As To Njenhuis Norm-State-Projections

Sometimes, there is a given arbitrary Calabi-Yau field -- that would here be represented by an orbifold eigenset, to where such as a particle, whose immediate field would thence work to form either an f-field or a d-field -- will work to bear a Gliossi-Sherk-Olive ghost, that is comprised of an integration of directly inter-related cohomological indices.  This is to where these so-stated ghost-based indices may here be occasionally scattered by norm-state-projections, that are not innately from our general universal setting.  For instance, one may often have a Calabi-Yau manifold that is comprised of an orbifold eigenset, that bears a lack of those norm-based conditions with certain other Calabi-Yau-based manifolds that are here relatively adjacenet to one another -- to where the two sets of Calabi-Yau-based manifolds discussed here will have a tense of bearing a different Gaussian-based format, by which the two said different sets of such physical mass-bearing manifolds will here be of two different universes.  Let us now say that there is a given arbitrary norm-state-projection -- that had here just guided the second so-eluded-to set of Calabi-Yau manifolds, in such a manner to where the group attractor matrix that I have just eluded-to here, as helping to work at adjusting the said second mentioned set of Calabi-Yau manifolds, is pulled into the immediate either f-field or d-field of the first mentioned Calabi-Yau manifold. (The so-eluded-to initial set of mass-bearing manifold, of which is here, in this respective given arbitrary case, a single of such manifolds.)  The norm-state-projection that is not of a Real Reimmanian-based inter-relationship to the initially mentioned Calabi-Yau manifold, will then bear a Gliossi-based interaction upon the initial mass-bearing manifold (Calabi-Yau manifold), to where the Gliossi-Sherk-Olive ghost-based pattern that had then been initially formed by the so-eluded-to particle of mass that I had started talking about here, will have its integration of cohomological-based indices annharmonically scattered to one extent or another.  This is to where there will be a certain degree of a Rayleigh scattering, of the initial ordering that had been formed by the prior-based Reimman scattering -- the latter of which had worked here to form the so-stated ghost-based pattern, that had come together in so as to form the physical memory of both the existence and the activity of that respective given arbitrary particle -- whose projected trajectory had formed a mappable tracing that left a trace of as to the where, how, and when, the said mass-bearing particle  whose ghost-based indices had been scattered, had been. This genus of a Rayleigh scattering will not necessarily form as viable of an effect upon the said starting particle itself, as it would have had upon its mappable tracing, yet, either way, there would then be at least some sort of a direct relationship between the indices that would here be directly affiliated with one Gaussian-based setting of one universe -- to the other Gaussian-based setting of what would here be another of such universes, in this given arbitrary case scenario.  I will continue with the suspense later!
To Be Continued!!! Sincerely, Sam Roach.

Static Charges

When one d-field that is directly associated with the immediate field of one given arbitrary electron, rubs against another d-field that is directly associated with the immediate field of another given arbitrary electron, there is -- to one extent or another -- an electrostatic charge that would here involve a certain degree of the scattering of the two so-eluded-to Calabi-Yau manifolds, that are here directly related to the scattering of the two general respective d-fields -- that would here work to form the two electric fields that are directly correlative to the two said electrons of this case scenario.  When two electric fields that are directly affiliated with the respective presence of two respective individual electrons, each, scatter amongst each other -- via the interchange of their correlative Yakawa-based indices, then, not only are the directly affiliated respective given arbitrary Calabi-Yau manifolds scattered to one extent or another, yet also, the directly affiliated Gliossi-Sherk-Olive ghost anomalies that are directly associated with each of such individually taken electrons, are also each scattered -- to one extent or another.  As the so-stated respective Gliossi-Sherk-Olive ghosts of the two given arbitrary electrons are scattered, the dual states of the Reimman-based cohomological indices -- that had initially here worked to form the physical memory of both the existence and the activity of the initial eigenbase of the two said respective given arbitrary electrons -- are scattered annharmonically, via  a Rayleigh-based scattering -- from the initial chiral-based and Reimman-based integrative cohomological-based ordering, into an entropic antichiral-based disorganization of the directly affiliated cohomological-based indices, that had initially worked to form the individual respective Gliossi-Sherk-Olive ghosts, that had been the mappable tracings of the two said respective given arbitrary  initially superconformally invariant electrons that will have here diverged from such a Majorana-Weyl Invariant mode by scattering amongst each other here.  To Be Continued!  Sincerely,
Sam Roach.

Different Formats of Certain Ghost Anomalies

Initially, as I have mentioned before, the ghost anomalies or the  cohomological-based indices, that are formed by the mappable tracings of two-dimensional superstrings of discrete energy permittivity, tend to bear a relatively torroidal tense of morphology -- while, the ghost anomalies or the  cohomological-based indices that are formed by the mappable tracing of one-dimensional superstrings of discrete energy permittivity tend to bear a relatively conical tense of morphology.  So, Gliossi-Sherk-Olive ghosts tend to bear either a torroidal or a conical shape -- via the mappable tracings of their respective trajectory, over time.  Yet, the shape of a Neilson-Kollosh ghost takes a little bit more of an explanation to tell here.  In general, the shape or the morphology of a Neilson-Kollosh cohomological-based mappable tracing (one eigenset of the directly inferred general genus of such indices) will either tend to be the shape of an annulus of either  a converging or a diverging hyperbolically-shaped toroid, or, the shape of a Neilson-Kollosh ghost may often, instead, be of the outer perimeter of the Ward-Neumman bounds of the respective shape of an annulus of either a converging or a diverging hyperbolically-shaped toroid.
I will continue with the suspense later!  Sincerely, Sam Roach.

Part Two of What may be my Third Session of Course 18

The condition of each individual layer of reality of each set of parallel universes, as existing in a completely diversified manner of delineatory index -- in a granular-based flow of homotopically-based indices, in such a manner in so that each of the so-stated layers of reality of each set of parallel universes -- may be termed of as an extremely staggered tori-sector-range, to where this is related to what is termed of as the Gliossi-Sherk-Olive-Theorem.  Under the just mentioned multiplicit Ward-Caucy conditions, each layer of of reality, or, in other words, each tori-sector-range of each individual set of parallel universes, is intricately woven into the general fabric-based boundary conditions of all of the other parallel universes of a given arbitrary set of parallel universes, in so as to work at forming an inter-relationship of all of the layers of reality of one given arbitrary set of parallel universes, in retrospect to one another -- in an interdependently respective eminent manner.  The general condition of those directly applicable ghost anomalies -- as well as their directly associated cohomological-based projections -- as being formed as the multiplicit mappable tracing of the physical memory of the correlative superstrings of discrete energy permittivity -- is the basis of  what is formed of as a result of this genus of activity,  to where this works to form what are known of as Gliossi-Sherk-Olive ghosts.  The integration of such just-eluded-to ghost-based indices works to form those cohomologica-based entities that are directly related to the extrapolation as to the what, where, and how, those so-stated superstrings of discrete energy permittivity had kinematically differentiated, over a sequential series of group instantons.

Part Two of the Test Solutions to the Last Test of Course 17 -- the Ricci Scalar

6)  Mass-based superstrings have a Yau-Exact eigenbase of Gliossi-Sherk-Olive cohomological index, in those manifolds of superstrings that appertain directly to the topological existence of bearing mass, over time.  Cohomology-based topological manifolds that are of Yau-Exact nature work to bear a more direct influence upon the relative given arbitrary eigenbase of gravity.  Gravity acts via the existence of the Ricci Scalar -- via the physical presence of the Rarita Structure.  Yau-Exact phenomena bear no viable Chern-Simmons singularities in and of themselves -- when this is considered at the Poincaire level of a Majorana-Weyl invariant setting.  This lack of singularity-based instability works to cause superstringular phenomena that are directly of a mass-bearing genus to be most directly influencing and to be most directly influenced by the Ricci Scalar.

7)  Plain energy bears significant Lagrangian and/or metrical-based Chern-Simmons singularities -- when this is taken along the mappable tracing of its Lagrangian-based path.  This general conditionality of a lack of singularity-based stability, works to cause phenomena of plain energy to bear less of a direct influence upon gravity -- than an equal correlative give arbitrary quanta of mass-bearing energy.  Thus, plain energy is relatively less influenced by the Ricci Scalar than mass.

8)  Light is partially hermitian -- when in consideration of those singularities that are produced by the propagation of the said light.  Such eluded-to Chern-Simmons singularities tend to be of a metrical-based tense.  This works to make light to not be of a Yau-Exact nature.  Thus, light is relatively less influenced by the Ricci Scalar than an equal correlative given arbitrary quanta of directly corresponding mass.

9)  Light is partially perturbative, due to the cyclical pulsation of its correlative mass-bearing photons -- that are propagated off of the relative Real Reimmanian plane, over time.  Singularities of a metrical-based nature, that are produced by the propagation of light, are of such a pulsation to where such phenomenology is guided by the fluctuation of its directly corresponding electric field -- via the nature of its respective given arbitrary wavelength.  A partially hermitian eigenbase of singularity-based nature may be described of as partially perturbative.

Part One of the Fourth Session of Course 16

The activity of the kinematic spatial differentiation of superstrings, in the process of their delineations and re-delineations is what works to form the world-sheets that exist in the substringular -- the sequential series of the re-delineations of superstrings, as these are projected over time through their respective Hamiltonian-based operands, is what works to form those physical memories of the so-stated superstrings, of which is what works to form ghost anomalies in so as to form the respective given arbitrary cohomologies.  Ghost anomalies are formed by the harmonic scattering of relatively forward-holomorphic-based norm-states, that are applied to the correlative differentiation cites by zero-norm-state projections that are forward-holomorphic in nature.  The format of norm-states that work to comprise the majority of the respective Hodge-Index of ghost anomalies, are the composite of Campbell-states, Hausendorf-states, and/or Campbell-Hausendorf-states.  Zero-Norm-States -- even though these are essential for the process of ghost anomalies to become static enough in composition to be superconformally invariant over time upon the activity of the harmonic scattering of any given arbitrary path operand that may be integrable -- in so as to allow for the delineation of the eluded to genus of any type of ghost anomaly-based pattern that may be Yakawa to any local cite in which such ghost anomalies may possibly be formed -- are that format or genus of projection that makes it possible for the other format-types of norm-states to be able to behave as these do when these said ulterior-type of norm-states and norm-state-projections are harmonically scattered upon by the sequential series of motion that superstrings imbue upon Fock Space as these so-stated superstrings are being delineated and re-delineated upon over time.  All world-sheets that are defined by the harmonic scattering of forward-holomorphic norm-states are directly existent, due to the existence of Fock Space.  Fock Space is that general bearing of region-based genus that is outside of both superstrings, their counterstrings, and Fadeev-Popov-Trace eigenstates.  All ghost anomalies, and thus, all cohomology, is the result of the condition of Fock Space as acting as the holonomic substrate that works to define the physical memories of both the existence and the activity of superstrings over time.  Such loci of Fock Space works to exist as the Hamiltonian-based operands of superstrings, as such superstrings are distributed and re-distributed throughout the Ultimon over those sequential series of the iterations of group instanton that work to act as the metrical path of discrete energy over time.  The result of the ensuing anharmonic scattering of Gliossi-Sherk-Oliove-based ghost anomalies over time by reverse-holomorphic norm-states -- which is imbued upon by the respective interaction of reverse-holomorphic zero-norm-states and reverse-holomorphic zero-norm-state-projections that work to settle the Ward-Caucy bounds of the perturbations that are caused in part by the ellimination of what were the respective ghost anomalies -- works to form the physical entities that act as gravitatonial-based particles that thence kinematically differentiate off of the Real Reimmanian Plane -- in so as to allow for the existence of gravity, while, the ellimination of what I will later describe of as Neilson-Kollosh ghosts works to form the basis of the replenishment of Real Reimmanian-based norm-states and norm-state projections.  I will continue with the suspense later!  Sincerely, Samuel David Roach.

More About Kaeler conditions

The center state of the perturbation of a cohomological set of indices that exists during the metrical duration that occurs right as the Wick Action eigenmetric is initiated, is the path operand as to where the center state of the ensuing relatively local directly corresponding Gaussian Transformation is to happen.  So, when there is a Kaeler condition that is antiholomorphic -- to where it is initiated upon a general substringular region -- in which a directly associated Wick Action is activated in the primal-based locus of the said general locus -- there will be an alteration in the morphological index of the eluded to corresponding cohomology, of which is comprised of interconnected ghost anomaly-based indices that are kinematic upon the on-shell topological stratum of the corelative substringular neighborhood.  Such an alteration in the morphological index will here be associated with a streaming of divergent Minkowski-based norm-state indices that bear Njenhuis norm-state projections that are tied together into what may often be an integrative Hilbert space that is annharmonic in terms of topological sway.  The center state of the eluded to perturbation of cohomological bearing is here comprised of the relative peak in topological Clifford-based divergence -- in terms of the sway of the here eluded to peaks and troughs of Gliossi-Sherk-Olive substringular field covariance.  The just eluded to Majorana-Weyl covariance will here be annharmonic in terms of both the metrical and the Lagrangian-based flow of Chern-Simmons singularites that are imbedded upon the holonomic substrate of the directly corresponding cohomological stratum.  The Laplacian-based coniaxial that may be extrapolated from one endpoint of the said general cohomological index of the here given arbitrary topological ebbing to the other endpoint of the said general cohomological index of the here given arbitrary topological ebbing -- at the conimetrical onset of the directly corresponding Wick Action that is being considered in this scenario -- is the traceable mapping as to where the center state of the ensuing Gaussian Transformation is to occur.  This  is to happen during the ensuing Kaeler Metric eigenmetric.  The higher the genus of the directly associated Chern-Simmons singularity-based perturbation is at the onset of the activation of the here eluded to Wick Action eigenstate, the more iterations that the directly affiliiated format of Kaeler Metric eigenmetric is to occur at the general substringular cite, as to where the eluded to perturbation is to occur.  Each of such iterations of Kaeler Metric that I have eluded to here will be at slightly different specific loci from within the general cohomological locus of index that I have here brought to the attention of the reader -- each of which will be centered at the specific locus that bears the best angular momentum to handle the readjustment of the substringular change in norm conditions best, via the appropriate centralization of the Hilbert gauge quantizaton that is structured kinematically along the previously discussed "longitude" of the eluded to format of a coniaxial-based Lagrangian of traceable mapping.  I will continue with the suspense later!
Sincerely, Samuel David Roach.

As To The General Nature Of Ghost Anomalies

The substrate of the mapping of the trajectory of substringular phenomena is known of as ghost anomalies. Over a sequential series of iterations of instanton, a substringular phenomenon exists in a given arbitrary display of distributions that integrate in such a manner in so as to form a path that may be mapped out via the existence of those positive-norm-states that indicate the directly prior delineatioins as to where the said substirngular phenomenon had existed in in the just mentioned metric. The physical trajectoral path of which may be mapped out -- in a Laplacian manner -- is known of as a ghost anomaly. Ghost anomalies may be Rham-based (supplementally based) or Doubolt (complementary based). Ghost anomalies often bear a certain degree of symmetry -- whether such a symmetry is trivially isomorphic, non-trivially isomorphic, trivailly assymetric, or non-trivially assymetric. The physical entities of ghost anomalies are gradually scattered by negative-norm-states so, via there counter-motion in codeterminable covariance with their corresponding positive-norm-states,such activity may work to allow for that substringular room that is necessary for room to be made in the substringular so that superstrings and their corelatively-related phenomena may continue to spontaneously move over time. Often, Gliossi-Sherk-Olive ghosts interchange with Kollosh ghosts so that there may be a recycling genus that can exist between superstrings of discrete energy and gravitational-based superstrings. The flow of ghost anomalies forms a basis of an allocation of residue of substringular phenomena that allows for certain indistinguashable replacement to exist from all three sets of universes that here exist within a few millimeters or so of everywhere one may go from within the confines of our universe --- even though all of the universes of our set of universes literally exist within every millimeter or so of anywhere where one may go witihin our universe. The norm-conditions of ghost anomallies work to complement the norm-conditions and the changes in norm-conditions of kinematically differentiating substrinular phenomena over time, while such mentioned ghosts work to recycle over time into various regions in so as to also allow for the appropriate redelinetion of first-ordered point particles that is necessary so that the proper point commutators may be localized where these may be needed so that the needed norm-based projections may be physically coherent enough to allow for those activities that are necessary for both changes in norm-conditions of superstrings, and, so that superstrings may go through those motions that allow for these to do their essential closing and opening over time (so that light may be formed from plain kinetic energy, and, vice versa).

A Little About Mobiaty Conditions

Here is an explaination of the mobius twists that exist from within either the Royal Arc, or, in one of the Overall world-tubes.  In an arbitrary given example here, a one-dimensional superstring iterates in a spot that exists within either the Royal Arc, or, in one of the Overall world-tubes.  A hyperbollically-shaped region that is local to the mentioned superstring is physically applied to the said superstring.  After many iterations, the one-dimensional string mentioned integrates cohomologically into a folded strip-like-shape via the contorsion of its disc-like two-dimensional field that it is Gliossi with.  This folded strip here bears a mobius shape.  So, when a hyperbollic spin is applied to the said one-dimensional superstring, and also, the associated Planck Phenomena are utilized to detect the said one-dimensional string, the mentioned superstring's field will appear as a mobius strip -- or, similar to a mobius twist -- that iterates as a toroidal-shaped "figure-eight" instead of as a vibrating strand.  The one-dimensional stringular field would more specificallly be detected as a mobius strip, while the said one-dimensional string that I am relating would appear as a mobius twist that is physically integrated in a Laplacian-like manner along the mentioned mobius strip.  In another arbitrary given case, a two-dimensional superstring iterates in a spot in the Royal Arc.  A two-dimensional hyperbollic spin is physically applied to the said two-dimensional superstring over a relatively brief Fourier Transformation.  After a sequential series of instantons, the said two-dimensional stringular field integrates physically in a Laplacian-like manner into a folded strip-like shape via the contorsion of its spherical three-dimensional field that the said string is in Gliossi contact with.  This folded strip, if detected, will "appear" as a mobius strip-like shape, yet, in a different manner than how a corresponding one-dimensional field would appear.  So, when the prior mentioned two-dimenisonal hyperbollic spin is physically applied to the associated two-dimensional string that I am here discussing, and also, the directly related Planck phenomena are used to detect the substringular phenomena of the here given scenario, the two-dimensional stringular field wil appear as another form of another type of mobius strip, or, as a mobius "chain" -- in a manner that I am about to describe.  When a one-dimensional hyperbollic spin instead of a two-dimensional hyperbollic spin is applied to the two-dimensional string here, the said superstring will appear as a contorted doughnut-like shape (a torus), and the two-dimensional stringular field would here appear as a contorted sphere with a pinprick annulus in its conicenter.  This would be potentially detected, after many instantons of the said directly related two-dimensional stringular field, from within the Royal Arc of the Ultimon.  The Gliossi-Sherk-Olive ghosts that are here detected via the condition of the mentioned applied forms of hyperbollic spin that here act directly upon the mentioned superstrings and their respective fields are what I was mentioning yesterday as "Mobius-Ghosts."

A Little More About Ghost Anomalies

Let us consider a substringular condition in which a set of one or more superstrings moves around in a general locus that is undergoing a tense of conformal invariance -- if not superconformal invariance -- in which the said superstrings that are involved iterate and reiterate within a common general locus that is kinematically invariant over a repeated pattern that involves a sequential series of instantons that form a pattern of static equilibrium over a relatively tightly-knit Fourier-Transformation that works to form a tight-knit mapping as to the location and operation of the related given arbitrary superstrings that we are forming a scenario as to their behavior in this case.  The ghost anomalic residue that works to form the general pattern that works to indicate the topological history as to the activity and operation of the corresponding superstrings that I am describing here, may be exrapolated as a general type of ghost anomalic substrate that is transient in the given case until the holonomic phenomenology that works to describe the general entity that comprises the said ghost anomalic field that acts as the denoted discharge of physical memory that is the field-mapping of where the related superstrings whose Fourier-based kinematic activity that formed the said ghost anomalies is scattered by negative-norm states that work to redistribute the indices of the said ghosts so that the room that was initially filled in part by the related initial ghosts may be utilized by other phenomena that need to occur in the prior implied general locus so that the motion of holonomic discrete energy may have a place to happen and interact so that that motion that is necessary for the continued existence of reality may occur so that reality may continue to exist.  Such ghosts that I have just described -- that inter-play in a relatively tightly-knit locus in a repeated manner so that the condtition of the corresponding kinematic operation that I thus related is here either a conformal if not a superconformal invariance of Fourier differentiating superstrings -- whose ghost-like membranes that here involve a higher genus of discrete energy phenomena that is known as kinematically inter-active orbifolds and kinematically inter-active orbifold eigensets that form a pattern of a relatively compactified static equilibrium are what are known of as Gliossi-Sherk-Olive ghosts.  I will continue with the suspence later!  Sincerely, Samuel David Roach.

Just To Make Sure

Superstrings are made up of beaded first-ordered-point-particles that exist in a Laplacian-based radial path for two-dimensional superstrings and of beaded first-ordered-point-particles that exist in a Laplacian-based linear path for one-dimensional superstrings.  Two-Dimensional superstrings are vibrating hoops of discrete energy permittivity.  One-Dimensional superstrings are vibrating strands of discrete energy permittivity.  The first-ordered-point-particles that comprise superstrings are interconnected via what I term of as mini-string.  Mini-String phenomena comprise the fields of superstrings.  Mini-String is beaded second-ordered-point particles that are interconnected via sub-mini-string.  The second-ordered-point-particles are comprised of by third-ordered-point-particles that are interconnected via sub-mini-string.  Mini-String interconnect superstrings.  The first-ordered-point-particles that comprise superstrings are comprised of metaphoically-based balls-of-yarn-like compactified mini-string.  As superstrings move, the mini-string that comprises the first-ordered point particles that comprise the said superstrings ebb away and back into the first-ordered-point-particles so as to provide a continuous flow of substringular fields.  Second-Ordered-Point-Particles are comprised of third-ordererd-point particles that fill the said second-ordered-point-particles in a metaphorically-based balls-of-yarn-like manner.  The sub-mini-string mers are held together via a fractal of pressurized vacuum-like activity.  The motion of the substrings, their fields, and the entirety of substringular activity is what forms the prior mentioned fractal of pressurized vacuum.  The Fadeev-Popov-Traces which are like a directly reverse-holomorphic field trajectory of superstrings are discrete energy impedance.  Fadeev-Popov-Traces are comprised of by beaded mini-string that forms a Chi-Shape that is interlaced with a figure-eight shape in a Laplacian-like manner.  The motion of discrete energy forms Gliossi-Sherk-Olive ghost anomalies that act as a substrate for the dilatons and dilatinos that are formed when such ghost anomalies are scatterd by the norm-states that strike the said anomalies in the process of the said norm-states motion in the reverse holomorphic direction relative to the arbitrary holomorphic motion of any given superstrings.  So, as superstrings move in an arbitrary holomorphic direction, the norm-states that move in the same arbitrary given holomorphic direction form Gliossi-Sherk-Olive ghosts.  The motion of norm-states that move in the reverse general holomorphic direction at some later metric scatter the mentioned ghosts so as to form that phenomena that consequently form the dilatons and dilatinos that are pulled off of the Real Reimmanian Plane so as to form gravitons and gravitinos that are the gravitational particles that cause the activity of gravity via their affect upon the Rarita Structure via the Ricci-Action.     

More About On-Shell Mass

A two-dimensional superstring has a three-dimensional field associated with it. When                                                                                                
                        
a relatively knit Fourier Transform that is highly Laplacian forms a torroidal structure

with an annulus at its central coniaxial, the whole Majorana-Weyl supercharge associated

with the operation of the associated superstring’s conformally invariant kinematism

is delineated, after the group metric that forms the basically Gliossi-Sherk-Olive field

described, at the outer shell general locus of that given M-field that is associated with

the described kinematic differentiation of the given two-dimensional superstring’s three-

dimensional field. This considers the fact that every superstring, whether it partakes

of mass or not, has a mass index. Such an on-shell supercharge as taken thru a Fourier

Transform that alters the spin-orbital and angular momentum distribution, delineation,

and directoralization of the associated three-dimensional field toroidal structure converts

the Yau-Exact indices transport in such a way as to form a discrete unit of mass as

to the M-field structure that I have conveyed. This is tantamount to that a spherical

shell with a physical charge in its center delineates all of the energy of its charge along

the topography of its associated shell. Likewise, the norm state Ward conditions of

the annulus of a toroidal 3-D field of a 2-D superstring delineates all of the angular

momentum and spin-orbital distribution indices at the outer shell of that given toroidal

3-D structure. Likewise, the “figure-eight” twisted toroidal structure created by certain

fermionic superstrings forms the point mass of electrons and neutrinos. This mass

of certain fermions is created by this: The norm state conditions when considering

the Ward conditions of the annuli of the two relatively Mobius ends of the “figure-

eight” described have angular momentum and spin-orbital momentum that transfers

their distribution and directoralization indices outward to the outer topology of the

given “figure-eight-like” structure. The kinematic differentiation of the Yau-Exact

indices of the “figure-eight” structure as a whole causes the given phenomenon to

translate, thru the Fourier Transform of the given M-field thru a Minkowski or Hilbert

Lagrangian, its mass indices into an integration of Hamiltonian eigenstates that allow

the Kaluza-Klein phenomena, as with 3-D fields of 2-D superstrings, to convert and/or

maintain as a mass. The abelian geometry of the light-cone-gauge of such Yau-Exact

structures causes the E(6)xE(6) gauge-bosons related to form Schwinger indices that

keep the M-fields oriented to coalesce their Noether indices into a conformally invariant

manner that has to be orientable per general locus in order to translate to a proceeding

general locus as long as the mass indices associated are limited. Since any M-field needs

a limited Lagrangian distribution in order to delineate its Majorana-Weyl indices over a

group metric that is based on a harmonics or anharmonics that may not coincide with a

group directoralization of Noether flow unless the associated superstring is unorientable,

Kaluza-Klein mass is always under light speed, per iteration, and mass must become

Yang-Mills as in a worm-hole or Yang-Mills also, if otherwise tachyonic, which is true

when mass bears unorientable yet finely directoralized motion via a Ward polarizable

dark matter holomorph. Unorientable superstrings may only be as such temporarily when

in a large group even if Reverse-Lorentz-Four-Contracted. Mass may become Yang-

Mills and tachyonic if its field delineation is majorized.                                                                                                                                                                                                                    

Part One of the Thirteenth Session of Course Six

Well hello again world, this is Samuel Roach here!  I hope that you are having a phenomenal day!
Here is the first part of the thirteenth session of course six.
                
There is a space at the end of each Chi-related endpoint that extends beyond the central substringular encoder of each general world-sheet (that is, of each Main world-tube).  This space is interconnected to the general stratum of the substringular via mini-string.  This space is always just a fraction of a radii from the endpoints of the semicircles and the upside-down semicircles of a cross-sectional region of the Royal Arc where there is to be a Basis of Light to differentiate via a sub-metric that happens right before instanton-quaternionic-field-impulse.
This region here is due to the fields exerted by the substringular encoders of the world-sheets that are located here.  All superstrings have fields associated with them.  One dimensional stringular fields tend to be thinner than the fields of two-dimensional superstrings (with the exception of certain relatively large Gliossi-Sherk-Olive fields that relate to certain one-dimensional superstrings that are undergoing  a strong degree of regional conformal invariance).  The integration of all of the superstrings that indirectly associate with one of the semihooops supports the existence of the described semihoop.  The slight curve inward that the recycleable material has to travel through is why when stringular residue is first taken up, there is a slight "time" or gauge-metrical lag that happens,and this so-called "lag" allows for the observation of kinematic Fourier or the discernment of time-wise active differentiation.  Once this lag is brought to the point of the Royal Arc where the pointal material may be recycled promptly, the travel of phenomena in the general world-sheets responds to Ultimon speed just about instantaneously.  The only factor here now would be the recycling mode as I taught in lessons earlier, and as I will teach later.  Superstrings in the substringular may only be so close due to the fields that these exert.  The fields that superstrings exert generally repel when these fields oscillate asymetrically , especially when these mentioned strings are encoded for as coming from another general world-sheet.  This extra need to repel is due to the extremely different sequences of the strings between these AND also their differences in how the waves in these are built up at any given instant (series iteration differentials).                                                                                            
I will continue with the suspense later!  I hope for the best of all of my readers.
I think of mankind as my family.  I won't lose, because I have Tau on my side!  God Bless!  Sincerely, Sam.

A Little Explaination Of Tori-Sector-Ranges

Hi there, this is Samuel Roach here! How are you doing today folks!
Today, I am going to provide a little bit more of an explaination as to what I mean by tori-secor-ranges.
What I mean by a "tori-sector-range" is a set of substringular phenomena that comprise one layer of actual reality in one set of parallel universes. The reason as to why I call these individual "layers" tori-sector-ranges is because, when one detects a conformally invariant superstring that is not superconformally invariant, it often appears via detection to behave as a torus when one includes the associated Gliossi-Sherk-Olive field. So, when a very high quantity of such often torroidal appearing phenomena interact as one layer of reality within the multiplicitly Minkowski Space that is integrated into six additional Njenhuis dimensions to form a relatively Hilbert Space (which is thence not defining a holographic space), such a sector of substringular neigborhoods defines a range that comprises one actual layer of reality.
So, how are there layers of reality while yet there is an Overall reality? Every so often, one-ten-thousandth of history -- including the relative past as well as the relative future -- alters. Such a perturbation is when the most kinematic layer of reality switches to a different "tori-sector-range." Yet, during each instanton, all of the tori-sector-ranges are interactive, even though only one of such layers is kinematic in a reverse-fractorially "Gliossi" manner at a time.Every time history alters to an extent, I call this perturbation a Major Reality Change. Yet, since space-time substance tends to be more granular than fabric, it is easier to change the future than the past.
Also, what do I mean by the "Bases of Light?" During the brief metric of what I call the "space-hole" which is in-between the majority of Ultimon Time that is based on Imaginary Time and the quaternionic-instanton-field-impulse-mode which is directly before instanton, the substringular encoders are attached to what reties into Planck Phenomenon related phenomena just as the related substrings are reorganizing in such a manner so as to allow for the appropriate norm conditional sequential spacial differentiations that allow for subsequent Gaussian Transformations, the prior described Planck Phenomenon related phenomena are, for one brief sub-metric, tied together into very large sets of phenomena that are shaped like Planck Phenomena. So, just as quaternionic-instanton-field-impulse begins, which is just before instanton, such large manifestations of Trace untie homotopically and retie homotopically into the googles of Planck Phenomenon related Phenomena that are associated with their correlative substrings.
So, how do these interact without breaking homotopy? Since there is so much potential of abelian-like untying of compacified condensed oscillation among first-ordered-point particles, there is a constant back-and-forth ebbing of mini-string which allows for very distant and close wave-tug interactions.
I wil continue with the suspense later! Sinerely, Sam.

The 15 Categories Of Ghost Anomalies

These are:
1) Gliossi-Sherk-Olive ghosts

2) Fadeev-Popov Ghosts

3) Neilson-Kollosh Ghosts

4) Rham Ghosts

5) Doubolt Ghosts

6) Ghosts of Light-Cone-Gauge Eigenstates

7) Ghosts of Schwinger Indices Via The Rarita Structure

8) Campbell-State ghosts

9) Hausendorf-State ghosts

10) Campbell-Hausendorf-State ghosts

11) Ghost of Campbell-State-Projections

12) Ghosts of Hausendorf-State-Projections

13) Ghosts of Campbell-Hausendorf-State Projections

14) Ghosts of Klein Bottle Eigenstates

15) Ghosts of Higgs Action Eigenstates

The 15 Categories Of Ghost Anomalies

These are:

1) Gliossi-Sherk-Olive ghosts

2) Fadeev-Popov Ghosts

3) Neilson-Kollosh Ghosts

4)

About On-Shell Mass Structure

A two-dimensional superstring has a three-dimensional field associated with it. When a relatively knit Fourier Transform that is highly Laplacian forms a toroidal structure with an annulus at its central coniaxial, the whole Majorana-Weyl supercharge associated with the operation of the associated superstring’s conformally invariant kinematism is delineated, after the group metric that forms the basically Gliossi-Sherk-Olive field described, at the outer shell general locus of that given M-field that is associated with the described kinematic differentiation of the given two-dimensional superstring’s three-dimensional field. This considers the fact that every superstring, whether it partakes of mass or not, has a mass index. Such an on-shell supercharge as taken thru a Fourier Transform that alters the spin-orbital and angular momentum distribution, delineation, and directoralization of the associated three-dimensional field toroidal structure converts the Yau-Exact indices transport in such a way as to form a discrete unit of mass as to the M-field structure that I have conveyed. This is tantamount to that a spherical shell with a physical charge in its center delineates all of the energy of its charge along the topography of its associated shell. Likewise, the norm state Ward conditions of the annulus of a toroidal 3-D field of a 2-D superstring delineates all of the angular momentum and spin-orbital distribution indices at the outer shell of that given toroidal

3-D structure. Likewise, the “figure-eight” twisted toroidal structure created by certain fermionic superstrings forms the point mass of electrons and neutrinos. This mass of certain fermions is created by this: The norm state conditions when considering the Ward conditions of the annuli of the two relatively Mobius ends of the “figure-eight” described have angular momentum and spin-orbital momentum that transfers their distribution and directoralization indices outward to the outer topology of the given “figure-eight-like” structure. The kinematic differentiation of the Yau-Exact indices of the “figure-eight” structure as a whole causes the given phenomenon to translate, thru the Fourier Transform of the given M-field thru a Minkowski or Hilbert Lagrangian, its mass indices into an integration of Hamiltonian eigenstates that allow the Kaluza-Klein phenomena, as with 3-D fields of 2-D superstrings, to convert and/or maintain as a mass. The abelian geometry of the light-cone-gauge of such Yau-Exact structures causes the E(6)xE(6) gauge-bosons related to form Schwinger indices that keep the M-fields oriented to coalesce their Noether indices into a conformally invariant manner that has to be orientable per general locus in order to translate to a proceeding general locus as long as the mass indices associated are limited. Since any M-field needs a limited Lagrangian distribution in order to delineate its Majorana-Weyl indices over a group metric that is based on a harmonics or anharmonics that may not coincide with a group directoralization of Noether flow unless the associated superstring is unorientable, Kaluza-Klein mass is always under light speed, per iteration, and mass must become Yang-Mills as in a worm-hole or Yang-Mills also, if otherwise tachyonic, which is true when mass bears unorientable yet finely directoralized motion via a Ward polarizable dark matter holomorph. Unorientable superstrings may only be as such temporarily when in a large group even if Reverse-Lorentz-Four-Contracted. Mass may become Yang-Mills and tachyonic if its field delineation is majorized.