Regional Nodes Of Mini-String-Related Segmentation

 Regional nodes of mini-string-related segmentation that are hyperbolically approached, most appertain to the multiplicity of the cotangent bundle of discrete energy quanta; however, -- regional nodes of mini-string-related segmentation that are approached in a euclidean manner, most appertain to the multiplicity of the cotangent bundle of those physical norm-state-projections (either zero-norm-state-projections, Campbell norm-state-projections, Campbell-Hausendorf norm-state-projections, and/or Hausendorf norm-state-projections), that are here to make a direct contact with the core-field-density of discrete energy quanta, in order to work to form that general tense of cohomology, -- of which is to reverse-fractal into physical charge, so that the physical processes of adhesion and cohesion may be facilitated into the possibility of both existing and persisting. I will continue with the suspense later! To Be Continued Soon! Sincerely, Samuel David Roach.

Mini-Stringular Segmentation And First-Ordered Point Particles

Mini-Stringular segmentation is drawn into nodes -- in a multiplicit manner, in so as to work to form what may be termed of here as being the essence of first-ordered point particles.  First-Ordered point particles come together as building blocks of the topological stratum of discrete energy permittivity, in so as to work at helping to form both superstrings of discrete energy permittivity, as well as these said superstrings' counter parts.  First-Ordered point particles are also existent, in so as to work to help at forming part of the topological stratum of norm-state-projections.  These node-like holonomic substrate-based phenomenology, of what I have just termed of here as being first-ordered point particles, come in the form of a parabolic-shaped twining of mini-stringular segmentation, -- of which is utilized, in so as to work at forming that level of Ward-Cauchy-related building blocks, -- that exist multiplicitly at one level of the holonomic substrate of topological stratum that is below the composition of discrete energy itself.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Cohomologies, Ghosts, And Distortions, Part One

Remember back at the condition that I have mentioned in the past -- that the projection of the trajectory of a substringular phenomenology is a world-sheet.  The mappable-tracing of a world-sheet is a cohomology.  That manner of considering a cohomology -- to where this may be viewed of as a relatively transient phenomenology, that is generally not to be apprehended -- is a ghost anomaly.  Cohomologies are initially harmonically scattered into place, via a correlative Reimmanian scattering, into a set of norm-state-projections -- that work in so as to help at indicating the physical memory of both the where, the how, and the when, that any particular given arbitrary respective substringular phenomenon had physically differentiated -- over any correlative proscribed sequential series of instantons.  The initiation of such a general genus of Reimmanian-based scattering, works to form a harmonic perturbation of those norm-state-projections, that had just been in the Lagrangian-based path of that Ward-Cauchy-related phenomenology, that is here to be forming an integrable set of cohomological eigenindices, as a set of Hamiltonian operand-related eigenstates, -- in so as to work to form a Wess-Zumino distortion of those point commutators that had eminently been in the path of the said substringular phenomenology, that had just formed the said cohomology.  Such a general genus of a Wess-Zumino distortion, is here to be formed by a set of relatively forward-holomorphic tending norm-state-projections -- that are here to have come into contact with that Ward-Cauchy-based phenomenology, that is here to form the so-eluded-to set of the so-stated physical memories.   I will get to the topic, as to the conditions that are related to those Cevita distortions of point particle-related motion -- soon.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

More As to The Idea Behind Substringular Recycling

Mini-Stringular segmentation is a general genus of phenomenology -- that is constantly being fed both into and out of both superstrings, first-ordered point particles, norm-state-projections, along with such a general genus of phenomenology as well as also being fed into other Ward-Cauchy-related phenomenology.   Such a constant re-distribution of mini-stringular segmentation, is part of what works to recycle substringular ground-states to norm-states -- and vice-versa.  Mini-Stringular segmentation is both: what works to form the holonomic substrate of substringular fields, what works to form the "yarning" of first-ordered point particles, what works to form zero-point-energy, etc... .  As far as I can currently surmise, the smallest phenomenology that can be divied-out, is on the order of mini-stringular segmentation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Part Two of Session Four of Course 19 -- The Klein Bottle and Orbifold Differentiation

The interior of the cohomological-based pattern that is formed by any respective given arbitrary Klein Bottle --is like a limited contorted "toroid" that contains both forward-holomormphic and reverse-holomorphic-based norm-states.  These multivarious norm-states of which tend to differentiate in a Fourier-based manner that is of a relatively harmonic manner, over time.  Yet, when the interaction of the norm-states, that exist from within the Ward-Neumman boundaries of the interior of the holonomic substrate of any respective given arbitrary Klein Bottle eigenstate, act in so as to differentiate kinematically in a relatively rigorous  annharmonic manner over time, the cohomological-based pattern that is formed by both the existence and the activity of the so-stated given arbitrary Klein Bottle eigenstate, eventually is perturbated into a Rayleigh-based scattering of those norm-state indices that had previously existed within the Ward-Caucy bounds of the said Kliein Bottle eigenstate.  This just mentioned general genus of activity of which may often cause the composition of the specific respective given arbitrary Klein Bottle eigenstate to be indistinguishably replaced, via those immediately surrounding eigenindices that may here work to both antiderivate the previous Klein Bottle eigenstate, while yet re-constructing a newly established Klein Bottle-based construction -- in a manner that works to bear a tendency of an indistinguishable difference.  This just-eluded-to recycling-based tendency of a "worn-out" Klein Bottle eigenstate into a newly established so-stated Klein Bottle eigenstate, works to conform to the overall tendency -- that is directly affiliated with the recycling of norm-state-projections, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

Different General Formats of Ghost-Based Scattering

When any given arbitrary cohomological setting is scattered from its initial Reimman-based configuration, into a relatively annharmonic dissaray -- this so-stated condition of dissaray, of which would here be due to the activity of a Rayleigh scattering of the here just eluded-to ghost-based configuration, in which this happens to where this said general genus of a scattering of ghost anomalies -- of which annharmonically work to scatter a set physical memories of both the existence and the activity of the projection of the trajectory of either a superstring, an orbifold, and/or an orbifold eigenset into a residue of norm-based projections, this will happen to where these will here then be moved into an ensuing stage of the recycling of ghost-based indices.  The previously mentioned helicit-based torque that is applied to the motion of any given respective arbitrary orbifold eigenset -- of which is caused by the re-positioning of the correlative gauge-bosons, in the manner of a directly corresponding re-delineation of the differential angling of the so-stated gauge bosons (E(6) X E(6) stings), will here tend to be a major factor in the reason as to the why and the how as to the bringing-in of relatively reverse-holomorphic norm-state-projections upon a relatively forward-holomorphic Reimman-based configuration -- to where a respective given arbitrary cohomological setting is then scattered by a Rayleigh-based scattering, which, in effect, will here then work to form a dissaray of the initial ghost-based scattering that I have been reffering to in this post.  If the re-distribution of the angling re-delineation of the differential geometry of the correlative respective gauge-bosons that would directly apply to this case, are pulled into the here just eluded-to perturbative-based re-delineation of the said E(6) X E(6) strings, as such said gauge-bosons are altered in the differential geometry of as to the genus of their Gliossi-based wave-tug/wave-pull that these imbue upon their respective given arbitrary second-ordered light-cone-gauge eignstates -- that these "pluck" during a state of a consecutively sequential series of group-related instantons, over time, in a relatively acutely-based  Ward-Caucy-involved manner, then, the scattering of the said cohomology will then here tend to be of a relatively conical-based kinematic differentially geometric manner, yet, if the re-distribution of the angling re-delineation of the differential geometry of the correlative respective gauge-bosons that wold directly apply to this case, are pulled into the here just eluded-to perturbative-based re-delineation of the said E(6) X E(6) strings, as such said gauge-bosons are altered in the differential geometry of as to the genus of their Gliossi-based wave-tug/wave-pull that these imbue upon their respective given arbitrary second-ordered light-cone-gauge eigenstates that these "pluck" during a state of a consecutively sequential series of group-related instantons, over time, in a relatively obtusely-based Ward-Caucy-involved manner, then, the scattering of the said cohomology will then here tend to be of a relatively toroidal-based kinematic differential geometric manner.

Part Three of the Interim Between Course 17 and Course 18

The condition of the recycling of ground-states converting into norm-states and vice-versa works to cause a flow of the directly corresponding indices -- these indices of which move in such a manner in so as to reach a relative center-state, which localizes toward the activity of that permittivity which exists as to where the correlative ground-states are most prime.  Meanwhile, the correlative norm-state-based associations work to cause Real-based first-ordered point particles to be over half of being fully compactified -- while at the same general genus of metric, working to make the correlative Fock-based states to be less than half of being fully compactified.  This is because the directly associated covariant differential geometries that work to correlate the so-stated ground-states with the so-stated norm-states works to allow for a more "ionic" distribuation of condensed oscillation, -- even though any viable wave distribution must bear a certain level of quantum-based state of conservation, over the course of space and time.  This works to make a condition of indistinguishable replacement, as to the conformally invariant manner of the maintanence of those ground-based states that work to comprise any give arbitrary superstring of discrete energy permittivity.  This process of the recycling of ground and norm states -- the one general genus of state to the other and vice-versa, pertpetually -- works to involve from one relatively Real-based state to many Fock-based states, to vice versa, over the eigenbase of certain of those gauge-metrics that are most activated over the generally reiterative metrical-based activities that happen during the generally unnoticed durations of Ultimon Flow.  This acts as if a given arbitrary respective set of substringular globalizations were to be exerted upon the directly corresponding net field impulse range -- and thus, part of the reason as to why I call a layer of reality that is to exist from within a set of parallel universes as being termed of as a tori-sector-range.  I will continue with the suspense later!  To be Continued!  Sincerely, Sam.

The Fifth Part of the Interim Between Sessions 13 and 14 of Course 17

When in terms of the Chi-shaped Trace of any given arbitrary Basis of Light -- as such a Basis is existent in the manner of which it is in, during the part of the generally unnoticed portion of Ultimon Flow that happens right before the quaternionic-instanton-field-impulse mode, in which the space-hole is kineamtically Gliossi to the so-eluded-to substringular activity -- the general locus as to where collected ground-state-based mini-string segments are most richly delineated, in the process of their indistingiuisably conversion into norm-states -- works to form the general designation as to where the so-stated Trace will topologically sway -- over the so-eluded-to course of gauge-metrical-based activity.  This is where the said Trace is momentarily fattened.  As norm-states recycle in different associated wave-tug locants, the directly associated ground-state quantum is relocalized -- putting the morphology of the correlative topological flow into a reiterative ensuing sequence of different local translation.  So, by nature of the so-stated Trace, morphological sways are always countered by the collective condition of each sub-group heterotopy -- as the covariant differential associations that work to define these, are propagated by the ongoing recycling.

More As to a Description of Topology in reference to Iterations

A zero-norm-state may often act as a benevalent "tadpole" -- by latching to the general cite of a world-sheet distributioin, by the Gliossi interaction of the directly corresponding zero-norm-state-projection with the general topological stratum of an operational stratum of cohesive ghost-based indices.  These so-stated indices of which work to function as a ghost-inhibitor-based group attractor that is to be facilitated as a counterpart Hamiltonian operation, in order to allow for the said operation of the so-eluded-to wholeistic ghost anomaly.  Here is a basic run-down as to how what I am implying works:  Positive-Norm-States form ghost anomalies at the cite of activity where a world-sheet had traversed -- the kinematic flow of the motion of superstrings works to displace those norm-states and norm-state-projections that are moving in the same general director eigenbase of Lagrangian flow as the so-stated superstrings.  Norm-States and norm-state-projections tend to iterate and reiterate in more of a tense of conformal invariance than whatever the local superstrings are bound to move in over a discret period of time in which the so-stated given arbitrary superstrings move in a sequential series of multiplicit instantons, in so that the resulting relatively mild collisions of the said superstring with the so-stated relatively forward-holomorphic norm-states and norm-state-projections works to form a physical memory as to the directly prior existence and activity of the said given arbitrary superstrings.  Although all superstrings and norm-state-projections move by either Noether Flow or tachyonic flow, the Noether-based flow of norm-state projections tends to be in more of a state of static equilibrium than the Noether-based flow of the immediately surrounding superstrings that cross their path, in the course of the eluded-to interaction of superstrings with norm-states.  This is why the world-sheets, which act as the trajectory of the projection of superstrings -- are the arena of the harmonic scattering of forward-holomorphic norm-states and norm-state-projections that work to form ghost anomalies.  With forward-moving-time-based motion, forward-holomorphic norm-states are positive-norm-states.  Norm-State-Projections are any given arbitrary group of operational physical indices of first-ordered-point-particles that operate to perform a specific function.  First-Ordered-Point-Particles are attached by mini-string.  The so-stated mini-string acts as the holonomic substrate of substringular core-field-density, and, mini-string works as that physical entity that forms homotopy by both directly and indirectly binding all unfrayed superstrings with each other over Ultimon Flow.   I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

Part Four of Session 12 of Course 14 About Group Action

The world-sheets of a superstring of discrete energy permittivity may be any of several various forms of paths, that work to map-out the physical memory of the trajectory of the said given arbitrary superstring over a period, or duration, of many iterations of instanton.  The length of a world-sheet may vary, based on both the number and the Hodge Volume of the directly corresponding ghost anomalies -- that are formed by the interaction of the said format of superstrings with forward-holomorphic-flowing-norm-states.  For superstrings that directly correspond to the forward-moving time-tense of motion, forward-holomorphic-flowing-norm-states are positive-norm-states.  The eluded to ghost anomalies that are thence formed act as a template of the extrapolatory-bases of the physical memory, as to the prior activity and existence of the related superstrings -- in the paths that the said superstrings kinematically differentiated in, per iteration of these superstrings.  This is as these form a sequential series of perturbations that work to facilitate the formation of  the viable energy of the Main-World-Tubes.  So, world-sheets of any superstrings of discrete energy permittivity, that are of any given arbitrary case -- end in their partial-based paths -- once a given arbitrary multiplicit set of superstrings diverge from a convergent set of trajectoral path-delineation, in so as to form a sequential set of respective path-based-trace singularities.  These singularities work to relate a set of redelineaetions of the bases of the eluded to Ward-Caucy-bounds of the said superstrings. This set of redelineatory-bases happen simultaneously through the vantage-point of a central conipoint.  This works to help cause the format of the said path-based-trace singularities, which will then diverge from the directly corresponding multiplicit limits of integration, in so as to then correspond to the eluded to perturbations of the directly correponding cohomologies that had exited amongst the world-sheets, directly prior to the mentioned completion of the activity of the formation of the respective world-sheets.  So, the world-sheets of all of the superstrings that are to be recycled, via the continual indistinguishably different redistribution of the intrinsic mini-string segments, over a sequential series of multiplicit inter-bound group metrical activity -- works to form the tractibility of the energy of the arena of the Overall-Physical-Space-Time-Continuum.
Sincerely, Samuel David Roach.

Manifolds of Superstrings That Act As Groups

The key to substringular phenomena moving together in sets or groups is the concept of orbifolds and orbifold eigensets. Superstrings tend to move together in groups that exist in membranes that may be described of as orbifolds. Orbifolds tend to exist in groups that may be described of as orbifold eigensets. Subatomic particles known of as quarks and leptons are comprised of certain basic orbifold eigensets. Such groups of membranes that are comprised of superstrings that work together for a common codifferentiable purpose act as sets of covariant interactive sets of substringular phenomena that work to fulfill their given respective operations. Often, in other cases, certain superstrings act to an extent alone in terms of an independant operator that is covariantly codifferentiable with its surrounding phenomena in order to fulfill a given arbitrary operation. Often, too, certain substringular phenomena other than superstrings work as sets in such a manner so as to fulfill other given arbitrary operations. Norm-States often tend to be comprised of multiple first-ordered point particles that work together as a group in order to permorm a certain operation. Norm-States often work in projections that operate as groups of norm-states that perform given arbitrary operations. Often, too, point commutators act in projections that behave as groups or sets of such said commutators in order to perform certain essential operations. All of the operations of the substringular act as a multiplicit covariantly codifferentiable group or set of smaller substringular phenomena that act in such a manner over time in such a fashion so that phenomena may coexist as a rather interconnected whole that allows the substringular to function. Enough for now.

Solutions To Test Two About Orbifolds

1)  An orbifold kernel is a region that exists in-between adjacent orbifolds that interconnect in a Gliossi manner.  Such a region exists as a relatively open gap that is basically free of substringular phenomena with the exception of mini-string segments and norm-states.

2)  An orbifold neighborhood is a general region that surrounds a given arbitrary orbifold, while yet directly involving the operation of the said given arbitrary orbifold mentioned.

3)  Ideally, an orbifold is shaped in either a parabollic, or, in an elliptical general format.

4)  Ideally, an orbifold kernel is shaped like a region that would involve adjacent assymptotes of tangency, with the exception that these are interconnected at their endpoints in a manner that is both Gliossi and also multidimensional.  Such a region gives a similar appearance of two "chocalette kisses" that are interconnected bottom-to-bottom with no gap or superfilous changes in concavity in-between these.

5)  Some orbifolds are other than either parabollic-shaped-based or elliptical-shaped-based.  Such alterior-shaped-orbifolds may be parallelopiped-shaped-based, pyramid-shaped-based, trapozoidal-shaped-based, or, even having other alterior-based-shapes.

6)  An orbifold permutation is a variation in the Laplacian-basis of the general topological construction of any given arbitrary orbifold.

7)  Some orbifold permutations may be pointal, some may be sherically-based in shape, some may be elliptically-based in shape, these may bear a triangular-basis in shape, a parabollic-basis of shape, a rectangular-basis of shape, a pyramid-basis of shape, or a trapezoidal-basis of shape.

8)  Orbifolds are connected as an anzantz by mini-string segments.  At more of a reverse-fractalled-tense, orbifolds are interconnected via E(8)XE(8) strings.  E(8)XE(8) strings work to interconnect orbifolds via their combination of spin-orbital and sway momentum indices and their combination of spin-orbital and sway momentum Hamiltonian operations,these of which occur over directly associated brief periods of time.

9)  Depending upon the placement of E(8)XE(8) strings over the course of their spin-orbital and sway Hamiltonian operations over time, such mentioned conditions may work to effect the associated conditions as to the delineation and the super-conformally-invariant motions of adjacent given arbitrary orbifolds.

10)  As time goes by in reference to an orbifold, the formats of both the Laplacian-based and the Fourier-based differential geometries of those permutations that exist along both the interior-based and the exterior-based topological permutations that correspond to a given arbitrary orbifold may either alter, vary, and/or exchange in their corresponding delineation(s).

Substringular Recycling

Substringular Recycling -- The indistinguishably different exchanging of the condensed oscillation of mini-string that allows for the indistinguishable exchanges of superstrings into norm-states that re-exchange back in an indistinguishable manner into superstrings and vice-versa.

The Next Part As To Stringular Encoders

Superstrings of the same universe are interconnected with the same general Planck-phenomena-basis of wobble, when in consideration of their codifferentiating covariant norm-conditions -- when this is considered over any given arbitrary viable Laplacian condition that involves a given arbitrary locus during instanton.  Such norm-conditions involve the most directly involved first-ordered point commutators, to where the said point commutators, of which exist as norm-states, are either zero-norm-states, Campbell-norm-states, Hausendorf-norm-states or, Campbell-Hausendorf-norm-states.  Stringular counterparts are interconnected with point particle counterparts that exist in the respective general locus of those point commutators that exist. as most directly interconnected with the directly prior mentioned stringular counterparts.  Stringular counterparts, during instanton, and when orientable with their corresponding superstrings, always exist in the forward-holomorphic directoralization -- when taken relative to the positioning of the corresponding superstrings.  Point commutators that are of positive-norm-states bear counterparts that tend to exist in the forward-holomorphic directoraliztation of the relative positioning of their corresponding point commutators.  Point commutators that are of negative-norm-states bear counterparts that tend to exist in the reverse-holomorphic directoralization of the relative positioning of their corresponding point commutators.  The relative positioning of the counterparts of zero-norm-state counterparts varies in the holomorphic directoralization-based-format as to where these are positioned, during instanton, reltative to their corresponding zero-norm-states.  This Laplacian generalization of tendancy is a condtion that works at tending to happen during instanton.  I will leave this short yet brief for now.
I will continue with the suspense later!  Sinererly, Samuel David Roach.

A Little More As To Common "Wobble"

When a black-hole forms, the directly associated Planck phenomena that initially enter the said black-hole belong to the universe that inolve those Planck phenomena that are normal to the frayed stringular topology by a wobble of 1.104735878*(-81)Idegrees.  Next, Planck phenomena enter the said black-hole that are normal to the frayed superstrings related Planck phenomena that are normal when in consideration of a relative wobble that exists within a factor of 9.1*10^6* the most discrete adjacent-based covariant wobble that exists among two arbitrary given Planck phenomena that are of the same universe.  Next, the tendancy is toward the motion in the direction of Planck phenomena to enter the mentioned black-hole that are off of normalcy -- in terms of adjacent covariant wobble -- by up to 91*10^81.  (Black-Holes are to never get to that point of potential danger, if one may be able to ward them off by then.)  While some of our universe is being eaten up by any given arbitrary black-hole that has existed for any noticable period of time-based duration, some parts of paralllel universes are eaten up by black-holes as well.  A black-hole is elliminated when the whole black-hole sector is filled in a manner that I will not describe.  Black-Hole sectors "try" to eat up the universe.  That is why these are unwanted.  Black-Holes fray substringular material.  Black-Holes are formed by accumulative dilation build-up that interacts with normal substringlar Fourier-based differentiation.  Dilatons are the massless set quantum of gravitational-based angular momentum energy.  Excessive dilaon accumulation exists after a star has collapsed.  Dilatons accumulate when ghost anomalies are not efficiently annhilated by negative-norm-states.   When two-dimensional superstrings have anharmonically differentiated in a Fourier-based manner too much in a relatively limited region, the corresponding negative-norm-states do not have the adequate opportunity to orphoganate the related norm-conditions that are formed by the related positive-norm-states.  Masses that exist for a relatively long time tend to undergo more entropy.  Entropy produces annharmonics of the corresponding substringular fabric.  Annharmonic stringular Fourier-based differentiation produces multiple zero-norm ghost states, since the zero-norm states cannot form Jacobian-based spatial tangents with the active surface of the directly related ghost anomalic eigenbases.  This lack of multiplicit cohesive parity puts world-sheet paths in the way of each other, in terms of what should become their Laplcacian-mapped paths.  This works to breaksup the related topology, and thus form black-holes.

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.

The Glossary That Goes To Courses Nine And Ten

1)  Substringular Real Residue -- Substringular residue that happens during BRST.  

2)  Substringular Imaginary Residue -- Substringular residue that happens during Ultimon Time.

3)  BRST -- Substringular activity that happens during that part of instanton when the Polyakov Action and the Bette Action are happening simultaneously.

4) Iteration -- The globally distinguishable noticeable pulses when the noticeable time known of as instanton happens.  

5)  Ultimon Time -- Time that happens in-between iterations.  Such time may be expressed by Imaginary Numbers.

6)  Real Exchange -- Substringular exchange that happens on the Real Reimmanian Plane.

7)  Imaginary Exchange -- Substringular exchange that happens off of the Real Reimmanian Plane.

8)  The Core Of BRST -- The Real Residue that is exchanged during the Imaginary Exchange, of which happens during BRST.

9)  The Light-Cone-Gauge -- The connections between Planck-Phenomena-Related phenomena and their corresponding superstrings.

10)  Fock Space -- Substringular phenomena that exists besides substrings, counterstrings, Planck-Phenomena-Related phenomena,  stringular encoders, stringular encoder counterparts, and heterotic strings.

11)  Gravity -- As a force that is weaker than the "strong" force as well as weaker than the electromagnetic force, gravity is that general category of phenomena that pulls phenomena into order so that the whole of phenomena may be able to inter-relate and codifferentiate through time.

12)  Dilatons -- Transversal indices that quantize to become transversal-based gravity.  These are formed by posivive-norm states that are scattered by negative-norm states that are "scraped" off of their respective world-sheets, such world-sheets being comprised of by Gliossi-Sherk-Olive-Ghosts, in such a manner in that these are moved off of the Real Reimmanian Plane to help in the formation of gravitational particles.

13)  Negative-Norm-States -- Antiholomorphic Fock Space that works to scatter world-sheet indices in such a manner so that the corresponding ghost anomalies that had directly before comprised the related world-sheets may be able to redistribute so as to both free up room for the motion of superstrings, as well as thus providing a basis for the formation of gravitational particles.

14)  Positive-Norm-States -- Holomorphic Fock Space that moves in such a manner so as to form ghost anomalies that comprise a physical-mapping known of as world-sheets that act as a substrate for both an indication as to where and how superstrings had just iterated, as well as providing a substrate for negative-norm-states to scatter these so that gravitational particles may subsequently form indirectly because of this.

15)  Dilatinos -- Spin-Orbital indices that are formed by the scattering of Gliossi-Sherk-Olive-Ghosts that quantize to form the spin-orbital-basis of gravitational particles.

16)  Gravitons -- The transversal particle/wave discrete phenomenology that is due to the transversal kinematic translation of gravitational particles.

17)  Gravitinos -- The spin-orbital particle/wave discrete phenomenology that is due to the spin-orbital kinematic translation of gravitational particles.

Part Two of the Twelvth Session of Course Six

Well hello again world, this is Samuel Roach here!  I hope that life is o.k. for you today!

Interconnecting the conicenter of the troughs of each of the dual ends, at both the the general locus of forward moving time and at the general locus of backward moving time, of each of the six eigenbases of the Royal Arc structure --  as integrated into the majorized structure of the Royal Arc for each associated layer of reality -- is an endpoint of what forms as a Chi Shape that forms as a Trace that exists in the Main Heterotic String Fabric topological region.  This Trace Basis functions in such a manner so as to take norm residue into the holonomic entity of the mentioned Trace eigenstates in such a way so that the said norm-state residue may recycle into ground-state residue that recycles back into norm-state field topological metric-gauge-like phenomena at the opposite corner from where the initial norm-state residue -- that consists of mini-string that needs to be re delineated -- is reincorporated back into norm-states.  The sub-metric in which the previous activity happens is during the sub-metric in which the Bases of Light exists as an integration of what is then soon to be the very many Planck phenomenon related phenomena of one layer of reality.  This exists in the same type of way for each Basis of Light.  If it were not for the Chi-Shaped phenomena that I just described, and if it were not also for the Main Heterotic String Fabric, the semicircles that comprise the eigenbases of the Royal Arc as a cross-section like phenomena that occurs right before instanton-quaternionic-field-impulse would consist of circles instead of semicircular phenomena -- and the Continuum would then need to exist as three plain hoops interacting with the twelve Main world-tubes in such a manner that superstringular commutation and superstringular recycling would then be impossible.  Superstringular commutation is essential for the group instanton interaction to bear any terrestrial simultaneous unitarity, which is essential for phenomena to interact in any organized way.  Superstringular recycling is essential for mini-string or substringular fields to interchange indices in such a manner so that the basis of jointal differential geometry to interchange into the basis of smooth-curved differential geometry and then back again into jointal related phenomena, and also so that the basis of smooth-curved differential geometry may interchange into the basis of jointal differential geometry and then back again into smooth-curved related phenomena.  Such interchanges are essential so that ground-states and norm-states may bear an optimum fractal and elastic modulae.  As stated before, all point particles flush through the Continuum in a manner of which we would term of as intantaneously.  In this way, all of the information that is regulated recycle-wise via the described majorized "semihoops", and is  communicated potentially  in a way that is more observably via the twelve Main world-tubes in a consant fashion in such a way that there is a constant relationship among all kinematically physical phenomena.  The Royal Arc acts as a regulatorial operator due to the fact that its volume allows for the condition of the degree as to how much more Fock Space there is then ground-state-based space.  The regulatory operation that I described is also due to the condition that the Royal Arc acts as a membrane that forms a vacuum comprised of Fock Space that kinematically differentiates in such a way so as to settle the gravitational indices of the phenomena that exists in the world-tubes in such a way that fascillitates the process of Ultimon Flow.  In courses nine and ten, I will explain more as to what wave-tug phenomenology springs phenomena from instanton into the main operational conditionality of Ultimon Flow.                                                                            
I will continue with the last part of this session later!  Until then, keep a positive attitude, and things should look up for you.  Bless You and you have a phenomenal day!  Sincerely, Sam Roach.

I Would Like To Know What You Want To Learn

Hey there world!  This is Samuel Roach here.  I am writing a post today that aims at finding out what you -- the reader -- wants to learn from my blog that I perhaps am not being clear enough at describing.

Would you like to know more about norm-states?
Would you like to know more about superstrings?
Would you like to know more about counterstrings?
Would you like to know more about gauge-bosons, heterotic strings of different natures, gauge-metrics, metric-gauges, what I describe as the Bases or Basis of Light, what I describe as the Main Heterotic String Fabric, what I mean by some of my analogies, the Higgs Action, the Klein Bottle, etc... .

So, what you may do in the near future is to think about what you would like me to explain better by asking me good questions, and afterwards, type these questions down to me so that I may be able to adequately answer the questions that you may ask.

If you have any disagreements with some of the general ideas that I describe in my posts, please feel free to try to form a dialogue with me.  You see, although I can see basically what I am writing about, once in a great while I might make a little mistake here or there.  Communication among many people who are seeking to see a common accurate view always involves at least a certain amount of dialogue.  Dialogue, to me, means -- I can make mistakes, you can make mistakes, I do many things without conceptual errors, and yet, you too do many things without conceptual errors.  Perhaps, if we put our heads together metaphorically, we will be able to synergetically do a lot more with more accuracy than what we would only be able to do on our own.
Yet, my concept of string theory on the whole as a general picture I know is right because I can see what I am "talking" about.  So, if one were to disagree with me on something that I know is true, I will try to see the other person's point, yet, I would feel obligated to explain to the described other reader why certain things have to be the way that they are.  Sometimes, I'm guessing that, although the concept is basically there pretty good (perfection is a falacy), I may describe certain things with the wrong term or with incorrect spelling (the latter I am certain is more often the case).  So don't be afraid of helping me to word my ideas in a manner that is more appropriate if and when this is the given situation.

I am here to help others.  That is my main goal in this blog.  That is my main goal in life. If we all pitched in more that we pitched out, this world would be a much better place.  That is why I only want comments and questions that show a yearning to improve the knowledge of string theory in one significant and important way or another.
To the people who want to advance the knowledge of mankind, I am very gratefull.  
Sincerely, Samuel David Roach.

A Description Of Ghosts Of Campbell Projections

A Campbell Projection is an interonncection of Campbell norm-states.
Such a Projection may scatter either other norm-states and/or this may scatter inexact and nonlinear Fock Space. Inexact and nonlinear Fock Space is comprised of first-ordered point particles that do not have an abelian interconnection between the individual first-ordered point particles described. This would mean that, in inexact and nonlinear Fock Space, you have individual first-ordered point particles that are connected to other individual first-ordered point particles by mini-string that is not supplementally norm in-between these. Such a non-abelian wave-field may be either hermitian if smoothly curved in all of the derivatives that exist in all of the dimensions that it is in, or it may be Chern-Simmons if there are indiscrete limits in the curvature of such a random neighborhood of first-ordered point particles. Since it is the tendency of phenomena to come to a state of relaxation, without Campbell ghosts, Hausendorf ghosts, Cambell-Hausendorf ghosts, and the ghosts of their Projections, point commutators would have the tendency to become to non-abelian in covariant kinematic differentiation over time.
This would produce spurious tendencies which could fray substringular phenomena.
You don't want this to happen. Such is the importance of not only ghost anomalies, that are transient, and the ability of hermitian non-abelian behavior. Yet, not to worry, the sub-mini-string interconnection in-between second-ordered point particles that interconnect and compactify to form first ordered point particles as well as the nature of sub-mini-strings interconnecting in-between second-ordered point particles to form the webbing of mini-string caused the spontaneous nature of the bending of substringular fields to have a high elastic and a high fractal modulae. This is the only way third-ordered point particles could interconnect to form the only way second-ordered point particles could interconnect to connect first-ordered point particles to each other so that homotopy may exist as well as to allow superstrings to be formed by the said first-ordered point particles. Remember, third-ordered point particles only exist where there are second-ordered point particles, since mini-string which is comprised of second-ordered point particles is what forms the field networking which allows for the interconnection of superstrings that causes homotopy to exist. Homotopy allows for interconnection so that phenomena may covariantly differentiate over time and thus exist.
I will continue with the suspence later. Have a phenomenal day!
Sincerely,
Sam.