More About the Activity of the Light-Cone-Gauge

During BRST, which is the main part of a duration that is known of as instanton, superstrings and their counterparts go thru a gauge-metric that I call the Imaginary Exchange of Real Residue.  During this activity, the substringular fields, appertaining to superstings that are discrete units of energy permittivity, that interconnect superstrings with their counterparts -- the field eigenstates which are in the form of mini-string segments -- cause a wobbling motion that initially moves the counterparts of arbitrary superstrings in the forward holomorphic direction while counter-wobbling the corresponding superstrings in that same given forward holomorphic direction.  Such a gauge-metric consequently moves the given corresponding superstrings to wobble back in the associated reverse holomorphic direction while counter-wobbling the corresponding superstrings in the corresponding reverse holomorphic direction.  This happens while the Polyakov Action and the Bette Action are taking place.           
During the simultaneous activities of the Polyakov Action and the Bette Action, the associated superstrings and their corresponding counterstrings alter in scalar relative size via the increase of substringular wave or mini-string segment scalar increase in such a way that the associated superstrings and their corresponding counterstrings largen just enough to be at the length (for 1D strings) or circumference (for 2D strings) that corresponds to how small the associated Lorentz-Four-Contractions are.  As an example, if the Lorentz-Four-Contraction upon a given superstring is zero, then, the associated 1D strings increase during BRST in length by a factor of 3*10^8.  Or, as another example, if the Lorentz-Four-Contraction upon a given 2D string is zero, then the circumference of the associated superstrings increases by a factor of 3*10^8.  This is done with a maintainence of homotopy on account of mini-string being brought into the Gliossi field of where the mentioned superstrings and their counterstrings are at.  Once the corresponding superstirngs and their counterstrings have wobbled back into their original general locus via the reverse holomorphic wobbling of the associated counterstrings counter-wobbling the corresponding superstrings, the effect of this activity springs superstrings and their counterstrings into the Regge Action while then going into Ultimon Flow directly afterward, if their is no Kaeler-Metric during the course of the associated eigenstate of instanton.  If Kaeler-Metric is to happen during a particular arbitrary eigenstate of instanton, then, immediately after BRST, the mentioned superstrings initially enter their corresponding Klein Bottle eigenstate-like phenomenon for half of the rest of instanton -- the superstings of which in the process recontracting to the size that these had directly before these had expanded on account of the Polyakov Action, due to the differential geometry of the norm-states that exist in the given Klein Bottle eigenstates -- while then the superstrings go into the Regge Slope via the Regge Action for the other half of the rest of the arbitrary given eigenstate of instanton.  What we tend to notice in terms of time is instanton, or, more specifically, the BRST portion of instanton.  BRST happens for
6hbar time, while the rest of instanton happens for ((2pi hbar)-(6hbar)) time.  We only tend to notice instanton on account of the condition that superstrings are at a relatively organized standstill during the individual eigenstates of instanton.  By far though, most substringular activity happens in-between the individual eigenstates of instantons.  The Klein Bottle eigenstates are organized to be at the proper location on account of:  1) The abelian propagation of the Wick Action that is tensorically directoralized via the harmonics of wave-tug of the corresponding Schwinger Indices that travel as vibrational eigenstates along the Rarita Structure.  2) The corresponding abelian propagation of the Landau-Gisner-Acion upon the associated  Douboult cohomological section of the Rarita Structure known of as the field where the Fischler-Suskind-Mechanism happens. 3) The abelin nature of the Higgs Action eigenstates upon their associated Klein Bottle eigenstates toward the resultant of the hermitian Ward path that moves in the path of most resistance to the general location where the Kaeler-Metric is to happen.  The combined activities mentioned in the prior are what cause the proper inter-relations that allow for the correct distributions of Klein Bottle eigenstates with their corresponding superstrings so that the superstrings that need metric-gauge -- as well as the superstrings that may also then need to change in light-cone-gauge topology --  may be properly organized so that Gaussian Transformations may happen appropriately.  Sam Roach.      

About the Retying That Happens During the Space-Hole

While the duration that happens when the Bases of Light are undergoing their metric, certain conicentral conipoints of an arbitrary coniaxial's sub-mini-string segments at certain loci relative to superstrings that are about to go thru the process of an eigenmetric of the quaternionic-instanton-field-impulse-mode just begin to disconnect at their relative respective forward holomorphic ends in correspondence to the mentioned conipoint of the conicentral of an arbitrary coniaxial's loci where these just begin to temporarily lose the fractal of pressurized vacuum that is generated by the motion of substringular phenomena.  The very temporary disconnection that begins to happen during that general metric that exists in-between the durations of two arbitrary instantons happens multiplicitly where it happens on account of the condition that the conipoint-related conicentral loci as to where the mini-string exists is at in a very tightly-knit Fourier Transformation --  that would tend to be considered a Laplacian condition due to the fact that this happens during a sub-metric that is in-between two successive discrete units of time -- is where homotopy tends to be at its relative potential weakest.  The activity of the formation of the Bases of Light works to help keep homotopy to be maintained then.  I will complete this picture later.  Got to go!  Sam.                                   

Here Is Some Knowledge To Help You To Better Understand Sub-Mini-String

Sub-Mini-String is what interconnects both third-ordered-point-particles to each other as well so as to interconnect second-ordererd-point-particles into the type of mini-string that forms the fields that are exhibited by superstringular phenomena.  First-Ordered-Point-Particles are formed by the "yarning" of mini-string into the various forms of compactifications that allow for the respective various forms of first-ordered-point-particles that exist in the arena of space-time-fabric.             
Sub-Mini-String segments bind via an extreme fractal example of a pressurized vacuum.  Ideally, one would think that sub-mini-string segments would be flushly homeomorphically cylindrical.  Yet, the ends of the segments of sub-mini-string are not necessarily a fractal of cross-sectional orientafolds.  Often, either end and/or both ends of sub-mini-string segments are conically angled by up to 11.25 conical degrees if one were to observe such a conical angling at such a close range that a given arbitrary sub-mini-string segment would here appear to be three-dimensional.  Such an angling may be singularized, trivially isomorphic when one considers both ends of such a mentionable segment, or non-trivially isomorphic when one considers both ends of such a mentionable segment.  So, when such a said segment is non-trivially isomorphic at its maximum conical slanting at both ends, the overall conical angling difference would, in under a Laplacian condition, be a 22.5 degree difference.  This coincides with the condition that a Higgs Action eigenstate subtends to an angling of 22.5 degrees to the relative left of a relatively straight up and down subtending when a Klein Bottle eigenstate is to move holomorphically and that the same arbitrary Higgs Action eigenstate subtends to an angling of 22.5 degrees to the relative right from a relatively straight up and down subtending when the respective Klein Bottle eigenstate is to move antiholomorphically under the same eigenmetric of any arbitrary Kaeler-Metric eigenstate.  Either way, when one considers a Wilson Line that measures the general length of a sub-mini-string segment, the length of that segment is always 16 times as long as its thickness at its center.  Sub-Mini-String is always the same thickness.  Again, this is not a length that is derived by a theoretical Gliossi-based Laplacian measurement, yet, this considered length, which is always the same, is based on a Wilson Line that measures the general length of any given sub-mini-string segment.  Here is what I mean.  Take both ends of any of such said segment.  Consider pseudo-orientafolds that extend "above" or "below" a given segment that we are discussing.  Draw a line that is straight that connects the orientafolds.  That given line will always be the same length, whether the said segment is homeomorphically cylindrical, conically angled at one end, trivially isomrphically conically angled at both ends, or non-trivially isomorphically conically angled at both ends.  This is what I mean by a Wilson Line.  The ends of sub-mini-string always flushly touch in a Gliossi Manner, whether the given ends are conically angled or not.  This goes to show that the slanting of the conically angling of the ends of such said sub-mini-string segments are always bimorphologically isomorphic to the degree that such segments are angled.  The number of variations of such slantings is the following:  Take the reciprocal of
(~1.104735878*10^(-81)), and divide this number by 16.  During the space-hole, the relatively forward holomorphic ends of the segments of sub-mini-string that bind those loci of mini-string (reverse-fractaled of sub-mini-string) that are to temporarily disconnect to retie before the quaternionic-instanton-field-impulse-mode.  Such a sub-metric of brief disconnection is due to the virtual lack of a fractal of pressurized vacuum in loci of substringular field.  Based on the Laplacian condition that is in consideration of the placement of the substringular field eigenstates as this is happening, the sub-mini-string segment ends that nearly break homotopy reconnect in the manner that involves the least resistance.  This retying is what allows for the continuation of Gaussian Transformations, of which allows for the spontaneous kinematic covariance that is essential for metric-gauge to be activated so that superstrings may be discrete energy so that reality may continue.  I will continue with the suspence later.                                    

More About the Importance of Not Singling Out Gluons

The metrical activity of gluons is what effects the Rarita Structure via the multiplicit kinematic Fourier differentiation of Schwinger Indices to form the Wick Action.  The Wick Action is the most important type of Hausendorf Projection, and is implemented on accout of the gluonic force (the strong force) to move the Landau Gisner Action (which is the most important type of Campbel-Hausendorf Projection) so as to allow for the leveraging of the Fischler-Suskind Mechanism upon eigenstates of the Higgs Action so as to move the respective corresponding eigenstates of the Klein Bottle so as to allow for the condition of Kaeler-Metric to be in place so that superstrings that lack metric-gauge may regain their mentioned metric-gauge so that discrete energy may remain as discrete energy so that reality may continue to exist.  The Kaeler-Metric always happens so as to also allow for the proceeding Gaussian Transformations to occur.  Gaussian Transformations are essential so that different sources of kinematic vibrations may inter-relate in a covariant manner so that the continuation of the existance of energy may continue to be kinematic.  So, since the metrical activity of the gluonic force is what causes the Rarita Structure to cause the existance and covariant relation of the Wick Action so as to indirectly allow for the continuation of unfrayed substringular fabric.  This is not to mention the fact that the gluonic force is what binds together quarks and/or leptons to other quarks and/or leptons.  So, one should not try to isolate the gluons in a manner that causes these to not perpetually funcion as the strong force.  Minor attempts to isolate gluons may cause just a "fissure" in space-time-fabric, yet, this would be like metaphorically saying that a damm just has a tiny hole in it.
This is just one of about a handfull of reasons as to why the Hadron Colliding Experiment should be shut down.  In so long as the right hardware may be formed via certain extrapolations that involve how to use practical sense so as to utilize the activities of such particles, it is otherwise completely dangerous and unnecessary to try to isolate/illucidate certain particles when such isolation/illucidation is so potentially harmfull to the continued existence of the world.          
God Bless You,               
Sam.                  

A Little About What Caused What

If it wasn't for the Logos, the Higgs Action would never have been activated to begin to create a discrete reality out of the Big-Bang.          
If it wasn't for the Higgs Action, metric-gauge would never have been created to allow for the soon to be created superstrings to act as discrete units of energy permittivity -- as well as to allow for the soon to be created Fadeev-Popov-Traces to act as discrete units of energy impedance.
If it wasn't for the kinematic multiplicit redistributions of superstrings, there would be no ghost anomalies.
If it wasn't for ghost anomalies, there would be no Njenhuisly placed gravitational particles.
If it wasn't for Njenhuisly placed gravitational particles, the Rarita Structure would serve no purpose, and the Ricci Action would never take effect.
If the Ricci Action never took effect, gravity would never be attainable, and mass would never be able to be attained.                       
If there was never any mass, the perpetuation of electromagnetic energy would not be sustainable -- since soon after the Big-Bang happened, electrons dropping back-and-forth an energy level is what has subsequent to then been the activity that releases discrete energy known as photons, or, in other words, since soon after the Big-Bang happened, it has taken a type of mass known as an electron in order for light to be perpetuated and sustained.
If it wasn't for electromagnetic energy, the absence of light would cause mass to have no relativity and also no ability to have any heat.
If it wasn't for heat, mass would have no vibration, and thus mass would not be sustainable.
If it wasn't for phenomena to differentiate relative to light, there would be no time, length, nor mass relationships.
If it wasn't for there to be a relationship of mass toward its environment -- mass, heat, gravity, and motion period would fly apart into nothingness.
Yet, certain realities are the way that they are period. -- Just like basic math is just a fact of reality that can not be changed.
Since reality has been perpetuated from soon after the Big-Bang, the activity of Schwinger Indices upon the Rarita Structure has been what causes the Wick Action that causes the Landau-Gisner-Action to cause the Suskind-Fischler-Mechanism to have a leverage to allow the Higgs Action to move the Klein Bottle so that Gaussian Transformations are possible so that energies existence may be sustainable so that reality may continue to exist.                      

About Point Particles

First-Ordered-Point-Particles comprise superstrings.
Second-Ordered-Point-Particles comprise the mini-string that "balls-up" to form first-ordered-point-particles, while these second-ordered particles also form all mini-string that forms substringular fields.
Third-Ordered-Point-Particles only exist so as to form the composition of second-ordered-point-particles.
Sub-Mini-String binds together third-ordered-point-particles as well as interconnecting the said second-ordered-point-particles.
Just as mini-string forms all substringular fields -- and also considering the condition that second-ordered-point-particles are two orders lower in diameter than superstrings --  sub-mini-string is what binds the mentioned second-ordered-point-particles. 
Catch You Two,
Samuel David Roach.                                      

A Mild Description of the Light-Cone-Gauge

The light-cone-gauge acts like a "springing" mechanism that allows for superstrings that iterate during BRST to be able to go thru the Regge Action and/or the Kaeler-Metric while then going into Ultimon Flow.  As I will show in words in both the end of Course Nine, during Course Ten, and during Course Twelve as well, what we tend to observe of in terms of discrete units of time are instantons.  During instanton, superstrings are relatively motionless.  After each successive instanton, each superstring physically alters in its position.  The successive series of such displacements forms the basis of what we tend to think of as the kinematic differentiation of superstrings that are put thru the multiplicit various Fourier Transformations that allow motion and thus energy and existence to be actual.  The metrical activity of the light-cone-gauge during BRST forms a spring-like activity that forms a Reverse Dirac mechanism that causes superstrings to go thru those differentiations during Ultimon Flow so as to allow for the proceeding repositioning of superstrings so that the said Fourier Transformations that allow for existence to be to happen.  I will continue with the suspence later!  Sincerely, Sam Roach.    

About Different Forms of Cohomology

Let us take into consideration a specific arbitrary case of a cohomological scenario.
Let us consider a case in which there is one bosonic string that has a non-abelian light-cone-gauge topology with an antiholomorphic tendency that is at a given relatively limited number of instantons interbound with two bosonic strings that have an abelian light-cone-gauge topology with a holomorphic tendency.  The mentioned interbinding interaction is Yakawa, yet, the said binding is not completely Gliossi in terms of the relatively borne tangency that exists between these three interactive and covariant superstrings.  The topological stratum of the three Yakawa-based-interactive superstrings is separated by a multiplicit mini-string field network that allows just enough room in-between the holonomic topology of each individually considered superstrings so that each of the three mentioned superstrings may be able to undergo an eigencondition of a  Polyakov Action followed by an eigencondition of a Bette Action followed by an eigencondition of a Regge Action.  Such an interbinding here makes the three cohomologically-based superstrings to be non-orientable during the triune eigenmetric of Bette Action, yet, generally, the three described superstrings considered in this arbitrary case will normally, under these conditons, be orientable during the ensuing triune eigenmetric of Regge Action.  If the three mentioned superstrings taken individually are not orientable during the said Regge Action, the three said superstrings will then become tachyonic.  Yet, since under the initialy considered conditions, such superstrings taken individually will be orientable during the Regge Action in the process of  such strings going thru their Lagrangian-based operands, which are, in general, called the Regge Slope.  Each of such Lagrangian-based operands is an eigenregion in which superstrings that are not orientable during the Bette Action may become orientable under normal conditons.  If such a cohomology as originally mentioned is existant over a sequential series of instantons, then, the said cohomology is said here to differentiate in a Fourier manner according to Noether Flow.  The mentioned cohomology -- when one is to map out the theoretical overlapping that one may determine under Laplacian conditions that involves individual instantons -- would not directly overlap with pure chirality.  Thus, such a described coholomology is said to bear a non-trivial isomorphism in terms of the handedness of symmetry that one may determine via such a theoretical overlapping that one may map out during any particular Laplcain condition that would exist during the BRST portion of any given instanton. 
  Yet, since the symmetry here is non-trivially isomorphic, and, since the wave-tug of the two said bosonic superstrings that I described as having an abelian light-cone-gauge topology are angled acutely when one considers a Laplacian Wilson Line that is to be determined from the relative holomorphic endpoint of the non-abelian-based bosonic superstring that subtends in the relative holomorphic direction, the overall wave-tug forms a tense here of conformal invariance in terms of the general limited locus where the substringular cohomology exists over a said sequential series of instantons.  Yet, as an ansantz, the tendency of such a cohomological basis will tend to begin to relatively slowly propagate in the relatively holomorphic direction.  World-Sheets tend to form more of a Gliossi Yakawa-based cohomology when these phenomena interbind both in terms of Rham, Douboult, and also in terms of Rham-Douboult cohomological interaction.  You have a phenomenal day!  Sincerely, Sam Roach.                                                  

More About the Activity of the Schwinger Indices

Gauge-Bosons pluck second-ordered light-cone-gauge eigenstates to form second-ordered Schwinger Indices.  The just mentioned Schwinger Indices exist as vibratory eigenstates that propagate along the Rarita Structure while also propagating along the topological region of the multiplicit Real Reimmanian Plane eigenregions where discrete units of energy permittivity and discrete units of energy impedance interact via mini-string (the mini-string of which is the field eigenstates of superstrings, the field eigenstates of the associated counterstrings, and the field eigenstates of the Fadeev-Popov-Traces that act as the inverse field trajectory of the just mentioned superstrings) to work toward the periodicity of the Kaeler-Metric via the activation of a Hausendorf Projection known of as the Wick Action.            
The vibratory oscillations which are comprised of second-ordered Schwinger Indices that allow for both the Laplacian and Fourier spin-orbital conditions of both orbifolds and orbifold eigensets cause those harmonic and anharmonic wave-tug conditions among substringular phenomena that allow for the spontaneous changes that are necessary so that the norm-conditions that exist among superstrings may, for the most part, be orientable in such a balance so that only a strong exterior force would otherwise be able to cause a disorientation in the prior mentioned general type of conditions.  Since the Rarita Structure eigenstates bear their covariant orientation between superstrings and particles that act as discrete units of gravity, and also while the vibrations that exist among both superstrings, orbifolds, and orbifold eigensets is synchronized by the tempering of Schwinger Indices with the topological Fourier activity of the substance that comprises substringular discrete energy along with the membranous phenomena that these exist in, this causes such a substringular conformity that fascillitates the ongoing existance of the covariantly kinematic norm-conditions which are to continue as these perturbate so that continued exist may occur.  When a Gaussian Transformation is thus necessary so as to allow the necessary alterations that are necessary so that the covariance of norm-conditions may be kinematic as described before, the Wick Action is thence pulled out as a Yakawa-Based natural response to such a need.  This here indirectly -- after more steps that I will not describe here -- cause Gaussian Transformations to occur.  Whenever there is a Gaussian Transformation, there is a sequential set of instantons that involves the Kaeler Metric.  The most common form of Gaussian Transformation is known of as a gauge-metric.                        

The Importance of the Interaction That Exists Between the Light-Cone-Gauge and the Rarita Structure

Each second-ordered light-cone-gauge eigenstate is plucked like a string of a harp to allow for vibrations known of as Schwinger Indices to propagate along the Rarita Structure in such a manner so that there is an interconnection in-between both discrete units of energy permittivity and discrete units of energy impedance with gravitational particles so that the amplitude of the Ricci Scalar may be, within reason, able to spontaneously allow gravity to take a certain degree of hold upon the basis of substringular interplay.  The phenomena that "plucks" the second-ordered-light-cone-gauge eigenstates are known of as gauge-bosons.  Gauge-Bosons are also termed of as E(6)XE(6) strings.  So, the harmonics and the anharmonics of the Schwinger Indices along the topological Fourier-Based trajectory of where the holonomic substance of the Rarita Structure is located at any given arbitrary sequential series of instantons in which the interaction of the said Rarita Structure upon gravitational particles bears a type of multiplicit gauge-metrical basis that causes gravity to be applied to discrete units of energy so that gravity may exist in the manner that it is applied to be is thus the phenomena activity that allows for the general basis of a type of amplitude known of as the Ricci Scalar.                                       
Just a little bit for now.
Sincerely,
Samuel David Roach.

A Little Bit More About Cassimer Invariance

So did you think a little bit about what I have written about Cassimer Invariance?
To bring back a recollection, Cassimer Invariance is the perpetual tendency of substringular phenomena interchanging eigenstates to maintain homotopy per instanton.  
Here is some more knowledge that may help you to better understand what the directly prior deffinition means.:  Phenomena that is substringular moves through Ultimon Flow in-between each instanton.              
In ((2pi hbar-6hbar)+hbar Imaginary time) until an Imaginary Planck-Bar moment before instanton, phenomena goes through a duration that involves what I have described as the "space-hole" -- during which the Bases of Light appertaining to the ensuing instanton is organized.  During this mentioned duration, substringular phenomena goes through relatively mild untying and retying of topology that is necessary for the changes that are necessary for substringular phenomena to not be frayed along with that phenomena that is frayed due to black-hole activity, as well as the mentioned untying and retying of topology just described is necessary in order for ensuing Gaussian Transformations to be spontaneously adjusted and allowed to happen.  The condition that I have just described in terms of fascillitating Gaussian Translations and Gaussian Transformations to happen is necessary on account of the condition that space-time-fabric is not completely hermitian in terms of the multiplicit codifferentiation that surrounds any particular orbifold neighborhood.  This may be related on account of the ansantz that not all orbifolds are Yau-Exact -- only mass and mass that is translated through a worm-hole is Yau-Exact.  The condition that there is partially Yau-Exact and Chern-Simmons activity that sorrounds any substringular neighborhood that is completely Yau-Exact is evidence that shows the validity of the concept of the sentence that I typed just before this one.  Wherever there is a mass, there is at least a certain degree of heat that is directly associated with that mass when one considers the duration in which any arbitrary mass that one could consider has vibrated in some sort of molecular manner over any measurable amount of time.  Even if you could get a molecular arrangement to acheive absolute zero Kelvin over a certain arbitrary duration, there will always be a certain amount of electromagnetic and/or plain energy interaction that sorounds the general region in which an arbitary mass is existent in in any duration in which the said mass is able to molecularly vibrate.  The condition that there is always a certain amount of partially Yau-Exact and Chern-Simmons differentiation that surrounds any arbitrary mass that is existent over any period in which any said mass is able to molecularly vibrate is proof that all Fourier Transfomations that are based on Yau-Exact orbifold translations are sorrounded to at least some extent by electromagnetic energy and/or plain energy.  Since only Yau-Exact orbifold conditions are completely hermitian and non-spurious, both plain energy and electromagnetic energy always have a certain degree of Chern-Simmons behavior.  Although electromagnetic-based energy is formed based on the hermitian motion of  Fujikawa Coupling activity, the motion of plain energy and electromagnetic energy when scattered upon a mass always bears a certain degree of a lack of hermitian-based motion.  This is why Fourier-based Gaussian Translations and Fourier-based Gaussian Transformations may only happen when there is a certain amount of retying of substringular activity.  This retying can not happen during instanton on account of the need to maintain homotopy.  Such retying can only happen right before the quaternionic-instanton-field-impulse-mode.  Such a duration then is to happen during the duration in which the "space-hole" and the Bases of Light are organized.  It is during the prior mentioned duration that the relatively Laplacian conditions that correspond the two general simultaneous gauge-metrics that the brief relatively mild retying of space-time-fabric is able to happen to the necessary extent so that the necessary norm-conditons of any particular region may be tweeked so that the said norm-conditions may contiue to codifferentiate with its surroundings.  I am only able to describe so much at once.  In time, you will get a clearer meaning as to what I am saying.       
I will continue with the suspence later!  God Bless You, and have a phenomenal day!
Sincerely,
Samuel David Roach.

Course 9, First Course of Fock Space and the Light-Cone-Gauge, Session 12

How do Planck Phenomena propagate?:   Strings are in iteration in the following arbitrary case scenario.  Imaginary exchange as described by an odd function happens as real residue is given off here and received.  This means that the relative bottoms of the here mentioned superstrings are exchanged with the corresponding relative tops of the respective substringular counterparts.  (The superstrings & their counterparts are now decompactified by a factor of one to 3*10^8.)  This prior activity rasises the stringualr counterparts and moves these "down" closer to the prior mentioned superstrings.  The slack here causes the discussed bottom of the substringular counterparts to exchange with the said tops of the corresponding superstrings (reciprocal imaginary exchange).  The prior activity lifts the superstrings (not to be confused with their counterparts) and moves these down closer to their corresponding Planck Phenomena.  The Planck Phenomena stays relatively stationary in the meanwhile -- when not including the wobble of the said Planck Phenomena.  This motion that I have just described contracts the light-cone-gauge like a spring, causing the ensuing Ultimon Flow.  This springing flaps the angular momentum of indices of the said Planck Phenomena in an anharmonic/harmonic cycle that flaps just enough to allow Ultimon Flow, like a paint stirrer twitches then flapped.  The twists in the light-cone-gauge eigenstates that are related to what I just mentioned bears gauge-metrics that help determine whether or not the superstring travel at any given velocity and/or tensorically based speed or not. (The "tensorically based speed" would be a velocity that is based on the directoralization of a tree amplitude.)  A full twist in the fabric of the light-cone-gauge allows for a relatively "infinite" speed, such as the amplitude of phenomena displacement that happens during Ultimon Fllow,  while any twist quotient in-between allows for any speed of the superstrings in-between, since tachyonic motion may redistribute phenomena to basically any other location in just one sequential series of instantons.  Such a displacement that is derived in-between the Real Reimmanian duration that exists from one instanton to the next one may redistribute phenomena as such on account that Ultimon Flow is the Imaginary based flow that cycles the Ultimon in-between two consecutive Real Based instantons.  These mentioned twists are never entangled when unfrayed, yet, the twists are in the individual fabric of the five-quantum-based and ten-quantum-based first-ordered light-cone-gauge eigenstates that are associated with one-dimensional and two-dimensional superstrings respectively.  Two-Dimensional superstrings may influence one-dimensional strings to have their light-cone-gauge first-order-based quanta to twist to an arbitrary proscribed extent and vice                                                        versa.                                                                                                                                                      
I will continue with the suspence later.  Expect a lot of posts soon now that I have my time freed up and my computer is working better now!  God Bless.  Samuel David Roach.                                                                            

Coming Back To Life

Hello, this is Sam Roach here! 
Sorry that I have not posted lately, yet, since May 2nd, I have not only been "burned out," yet, also, I have been working on ideas that I will not mention here that were far more important than anything that I ever put into my blog.  I don't care if some people think that I know nothing, everything, or anything in-between.  I need to keep certain things basically to myself and my associates.
I will say this though, the light-cone-gauge is the field-substance and directoralized and/or tensoric amplitudanal force that is essential for the continued propagation of superstrings so that these strings may procede from instanton to instanton.
The Rarita Structure is the field-connection that allows for gravity to take effect upon superstrings that are discrete units of energy permittivity.                   
The Ricci Scalar is the amplitudinal directoralization/tensorism that is due to the interaction of the Rarita Structure upon the covariant activity that exists between superstrings and gravitational particles.
The means of immediate substringular interaction is due to the leverage of the Rarita Structure upon strings, orbifolds and orbifold eigensets.
Mass may be translated faster than light by changing its light-cone-gauge from Kaluza-Klein to Yang-Mills, yet, during such a translation, the mass is not technically a mass.
The reason as to why a mass as a mass may not go at the speed of light is because one can never have more than one-hundred percent fractal modulae.  This is due to the condition that an abelian light-cone-gauge that has Yau-Exact singularities among the here adjacent superstrings and the here adjacent orbifolds may not bear a field that would thus hyperextend and thereby tear topology.  Yet, due to the fact that wherever there is a mass, there is always an interaction between the said mass and electromagnetic energy -- this causes the prior mentioned dillema to never potentially happen.
Mass may never be translated into light via having purely Chern-Simmons singularities in-between the arbitrary superestrings and the arbitrary orbifolds here withoug turning it into a form of entropy.
Gotta Rush!  God Bless You!                                                                       
Sincerely,
Samuel David Roach.             

Mild Correction

Every Basis of Light has one trillion different types of Planck-Related-Phenomena.
Two posts ago, I described, in general, the conditions that may be used to determine the 159,000 different types of Bases of Light -- each Basis of Light corresponds to one layer of Reality.
Each Layer of Reality is reflected in all of the parallel universes.
The intensity of the hermitian curvature of a PRP works to determine specifically what one is dealing with, yet, besides the hyperbollic intensities, the manner of the conditions of the PRP as described two posts ago works to describe which layer of reality one is dealing with with any given arbitrary parallel universe that one is either in or wishes to be in.                              

How the Bases of Light Are Fractored By the Planck-Related-Phenomena

When the Bases of Light are retied -- via the quaternionic-instanton-field-impulse-mode -- the same basic type of morphological nature of each Basis of Light taken individually is fractored by the corresponding Planck-Related-Phenomena.  Aside from the 159,000 different types of Planck-Related-Phenomena morphologies that may be generalized by what I had discussed in my previous post, there are close to one trillion manners in which the hyperbolically concave up morphologies of the "Chi" shapes of the given mini-traces may formulate in terms of the intensity of such a prior mentioned type of curvature that may be mapped out under any given Laplacian condition of such Planck-Related-Phenomena that involves forward moving time during BRST.  Likewise, there are also close to one trillion manners in which the hyperbolically concave down morphologies of the "Chi" shapes of the given mini-traces may formulate in terms of the intensity of such a prior mentiones type of curvature that may be mapped out under any given Laplacian condition of such Planck-Related-Phenomena that involves backward moving time during BRST.  In the region to where the Bases of Light moves primarily forward, there is one Basis of Light that involves forward and backward moving time equally.  In the region to where the Bases of Light moves primarily backward, there is one Basis of Light that involves forward and backward moving time equally.  So, one not only has the 159,000 basic variations of Planck-Related-Phenomena as I described in my previous post, yet, there are three different general types of intensity in terms of the hyperbollic nature of the basic curvature of the "Chi" shapes that are an integral part of the mentioned Bases of Light as may be determined by the detection of the corresponding mini-traces.  Regular mini-traces bear a hyperbollic concave curvature along the mapping out of the "Chi" shapes under Laplacian conditions that is strictly eucildean and hermitian.
Virtual mini-traces bear a hyperbollic concave curvature along the mapping ot of the "Chi" shapes under Laplacian conditions that is determined via a power series of observed extension. While Planck-phenemenoa visages bear a Laplacian tracing that is exponential in terms of how one may map it out from the center of a mini-trace to its exterior Ward Neumman bounds.  Likewise, for every Regular-Planck-Phenomena, or, RPP, there are 10,000 times as many total RPP and virtual PP combined, and, for every RPP, there are 100,000,000 total virtual PRP, visage PRP and RPP combined. Virtual visage Planck-Related-Phenomena, or, VVPRP, bear an exponential mapping as before, except, the related traces bear a Laplacian condion of extended sub-mini-string in-between the second-ordered point particles that comprise the traces that comprise the mentioned "Chi" shapes. Again, for every RPP, there are one trillion total RPP, virtual PRP, visage PRP, and VVPRP.  You have a phenomenal day, and I will continue with the suspence later!  Sincerely, Sam Roach.                                                                                                       

More About P-R-P Modes

Here is more as to how to determine if the tense of a parallel universe that you are searaching to be in is of a particulaar tori-sector-range -- or, in other words, if the tense of a particular universe that you are searching to be in is of a particular "layer of realilty."        
Each Basis of Light that is unfrayed is of a particular "layer of reality", of which is based on seven general solution modes that also incorporate the three-dimensional Laplacian placements that the mentioned arbitrary Basis of Ligh,t relative to the other Bases of Light, that one is considering, is in during the duration of an arbitrary metric of what I call the "space-hole."  Based on the condition that electrons exist in D-fields that are of a Fourier minimum of six spatial dimensions plus time is why there are six types of heterotic vibration modes of the tori-sector-ranges relative to one another, which multiplies by a factor of six the potential determination of the number of "layers of reality" in and of itself.  The seven general solution modes that I have mentioned bear a 49 membered particular solution that bears three overlapping or redundant modes -- not including the member of the described solution that is associated with a constant.  Now, if you consider the ten tenses of topological sways that exist per sub-dimension (that is, what would appear as a three-dimensional setting when one detects the arbitrarily given Planck-Based phenomenon up close), taken individually, that form an overall substrate of 1,000 different multiplicitly arranged topological sways, one may be fascillitated to determine which of the (46+1+6)*3*1,000 types of tori-sector-ranges, or, in other words, which of the types of "layers of reality," is applicable to the tense of the parallel universe that you wish to enter in one set of parallel universes.  Thus, one is to consider the covariant Laplacian placement of the Bases of Light of one set of parallel universes relative to the others.  (159,000 layers of reality happen, over the courese of the existence of space and time PER set of parallel universes, and there are three sets of parallel universes in physical space-time-fabric.)  As implied earlier, each of the unique members of the prior described particular solution, along with the constant that is determined when one integrates to form the described particular solution -- and this given constant of which is a determinant factor in representing a parallel universe that is most similar to ours, along with the six types of heterotic vibrations that exist among the Bases of Light that corresponds to the minimum of six spatial dimentions that exist for an electron, along with each of three-dimensional up-close Laplacian placements of each Basis of Light as it exists during the duration of what I call the "space-hole",  (NOTE:  The configuration of Planck-Related-Phenomena is based on the directly prior configuration of its corresponding Basis of Light that it untied from in-between two successive instantons.), -- which corresponds to a specific tori-sector-range --, along with each of the 1,000 combinative formats of the topological sway, and finally considering if the curvature of the corresponding "Chi"-Related shape is hyperbolically concave up (for positive-moving-time-related Planck-Related-Phenomena) or if the curvature of the corresponding "Chi"-Related shape is hyperbolically concave down (for negataive-moving-time-related Planck-Related-Phenomena), works together to describe a specific Basis of Light that is mirrored fractorially in the "mini-traces" or the Planck-Related-Phenomena in order to help determine which "layer of reality" that you are dealing with.  The just mentioned knowledge also helps to determine which tori-sector-range is -- at an arbitrary locus of time -- appertaining to a tense of a parallel universe that one may wish to enter.  I will continue with the suspence later.  If I make any mistakes, at least I know that I am moving in the direction of the truth.  The knowledge above is a good filler in-between Session 11 and Session 12 of Course One on Fock-Space, gravity, and the light-cone-gauge.  This, being Course "9."  You have a phenomenal day!
  Sincerely, Samuel David Roach.                                                                                                                                                                   

Session 11 of Course 9 on Fock Space, Gravity, and the Light-Cone-Gauge

One-dimensional strings attach to five light-cone-guage quanta, while two-dimensional strings attach to ten light-cone-gauge quanta.  When a Planck-Related phenomenon reverberates in terms of its angular momenta indices, both ends of the corresponding Planck-Related phenomenon reverberate.  The light-cone-gauge quanta attach to the center of another Planck-Related phenomenon.  the light-cone-gauge-eigenstates are much thinner than superstrings, so the spring-like action that is associated with this activitiy is geared to place the strings and their corresponding reversely-holomorphically placed field trajectory back to the same spot, except for the twists in the light-cone-gauge quanta -- when one particularly considers the conditions that exist for phenomena that has a Yang-Mills light-cone-gauge topology.  Twists in the light-cone-gauge quanta are produced by the normalization modes of the other substringular phenomena that arbitrarily here are acting upon a given set of Planck-Related phemena.  The dilaton, the third-ordered point particle, and the negative-norm point commutator modes act upon the Planck-Related phenonema to directoralize the Poincare, Weyl, and Majorana indices to activate the transfiguration of Planck-Phenomena-based normalization via Ward Caucy differentiation to allow an operand for the given changes in the flow of the associated Planck-Phenomena differentiation over a set of the iterations that happen per instanton.  As the affiliated instantons differentiate interactively thru the kinematic operation of time, the described field trajectory of the mentioned arbitrary superstring that I am describing here forms a pattern of normalization differentiation in such a manner that allows chaos, or entropy, to return to harmony.  This follows the pattern of anharmonic Planck-Related differentiation to harmonize indirectly the adjacent Planck-Related differentiation, except, this other pattern I have mentioned takes the history of the expansion of the universe.                    
I hope that you have a phenomenal day!
Sincerely,
Sam.                                              

A Little Bit Of A Refresher As To The Nature Of The Light-Cone-Gauge

Eigenstates of a first-ordered-light-cone-gauge act as a substrate of a spring-like activity that allows for substringular phenomena that are undergoing BRST to be pulled into the Regge Action so that Ultimon Flow in-between the durations of individual instantons may transpire. 
The substrate that I just described is comprised of chords of mini-string that are abelian when dealing with a Kaluza-Klein light-cone-gauge topology, and such chords are non-abelian when dealing with a Yang-Mills light-cone-gauge topology.  An abelian light-cone-gauge topology bears more of a direct substringular field in-between the reversely-holomorphically positioned field trajectory of a superstring with the inferred arbitrary superstring.  What I mean by a direct substringular field is that the wave-tug that exists in this region bears a tightly associated pull that is relatively high in fractal modulae while being relatively low in elastic modulae -- in terms of substringular holonomic focus upon the arbitrarily given superstring that one would be refferring to when one reffers to a Kaluza-Klein light-cone-gauge topology.  A Yang-Mills light-cone-gauge topology -- although the chords of mini-string that exist in the prior mentioned type of region also bear a strength of wave-tug that is both Gliossi to both an arbitrary superstring and its reversely-holomorphically positioned field trajectory -- bears more of a elastic-modulae and less of a fractal-modulae in terms of the activity that happens both during and after the activities that happen during BRST.  Yet, in either case, the flow of the Imaginary Exchange of Real Residue that happens here (motion that happens in a Dirac manner that bears a multiplicitly associated wave-tug and pull that happens back-and-forth on and off of the Real Reimmanian Plane that one would associate with a specific positioning that one would initially think to be inherent to the Laplacian Condition of a superstringular setting during BRST  ("Imaginary"),  while yet this activity of sub-metrics happens during the core of an instanton in any arbitrary case (Real)) in such a manner that the  combined synergy of the mild re-delilneations of the mini-stringular fabric that ebbs to-and-frow from a supersting to and from its counterpart (which thus forms a strong wave-tug upon the associated first-ordered light-cone-gauge eigenstate) so that the hyper-extension of the relatively Laplacian condition of a given first-ordered light-cone-gauge bears a Hodge Index of impedance that consequently (after the Imaginary Exchange of Real Residue) resulves from a high potential gauge-metric to a high kinetic gauge-metric due to the springing potential of the light-cone-gauge once it is released from a stretched or addendumed-related stretched condition that happens due to the synergy that I earlier described.
With superstrings that have a Yang-Mills light-cone-gauge topology, the stretching activity that I mentioned is more literally stretched in and or itself due to the wobble that occurs during BRST.
With superstrings that have a Kaluza-Klein light-cone-gauge topology, there is mini-string that is pulled into the region in-between an arbitrary superstring and its reversely-holomorphically positioned field trajectory that is stretched in a euclideanly proportional manner while it binds with the chords of a first-ordered light-cone-gauge topology in such a manner that is respective to the high fractal/low elastic modulae of the substringular field that exists in the described region during BRST.
Since the stretching of the extrapolatorial field that I described as a light-cone-gauge eigenstate pulls the sub-mini-string that comprises the second and third-ordered point particles that form the chords that work to define the core of the field of the region of a first-ordered light-cone-gauge eigenstate to as close to the brink of fissuring without the condition of anharmonic resonance, such an activity that happens during BRST is the type of activitiy that operates to cause superstrings to go into the multiplicit Regge Actions, the Regge Actions of which happen with such a slope that pulls superstrings into the Ultimon Flow that is necessary for the countless sub-metrics that happen during the duration that happens in-between ensuing instantons.
Instantons are considered to be the smallest units of time that may actually be called "time" becasue the core of instanton (BRST) is when superstrings are relatively organized and motionless.
(6/2pi) of instanton is during BRST.  The activities of Kaeler-Metric (if this is to happen during an arbitrary situation or not) and Regge Action finish the pull of superstrings into Ultimon Flow.
When there is no Kaeler-Metric, the whole duration of (2pi-6) of instanton involves the Regge Action.
When there is a Kaeler-Metric that happens under a particular circumstance, the Kaeler-Metric happens over a duration of ((2pi-6)/2) and Regge Action happens over a duration of ((2pi-6)/2).
Unfortionately, it is impossible to explain everything at once.
I believe that this is enough for you to mentally digest for now!                            
You have a phenomenal day!                                                          
Sincerely,                  
Samuel David Roach.               

More About Ghosts

When you detect what seems to be superstrings over a tightly-knit Fourier Transformation, mainly, what you will be detecting will be Gliossi-Sherk-Olive-Ghosts.  It is easy to confuse these with superstrings in and of themselves.  The difference is that superstrings and their reversely-holomorphically-positioned field trajectories are designed as I have stated, while, Gliossi-Sherk-Olive-Ghosts will always be detected as relatively torroidal -- such as may be described in M-theory.  Yet, orbifolds that consist of superstrings may, at times, also be relatively torroidal in nature.  The difference is that the prior mentioned ghosts are much closer to the Planck-Length than the length of an orbifold.  Got to go!  I will continue with the suspence later!                   
Sincerely,
Samuel David Roach.                          

A Little About Singularities That I Feel Like Mentioning

Well hello again world, this is Sam Roach here!  How are you doing?!
Do you remember when I had mentioned that a hermitian curvature -- whether one is talking about a Laplacian setting that reffers to a "snapshot" of duration, or whether one is talking about a Fourier setting in which a curvature is developing over a sequential series of instantons -- is a curvature in which all of the derivatives equal to the number of dimensions that a given phenomena is present in are smoothly tranlated either thru a mapping of the tracing of the curvature for a Laplacian setting or thru a developmental mapping of the curvature that is traced over a duration of a sequential series of instantons?!  Well, here is a simple idea that will be an epitheny to you when you hear it: 
When a substringular curvature is translated either purely pictorially or via a kinematically mapped redistribution that is studied over a timewise delineation, if you go from one part of the curvature to another in the course of a relatively tight locus -- and there is a location in-between where there is a singularity (in so that the limits of the integration that describe the translation of the given curve thru space do not exist), then, the locus that I had just arbitrarily described may be considered to have a Chern-Simmons singularity.  If the prior mentioned limits of integration may only be described with imaginary numbers that are within the degrees of freedom that exist in terms of the number of dimensions that are associating with the either timeless or timewise translation of the given curvature through space, then, one may still determine that the curvature is Ward hermitian in accordance with the Ward Caucy bounds of that given subspace.
Now, if a given curvature bears three or more dimensions of the prior type of singularity in terms of three or more derivatives that bear limits that do not exist in-between to loci that are relatively neighboring in a tight locus of subspace, then, the inter-relationship between the two eigenloci mentioned is considerd to be spurious for even p-fields.
Spurious cusps where there is such a perturbation in the delineation of singularities over a relatively small locus of field translation always only allow for a purely Chern-Simmons redistribution in the field that interconnects the eigenfields that I was describing.  Such purely Chern-Simmons boundary conditions, since these are spurious by forming a trilateral cusp, are never spontaneously partially hermitian until there is a Gliossi perturbation that alters the described arbitrarily tight locus where the associated critical cusp is localized at.  Such Chern-Simmons conditions that I mentioned before form a non-trivially assymetric abelian geometric substringular field  that will just about alway only have a chance to be altered by either a Campbell Projection, a Hausendorf Projection, or, a Campbell- Hausendorf Projection.  I will continue with the suspense later!  Until then, have a wonderfull day, and please pray for world peace.  Sincerely, Sam.                                              

A Little Bit of Knowledge To Correct A Possible Mistake

I am not sure whether I mistakenly said otherwise, or, if I said what I am about to say in the correct manner.                      
Superstrings that are discrete units of energy permittivity, in order to be able to have hermitian flow and field fluctuation, must be comprised of first-ordered point particles that are smoothly adjacent and without segments EXCEPT for one partition in one dimensional superstrings -- one separation of a first-ordered point particle from its normal Laplacian condition of linearity, &, two partitions in two-dimensional superstrings -- two separations of two different first-ordered point particles from their nomal Laplacian flow, the flow of which is used to form a closed string.  If it were not for the "partitions", or separations of space-time-fabric that is minimally dilineated at the immediate side of where the theoretical normal flow of first-ordered point particles would exist in a Laplacian setting during any arbitrary instanton, the radial and spin-orbital vibrations of superstrings would not be able to bear the hermitian harmonics that are necessary for superstrings to vibrate so as to form the bases of various types of energy.  Or, in other words, the one discrepancy in one-d strings and the two discrepancies in two-d strings allow for the prior mentioned vibrations to occur without spontaneous damage to an arbitrarily local homotopy.  The condition of the distance traveled in one instanton is the full length of a one-d superstring, which makes some people think that a superstring is the smallest "thing."  Yet, if it were not for the particles that comprise superstrings and their fields -- as well as other "group actions" -- there would be no fields to interbind the described superstings.
So, superstrings are comprised of first-ordered point particles, stringular fields are comprised of second-ordered point particles on account of allowing for enough condensed oscillation to ebb to-and-fro, and, the second-ordered point particles must be comprised of third-ordered point patricles.  Since when thinking it becomes obvious that the phenomena that binds second-ordered point particles can not be first-ordered point particles, the smallest "group action" must be sub-mini-string that binds mini-string as well as binding the mentioned third-orderd point particles, while yet allowing for the ebb and flow of the holonomic substance of the third-ordered point particles that only reside during instanton in the Ward Neumman bounds of the locus where there are second-ordered point particles.                                                              

Session 10 of Course 9

Hello there world, this is Sam Roach here!  I hope that you enjoy the ensuing post!
Here's how the exchange between Real and Fock Spaces is Imaginary between Real and Fock superstrings:  As an example, the bottom of the bottom of point particles of Real-Based superstrings exchanges a little bit of mini-string to the top of the bottom point particles of a Fock strings point particles in a sinusoidal manner, lifting the Fock strings mentioned to a certain gauged distance.  This also goes for all of the first-ordered point particles that comprise Real and Fock-based superstrings. The superstrings then lower due to the added phenomena.  Once this is done, the botom of the bottom mentioned Fock string's point particles exchanges a little bit of mini-string to the top of the bottom point particles of Real strings in a sinusoidal manner, raising the Real strings to the same extent that the Fock strings were originally raised.  Agian, this also goes for all of the first-ordered point particles that comprise the arbitrarily mentioned superstirngs.  The strings then lower due to the added phenomena that I have been describing here.  This happens with superstrings during the course of what is known as BRST.  This helps settle the "dance" of the Planc phenomena that these strings are connected to by light-cone-gauge eigenstates via mini-string segments.  This exchange is Imaginary since the mini-string segments' ( exchange that happens between the point particles of the Real and Fock stringular counterparts) happens at the opposite ends of the point particles, causing the exchange to be off of the Real Reimmanian plane that is subtended between the point particles of the Real and Fock Strings.  Before the Imaginary Exchange, the Real Reimmanian-based superstrings' (as compared with their counterparts) point particles are just over half condensed oscillation, and the Fock strings' point particles are just under half full.  During the first Imaginary exchange under the condition of a superconformally invariant setting, both the Real and the Fock-related superstrings are half condensed oscillation.  After the Imaginary exchange of the given iteration (which is the duration during instanton),  the Real strings' point particles are just over half conesnsed oscillation, and, the Fock strings' point particles are just under half full.  So, even though a first-ordered point particle always has the same total locus of volume, the degree to which it is filled is defined by the density of the mini-string that comprises a said first-ordered point particle.  For instance, a just over half-filled point particle of the first order is just over 50 percent of the maximum density that second-ordered point particles -- in the context of mini-string -- can possibly fill the associated volume that a first-ordered point particle tends to have.  Yet, a just under half-filled point particles of the first order is just under 50 percent of the maximum density that second-ordered point particles -- in the context of mini-string -- can possibly fill the associated volume that a first-ordered point particle tends to have.  The relatively Laplacian-based degree of what I call point-fill here refers to a non-time oriented perspective as to the density of mini-string while it exists in the Neumman bounds of the locus where a first-ordered point particle is existing ( the density of such in one "snapshot" of duration).                      

Session 9 of Course 9

A dilaton is a quantum of phenomena that comprises gravity.  A graviton is a quantum of transversal gravity.  A gravitino is a quantum of radial  gravity.  Perturbations in the metrical directoralizaation of gravitons and gravitinos are examples of space-time-related spurious operations.  World-Sheet-related spurious operations are characterized by perturbations in the transversal and radial propagations of superstrings.  Anharmonic differentiation in the radial actions of strings during the general Ultimon metric, coupled with the anharmonic differentiation of norm-states that act upon these strings, are spurious -- and such a spurious operation acts to redelineate the spacial transfiguration of the surrounding gravitons and gravitinos.  When spurious states quantize and propagate in a differentiating Hilbert Fock Space -- after countless iterations of instanton -- in the threshold of a given tori-sector-range that is multiplicitly delineated in an arbitrary region, are initially made taut (the abelian geometry will here involve a more directly Gliossi tangency) relative to one another -- while the consequence of such an arbitrary Fourier Transformation is that the described superstrings are then sucked into a quantum of dilatons and dilitinos that are inactivated by the prior tadpole-related group action.  The pull of the mentioned dilatons and dilatinos, coupled by the described spurious operation of the mentioned tadpoles upon the either Yang-Mills or Kaluza-Klein topological surface (such a surface that the given activity acts upon may holonomically be, in and of itself, either abelian or non-abelian in terms of the topological geometry of its wave-tug through a given arbitrary Lagrangian over the course of an arbitrary Fourier Transformation that is occuring in the region, that may be arbitrarily perceived within a relatively limited locus) that may be metrically described as existing within a Majorana-Weyl tense of conformal invariance.  Such a metrically-based Majorana-Weyl-associated topological interaction of the described superstrings of the given tori-sector-range, when dangerous tadpoles increase in terms of the frequency of their summed Hodge-Indices, may fray the substrigular fabric of the given tori-sector-range in its multiplicitly delineated region to form a black-hole.  Meanwhile, the space-hole eigenstates of the other tori-sector-ranges of the Overall-Space-Time-Continuum reconnect their topologically-ordered eigenstates so that the operation of Cassimer Invariance may keep the here associated superstrings that are left into a more consolidated network that lets the existence of pre-existing black-holes to fray to some extent the phenomena of their regions.  This consolidation transfigures after each iteration of instanton in which phenomena is brought into the mentioned black-holes.  Such tranfigurations is allowed by the resettling mode of the space-hole via Cassimer Invariance before each instanton-quaternionic-field-impulse-mode.
Black-Holes may be elliminated in a fashion that alters these into a harmonic substance that is composed of homogeneous sets of kinematically covariant inter-relations of Campbell and Hausendorf Projections that still allow star and planetary cycling that does not eat up the mentioned stars and planets.  This mentioned operation also works to allow the assymetric radial and spin-orbital motion of galaxies in such a manner so that space-time-fabric will here no longer need to expand or contract.  The manner of such conversion I will not put on  the Internet no matter what!!!  Sincerely, Samuel David Roach.                                                     

About Benign Tadpoles and Cyclic Permutations

Zero-Norm-States are benign tadpoles, in the context of what is termed of as "tadpoles" in stringular physics.                                  
Zero-Norm-States operate to help close open strings and to open closed strings.
Although theoretically point particles are parabollic and spherical, the torsion that occurs to these makes these exist in a condition of having a relatively elliptical shape over the course of the Fourier Transformations that happen in multiplicit directoralizations to first, second, and third ordered point particles over any framework that involves gauge-metrics and/or time.  Since point particles are multiplicitly bound by many wave-tug holonomic field eigenstates, the torsion that occurs here involves sets of permutations upon the Gliossi structure of point particles.  When such permutations occur over a Fourier Transformation that tends to converge the sequential series as to the morphology and topologically hermitiatn and/or Chern Simmons Neumman Ward boundaries that work to define the construction of the general locus of a superstring, then, one may describe such a convergent series of the pattern of delineations that happen to such an arbitrary point particle over the Translaton of metrics and/or time that describes the torsioned motion of the said strings through an arbitrary Lagrangian as a cyclic permuatation. When a superstring exists in a relative state of conformal invariance, then the sequential series of the topological holonomic permutation pattern -- in terms of the pattern as to the convergent alterations in the topological surface of the point particles that comprise such a superstring -- is more likely to have hermitian cyclic permutations that tend to kinematically differentiate on the relative Real Reimmanian Plane.  Yet, whenever there is a Chern Simmons perturbation in the relatve directoralization of a superstring through a Lagrangian via a Fourier Series that involves a spurious Rham associated and/or a spurious Doubolt cohomoligical covariant integrable kinematic differentiation, then the permutations that operate upon the point particles that comprise the said superstrings tends to not converge with any Yau-Exact basis into what would otherwise be a definitive cyclic permuatation.  When the permutations that operate upon a point particle are not spontaneously cyclic, then, over the course of the neighboring Gaussian Transformations that differentiate through time in a relatively local region near such a spurious alteration in the pattern of the wave-tug delineations that occur upon the point particles that comprise a given superstrings will eventually bring the superstring back into a conditon to where the point particles that comprise such a string will rgain a convergent pattern as to the metrical and Lagrangian based kinematic delineation of its permutations.  Such a condition of regaining a convergent pattern of cyclic permutations is more likely under the conditions of a relatively conformal invariant operation.  So, all point particles bear permutations on account of the wave-tug applied to these, yet, such permutations are only cyclic in a convergent tense in terms of a smooth translation of an even metrical function that transpires over a discrete set of instantons when the associated superstirngs bear at least some sort of conformal invariance.  From a broader perspective, there is generally a tense of convergent to divergent and back to convergent pattern involved with the topological delineation of the permutations that are distibuted upon the outer Gliossi surface of point particls.  In this broader perspective, the pattern of the operation of permutations is, in a reverse-fractored way, always based on an even metrical function whose Hamiltonian operation defines such permutations as relatively cyclic.    I will continue with the suspense later.  Sincerely, Sam.                                                                    

A Little Bit About Ghost Anomalies

The ghost anomalies that are created and not elliminated from within the Real Reimmanian Plane of an arbitrary substringular setting often exchange places in terms of relative Laplacian settings with the Neilson-Collosh ghost anomalies that are Njenhuis to the arbitrary mentioned Real Reimmanian Plane.
Generally, the ghosts that are formed in the Real mentioned plane are elliminated by reverse-holomorphic norm-states that scatter the configurations of general physical memory that are temporarily formed by forward-holomorphic norm-states.  The same general tendancy exists also for the Neilson-Collosh ghosts that are formed in the corresponingly Njenhuis Plane where gravitational particles differentiate through the multiplicit Fourier-based Lagrangians that are necessary for the continued existence of the Ricci Scalar that exists due to the activity of the Rarita Structure.  Yet, when ghost anomalies that are covariantly Njenhuis relative to one another, as is the case for regular substringular ghosts versus their corresponding gravitationally-based ghosts, are not spontaneously elliminated so that there may be enough freedom of motion for superstrings to differentiate in a Fourier manner, these relatively Njenhuis ghosts exchange where these differentiate in terms of the norm-based Ricci Scalar Njenhuis Laplacian settings in such a manner so that such arbitrary ghost anomalies may be scattered so that there may be sufficient room for superstrings to differentiate over a sequential series of Fourier Translation.  Although the conditions of such a displacement is like a snapshot of covariant displacement, the activity of such a displacement is a relatively brief Fourier Transformation that is needed.  The scattering of ghost anomalies facilitates the motion of Hausendorf Projections to differentiate through the multiplicit Fourier Lagrangians that are necessary for the activity of an arbitrary Hausendorf Projection that is known as the Wick Action.  The Wick Action is created by the metrical activity of gluons.  The Wick Action indirectly causes the type of translation of the Higgs Action that is needed so that the Klein Bottle may be displaced so that the Kaeler-Metric may happen so that Gaussian Transformations may happen.  The activity of Gaussian Transformations thence allows for the spontaneous alterations of norm-conditions that are necessary so that Fourier Transformatons may be kinematic in their loci, and the prior allows for the necessary interchanges that allow for energy to be perpetual period.  Also, Gaussian Transformations are necessary for superstrings and their field trajectories to retain their respectice discrete energy permittivity and discrete energy impedance.  Gauge-Transformations, which are a fundamental form of a Gaussian Transformations, are needed in order for the switching of abelian conditions that are necessary in order for the scattering of electromagnetic energy to continue in any way that is feasible given the present conditons of space-time fabric.  Gauge-Transformations are also neede for the existence of entropy, and entropy is needed in order for there to be any change in physical states.
Thank you for your time.  Sincerely, Sam Roach.                                         

Some Remedial Work

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Whether Something is Fourier or Laplacian Based

A Fourier Transformation is time based, while a Laplacian Transformation is not time-based. Discrete units of time are not the smallest metrics, though. Duration that is smaller than a discrete unit of time is known as a gauge-metric. So, even though a gauge-metric involves kinematic activity that occurs during the course of either an instanton or during the course of Ultimon Flow that is not during an instanton, such activity is considered to be -- in a sense -- a transpiring that is to happen over a Laplacian Transformation, since such activity happens within a discrete unit of time. Fourier Transformations always involve at least two or more instantons -- no matter how you fractor the associated transformation. In Newtonian mechanics, a Laplacian Transformation may involve many instantons that, even together, considering the scenario, are relatively non-time-oriented. So, for the most part, what is considered Fourier (time-oriented) or what is considered Laplacian (non-time-oriented) is relative to the scenario that one is considering. Yet, non the less, any differentiation that happens within an instanton, is, in a real sense, of the nature of a Laplacian Transformation. So, even though gauge-metrics are of sub-time, understanding their activity is quintessential to understanding the relativistic mechanics that underline the activity of the light-cone-gauge. Whithout the light-cone-gauge, E(6)XE(6) strings would be unable to form Schwinger Indices. Without Schwinger Indices, the Rarita Structure would not vibrate -- causing gravity to not take effect via the Ricci Scalar. Without gravity, everything would fly apart and there would be nothing.                 

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