Part Three of the Fourteenth Session of Course 6

Well hello again world, this is Samuel Roach here!  Glad to converse with you!  Here comes part three!
            
Superstrings release the residue of their ground-states during the sub-metric that transpires during the Bases of Light because illuminated superstrings are almost always in a Main World Tube & because illuminated superstrings always acquire the residue of their respective tori-sector-ranges that is essential for the recyclling of differential geometries, and differential geometries recycle to allow for the Bases of Light.  You see, since the most overtly recycled ground-states are, as a fraction of the sum of all matter and energy, equal in quantum to the fraction of the back-and-forth sways that are released from the Klein Bottle during an eigenmetric of the Kaeler-Metric versus those associated back-and-forth sways that are fully confined in the Klein Bottle during the mentioned eigenmetrics of the Kaeler-Metric.  There are constantly Gaussian Transformation occurring.  This is a 15 to 1 ratio -- fifteen times as much dark matter and dark energy as light matter and light energy.  The integration of light's basis is light.  Light is the basis of perception.  Perception is the basis of communication.  Communication (here, specifically commutation) is the basis of iteration and reiteration.  Reiteration is the basis of prolonged existence.  Prolonged existence is the only way a reality can begin and continue.  The reason for the reverse-fractor relation of the Kaeler-Metric to the ration of dark matter and dark energy versus light matter and light energy is that the basis of Ward Polarization is equal to the fraction of relatively mildly worked upon recycled ground-states to relatively overtly worked upon recycled ground-states.  Also, there is fifteen times as many Hodge Indices related to norm-states as the Hodge Indices related to ground-states when one includes the Fourier Translation of states in both the Main-World-Tubes as well as in the Royal Arc.  I provide a more rigorous explanation as to why this is the way this is during the publishing of the fourth part of this session.  I will continue later with the fourth and last part of this session.  Until then, you have a phenomenal day!  God bless you in the name of Yahweh!  Sincerely, Sam.                                                                          

Part Two of the Fourteenth Session of Course Six

Well hello again world, this is Sam Roach here!  Here is the next part of Session 14.
           
One of the reasons for the torroidal shape of the field of such a two-dimensional superstring is because two-dimensional strings bear one and two-dimensional discrepencies along with a three-dimensional basis of field delineation over the course of each individual substringular Laplacian taken individually.  The extrapolated fields of one-dimensional superstrings bear two annuli given the condition that such fields are detected as a thin figure-eight-shape, yet such fields that are directly associated with one-dimensional strings are thinner during each individual Laplacian than those that are related to two-dimensional strings.  This is because, both one and two-dimensional superstrings exist in world-tubes that bear 32 spacial dimensions that have a basis in three spacial dimensions.  Yet one-dimensional strings generate primarily two-dimensional world-sheets.  Such world-sheets are the Gliossi mapping of where a world-sheet had just kinematically differentiated over a successive series of instantons, and bears a holonomic structure that consists of an organization of scattered norm-states.  Such "intertube" and "figure-eight" shapes ae examples of toroidal phenomena.  All illuminated superstrings that are detected are perceived of as having a toroidal shape for that reason!  Even though one-dimensional strings require being perceived of as toroidal, these fields are as such because the residue that these receive is acquired from within a general three-dimensional world-sheet as the assoiciated one-dimensional superstring is propagated through a Lagrangian.  The fact that one-dimensional superstrings primarily have only two-dimensional discrepencies helps to explain also why one-dimensional stringular fields eigenstates per Laplacian condition at instanton are always thinner than the corresponding field eigenstates that are associated with two-dimensional strings per Laplacian.  This is why superstrings are detected in the globally distinguishable as tori-related phenomena.  An individual eigenstate of a substringular field is an example of a torus.  (Such as similar in M-Theory.)  Superstrings are actually vibrating strands and vibrating hoops.  One-Dimensional superstrings are vibrating strands while two-dimensional superstrings are vibrating hoops, as you will remember from Course#2, yet, as detected from the surrounding fields of the superstrings, one-dimensional superstrings are detected as relatively thin propagated tori & two-dimensional strings are detected as relatively fatter propagated tori.  (As is always the case as shown by illuminated superstrings that are detected.)
I will continue with the suspense later!                                                       
Have a phenomenal day!
Sincerely, Sam.

Course 6, Session 14, Part One

What is the shape of a superstring in the globally distinguishable?  The shape of a superstring in the globally distinguishable is effected during the Polyakov Action by the Lorentz-Four-Contractions that are imposed upon such a phenomena in the substringular.  The illuminated superstrings in the substringular are those strings where the associated tori-sector-ranges are, prior to a given instanton, collected and recycled.  The residue of superstrings that is collected and recycled is operational during the sub-metric that transpires during the condition when the Bases of Light is active as I have described before.
                                                                                            
The actions of the instanton-quaternionic-field-impulse-range of the tori-sector-ranges in the Ultimon form a Lorentz-Four-Contraction effect upon the illuminated superstrings of each mentioned tori-sector-range taken individually for their related strings.  This effect forms a field that surrounds the superstrings when these strings are detected in the globally distinguishable.  What this effect does is that it curls the angular momentum around the magnetism of the very same field that detects the spacial parameters of the associated superstrings.  This mentioned effect curls the affiliated perception that we detect superstrings in such a way during a set sequential series of instantons, involving the Polyakov Action that the discrepencies of a two-dimensional superstring in this arbitrary case here, shows a hole in the middle of a surface that curls like an intertube around the just described hole or annulus.

Part Two of the Thirteenth Session of Course Six

Well hello again world, this is Samuel Roach here!  Here is the continuation of the thirteenth session of the sixth course of my string theory in accordance with the order of courses that I originally came up with the basis of making.
          
Superstrings that act as waves are like a "thread" and first-ordered point particles are like small "knots" in the previously mentioned "thread."  Superstrings are like "embroided ties" of the previously mentioned "knots."  The stringular fabric never breaks in normal phenomenology except during the space-hole and also except in the case of the unfraying of substringular fabric that happens in the course of phenomena entering into black-holes.  Phenomena that exit black-holes are turned into antimatter that eventually reorganizes into matter.  The good news is that frayed material that is within black-holes can possibly be reconstructed eventually into matter, yet I refuse to want such a fatalistic end result to overshadow a more positive possibility.  (NOYB).  The fields of superstrings are like organized tiny virtual frays that eventually wrap back into mini-string and norm-states (and norm-states are a simple organization of point particles), depending on the tori-sector-range situation.  The lagging of the substringular "information" before an eigenmetric of the recycling of the mentioned substringular phenomena is a perturbation of the other interacting substringular phenomena and also a perturbation of certain point particle "information" to retie in a manner that promotes the perpetuation of all of the related phenomena of the given related tori-sector-range.  God Bless You In the name of Yahweh!  Samuel Roach.

Part One of the Thirteenth Session of Course Six

Well hello again world, this is Samuel Roach here!  I hope that you are having a phenomenal day!
Here is the first part of the thirteenth session of course six.
                
There is a space at the end of each Chi-related endpoint that extends beyond the central substringular encoder of each general world-sheet (that is, of each Main world-tube).  This space is interconnected to the general stratum of the substringular via mini-string.  This space is always just a fraction of a radii from the endpoints of the semicircles and the upside-down semicircles of a cross-sectional region of the Royal Arc where there is to be a Basis of Light to differentiate via a sub-metric that happens right before instanton-quaternionic-field-impulse.
This region here is due to the fields exerted by the substringular encoders of the world-sheets that are located here.  All superstrings have fields associated with them.  One dimensional stringular fields tend to be thinner than the fields of two-dimensional superstrings (with the exception of certain relatively large Gliossi-Sherk-Olive fields that relate to certain one-dimensional superstrings that are undergoing  a strong degree of regional conformal invariance).  The integration of all of the superstrings that indirectly associate with one of the semihooops supports the existence of the described semihoop.  The slight curve inward that the recycleable material has to travel through is why when stringular residue is first taken up, there is a slight "time" or gauge-metrical lag that happens,and this so-called "lag" allows for the observation of kinematic Fourier or the discernment of time-wise active differentiation.  Once this lag is brought to the point of the Royal Arc where the pointal material may be recycled promptly, the travel of phenomena in the general world-sheets responds to Ultimon speed just about instantaneously.  The only factor here now would be the recycling mode as I taught in lessons earlier, and as I will teach later.  Superstrings in the substringular may only be so close due to the fields that these exert.  The fields that superstrings exert generally repel when these fields oscillate asymetrically , especially when these mentioned strings are encoded for as coming from another general world-sheet.  This extra need to repel is due to the extremely different sequences of the strings between these AND also their differences in how the waves in these are built up at any given instant (series iteration differentials).                                                                                            
I will continue with the suspense later!  I hope for the best of all of my readers.
I think of mankind as my family.  I won't lose, because I have Tau on my side!  God Bless!  Sincerely, Sam.

Part Three of the Twelvth Session of Course Six

Welll hello again world, this is Samuel Roach here!  I am here to conclude the twelvth session of the sixth Course of my writings on string theory.  (Although I started with two of the later courses.)
                     
On account of the "instantaneous" flow of point particles through the operand of the Ultimon, all of the information between the Main world-tubes is communicated constantly.  In this way, the world-tubes just mentioned are like hoops that are shocked open in a semi-permeable manner to an extent to allow for superstrings to enter the entity of their holonomic structure to allow -- after a relatively small number of sub-metrics -- for substringular formation.  This shock, or residue of imaginary supercharge, is due to the fact that there is a reiteration of first-ordered point particles during each instanton that is constant and allows for the organization and thus the existence of superstrings so as to allow for perpetual change.  This reiteration metaphorically boils down to, again, the fact that there is always jointal and curved motion.  The semihoops that represent a cross-section of the eigenbases of the Royal Arc are the tendency of curved-motion, and the Chi-like-shapes that form at the same general regional locus of cross-section which is where the cross-sections of the Royal Arc are, are the tendency of jointal motion.  The semihoops that I just described are the fractorial basis of magnetic field recycling, while the Chi-Shaped-Traces are the fractorial basis of electric field recycling.  This is since magnetism has to do with spin-orbital interaction, and electrical field has to do with angular momentum.  If something as an entity or as a phenomenon is based on the condition of stough in a spot, then it has angular momentum.  So, even if something is smaller than an electron, it still has a field that is related to electrical fields -- although such an "electrical field" would be a fractor of what is actually an electrical field.  Everything has a relationship to spin and orbit, so, even if something is below the energy level of hbar, if it moves, it is a group action that demonstrates a sub-energy that still has a fractorial relationship to magnetism.  I will continue next time with the thirteenth session of Course Six.  Until then, I will continue with the suspense later.  You have a marvelous day!
Sincerely, Samuel David Roach.                                                                                              

Part Two of the Twelvth Session of Course Six

Well hello again world, this is Samuel Roach here!  I hope that life is o.k. for you today!

Interconnecting the conicenter of the troughs of each of the dual ends, at both the the general locus of forward moving time and at the general locus of backward moving time, of each of the six eigenbases of the Royal Arc structure --  as integrated into the majorized structure of the Royal Arc for each associated layer of reality -- is an endpoint of what forms as a Chi Shape that forms as a Trace that exists in the Main Heterotic String Fabric topological region.  This Trace Basis functions in such a manner so as to take norm residue into the holonomic entity of the mentioned Trace eigenstates in such a way so that the said norm-state residue may recycle into ground-state residue that recycles back into norm-state field topological metric-gauge-like phenomena at the opposite corner from where the initial norm-state residue -- that consists of mini-string that needs to be re delineated -- is reincorporated back into norm-states.  The sub-metric in which the previous activity happens is during the sub-metric in which the Bases of Light exists as an integration of what is then soon to be the very many Planck phenomenon related phenomena of one layer of reality.  This exists in the same type of way for each Basis of Light.  If it were not for the Chi-Shaped phenomena that I just described, and if it were not also for the Main Heterotic String Fabric, the semicircles that comprise the eigenbases of the Royal Arc as a cross-section like phenomena that occurs right before instanton-quaternionic-field-impulse would consist of circles instead of semicircular phenomena -- and the Continuum would then need to exist as three plain hoops interacting with the twelve Main world-tubes in such a manner that superstringular commutation and superstringular recycling would then be impossible.  Superstringular commutation is essential for the group instanton interaction to bear any terrestrial simultaneous unitarity, which is essential for phenomena to interact in any organized way.  Superstringular recycling is essential for mini-string or substringular fields to interchange indices in such a manner so that the basis of jointal differential geometry to interchange into the basis of smooth-curved differential geometry and then back again into jointal related phenomena, and also so that the basis of smooth-curved differential geometry may interchange into the basis of jointal differential geometry and then back again into smooth-curved related phenomena.  Such interchanges are essential so that ground-states and norm-states may bear an optimum fractal and elastic modulae.  As stated before, all point particles flush through the Continuum in a manner of which we would term of as intantaneously.  In this way, all of the information that is regulated recycle-wise via the described majorized "semihoops", and is  communicated potentially  in a way that is more observably via the twelve Main world-tubes in a consant fashion in such a way that there is a constant relationship among all kinematically physical phenomena.  The Royal Arc acts as a regulatorial operator due to the fact that its volume allows for the condition of the degree as to how much more Fock Space there is then ground-state-based space.  The regulatory operation that I described is also due to the condition that the Royal Arc acts as a membrane that forms a vacuum comprised of Fock Space that kinematically differentiates in such a way so as to settle the gravitational indices of the phenomena that exists in the world-tubes in such a way that fascillitates the process of Ultimon Flow.  In courses nine and ten, I will explain more as to what wave-tug phenomenology springs phenomena from instanton into the main operational conditionality of Ultimon Flow.                                                                            
I will continue with the last part of this session later!  Until then, keep a positive attitude, and things should look up for you.  Bless You and you have a phenomenal day!  Sincerely, Sam Roach.

Part One of the Twelveth Course of Session 6

How are the three semi-hoops (each "semi-hoop" consisting of four world-tubes) that comprise the three sets of parallel universes interconnected?  Draw a relatively thin hoop that bears phenomena that moves in general to the relative left.  At the bottom of the mentioned thin hoop on the relative right side of your paper draw another relatively thin hoop that bears phenomena that moves in general to the relative right.  At the bottom of this latter mentioned hoop draw another of such hoops that that exists corresponding to the interior of the hoop that I began to describe at the beginning of this sentence that also bears phenomena that generally travels to the relative right such as the direction of travel of the interial indices that were mentioned that travel in the hoop that is just interial to the initial hoop that I have mentioned in this sentence.  At an arbitrary distance below the initial hoop that I have      mentioned the prior sentence, draw an upside-down semicircle of the same size and similar shape of the semicircle that exists just above the two world-tubes that exist in the relative norm-to-holomorphic direction from the corresponding "bottom" hoops, except that the "upper" hoops are directly associated with a concave down semicircle while the "lower" hoops are directly associated with a concave up semicircle.  Both of the prior mentioned semicircles are majorized into the two respective halves of the Royal Arc of one set of parallel universes.  Have the relatively concave up semicircle conically parallel the relatively concave down semicircle in such a manner that both semicircles that have recently been described are majorized in such a manner that the respective Royal Arc halves are also conically parallel.  So, to the relative interior of the relatively most exterior world-tube bears a world-tube that also contains phenomena that generally travel to the relative left when one faces the exterior of physical space-time-fabric.  The general tendency of phenomena in a world-tube to move holomoriphically is a condition that corresponds to forward moving time.  The general tendency of phenomena in a world-tube to move antiholomorphically is a condition that corresponds to backward moving time.  Each of the three "rings" that comprise the three sets of parallel universes exists in the same general manner that I just described earlier in this paragraph.  The world-tubes of different sets of parallel universes as well as the three sets of the Royal Arc (two of such semicircular Arc eigenstates that are majorized into parabollic hoops) are interconnected via hermitian yet non-abelian critical cusps that lace the three sets of parallel universes at the bottom of what could be explained as the "troughs" of each of these Royal Arc halves -- the described troughs being at the relatively open end of each of the Royal Arc structures of concavity.  Substringular Fock residue is contained thereby by the Ward Neumman Conditions of the peaks of each Royal Arc half, when one considers the curl of the majorized plane of such curvatures to form a semihoop that has a compacified peak at the relatively norm-to-holomorphic end that relates to the phenomena of the forward moving time associated world-tubes of each set of parallel universes,and a semihoop that has a compacitfied peak at the relatively norm-to antiholomorphic end that relates to the phenomena of the backward moving time associated world-tubes of each set of parallel universes.  Such an interbinding of hermitian yet non-abelian topology involves a locally multiplicit mini-string interconnection between the Laplacian directed interialized Royal Arc semi-hoops that exist with the same concavity with the relatively exterior world-tubes (This exists, yet with opposite concavity, for the relatively exterior world-tubes involving forward moving time and the relatively exterior world-tubes involving backward moving time) to the relatively interial world-tubes that involve the more interior world-tube of the more interial set of parallel universes.  Such interconnection exists between the most exterior set of parallel universes with the next interial set, and between the central set of paralle universe with the most interial set of parallel universes.  I will continue with the suspense of the next two parts of this session later!  I have written enough for now.  You have a phenomenal day!
Sincerely, Sam.                                                                                               

Part Three of the Test Solutions For the Second Test of Course Six

9)  "Steady-State" superstrings, which are superstrings that obey Noether Flow, flow through all three sets of parallel universes in-between the durations of each instanton in order to share unified commutation that works to pull the three mentioned sets of parallel universes into one kinematically-based physical portion of space and time.                                                                                                                                  

10)  The symmetrism/assymetrism of the spin-orbital momentum that is fractorially associated with the activity of first-ordered point particles -- if these are respectively orientable or non-orientable via their intersymmetrisms of substringular field or mini-string -- allows for the proper associations that exist between superstrings that respectively obey both Noether Flow and/or tachyonic flow in such a manner so as to maintain homotopy with optimum ability.

11)  Superstrings remain in motion so that these may stay as the discrete units of energy that allow energy and thus existence to exist at all.  So, in-between each duration of an instanton, each superstring commutes throughout the Ultimon so that these may be tweaked to slow down just enough at instanton to allow us, as life forms, to experience the organization of integrated instantons that we know of as time.

12)  Dark matter exists in the proportion, relative to us, that the reverberation-half of a Kaeler-Metric eigenmetric that pulls a superstring out of a Klein Bottle eigenstate is in relation to the sum of the other reverberation-halves associated with one eigenmetric of a Kaeler-Metric, when taken as a fraction of one sub-metric out of one whole discrete gauge-metric of the described Kaeler-Metric.  Phenomena in a Klein Bottle eigenstate that are not being pulled out at a set general Laplacian bear a Ward Polarization condition relative to the associated reverberation-half that is put into the gauge-metric of the Regge Action.  Such a proportion is reverse fractored by the ratio of dark matter to light matter -- 15 to 1.
Without the Kaeler-Metric, superstrings would lose their permittivity that these need to be the energy that makes up reality.  So, the reverse fractor of the existence of dark matter is an essential product of those Ward Polarized reverberation-halves that mold the mini-loops of superstrings into the relatively discrete eigenstates of metric-gauge that exist as the topological holonomic field structure that maps out discrete loci of substringular permittivity.

Part Two of the Second Test Of Course Six

5)  When both limits of the Royal Arc are thus connected through recycling, the shape appears as a circle.
 
6)  Such a majorized shape through the Lagrangian of one set of parallel universes of the Ultimon appears from the outside as a giant but relatively thin hoop.  There are 12 of such general world-sheets that contain all of the superstrings that act as what we would determine as the kinematic region throughout all of the multiplicit sequential series of instantons.

7)  Before each instanton, there must be an instanton-quaternionic-field-impulse in order to act as an equal and opposite reaction to the virtual break in homotopy during what I term of as the "space-hole."  Such an impulse-mode molds the substringular encoders so as to form that pattern that is fitting for the relativley Laplacian condition of the ensuing instanton.

8)  Tori-Sector-Ranges vary very little in flow rate (within a googleth of a variation in covariant metric), while yet coompensating for their corresponding approaches via the reversal in their associated multiplicitly covariant differences in flow rates.  This is due to velocity being relative to the observation of a phenoman at the varying given positions, and such varying positions are here to be considered arbitrary.

I will continue with the suspense later!  Until then, you have a wonderfull day and a wonderfull night.
Sincerely, Sam Roach.                                                                                     

Part One of the Test Solutions For the Second Test of Course Six

1)  The number of stringular mers that comprise a particular substringular encoder determines the number of instantons that it takes for a particular ground-state to recycle into its opposite type of state of tangency and back.
If a ground or a norm-state switches in tori-sector-range that these correspond with, the total number of instantons required for full recycling will equal the total number of substringular mers existant in the framework of the multiple substringular encoders that such a perturbated superstring directly associates with over a set sequence of unitary Fourier differentiation that locally maps out the recycling of one ground-state or locally map out the recycling of one norm-state.

2)  Ground-States and Norm-States.

3)  Norm-States recycle into ground-states involved with the kinematic sequential series of the local group Chi-Shaped-Trace, while then recycling back into norm-states via their local group cross-section that is directly involved with the Royal Arc.  Each step of such recycling happens during the sub-metric that happens during the duration that happens via the sub-metric that is directly associated with the Bases of Light, -- and in an indistinguishably different manner so that order is maintained in the localization of covariant norm-states and ground-states.

4)  Ground-States are recycled as in "3," except that these initially recycle into norm-states via the Royal Arc, while then recycling back into ground-states via the local group Chi-Shaped-Trace associated with the corresponding Basis of Light that the described ground-states are associated with (ground-states that return to their home-tori-sector-range are recycled into norm-states and then back into ground-states that are directly associated with their original Home-Basis of Light), during its metrics -- such a trace existing in the general locus of the Main-Heterotic-String-Fabric.

The next four test solutions will be provided in the next post, while the last four test solutions will be provided in the post after that.  I will continue with the suspense later!  Until then, you have a phenomenal day!
Sincerely, Sam Roach.                                                                               

Test Questions For The Second Test Of Course Six (6)

1)  What factor allows one to know how many instantons of a set tori-sector-range needs to iterate  in order to define when a first-ordered point particle of a superstring, of the described tori-sector-range, will be recycled  from being converted with indistinguishable difference into a different form of differential geometry while then being recycled back with a similar tense of indistinguishable difference back into the same general format of differential geometry?

2)  What are the two general differential geometry types?

3)  Describe in general how norm-state-related first-ordered point particles of the substringular are recycled.

4)  Describe in general how ground-state-related first-ordered point particles of the substringular are recycled.

5)  When both limits of the Royal Arc are commuted through recycling, what is this shape?

 6)  What is this prior mentioned shape in reference to test statement "6" as integrated along one general main world-sheet?

7)  Describe why there are, in-between the durations of each instanton, instanton-quaternionic-field-impulses.

8)  Describe how tori-sector-ranges vary in flow.

9)  Describe why a "steady-state" related superstring must constantly, in-between the duration of each instanton,  travel along the whole orbit of the Continuum.

10)  What fascillitates the binding of superstrings in the globally distinguishable?

11)  Why must substringular travel be almost instantaneous in terms of our terrestrial time?

12)  Why is dark phenomena essential in order for any phenomena to exist at all under our present conditions of time and space?                                                                                                            

A Precursor To Courses Nine And Ten

The reason as to why the superstrings related to electromagnetic energy and the corresponding Planck Phenomenon related phenomena that are directly associated with such bosonic superstrings always have a Yang-Mills light-cone-gauge topology -- which is always non-abelian -- is because the completely contracted form of light that becomes mildly first-ordered point particle-wise/covariant delineation-wise disconbobulated must not have mini-string that attaches these directly to each other in any way that over-stretches the fractal modulae of the holonomic "sensitivities" that are intrinsic to the nature of superstrings.  So, since bosons of electromagnetic energy do not have an even Grassman Constant during BRST, the mini-string in between such bosons and their corresponding Fadeev-Popov-Traces must also bear Hodge Index based Lagrangians that are also not even in  
terms of the amplitude of their associated covariant Laplacian scalars.  Yet, since such a disconbobulation is minimized to allow for the condition of Light to be the foundation of the relative covariance of the kinematics of physical space-time fabric, the "slack in the line" which here has no lack of necessity must provide a consistant harmonic wave-pattern that is homeomorphic throughout the Laplacian mapping out of the length of one-d strings or the circumference of two-d strings, given the vibratory oscillation mode that a given superstring bears during a given instanton.  This makes, out of necessity, the condition of a non-abelian light-cone-gauge topology or a Yang-Mills topology for bosonic strings appertaining to electromagnetic energy so that homotopy may be maintained without any unnecessary wave residue.  Fully contracted superstrings that are not -- through their corresponding sequential series of iterations -- going at light speed have first-ordered point particles that are only disconbobulated in terms of their spin-orbital isosymmetries instead of being disconbobulated in terms of the non-even Grassman Constants that are related to all superstrings of this nature.  The condition of an odd-integration of first-ordered point particles in terms of the Grassman Constant in relation to electromagnetic energy is the reason why light-speed in the globally distinguishable is the general maximum for speed in a given direction.  The exceptions to this is light that is sped up by certain attributes of gravitational-like forces (Kirchoff radiation) worm-hole transportation (which is mainly a speed-up due to the bending of space), and something else (NOYB, AIIF).  Electromagnetic energy is the envolvement of  a linear generated propagation of Noether Flow that is directoralized through the basis of unitary Lagrangians through the operand of the space-time-fabric that exists in the domain of its cross-product.  So, when one has a mass that is going just under light speed that is to soon go faster than light, the spin-orbital isomorphms that bear a mapping of assymetric Laplacian axial torsion that does not wobble at any moment toward the other related first-ordered point particles due to the intense fractal modulae of the mini-string that interbinds the described point particles, while yet being perturbated to allow for a swivel attribute that is hermitian to still allow for a  conformal dimension of one for 1-d strings and a conformal dimension of two for 2-d strings, will not form an even Grassman Constant during the ensuing related eigenmetric of Regge Action due to the described torsional force that is applied by the described first-ordered point particles due to their assymetricly isomorphic spin-orbital "disconbobulation."  So, although the Laplacian mapping of such substringular field if unfrayed is going to have a strong homeomorphicity, the described lack in an even Grassman Constant throughout the region of instanton causes related superstrings to operate in such a fashion to where their next iteration will then need to function according to tachyonic flow instead of Noether Flow.  Such activity will always place the related superstrings into a Hamiltonian operand that alters the covariantly local differences in substringular neighborhood in such a way so that the norm conditions of the correlatively involved stringular orbifolds, and the correlatively involved stringular orbifold-eigensbasis, will change in terms of their Jacobian eigenbasis.  Whenever an orbifold and/or an orbifold eigenbasis is altered in its Ward Norm Conditions, seeing that the Jacobian eigenbasis of such prior mentioned phenomena will then be altered in terms of their Gliossi directoralizations and also in terms of the covariant angling of Planck phenomena related phenomena relative to one another given the related universe eigenstates involved and the angling of Planck phenomena related phenomena relative to one another given the related eigenstates of covariant layers of reality, will always involve one or more sets of Gaussian Transformations that will replenish the permittivity of the related superstrings.  A Gaussian Transformation always involves a Kaeler Metric, yet, a gauge-transformation is a type of a Gaussian Transformation that not only replenishes permittivity in superstrings, yet, in the process, due to the altered Grassman conditions of corresponding superstrings, changes light-cone-gauge-topology from non-abelian to abelian and vice-versa.  Gauge-Transformations always happen when light scatters.  The scattering of light causes heat under present universal conditions.  Thus, gauge-transformations are what cause entropy.  The trick is to minimize the gauge-transformations so that harmony, peace, and development of self-actualization in the universe may be exemplified while still allowing for adequate heat and the necessary changes of physical states.  I will continue with the suspense later.  Until then, you have a phenomenal day!
Sincerely, Sam.        

Part Three Of Session Ten Of Course Six (6)

Let us say that one detected a superstring via the best means of extrapolation that one may consider.  By this detection, one would be able to directly visually perceive via an extrapolatory picture the general Gliossi field of the described superstring on acount of the ability of some sort of instrument.  10^(-51) of a theoretical second later, that superstring would not be there -- particularly since the smallest unit of discrete real time is 10^(-43) of a second, and 10(-51) of a second is less of a duration than 10(-43) of a second.  The radial Planck distance is the smallest unit of distance that an hbar of discrete energy may directly differentiate in within the Laplacian circumstances of an individual instanton.  The Radial Planck  distance is (3*10(-35) meter)/2pi in circumference when fully uncontracted, and the transversal Planck length is (3*10^(-35) of a meter when fully uncontracted.  When a superstring is terrestrially "standing still", it is fully uncontraced during BRST.  When a superstring is terrestrially moving at close to the speed of light, it may be contraced in each dimension (either in one or in two dimensions) by a factor of 3*10^(8).  Phenomena that move in consecutive sequences at a directoralized accelleration at light speed or faster may occur either unilaterally in one direction or in a constant speed in changing directions will always at that point bear a light-cone-gauge topology that is Yang-Mills and not Kaluza-Klein, and will therefore at that point not be a phenomenon of mass -- even though all superstrings have a mass index in spite of the fact that not all phenomena bear mass.  Superstrings that are thus fully contracted will be mildly disconbobulated in terms of organization although the corresponding fields that connect the associated superstrings with their counterparts will bear a homeomorphic field in terms of considering the Laplacian mapping of the described fields that exist across (for 1-d strings) or around (for 2-d strings) the topological field mapping that exists in-between a superstring and its counterpart during BRST.  So, superstrings that travel at light speed or faster over a sequential series of instantons do not bear an even Grassman Constant -- and are thus oriented during the ensuing Regge Action if the associated superstrings are not to be tachyonic.  When a superstring moves the distance of a Planck Radial transposition during a sequential series of instantons, and the described superstring as a unit is still at the same general spot that it was in in the first place, the superstring as a unit is still kinematically differentiating over the course of each instanton.  All phenomena always moves in one way or another in some manner in either one or more Planck Radial distances or in one or more Planck Transversal distances per instanton.  Each of such redistributions occurs on account of the Overall Encodement that transpires in-between instantons, to where it would appear via extrapolation that the described superstring has propagated in terms of its consecutive redelineations.  The sequential series of such motions works to define the relative covariance of a phenomenon, what velocity  the described phenomenon has, and whether the described phenomenon is Noether or Tachyonic.  Yet the reason for our three dimesional perception is that size outside of a worm-hole or outside of something of the like may only be perceived down to a globally distinguishable superstring.  The other dimensions are wrapped up with the substringular phenomena at very close distances.  Now do you see what I was preparing you for?!  I will continue next time with the test questions for the second test of this course.                                                                                                                                   
I hope that you have a phenomenal day!  Sincerley, Sam.    

A Little Bit More Of AN Explanation For Contractions

During Polyakov Action, a superstring seperates its first-ordered point particles in an overall      homeomoriphic manner so that the given superstring is uncontracted into the size that it must appear as as according to the associated Lorentz-Four-Contractions.  So, when a superstring related to a form of electromagnetic energy (the superstring here being of itself bosonic) is to go through Polyakov Action, its mild amount of dissociation is a mere yet relatively local disconbobulation in the Ward Newmann Conditions of the described superstring -- yet without any expansion in the holonimic "tapestry" of the associated string.  So, the increased sub-dimensional volume that exists in-between the first-ordered part particles that comprise a superstring is to the extent of a reverse-engineering of the apparent size of the superstring based on the present Lorentz-Four-Contractions that are here acting upon the described string.   Such Polyakov Action, the Bette Action, and the Imaginary Exchange of Real Residue all happen during  instanton as well as during BRST, while the Kaeler Metric and the Regge Action happen immediately after instanton.  So, if a superstring is to go into an eigenmetric of a Kaeler Metric metric-gauge-eigencondition, then the gauge-metrics of the associated eigenaction of the Kaeler Metric happens at the same overall rate as the ensuing Regge Action.  If the Kaeler Metric is not kinematic during a set of substringular instantons, then the Regge Action happens during half of the duration that it would undertake if it were not for the activity of the local eigenstate of Kaeler Metric.  So, when without Kaeler Metric, Regge Action happens in the duration of half of its otherwise speed  When  superstrings enter a Klein Bottle eigenstate-like metric-gauge, these upon contact with the topology of the top of the associated Schotky Construction, recontract to the extent of a fully contracted superstring.
Gotta Run!  I hope you have a phenomenal day!  Sincerely, Sam.    

Part Two Of Session Ten Of Course Six (6)

Well hello again world, this is Sam Roach here!  I am here to continue with the second part of the tenth session of the sixth course of my string theory!
               
A superstring in the substringular is 3*10^(8) smaller in length for one-dimensional superstrings and 3*10(8) smaller in circumference for two-dimensional superstrings than when these are detected in the globally distinguishable.  So, a one-dimensional superstring in the substringular is 10(-43)meter in length and a two-dimensional superstring is 10(-43) meter in circumference in the substringular.  Sorry I gotta run.  I will continue with the next part later.  You have a phenomenal day!  Sincerely, Sam Roach.