Nous Somme Ici

Worm-Holes are phenomena that inter-bind completely different spots in space by contorting space-time-fabric in such a manner in so that one may be able to go light years of distance into space in a relatively short period of time. It takes a dark matter source in order to temporarily form such a phenomenon. Many worm-holes simply exist at certain spots in the multiverse. Yet, many worm-holes may be temporarily created by a dark matter source in so that relatively instantaneous travel may occur. This is different from black-holes. Black-Holes are phenomena that are created by a collapsed matter source that ends up acting like an apex with a funneling phenomenon-based activity that torsions in so as to bring its surroundings into it in a manner that works to fray the space-time-fabric that enters it. These are two totally different formats of phenomena. Yet, both black-holes and worm-holes existence depends upon different distinctive geni of dark phenomena. The funneling phenomenon-based activity of a black-hole that works to bring its surroundings into it is a form of dark phenomena. Dark phenomena is phenomena that is Ward polarized from electromagnetic energy that moves into its general premesis. Worm-Holes as these are are an advantage if utilized appropriately, while black-holes as these are are a disadvantage to phenomena. There is a solution that is able to alter the condition of the seeming need for black-holes in the centers of our galaxies. We want space-time-fabric unfrayed for a continued existence of our world. Sam Roach.                                          

Course 6, Session 8, The Toroidal Nature of Superstrings

How does dark phenomena effect light phenomena?  Most phenomena from within the general Main-World-Sheet-like structures that carry superstrings are dark.  The whole process that allows center-state strings to be illuminated involves the rest of the superstrings of the given tori-sector-range, and is called the instanton-quaternionic-field-impulse.  The wave connection that binds this process is called the instanton-quaternionic-field-impulse-range.  As described in earlier course, this process allows for the recycling of differential geometries that help to form light.  Each tori-sector-range has one general part to play as a base for the integration of all of the light of the Continuum.  The four substrings that encode for all of the globally distributed strings, that exist for one tori-sector-range, from inside of the said Main-World-Sheets bear illumination at the central-state of a section of substringular fabric which is composed of point particles, just as any other superstrings that are illuminated.  As soon as a central-state superstring is formed within a sector of a Main-World-Sheet of the Ultimon, residue from all of the surrounding superstrings is pulled in to these central-state strings as an exact and opposite reaction to the process that these said central-state strings have in the process of shocking the surrounding superstrings away from them, and this equal and opposite reaction is directed toward the central directions that the said central-strings have as these said strings dissemble, since action is continuous.  Such central-state strings refers to the condition that there are 10,000 templates for each substringular encoder, and the process of instanton-quaternionic-field-impulse-mode molds these templates to the correct form of the proper substringular encoder.  The type of differential Fourier connections that exist between the substringular encoders and their corresponding superstrings works to determine what is illuminated.  Just as each Kaeler-Metric forms eight back-and-forth sways that involve 16 thrusts that allow for one added increment of discrete metric-gauge added to superstrings to allow for substringular permittivity, there is 15 times as much dark matter as light matter.  (16-1=15).  The interaction of substringular encoders with the rest of the substringular helps to allow for the recycling of substringular residue.The residue here is brought into the prior mentioned tori-sector-range.  (Two main conglomerations of substringular residues per section of majorized hemisphere.)  If you were to theoretically place the relatively norm-to- holomorphic and norm-to antiholomorphic (relative "up" and relative "down") Royal Arcs together, you would form a majorized circle, yet, these need to be separated to allow for the existence of the Main Heterotic Stringular Fabric.  I will continue with this fascinating session with session 9 later.           
In the mean while, think enthousiastic and you will be enthousiastic!  You have a phemenal day.
Sincerely, Sam.                                      

Solutions To Last Test of Course 4, Part 1

1) The substringular is the way phenomena appears when all of the Lorentz-Four-Contractions are optimized in order to indicate the actual occurrences that happen at the most sub-atomic levels.

2) The globally distinguishable is the way that things appear based on the measurements made by life forms from a relatively macroscopic level.

3) The co-differentiation between photons and the other substringular phenomena taken as a multiplicit set of Fourier Transformations that are constantly kinematic is what causes the substringulara to appear as the globally distinguishable.

4) Phenomena circle the Ultimon in-between instantons in one unit of Imaginary Planck Time.

5) Most physical phenomena is a vacuum at any given time because norm states are the result of non-linear and/or inexact differential eigenstates, and such eigenstates are more common than exact and linear differential eigenstates.

6) A string is a string during instanton. An instanton is when the point particles that are encoded to be organized phenomena form cohesive sets of exact and linear differential eigenstates over the relatively Laplacian condition of one unit of Real Planck Time.

7) Superstrings find their way back in order to reiterate due to homotopy, exterial and interial cohesive binding due to the action of the substringular's attempt to orientate the said strings, the repelling force applied to such superstrings via norm-state wave-tug that helps to settle the point particles that comprise superstrings, the inevitability of exact and linear differential eigenstates that reiterate due to multiplicitly engaged covariance, and due to the effect of the substringular encoders upon individual superstrings.

8) The spin of superstrings forms a reverse-fractored effect that causes electrons of the same pair to spin asymmetrically in order to not collide. This relationship allows electrons to have a non-perturbative magnetic field under normal conditions.

Course 4 On The Substringular Vs. The Globally Distinguishable, Session 16, Last Test

1) What is the substringular?

2) What is the gloabally distinguishable?

3) How does phenomena differentiate relative to make the substringular appear as the globally distinguishable?

4) How fast does phenomena "circle" the ultimon?

5) Why is most physical phenomena a vacuum at any given moment?

6) When is a string a string? Describe an instanton.

7) How do point particles find heir way back to form a specific string?

8) How does spin effect the relationship between the subsringular and the globally distinguishable?

9) How does roll effect the relationship between the substringular and the globally distinguishable?

10) Describe point reformation.

11) How does point reformation effect he relationship between the substringular and the globally distinguishable?

12) Describe how point particles may form a vacuum when altered.

13) Describe how a vacuum may change into strings.

14) How does the multiaxial codifferentiation of a supersting effect its relationship to light.

15) Why must the multiaxial codifferentiation of a string be fully normalized in order for the associated superstring to be tachyonic?

16) When may a particle "catch up" with light?

17) Is the multiaxial codifferentiation of a "normal" superstring normal to or parallel with the general flow of point particles? Why?

Course 4 On The Substringular Vs. The Globally Distinguishable, Part 2

As a start to this second part of Session Four, we will begin with a concept that involves patterns as I have mentioned.

Have you ever heard of a code? Strings have physical points that comprise them. In a one-dimensional string, these strings tend to be in a basically straight line during the sliver of one iteration. Such a straight line is physical yet not ideal. Ideal is theoretical, and theoretical is not the way things really work. So, the "straight" line has discrepancies! In this case, the given discrepancies are physical points that lay outside of the flush path of the general line that defines the particular locant (not neighborhood, since neighborhood is more general) of the given string as it iterates in its sequence.) Note, we are dealing with slices of space where the strings are iterating. Even then, the phenomena that comprises the given string is constantly in some sort of motion. Yet, a slice refers to those Caucy Ward conditions that define the string at as close to a standstill as you can without changing those properties of the string as it would be to form the demonstrated eigenstate of the eigenstate of energy we are talking about (Here, we are now referring to the discreteness of a single increment of energy that happens to be the basis of kinetic energy. I'll show you in words later!) as an eigenbasis so that we may be able to define an individual string as an eigenstate instead of a mere action. This is so that the existence of the points that comprise the string may be viewed of as indical actions instead of such small phenomena that their general differentiation as something that comprises the string is insignificant. So, where the points of a string are along its particular slice locant during a specific iteration work to define what it will do next. Also, how much stuff (condensed oscillation) is in each of the given points, where this stuff is located in each point particle neighborhood, and the mini-fields that exist in each point particle neighborhood -- taken for each point of the given string -- work to define what the string will do next. The points of a string as we would detect them are actually neighborhoods -- the condensed oscillation or field density of each neighborhood is actually smaller as compared to that neighborhood. The synergetic tensor of such a "slice" development gives a string its encodement for where it is to go next!

Course 3 on Lorentz-Four-Contractions, Session 12, Part 1

Strings move to form themselves and larger objects/phenomena. When strings move, they may move either dependently, independently, or interdependently with certain other superstrings. If a group of strings move in such a way that a certain specific string needs the action of the other strings, even though the other strings have no direct need for that individual string, then the given individual string is dependent on the group of strings that it is associating with in the course of its kinematic differentiation. (If a string ceased to differentiate kinematically, it would cease to exist.) If a string moved around in such a fashion so as to not need the direct influence of certain other arbitrary strings as part of what would allow it to exist as a stringular entity at all, then the given individual string that I mentioned would be independent of any of the stated arbitrary strings in terms of direct influence. This Independence would mean that, although everything has some relationship to everything else, the string mentioned above would not be directly interacting with and influenced by certain other strings. If a string is dependent upon other certain strings yet not interdependent upon them, then the other strings would be able to maintain their shape and behavior without the other individual strings. If a set of strings were interdependent, then the set of such strings would need each other to allow for the maintenance of their shape and behaviours in general. I will conclude with the purpose of this session with my next post.