Course 6, Session 4, Part Two

Well hello again world, this is Sam Roach here! I hope that I am keeping up with your attention span!

                   

So, the metrics of the substringular phenomena based on the past and future occurances that happen among such tiny particles and gauge-actions effect the metrics of the rest of the substringular arena that exists along the kinematically Fourier differentiation of phenomena that interacts from within and from outside the Ultimon. The main exception to the condition of metrics that do not have as much of a probability of effecting the surrounding metrics in a necessarily spontaneous way is when eigenstates of space that proceed within a series of space matrices are re-distributed to a sequence that functions as part of a different universe. (Parallel universes that are different do not necessarily have a directly corresponding spontaneous interaction with other universes during covariantly determined group intanton.) All of the parallel universes and time-potentials and sets of parallel universes are the fabric of the Ultimon. For an allegorical example, the earth appears flat, yet the earth is not flat. The direct fabric of the Ultimon appears completely topological and smooth, yet during certain metrics and submetrics that exist over the stretch of space and time, this is not always so. This means that after each duration of the Bases of Light, the flow of phenomena of the Continuum adjusts by one or more discrepancy interiorly on either side of its construction. This discrepancy is due to the fact that there is no such thing as a completely one or two dimensional phenomenon. The conditions that define certain phenomena as one or two dimensional are the Ward Conditions that define the spacial parameters that are used to scope the conformal dimensionality that is used to determine the inter-relationship of dimensionality itself. So, based on certain physical definitions that are used to extrapolate what determines something to be one, two,...to 32 dimensional has to do with discrete physical Ward Conditions. Remember, everything has length, thickness, and width. Accordingly, a tori-sector-range has phenomena on either side that curve relative to the prime given exterioralized phenomena by the radius of a discrete number of second-ordered point particles. A second-ordered point particle is the "skinnyest" type of phenomena that exists in free space. Third-Ordered point particles only exist where second-ordered point particles are at.

I will continue with the suspense later. Sincerely, Sam.

Part Two Of The Fourth Session Of Course Six

Well hello again world, this is Sam Roach here! I hope that I am keeping up with your attention span!

                     
So, the metrics of the substringular phenomena based on the past and future occurances that happen among such tiny particles and gauge-actions effect the metrics of the rest of the substringular arena that exists along the kinematically Fourier differentiation of phenomena that interacts from within and from outside the Ultimon. The main exception to the condition of metrics that do not have as much of a probability of effecting the surrounding metrics in a necessarily spontaneous way is when eigenstates of space that proceed within a series of space matrices are re-distributed to a sequence that functions as part of a different universe. (Parallel universes that are different do not necessarily have a directly corresponding spontaneous interaction with other universes during covariantly determined group intanton.) All of the parallel universes and time-potentials and sets of parallel universes are the fabric of the Ultimon. For an allegorical example, the earth appears flat, yet the earth is not flat. The direct fabric of the Ultimon appears completely topological and smooth, yet during certain metrics and submetrics that exist over the stretch of space and time, this is not always so. This means that after each duration of the Bases of Light, the flow of phenomena of the Continuum adjusts by one or more discrepancy interiorly on either side of its construction. This discrepancy is due to the fact that there is no such thing as a completely one or two dimensional phenomenon. The conditions that define certain phenomena as one or two dimensional are the Ward Conditions that define the spacial parameters that are used to scope the conformal dimensionality that is used to determine the inter-relationship of dimensionality itself. So, based on certain physical definitions that are used to extrapolate what determines something to be one, two,...to 32 dimensional has to do with discrete physical Ward Conditions. Remember, everything has length, thickness, and width. Accordingly, a tori-sector-range has phenomena on either side that curve relative to the prime given exterioralized phenomena by the radius of a discrete number of second-ordered point particles. A second-ordered point particle is the "skinnyest" type of phenomena that exists in free space. Third-Ordered point particles only exist where second-ordered point particles are at.

I will continue with the suspense later. Sincerely, Sam.

Part 2 of the First Session of Course 6

Well hello again world, this is Samuel Roach again! I hope that everything is o.k. with you!


                 
The reason why certain point particles do not always for as strings within their home tori-sector-ranges is becauses some point particles are residue that is about to be integrated into the substringular phenomena. When light brings in nodes as ripples OR releases rippled nodes within the Basis of Light within a moment, these extra nodes do not exist within strings, yet these nodes are about to be incorporated into superstrings or relaeased into the general point particle stratum of their "home" sector-ranges. If the rippled nodes are released residue that flows into the stratum of the point particles of a tori-sector-range, then the point particles of the said sector-range will mold the nodes so that these will eventually form as strings (superstrings) -- yet not necessarily as superstrings of that sector. If a node is rippled toward the strings of an instanton-quaternionic-field-impulse-range during a moment, then this node will help to form a superstring during a later iteration. The more iterations of the Ultimon that happen, the more point particles that find a "home" in any given tori-sector-range. Many point particles find a "home" in any given tori-sector-ranges over the Fourier Transformation of a sequential series of instantons. Certain point particles may never find a home in more that one tori-sector-range. Since all residue is used, all point particles eventually have a home tori-sector-range. Home-Tori-Sector-Ranges help to perpetuate existence so that the layers of the reality of individual universes are not scattered to the point of disorientation. Such orientation is partially due to the Bette Action that orientates superstrings with their counterparts via the Laplacian Poincaire condition known as the Grassman Constant, which happens during instanton. The existence of the Bases of Light and the existence of the Space-Hole, as well as the Laplacian Ward Caucy codifferentiation between the Bases of Light and their corresponding supserstrings, as well as the "space-hole", and even as well as the condition that each Basis of Light has a different Laplacian topological surface-based trajectory along with the fact that the Basis of Light that equally involves forward and backward moving time flow is always the main kinematically based Basis of Light -- effects the condition that superstrings and point particles of a specific Hodge nature have a tendency of "wanting" to belong to their home-tori-sector-range. I will continue with the suspense later!

To me, these posts utilize more imagination and cognitions than most of the other things that I am willing to talk about. I sure hope that you have a marvalous day! What a phenomena! Sincerely, Sam.

Test One of Course Five (5)

1) If two masses differ in compactification, these masses differ in the amount of space that exists in-between the core densities of the masses considered individually while then being compared.


                      
2) If two masses of the same volume differ in compactification, then one mass has more spaces in-between its core densities than the other.

3) When an umbrella is open, it is relatively uncompacitfied. When an umbrella is shut, it is relatively compactified.

4) The empty spaces in-between the fabric of a quilt shows a degree of a lack of compactification in the said quilt.

5) When space is composed of a mass, kinetic energy, or an electromagnetic energy, when composed of discrete phenomena, it is an overt thing. When space is empty, it is nothing.

6) Differentiating space forms energy when it differentiates over time in a kinematic directoralization. Energy in static equilibrium is matter. Matter with relatively little empty space is relatively compactified.

7) A point particle that is first-ordered is like a ball of yarn because it consists of intertwined mini-string.

8) Point particles that are first-ordered that are unfrayed are all interconnected via mini-string during instanton, just as balls of yarn in a hoop may all directly or indirectly interconnect via the ends of these balls of yarn interconnecting.

9) All first-ordered point particles interconnect via the transit of Ultimon Flow.

10) The spin and roll of first-ordered point particles causes the emission of mini-string. The emission of mini-string interconnects the said point particles Such spin and roll also makes the said point particles kinematic. The kinematic interconnection of such particles tug these phenomena along the Ultimon, thus causing Ultimon Flow.

11) Spin and roll are related to magnetic field.

12) The drive in a direction of a point is related to angular momentum, and produces the sub-basis of electric field.

13) A Yakawa Coupling is the touch, rub, and curl of substringular phenomena upon each other.                 

About the Importance of Point Particles to String Theory

In order for superstrings to be able to differentiate and interchange kinematically, there must be point particles that are smaller than these discussed superstrings. A superstring has a length, for 1-D strings, and a circumference, for 2-D strings, of 3*10^(-35) meters in the globally distinguishable. When in a totally contracted state, such a scalar is 10^(-43) meters. A first-ordered-point-particle has a diameter of 10^(-86) meters in the substringular when including the Gliossi Field that is directly associated and thus comprises the said point particle. First-Ordered-Point-Particles are comprised of the substance of the field of superstrings, or, in other words, mini-strings. Mini-String is comprised of second-ordered-point-particles that exist adjacent to each other in exterialy bound "chains" of phenomena that are interconnected by third-ordered-point particles that are bound by sub-mini-string. Second-Ordered-Point-Particles are 10^(-129) meters in diameter in the substringular, third-ordered-point-particles are 10^(-384) meters in diameter in the substringular, and sub-mini-string is 10^(-1152) meters in diameter in the substringular. Sub-Mini-String is the smallest phenomena that is a thing while yet also a gauge-action. Third-Ordered-Point-Particles only exist where there are second-ordered-point-particles. Not only does sub-mini-string bind third-ordered-point-particles together, yet these also work to interconnect the second-ordered-point-particles that comprise mini-string. A physical entity that is smaller than a superstring is termed to be a gauge-action. So how does such a tying of fabric rety while yet maintaining homotopy? The "space-hole" is what I call the duration right before Instanton-Quaternionic-Impulse-Mode, which is right before instanton, which is when homotopy just begins to undue to allow any essential retying of string, yet, to such a minor amount that homotopy during successive instantons is maintained except for when it is frayed in a black-hole. Such a resewing of substringular phenomena is brought back into a multiplicitly discrete homotopy due to the pressure that is impelled upon adjacent superstrings due to the equal and opposite wave-tug of point-particles that acts Gliossi upon the said superstrings to just enough of an extent so as to snap the temporarily untying topology described back into a unified multiplicit homotopic       topology.                                     

A Post of Course One on Relative Loci

If two things are next to each other, then these are near. If the same two things are separated by a substantial distance, then these are far. Two things that are near each other are relatively local. Two things that are far from each other are not relatively local. Two things that are made relatively local to each other have become localized. Two things, however, that were relatively local and subsequently became separated have become delocalized.

           
A man who lives by his neighbor is local to that neighbor. The man’s children, you might add, are even more local to that man. Yet the man’s neighbor is certainly more local to him than someone on the opposite side of the planet, at least in terms of physical nearness. As a standard, a locality in America is named by the county or city that that person lives in. You may say, “I live in Pinckney, Michigan, which is in the United States.” Likewise, one may always be able to grunge through more and more detail as to where a particle is, yet the precision of how specific you define your locality is often defined by the need that your specific description is to suffice. For instance, if you wanted to know where a cluster of molecules was, you probably wouldn’t delve down to the subatomic level. Rather, you would only need to search a level or two smaller than what you are looking for in order to find the region in which the thing you are looking for may be found. In this case, maybe searching down to the level of small molecules that may cluster in such a way so as to find what you are searching for.

Loci may mean spots where things interdependently differentiate, or it may mean spots that are near because these are attached. For instance, a uniform is near the body of a baseball player, yet it is not a part of that baseball player’s body. A chair may be near the table that it goes to, yet the chair is not part of the table. You might say, “Well, the uniform is local to the ball player’s body, yet it isn’t part of his body. And the chair is local to the table, yet it isn’t part of the table.” Exactly. So, if you consider certain phenomena as things that are made of parts, and these parts are made up of parts, when is something just local, and when is the object at hand in and of itself? What you need to define is what you are calling a specific thing. If the ball player’s whole body, including his hair, was the definition of a specific thing, then any part of his body would not be considered just local to his body – it would be part of his body. Yet, if the definition of the given specific thing was only the living portion of the ball player’s body, then his hair would be local to his body versus being part of the same specific thing.

The electrons of an atom are local to that atom, while the electrons of another atom are local to that other atom and not local to that first one. This is because we are not treating the atom as a static blob, but as a kinematic interplay of components that are interdependent. So, there is no “specific thing” that defines that entity of an atom, since an atom is the basis of the structure of matter, and matter is energy in static equilibrium. So, if you are talking about anything being local to the neighborhood of an atom, you are talking about a particle or object that is at least adjacent to the field of that atom. Yet if you are talking about something that is local to an atom, you are talking about something taking place within the given atom itself. For instance, anybody in a city is a local resident of that city, and everybody in that city is part of that city. If you were part of a pencil, you are considered localized within that pencil. This is because the members of a city, just as the electrons of an atom, are kinematic at their respective levels, whereas the parts of a pencil are not kinematic at an observers respective level.

Solutions To Course One Quiz

The point particle above a plane of scattered points is globally norm.



             
The rectangle with point particles along its topological boundary is globally ground.



The globally norm array implies point commutation.



The array of a globally ground state implies superstrings.                                                                                                



These different arrays types may interchange. This is because smooth curved topological

settings must recycle eventually, via an indistinguishably changed manner, into jointal

topological settings so that spin-orbital momentum may interchange with angular

momentum.

Course #9 -- Course One on Fock Space and the Light-Cone-Gauge, Session One

Well hello again world, this is Sam Roach here!  I am here today to provide an introduction to my first course on Fock Space and the Light-Cone-Gauge.  Here we go!

            
Point particles do a vast amount of their kinematic differentiation in-between the durations of individual instantons.  The duration of an instanton is what I call an iteration of the substringular as a unit.  First-Ordered point particles may be explained  by a Gaussian set per the successive series of the Laplacian conditions that work to define the Ward Norm conditions of both the substringular differential geometries through multiplicitly arrayed Fourier Transformations, as well as helping to determine the Ward Norm conditons of the norm-state differential geometries which are also multiplicitly arrayed through Fourier Transformations.  The interacion of the multiplicit Fourier Transformations of ground-states along with and including the multiplicit Fourier Transformations of norm-states forms the basis of kinematics, whereby, through a successive series of instantons, forms the procession of the activities of space via the integrable variations of time.  First-Ordered point particles of our set of parallel universes are associated with Imaginary (as opposed to Real Reimmanian) indices in the Gaussian positions ranging just over 0 to 32piI.  First-Ordered point particles of the central set of parallel universes may be explained relative to our universe with numbers in the Gaussian positions ranging from just over 32piI to 64piI.  First-Ordered point particles relating to the opposite side of  the Ultimon in terms of this set of parallel universes may be explained relative to our universe with numbers in the Gaussian positions ranging from just over 64piI to 96piI.  This corresponds to the condition that our Overall-Physical-Portion of space and time has 96 spacial dimensions plus time, & imaginary charge may be up to 96piIev per BTU that it associates with.  Any added imaginary charge density is automatically scattered from whatever source that the holonomic radiation that is being expelled is interacting with.  The Gaussian format of any particular space -- here we are talking about any particular orbifold -- must be the same, unless there is a Gaussian Transformation that alters the mentioned format.  The interaction of the countless Fourier Transformations causes the constantly inevitable conditions that cause Gaussian Transformations to happen all the time at various places over time.  Gauge-Transformations are the most common form of Gaussian Transformations.  Gauge-Transformations happen when the light-cone-gauge topology changes.  This happens (gauge-transformations) whenever photons scatter upon anything.  I hope that this is a good start to my ninth course!  Bless You, One and All!  Sincerely, Sam.                                                                                                

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?