Some Knowledge About Covariant Groups

Let's say that three covariant substringular groups going through a Fourier Transformation were Njenhuisly perturbated, to where the three groups which here represent three orbifolds consequently produce a perturbation in the related covariant codifferentiation that will potentially alter any potential Kaluza-Klein topology in the said three orbifolds into a Yang-Mills topology.  But, here, the homotopic residue of each mentioned substringular group will maintain its Fourier-Based generation of substringular field as the said groups propagate along the Ultimon.  I will continue when I have the time!  Sam.    

Part One of Sesson Five of Course Six on Fock Space and the Light-Cone-Gauge

Superstrings generally vary in position in one fashion or another by the Planck Length -- although in such a static equilibrium that these described superstrings usually do not move through a discretely directoralized Lagrangian over a sequential series of instantons  at the Planck Length per intanton so as to move at the speed of light -- unless the mentioned superstrings are of EM energy.  Otherwise, such a phenomena is phenomena that involves the bending back and forth of space fabric via a worm-hole, in which the phenomena traveling within a given worm-hole, while in this "hole", only have a Yang-Mills light-cone-gauge topology so as to be able to travel via their kinematically covariant locus up to the speed of light or faster.  You see, anything that is generally considered to us to be a mass always has a Kaluza-Klein light-cone-gauge topology that also has completely Yau-Exact singularities in-between the superstrings that comprise any given mass.  Such a phenomenon cannot go at the speed of light.  (There is no infinite mass).  Yet, if one were to convert the mass' light-cone-gauge topology to Yang-Mills, which is part of what happens when one is translated into a worm-hole (although well over 99 percent of the speed in a worm-hole is due to the back-and-forth bending of space fabric), such of what was translated may travel at the speed of light or faster.  A photon that has initially scattered over the course of relatively few instantons at first has its light-cone-gauge topology converted to Kaluza-Klein as it springs briefly tachyonically, yet a photon as a photon always has only partially Yau-Exact singularities involved directly with them.  (The described singularities are hermitian, yet these singularities vary from on to off of the Real Reimmanian Plane during the course of each instanton.  This is why such an initially scattered photon is not a mass -- yet alone the fact that such a photon does not have infinite mass.  As stated before, after relatively few instantons after a photon has scattered, its light-cone-gauge topology converts back into a Yang-Millls topology at just under the speed of light as it attempts to requantize into one or more beams of EM energy.  The general locus of the orbifold eigenbasis that appertains to any given photon as the described photon scatters is limited in its propagation due to the abelian geometry of the general relative locus, until correlative photons that have just scattered re-enter the mentioned eigenbasis of the associated p field.  The reason for the initial reaction of the photon is based on a similiar concept -- the concept of how and why a shock-absorber works.  The combined effect of the prior described knowledge works to more adequately explain Snell's Law.  (This here would be the why and the how  EM phenomena that travel through a medium other than a vacuum tend to travel at under the speed of light, while EM phenomena that travels through a vacuum travel right at the speed of light (unless the given phenomenon is Kirchoff Radiation).  The interior of a worm-hole is not a vacuum, yet, anything that travels through something like a worm-hole -- that well over 99 percent of its velocity is due to the bending back-and-forth of space fabric -- can, given the conditions, accelerate via its kinematically covariant locus (its actual individual accelleration besides the speed of the bending of space) up to and beyond the speed of light.  Kirchoff Radiation is EM  energy that travels ~6 times light speed, although it does not, in itself, travel in a worm-hole.  I will continue with the suspense later!  God Bless You in the name of Yahweh!  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.                                                                               

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.        

A Summary Of The Second Part Of The Fourth Session Of Course Six

Well hello once again, this is Sam Roach here!  I am here today to further summarize the fourth session of Course Six.
           
Phenomena of one set of parallel universes may exist in anywhere from one to 32 dimensions, depending on the conformal dimensionality of a given phenomena, the locus of where it is differentiating, and the Lagrangian that it is differentiating in, both in terms of the Laplacian and/or the Fourier Transformations that a said phenomena is being redelineated and/or redistributed through operationally via the operand of space.  Yet, when one gets right down to it, even though superstrings are either two-dimensional or one-dimensional -- depending on whether the said superstrings are bosonic or fermionic -- and point particles are considered as zero dimensional phenomena, the foundation of the existence of operational kinematic substance is based on the existence of three dimensions that interact on a fractored level when it comes to the very small phenomena that I described that has a conformal dimension of two, one, or zero, respectively.

So, a superstring that has a conformal dimension of one has a field that bears at least two spacial dimensions, and a superstring that has a conformal dimension of two has a field that bears at least three spacial dimensions. The condition of one-dimensional strings having a field that bears two spacial dimensions is based on the most fundamental Laplacian-based delineation of a one-dimensional superstring.
The condition of two-dimensional strings having a field that bears three dimensions is based on the most fundamental Laplacian-based delineation of two-dimensional superstrings.
A supersting moves through space over a Fourier Transformation that bears kinematic operation that is relative to the Fourier Transformations that appertains to the kinematic operation of the other superstrings that exist in physical space-time-fabric.  The mapping of the transference of a superstring from its basis of field dimensionality into one or more dimensions that incorporate the kinematic operation of the said superstring over the course of instantons via a Fourier Transformation describes a multidimensional setting that is propagated through the operand of space into other dimensions that may be described by one or more axial directoralizations.  Such a framework of dimensionality that is propagated through via the basis of one or more axials that allows for the kinematic operation of a superstring over the course of a relatively limited Fourier Transformation is what I mean in my writings as a Lagrangian.  As you will learn in later courses, the norm conditions of corresponding Planck phenomenon related phenomena relative to one another is one of the main reasons why superstrings of one universe tend to operate kinematically through time in that universe as a general tendency unless such norm conditions are altered.  You will learn more about what I mean by such norm conditions later in courses nine and ten -- and I wish to sell courses nine and ten before then.
I hope that I am building tremendous suspense for my readers, and I will continue the suspense later!
You have a phenomenal day!  Sincerely, Sam Roach.                

Summary Of Part Two Of Session Two Of Course Six

Well hello again world, this is Sam Roach here!  I am here today to help describe what I meant when I typed in the second part of the second session of Course six.               

In-Between each instanton, there are countless gauge-metrics and sub-metrics, with sub-metrics within these mentioned durations that are even more brief down to very infinitessimal yet discrete durations.  There are also countless, yet relatively fewer gauge-metrics, sub-metrics, and within these metric-related durations that are even more brief down to very infinitessimal yet discrete durations.  During the duration that operates (happens)  in-between instantons, there is alot of sharing of substringular field in terms of the mini-string that is utilized to interconnect all superstrings and norm-states in one giant web-like structure during instanton -- in both indirect and direct ways.  While the countless metrics, sub-metrics, down to the most relatively infinitessimal durations that happen in-between instantons, operate through the operand of space, the sharing of substringular fields occurs via the give-and-take of the ebbing of what I call mini-string that allows for the countless varieties of substringular field integrations that exist per the succeeding series of Laplacian Translations which come together to form the relatively countless yet fewer succeeding series of Fourier Transformations that define the covariant codifferentiation of the multiplicitly interbound substringular fabric -- which is more granular than fabrical -- to allow phenomena to happen through time relative to one another.  The recycling of substringular phenomena is able to hapen in part because of the existence of what I call the Royal Arc, in the general manner that I described in the last summary.  Sincerely, Sam.          

Course 4 on The Substringular Vs. the Globally Distinguishable, Session 1, Part 2

The shape and size and energy of the electron may, however, be pinpointed within a region by algebraic probabilities that corner the Ward kinemation of an electron within a specific locant, like a synchronized set of puzzles that define the only way that a condition may be applied. This is not even delving into the abilities of discrete that may be surfaced by the lower size and more varied degree of flexibility afforded by dealing with vvibrations that exist at a lower level than those that scientists are currently able or willing to deal with. If one were to measure, through current probability, the approximate shape of an electron, and came up with a ten-dimensional basis to its kinematic differentiation, then we are starting to get is business. Look at the 3 prime axes in terms of the electron's three main dimensions. View the electron as a motion that covers as small of a region of locus as you may detect without adulterating the primal Ward conditions that define those boundaries that allow the electron to be what it is. Mark any field gaps in homotopy in terms of spin-orbital differentiation. These work to define an error in how the detection reads the flow of radial to transversel kinematism of the electron, or it draws an aberration in how the electron's field is changing. If there is proof that the field of the electron is changing due to a discretely applied outward singularity, then this may be marked off from being an error of detection. Next, how to treat errors in detection.