A Tad-Bit More About Ghosts

A two-dimensional superstrings is resting in this case to all relatively Laplacian-based "appearances" in a differentiably integrable region in which it has iterated may times over a relatively tightly-knit Fourier-Transform.  The corresponding positive-norm-states here work to form a ghost anomalic region at the locus of the eigenbasis of the toroidal Jacobi that here work to define the related field of the angular momentum of the said two-dimensional superstring.  A set of zero-norm-states, acting as a projection, after a certain number of instantons, works to open the related toroidal eigenbasis so as to open the corresponding elluded to region up as a cylindrical shaft that is relatively thick.  After the said zero-norm-state projection do their work, the corresponding negative-norm-states work to orphoganate the related positive-norm-conditions that were previously existant in the described locus so as to elliminate the ghost anomalic eigenindices that had been mapped prior to the occurance of the mentioned scattering of ghost anomalies.  This ellimination works to scatter the related point commutators that had integrated to form the mentioned ghost anomalic eigenlocus so as to allowl a path for the operation of the incoming world-sheets, as well as to allow for a path for the other substringular fields that are also incoming.  Mobius-based ghosts are elliminated in the same general fashion, yet, such ellimination here involves more overall norm-states, and, thus, such ellimination involves a more prolonged Fourier Transform.  (It takes a duration of more instantons to elliminate these.) Such ghosts are elliminated at the critical cusps of the fold of the corresponding Mobius-based ghosts.  Two-Dimensional stringular world-sheets have ghost anomalic residue that is elliminated at multiple spots by both zero-norm-states and positive-norm-states.  Zero-Norm-States work to open the associated ghost anomalic eigenbasis at four general loci per codifferentiable pulse in which such a general activity occurs.  The said positive-norm-states work to alter the Gaussian conditions of the said corresponding negative-norm-states in order to supplement the field that was previously operated on by the succession of the kinematic activity of the two-dimensional field that we are discussing in this case.  This said supplementation works to clear what had just been a ghost anomalic field by scattering the said two-dimensional field's eigenbasis.  This kinematic activity works to open the described general overall locus in order for such a locus to remain as an operand for further substringular Fourier codifferentiation.  Sincerely, Sam.

A Little Bit Of Remedial Knowledge To Clarify Course Nine

For every one-dimensional superstring, there are many two-dimensional superstrings.  So, when an electron forms a photon, a phenomenon with more one-dimensional superstrings directly inter-related with it than the two-dimensional superstrings that are directly inter-related with it -- an electron -- forms a phenomenon that is purely bosonic (consisting of one two-dimensional superstring) known of as a photon.  Nuclei tend to have more two-dimensional superstrings than one-dimensional strings on account of the condition that nuclei tend to bear much less pure kinetic energy than electrons -- particularly for their mass.  Superstrings may open, and superstrings may shut -- depending on the particular arbitrary scenario that is at hand.  Zero-Norm states (loose first-ordererd point particles) are what open or shut a superstring.  First-Ordered-Point-Particles that form a line of tangency with a planar-like-disc that consists of multiple first-ordered-point-particles are Campbell-Norm-States.  First-Ordered-Point-Particle configurations that form the substrate of tangency that physically comprise ghost anomalies are the positive-norm-states.  First-Ordered-Point-Particle configurations that scatter positive-norm-states are negative-norm-states.  Norm-States are a phenomena that exist in what is known of as the general region of Fock Space.  Line tangency forms ghost anomalies via the initial Laplacian-Like redistribution of the positve-norm-states that are moving in the relatively holomorphic direction that the associated superstrings move in during the statics of the trajectoral mapping as to where given superstrings had just iterated in in any arbitrary prior sequential series of substringular delineations that mark where superstrings had existed at over a given arbitrary set of progressive instantons.  The relatively reverse holomorphic norm-states that scatter those mapped out distributions that indicate where superstrings had iterated over a sequential series of instantons are known of as negative-norm-states.  The propagation of ghost anomalies that are formed, as well as the propagation of ghost anomalies that are scattered into a residue that undoes the physical mapping as to the trajectory where the corresponding superstrings had just iterated in an arbitrarily prior sequential series of instantons, helps to pull the related superstrings thru those operands that are either in need of the pseudo-field that ghost anomalies may form, while yet, also helping to pull the related superstrings thru those operands that need to be less crouded by the physical entities of the ghost anomalies, respecively.  This causes the potential for tadpoles when gauge-transformations go rampant over the associated entropy that would likewise happen over a relatively long period of time where there is a black-body that bears a lot of mass.  The scattering of positive-norm-states happens via the motion of negative-norm-states striking the conicenter of the associated positive-norm-states in an anharmonically metrical manner at a Ward-Based "global" angle that is based on the Real Reimmanian concept of a 45 degree relativistic strike.  The more dimensions that the said norm-states are kinematically differentiating in during the scattering, the more Njenhuis that the Gliossi impact of the "45 degree" strike bears in terms of the torsion of the basis of contact that causes the mentioned scattering.  The more Njenhuis the basis of contact is, the more anharmonic the metrical vibration of the scattering is.  "Tadpoles" need to be used quite often over billions of years to have much effect in terms of the endagerment of adjacent phenomena. -- A star must be very old in order to have a high probability of forming a black-hole.  Tadpoles happen when two-dimensional superstring-associated fields are made spurious after basically countless instantons.  Such a spuriousness is increased when two-dimensional superstrings have iterated thru a common set of paths that involve a high degree of entropy too many times over an astronomical age.  This is because the just mentioned activity works to weaken the fractal and elastic condition of superstrings during the ensuing metrics of the "space-hole."  The space-hole is designed to be able to realign the path operand of its affiliated world-sheets, if at all possible.  World-Sheets are spatially differentiated by  physical energy, and also potentially to an extent by thought energy.  Such thought energy may help to cause the proper covariance of the delineation of superstrings to a slight extent by altering the paths of certain arbitrary given superstrings so that entropy may be minimized enough to prevent the excess build-up of the mentioned "tadpoles."  This helpfull general activity would allow for life to differentiate in such a manner so as to adapt to an aging universe.
Life is the most important thing.  Sincerely, Samuel David Roach.           

Part Four of the Fourteenth Session of Course Six

Well hello again world, this is Samuel David Roach here!  Happy to be back!  Here we go!

               
Superstring-related ground-states that are indistinguishably different through a successive series of iterations, when not considering alterations in metric-gauge quanta and exterialized filled permutations by the related Fourier Transformations that happen to the given ground-states in the delineatory translation of the given ground-states in the course of their redistribution through the multiplicit operand of space, are superstrings that are detectable as relating to light matter and light energy.  (These are the illuminated superstrings.)  Superstring-related ground-states that are distinguishably different, through a successive series of iterations, in terms of the permutations that are Gliossi to the holonomic structure of the described superstrings over the related Fourier Transformations, that happen to the ground-states in the delineatory translation of the given ground-states in the course of their redistribution through the multiplicit operands of space, are superstrings that are detectable as relating to dark matter and dark energy.  Exterialized field permutations here are alterations in the fields that surround superstrings, yet are not appertaining to the topological Laplacian mapping of the here mentioned superstrings themselves, while permutations that are Gliossi to the holonomic structure of the described superstrings are alterations in the topological Laplacian mapping of the here mentioned superstrings themselves -- whether the exterialized fields appertaining to the associated superstrings here may or may not be altered in terms of the mini-string interactions in a Fourier tense, or altered in terms of the mini-string relativistic delineations as taken in a Laplacian tense.  Because I love the Human Race!
Sincerely, Sam Roach.                                                                                                          

Part One Of Session Ten Of Course Six

Well hello again world, this is Sam Roach here to provide you with another session on the sixth course that I had written the gist of back in 2002.  This course is about the toroidal nature of superstrings.
               
How does the flow of the point particles of all of the tori-sector-ranges, taken as a whole, fit together?
Some of the tori-sector-ranges within the Ultimon, at any given instant in-between individual durations of instanton, are flowing faster than others, and some of the tori-sector-ranges within the Ultimon are traveling slower than others at any given instant in-between individual durations of instantons.  There are many tori-sector-ranges within the Ultimon that are going through their transversal and radial propagations within their eigen operands, or, in other words, these ranges are flowing at such a rate so exactly similar that you may as well say that their flow is at the exact same rate with no significant differences here.  What allows the differences in the flow rates of these tori-sector-ranges relative to one another while still allowing for a smoothly running Ultimon and thereby a smoothly running Continuum?  Forward time momentum ironically moves relatively counterclockwise or, in other words holomoriphically, through the Ultimon.  Substringular encoders for forward moving time exist in a different "hoop" than that of substringular encoders of backward moving time.  Clocks move relatively clockwise.  Let's say that that a particular tori-sector-range flowed slower than average.  Several tori-sector-ranges "behind" it were moving faster than what here would be deemed as an average rate.  The tori-sector-ranges would gradually slow down to the rate of the slower tori-sector-range that was relatively holomoriphically positioned ahead of the said range for forward moving time ore positioned relatively antiholomoriphically ahead of the mentioned range for backward moving time.  Tori-Sector-Range flow rate a is almost instantaneous in-between the durations of instanton eigenmetrics, and instantons are the smallest units of discrete time that we may normally detect, since instantons are discrete units of organized duration.  Ultimon cycle is in about 10^(-43)I seconds, so, tori-sector-range flow does not differ in duration over the course of our Continuum by any significant degree spontaneously -- although instanton has slowed mildly since the "Big-Bang."  So, the differences in the rates of any tori-sector-ranges when taken in a covariant Laplacian manner in-between two specific eigenstates of instanton are always within a googleth of an imaginary second of Sub-Fourier Translation in terms of the group velocity of the individual of such ranges correlative to one another.  This means that that all of the action of the Continuum is defined in the substringular in what we may conceive of as the integration of both all of organized and unorganized time.  What I just stated here is the summation of all of the instantons plus the summation of all of the Ultimon flows that occur in-between the described instantons -- So, physical time equals the summation of all Real and Imaginary Time.  Imaginary Time is the summation of all of the gauge-metrics that occur in such a relatively disorganized manner in that we as people are not generally able to percieve of the eigenstates and the sub-eigenstates that transpire during such an unnoticed set of durations.  We as people are only able to detect time -- for all practical purposes -- when the superstrings that make up discrete units of energy permittivity are organized according to the Ward Laplacian conditions that are affiliated within their conformal dimensions.  One-dimensional superstrings have a basis of a conformal dimension of one while two-dimensional superstrings have a basis of a conformal dimension of two.  The condition of the organization of conformal dimension is based on the Laplacian mapping out of the associated hermicity that each superstring bears both individuallyand multiplictly during instanton while also simultaneously groupwise in terms of the iteration and the reiteration of all of the unfrayed superstrings that exist after instanton-quaternionic-field-impulse-mode on account of the fact that all unfrayed superstrings go through instanton simultaneously on account of the sub-metric that happens instantaneously in terms of a multiplicity terrestrial manner of determining the gauging of the metrics of the substringular.  I will continue with the suspense later!  I appologize that it is impossible  to describe everything about string theory in a few words without indicating all of the exceptions while still providing a vividly clear meaning as to what I mean.  I thank you for your reading time!
Have a phenomenal day!  Sincerely, Sam.