 types of tori-sector-ranges, or, in other words, which of the types of "layers of reality," is applicable to the tense of the parallel universe that you wish to enter in one set of parallel universes.  Thus, one is to consider the covariant Laplacian placement of the Bases of Light of one set of parallel universes relative to the others.  (159,000 layers of reality happen, over the courese of the existence of space and time PER set of parallel universes, and there are three sets of parallel universes in physical space-time-fabric.)  As implied earlier, each of the unique members of the prior described particular solution, along with the constant that is determined when one integrates to form the described particular solution -- and this given constant of which is a determinant factor in representing a parallel universe that is most similar to ours, along with the six types of heterotic vibrations that exist among the Bases of Light that corresponds to the minimum of six spatial dimentions that exist for an electron, along with each of three-dimensional up-close Laplacian placements of each Basis of Light as it exists during the duration of what I call the "space-hole",  (NOTE:  The configuration of Planck-Related-Phenomena is based on the directly prior configuration of its corresponding Basis of Light that it untied from in-between two successive instantons.), -- which corresponds to a specific tori-sector-range --, along with each of the 1,000 combinative formats of the topological sway, and finally considering if the curvature of the corresponding "Chi"-Related shape is hyperbolically concave up (for positive-moving-time-related Planck-Related-Phenomena) or if the curvature of the corresponding "Chi"-Related shape is hyperbolically concave down (for negataive-moving-time-related Planck-Related-Phenomena), works together to describe a specific Basis of Light that is mirrored fractorially in the "mini-traces" or the Planck-Related-Phenomena in order to help determine which "layer of reality" that you are dealing with.  The just mentioned knowledge also helps to determine which tori-sector-range is -- at an arbitrary locus of time -- appertaining to a tense of a parallel universe that one may wish to enter.  I will continue with the suspence later.  If I make any mistakes, at least I know that I am moving in the direction of the truth.  The knowledge above is a good filler in-between Session 11 and Session 12 of Course One on Fock-Space, gravity, and the light-cone-gauge.  This, being Course "9."  You have a phenomenal day!
  Sincerely, Samuel David Roach.                                                                                                                                                                   

Part Four of the Eigth Session of Course Nine

The added dimensionality of two-dimensional superstrings causes them to have not only two-dimensional discrepencies, yet also to have three-dimensional discrepencies.  So, one-dimensional superstrings have discrepencies that exist on the relative reverse-norm-to-norm-to-holomorphic side of the Laplacian settings that these exist in at their topological center.  (This center being closer to the relative norm-to-holomorphic Laplacian end of each individual superstring that is to be considered.)  Two-Dimensional superstrings have discrepencies that are both to the relative holomorphic side of the general topology of the mentioned superstrings per each Laplacian setting at the relative 90 degree mark, while these described discrepencies per each Laplacian setting are simultaneously placed in the relative norm-to-holomorphic position at the relative 90 degree mark of the same arbitrary two-dimensional superstring.  At the relative 270 degree mark of any given two-dimensional superstring, the discrepency from the hermitian Laplacian topological flow of the mentioned superstring exists in the reverse-holomorphic position, while the described discrepency per each Laplacian setting are    simultaneously placed in the relative norm-to-reverse-holomorphic position.
Again, one-dimensional superstrings that act as discrete units of energy permittivity bear one discrepency, while two-dimensional superstrings that act as discrete units of energy permittivity bear two discrepencies.
What I mean by discrepencies are seperations from the Laplacian hermitian topological flow of the delineation of the first-ordered point particles that comprise one and two-dimensional superstrings.
Substringular field in the form of mini-string still interconnects the described discrepencies with the rest of the  correlative superstrings during each Laplacian setting that form the basis of the conformal dimension of each superstring that exists in some sort of hermtian topological delineation during each  BRST duration that comprises the majority of the duration of each instanton that happens in the course of substringular iteration.  The added entropy that happens to the mentioned two-dimensional superstrings causes these to form more dilatons when these mentioned superstrings are propagated through space.  This configuration of discrepencies (partitions) causes these to "flap" a little bit more than one-dimensional supestrings when these are propagated through space.  The faster the mentioned two-dimensional superstrings travel transversally per iteration at under light-speed when the light-cone-gauge topology of the described two-dimensional superstrings is Kaluza-Klein,  (Kaluza-Klein meaning to bear an abelian light-cone-gauge topology.) the more that the associated two-dimensional superstrings tend to "flap."  As the Planck-Related phenomena that are associated with two-dimensional superstrings that are of a Kaluza-Klein light-cone-gauge topology flap, the corresponding two-dimensional superstrings flap in synchronicity with the prior mentioned Planck-Related phenomena.  Yet, Yang-Mills bosonic superstrings are often electromagnetic in nature, which causes these to travel at light-speed when in a vacuum, which decreases the inefficiency of the prior mentioned "flapping."  This is because the added wave holonomic condition that exists here provides a homostasis that tends to support the holonomic stability of the superstrings here due to an increase in the fractal modulae of the said superstring on account of the mentioned physical counterbalances that thus happen here.  One-Dimensional superstrings tend to orbit back-and-forth upon their axes as these are propagated through space.  I will continue with the last part of this session later.  Until then, God Bless You in the name of Yahweh, and I hope for only positive things for all of the readers who read my blog posts.               
Sincerely,
Sam Roach.             

About the Metrical Activity That Allows For Permittivity

                                   


                                   
Phenomena has to move to exist. Metric-Gauge is the topological Laplacian Poincaire Ward conditions that integrate through the Fourier Conditions of substringular multiplicit group metrics that must exist in order for superstrings to have the ability to move through space and therefore be the energy that is necessary for reality to exist. Superstrings are the discrete units of energy permittivity. Permittivity is the ability of phenomena to continue to move through space. If discrete units of energy could not move, energy would cease to exist. Without energy, there would be no light, nor would there be any mass. When superstrings circle the ultimon many, many times, these phenomena (superstrings) lose some of their permittivity. The process that causes superstrings to regain the permittivity that these need in order to remain energy so that energy may exist is known as a Gaussian-Transformation, which is usually a gauge-transformation. The initial situation is that gauge-transformations eventually lead to entropy. Yet, there is a way of limiting gauge-transformations to those that just allow for substringular permittivity without allowing for excess entropy. Entropy is essential for at least the change of physical states. I will say no more of this. The reason that energy started and still persists comes down to the existence of the Higgs Action. The Higgs Action is the main operator that allows for Gaussian Transformations. See my post of the leverage of the Higgs Action on my blog

samsphysicsworld@blogspot.com. I am doing this out of a love for mankind.

I am very blessed to have the friends that I have.

Sincerely,

Samuel

A Little More About Singularities

The potential Chern-Simmons singularity limits associated with the 191 given mini-loops

              
are as shown in the prior document where these were listed. So, all 191 Chern-Simmons

singularity limits exist fractorally along a vibratorially perturbated mini-loop right before

the first iteration of the Kaeler-Metric converts the Hamiltonian Momentum of such a

mini-loop into a hermitian mini-loop of discrete, Real Reimmanian metric-gauge that acts

as the physical substance of permittivity.

The hermitian limits of singularity of superstingular mini-loops that have just been

realigned and/or formed are as shown in the prior document where these were listed.

These discrete, topological limits of singularity form a twenty-five dimensional two-sided

Minkowski hermitian surface that bears a mini-string connectability to the twenty-sixth

related Minkowski Dimension by limits of singularity of

10^(-86)meters*((e^(.01)-e^(0))/2i) & 10^(-86)meters*((e^(0)-e(.01))/2i).

This topological set of singularities among those of all mini-loops that are connected into

a substance of permittivity, of which vibrate anharmonically toward the most adjacent

Gliossi-Sherk-Olive norm related states in such a way so as to form a harmonics of the

associated Gliossi-Sherk-Olive ghosts so that the adjacent light-cone-gauge eigenstates

may Diracly eliminate over half of their ghosts when such a hermitian group operation

interacts with the motion of the Rarita Structure.



The numbers subtracted from “infinity” need to be discrete, since the quantum world is

discrete. There are 96 dimensions in space and time, and each dimension has a general

condition of two sides. Electrodynamics is produced multifractorally by the permittivity

of superstrings. Electrodynamics involves a charged flow.

For every singularity that bears infinity, there needs to be a singularity that bears zero.

Electricity goes from negative to positive when in the direction of electron holes.

Mini-Loops indirectly produce electron holes.

All substringular mobiaty is virtual, since reality can not spontaneously undo itself.

Four times 48 is 192, and 192-1 equals 191.

This is why the Chern-Simmons limits of singularity when appertaining to the mini-

loops of superstrings are as these are.