A Little More About The Re-Positioning Of The Klein Bottle

Often, a general locus of superstrings alters in the delineation of its norm conditional basis in terms of the flow of its corresponding Gaussian Symmetry.   The norm conditions of a given arbitrary set of superstrings that form the substrate of a substringular setting often change in terms of the directoralization of the here related Hamiltonian basis of the corresponding fractal of angular momentum.  The said superstrings that exist in a general locus often alter in terms of a set framework of norm conditions, so that there may here be a relatively hermitian flow of kinetic energy, in such a manner so that energy may have both a relative degree of freedom of motion -- as well as also having a relative degree of continuity.  So, in spite of the here related condition of all of the superstrings that are involved in the general locus that here undergoes a said given arbitrary Gaussian Transformation are going through a change in terms of  a fractal of alteration in angular momentum, since all of the here related superstrings of the here said locus are multiplicitly going through the exact same perturbation of Ward-Caucy angular repositioning relative to one another, all of the here related Fadeev-PopovTraces also go through the exact same perturbation of Ward-Caucy angular repositioning -- in such a manner that synchronizes the change of norm conditions via the corresponding Gaussian Transformation in such a manner that the here alteration of norm conditions via the said Gaussian Transformation allows for a kinematic flow of norm-state perturbation in all of the said superstrings of the said locus.  This is so that all of the said superstrings of that said locus may here have a basis of kinematic re-delineation of discrete energy that will then involve a kinematic redistribution of superstrings that will thence be inter-active superstrings that belong to the same universe.

A Little Dittie About The Light-Cone-Gauge

The light-cone-gauge field of a first-ordered-light-cone-gauge eigenstate bears five links of mini-string when such a phenomena is involving one-dimensional superstrings, and, a first-ordered-light-cone-gauge eigenstate that corresponds to the topological Laplacian mapping of a two-dimensional superstring bears ten links of mini-string.  With the field of a light-cone-gauge eigenstate that involves a one-dimensional superstring, the five mini-loops consist of two segments of mini-string that are both looped around each other.  When it comes to the field of a light-cone-gauge eigenstate that involves a two-dimensioanl superstring, the ten mini-string links are not homotopically Gliossi to any mini-string except that of the ten mini-string segments that bind such a given arbitrarily associated two-dimensional superstring with its correlative Fadeev-Popov-Trace.  A Fadeev-Popov-Trace is the field trajectory of a superstring.  A Fadeev-Popov-Trace is a discrete unit of energy impedance, while a superstring is a discrete unit of energy permittivity.  A superstring, consequently, may be viewed of as a field trajectory of a Fadeev-Popov-Trace, yet in the opposite tense of holomorphicity.  Such a Laplacan mapping of the described field trajection directoralization is based on the same concept, except that here, the mapping bears the opposite chirality.  Light-Cone-Gauge eigenstates may either be abelian in nature, or, these may be non-abelian in nature.  An abelian light-cone-gauge eigenstate has a supplemental wave-tug in-between a given arbitrary superstring and its correlative Fadeev-Popov-Trace.  The light-cone-gauge topology of an abelian nature is known of a  Kaluza-Klein topology.  Light-Cone-Gauge eigenstates that bear a sinusoidal interconnection between the given superstring and its correlative Fadeev-Popov-Trace are said to be non-abelian.  A non-abelian light-cone-gauge topology is known of as a Yang-Mills topology.  I will continue with the suspence later!
Sincerely, Samuel David Roach.           

Course Nine, Session 14

Light-Cone-Gauge eigenstates always have quanta that twist to one extent or another.  Since there are a limited number of transversal, orbital, and/or radial components to the light-cone-gauge eigenstates of superstrings, the distance that strings move transversally, orbitally, and/or radially per instanton is controlled by the quanta-based-twists of the given superstrings' associated first-ordered-light-cone-gauge eigenstates which is controlled by both the region that the strings cycle thru,as well as the point commutative forces that act upon the strings and their associated second-ordered-light-cone-gauge eigenstates.  This is also to be considered along with what tori-sector-region is activated.  The more norm-states that act upon the mentioned superstrings, along with their associated light-cone-gauge eigenstates -- with limited spuriousnes inactivated -- (Since the operand of the world-sheet propagation is harmonic due to the cohesive normalizations of the corresponding Planck phenomena.) -- the faster the related strings and Planck phenomena will travel.  Not only that, but also, the corresponding substringular travel will not form excessive dilatons.  Light has an operand of world-sheet propagation that is harmonic on account of the smooth relationship of differentiating electric and magnetic fields.  Travelilng smoothly at over the speed of light has harmonic operands of world-sheet propagation.  This is because the radial, orbital, and transversal differentials are smoothly covariant.  This happens when phenomena that moves in a smooth or hermitian kinematic Fourier differentiation over the speed of light has harmonic operands of world-sheet travel.  Fast speeds just under the speed of light tend to cause relatively high, non-abrasive topological twists of light-cone-gauge quanta.  This tends to happen with a more anharmonic operand of world-sheet propagation when this speed is occuring via a tree-amplitude-based directoralization does not smoothly differentiate in a kinematic manner, over time, with a radial component.  Thus, light-cone-gauge quantization is constantly covariant throughout the Continuum during any discrete Fourier Transform.  Session 15 is expected to be revealed tomorrow!    

Part One of the Sixth Session of the Ninth Course Known As Fock Space and the Light-Cone-Gauge

There is one partition during instanton in any given 1-D superstring that is not an encoder, or, in other     words, every 1-D superstring has one separation from the general flow of the hermicity of its Laplacian topological delineation in space during instanton.  Such "partitions" in such superstrings that comprise the discrete units of energy permittivity that are utilized to form the space-time fabric that exists per each individual of such just mentioned type of superstrings in such a fashion so that its locus per individual superstring -- relative to the general flow of the hermicity of the Laplacian topological delineation in space of any arbitrary one-dimensional superstring -- is a variance that exists in the neighborhood of the center of the  described general topological Laplacian flow.  The condition of variance is that a     mentioned partition is always on the norm-to-norm-to-holomorphic side of any arbitrary one-dimensional superstring, when one considers the general directoralized flow of the Ultimon-Flow metrical circuitry that happens in-between the duration of each instanton.  For instance:  Superstrngs that involve forward moving time flow counterclockwise -- during the Ultimon-Flow that happens in-between the durations that happen in-between each instanton, relative to one that is facing the relatively "near" set of parallel universes.  (I will explain what I mean by "near" set of parallel universes later.)  No matter what the tensor-based directoralized angular and spin-orbital momentum that a superstring has in any given arbitrary position that the said superstring has at a given locus during an instanton, the variance from pure hermicity of the superstring that occurs in a Laplacian fashion in the region of the center of the said one-D superstring during that instanton is always situated in such a fashion so that the Laplacian separation that causes such a variance from pure hermicity is, in one way or another, norm-to-norm-to-holomorphic to the general directoralization of the flow of the superstrings of a given World-Tube -- that happens over the course of the first Ihbar of group-metrical-activity that correlatively occurs as the Ultimon-Flow that happens in-between the duration of each instanton.  The same general idea happens for superstrings that involve backward moving time, except that the relative forward holomorphicity goes in the opposite relative directoralization as the Flow that is related to superstrings that travel in such a manner that involves forward moving time.  I will continue with the second part of this session later!  Sincerely, Sam.             

A Little Bit More Explaination As To The Construction of the World-Tubes

Well hello again world, this is Sam Roach here!  I hope that you are enjoying my physics writings!
The "world-tubes" that involve forward moving time are interconnected via the Lagrangian-based majorized annuli that connect the adjacent of such tubes in an interior directed sense. Such annuli are existent at the interior center of such "world-tubes."
The "world-tubes" that involve backward moving time are interconnected via the annuli that connect the adjacent of such tubes in an interior directed sense.  Such annuli are existent at the interior center of such "world-tubes." 
The "world-tubes" of the substringular encoders are interconnected with the world-tubes of superstrings -- one of such encoder tubes per two forward moving time involved tubes that correspond to one set of parallel universes, and one of such encoder tubes per two backward moving time involved tubes that correspond to one set of parallel universes.  A substringular encoder of forward moving time has the same general Laplacian shape as the corresponding encoder of backward moving time, except that the isomoriphism of two of such encoders is in a reverse directoralization.  The substringular encoders are interconnected relatively just below the center of where the two "world-tubes" meet.  There is an open region between where a substringular encoder is and the spread of where the mini-string that these tie into are to interconnect the corresponding superstrings and their associated Planck phenomenon related phenomena.  This process makes a suppositional set of three tubes act as one tube, in a sense.
  The substringular encoders are relatively just above the relative top of the Fabric of the main initiating positions of what I call a Main Heterotic String.  So, forward and backward moving space-time fabric bear opposite tenses of what is relative "up" in the substringular fabric and of what is relative "down" in the substringular fabric if one where to observe such substringular fabric from its exterior.  So, there is more than one of such six-pointed-star majorized regions of the Main Heterotic Fabric that open up to allow for the flow of superstringular related phenomena per set of parallel universes.
When phenomena initially flows into the Main Heterotic String Fabric, such phenomena flows into the region where the substringular encoders were, since the encoders are relatively "below" where regular space-time-fabric as we know it exists, while then entering the prior named Fabric.  This would involve 8*10^(98) superstings for each universe of one main kinematically-based tori-sector-range and 8*10^(98) Planck phenomenon related phenomena for each universe of one main kinematically-based tori-sector-range in the forward moving time section of the Ultimon in-between instantons, and 8*10^(98) superstrings for each universe of one main kinematically-based tori-sector-range for each universe of one main kinematically-based tori-sector-range and 8*10^(98) Planck phenomenon related phenomena for each universe of one main kinematically-based tori-sector-range in the backward moving time section of the Ultimon in-between instantons.
The annuli that interbinds two forward or two backward moving time related world-tubes is larger than the annuli that interbinds such world-tubes of the arbitrarily other two sets of parallel universes.
If the time directed tense of superstrings is to go the other way, then some of the superstrings of one substringular encoder that involves one tense of time will ebb mini-string so as to allow certain of its corresponding superstrings to travel relatively "down" to the space-time-fabric of the opposite directed tense of time until a space-time-coordination is established, while then the forward moving space-time direction will become re-established from that point.  I will continue by providing the test questions for the last test of Cousrse 5 later.  You have a phenomenal day!  Sincerely, Sam.

Part Two of the Test Solutions to the First Test of Course 5

4)  If the "U" shapes involved with a Basis of Light are equally elliptically and hyperbollically concave, the time directoralization involved with such a a Basis will equally involve forward and backward moving time.

5)  If the "U" shapes of a Basis of Light are primarily ellliptically concave, then the time directoralization involved with such a Basis will primarily involve forward moving time.

6)  If the "U' shapes of a Basis of Light are primarily hyperbollically concave, then the time directoralization involved with such a Basis will primarily involve backward moving time.

7)  During the sub-metric in which the holonomic structure of the manifestation of the Bases of Light is overtly operational, the "knots" in the center of each related Basis bears a Dirac-operation of increasing in size mildly just as the main morphology of each respective Basis decrements in a euclidean manner in accordance to a Clifford-llke inverse proportionality right before instanton-quaternionic-field impulse-mode.

I will continue with the suspense of providing the rest of the solutions during my next two posts.  Sam.  Yes!

A Description Of Campbell Ghosts, Part One

A norm-state that is comprised of one first-ordered point particle that is supplementally norm to a set of first-ordered point particles that form a plane of surface area that is norm to reverse holomorphic relative to the originally stated first-ordered point particle is called a Campbell norm-state. Campbell norm-states that travel in positive time that are considered positive travel in a holomorphically-based directoralization. Campbell norm-states that travel in negative time that are considered positive travel in an antiholomorphically-based directoralization. Campbell norm-states that travel in positive time that are considered negative travel in an antiholomorphically-based directoralization. Campbell norm-states that travel in negative time that are considered negative travel in a holomorphically-based directoralization. As Campbell states move per sequential series of instantons, these scatter adjacent first-ordered point particles that are loose in certain regions. Such first-ordered point particles that are loose do not exist in a norm-state as is. The scattering of loose first-ordered point particles is a redistribution of anomalous Fock Space that exists along the Ward bounds of general homotopy. I will continue with the suspence later!
Sincerely,
Sam.

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

An electron as it is propagated along a path without any aberrations due to singularities that act directly upon the field generation has a homotopic electromagnetic field that defines the Ward Neumman boundaries of its emanated phenomenal discharge. As the electron is a sense of motion, it also moves as a unit as it is propagated in whatever direction/curvature that it is going in. Since this motion is moving, there is a tangency between the condition of the electron taken as an object And the energy released by that object moves along the operand of radiation that is defined by its constant change in directoralization. The electron always changes in its relative direction orientation seeing that it is constantly spinning. Whenever something moves, it gives off energy. Energy is always accelerating, and thus, always propagating energy. Radial motion that is constantly applied is always changing direction along with a discharge of a differentiating energy. Thus, radial motion of an electron is always dispensing a certain tense or tenses of energy, whether that energy is statically given off, or given off as electromagnetic energy (namely light). A tense of energy associated with a phenomenon as the radial discharge of an object is more associated with a magnetic field. The right-hand-rule works because the discharge of an electron's energy due to spin-orbital interactions tends to be 90 degrees to the discharge of an electron's energy due to its angular momentum. I will conclude with the suspense of this session of this course on my blog later.
Sincerely,
Samuel David Roach

Course 3 on Lorentz-Four-Contractions Session 13, Part 3

To find the velocities of these three lines, here. The lines are to be considered so extremely thin that the only impetus derived from these is in their endpoints. The lines connecting these points are merely a ghost of delineation. So a theoretical line in the middle of the directoral line that was orthogonal with the directoral line would bear no reality, and thus no motion while the horizontal (directoral) line moves. So, here, motion of interconnected lines is minimized at 90 degrees, and maximized at 0 degrees, when calling the horizontal line 0 degrees and the orthogonal position 90 degrees. So, if the "X lines" were at 3 degrees from the flat line each, and neither line fidgeted at all, then as the flat line traveled at .8c, then the two lines would travel at cosine of 3 degrees * .8c each. If there were 3 billion of such lines interconnected in the same fashion, then, to find out their velocity, multiply the cosine of the angle of each by .8c to find their velocity as a unit in the given direction. All three lines, however, would be traveling at .8c relative to the direction of the directoral line. You see, each line would be traveling as a unit in a sense quicker if all of their lengths were the same in a given direction, yet, take the endpoints into consideration. Take two pencils of equal length. Lay one flat. Angle the other one. Yes, the flat pencil goes the furthest along the surface. So, again, faster than light we shall discuss in future courses.