More As To The Leverage Of The Higgs Action

The leverage of the Higgs Action, is caused primarily -- due to the leverage of the Fischler-Suskind Mechanism.  The general multiplicit condition of the Fischler-Suskind Mechanism, is comprised of by a correlative set of norm-state-projections, that work to bear a consequent orthogonal relationship -- that works to bear a wave-tug-related leveraging of ~6.25*10^18 (which is the reciprocal of the scalar magnitude of the smallest tense of discrete charge, which is ~1.6*10^(-19)Coulumbs) upon the correlative multiplicit Higgs Action eigenstate -- in so as to work to bring the activity of a Gliosis-related relationship, that is to ensue between discrete energy and the here directly corresponding multiplicit eigenstate of the holonomic substrate of the Klein Bottle, via the Kahler-Metric, in so that such a general tense of a Fourier-Transformation is here to be brought into the process of working to allow for the said multiplicit discrete quanta of energy to here to be re-attaining their fractals of discrete energy, in so as to work to allow for discrete quanta of energy to both persist and exist over time -- via such a relationship of a correlative general tense of a Gaussian Transformation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Next Part Of Session 10 Of Course 20 -- Calabi-Based Interactions And Calabi-Based Manifolds

One can not have a fraction of an electromagnetic beam, yet, one may have a quantum of many electromagnetic beams that are quantized together.  One may have a quantum of electromagnetic energy that contains multiple types of electromagnetic energy that are integrated as one unit, which is usually the case from within the confines of a planet.  Let us say that a bunch of beams of electromagnetic energy are quantized, and are heading for an object of mass -- that is in its direct path.  The electromagnetic energy scatters, when it interfaces with the object of mass.  When the quantized beams of electromagnetic energy are about to strike the given object, the beams of energy that are here given, are to be situated with what may be termed of here as being of a Yang-Mills topology.  A Yang-Mills topology eludes to the condition -- that the Gaussian of the given light-cone-gauge is 90i degrees  to the Gaussian of the light-cone-gauge of the object of mass, that the beams of energy given are about to strike.  When the beams of quantized electromagnetic energy scatter upon the given mass, the scattered energy temporarily becomes of a Kaluza-Klein topology -- in that the Gaussian of the beams of quantized electromagnetic energy are then to be interfacing with an orthogonal Gaussian light-cone-gauge eigenstate -- that works to relate a supplemental Njenhuis set of Ricci tensors, that set a directly corresponding Klein Bottle eigenstate to interact with the Regge Slope, in so as to work to help at allowing for the correlative related phenomenology -- that is here to be going through a directly corresponding Gaussian Transformation -- to be Gliosis to the Kahler-Metric, over a relatively brief sequential series of group-related instantons.  This is here to be involved most specifically, in this given case, at the interface of the Gliosis-based interaction, that is here to exist between the said electromagnetic energy and the substances that it is to be scattering upon.  Remember, Lorentz-Four-Contractions only apply for phenomenology that have not been topologically frayed by a black-hole.  So, whenever light, or, for that "matter," whenever electromagnetic energy is to scatter, individual discrete electromagnetic quanta of energy are very transiently sped up for 384 consecutive iterations of group-related instanton, per each individually taken entropic photon that has here just respectively been scattered, while then slowed down (although such discrete electromagnetic quanta are slowed down as is according to Snell's Law, when detected by any overt means of physical extrapolation).  Such a very brief "tachyonic" propulsion, is here to be explained by the following:  Imagine a bright and hot electrostatic "ball," that is to go from traveling through a vacuum -- into traveling through a thicker medium -- all of the sudden.  As this "ball" of charge is to be going through the said thicker medium, the overall motion of the said electrostatic ball will be slowed.  Yet, the static electromagnetic energy that is at the perithery of the ball, may be imagined to very temporarily speed-up upon direct contact with the said thicker medium, while then such an external static charge will ensue, in so as to be brought back to the relative core of the said overall slowed hot electrostatic ball -- that has here to have lost velocity by moving into a relatively thicker medium.  As the photons that were very briefly made entropic, are to ensue in so as to be re-quantized with that respective beam of light -- that these had temporarily been scattered out of -- the so-eluded-to electromagnetic energy that is not "entropic," is then said to be back to having a Yang-Mills light-cone-gauge topology.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Gauge-Tranformations And The Kahler-Metric

Once any one given arbitrary photon has worked to strike the externalized core-field-density of the light-cone-gauge of another respective given arbitrary discrete quantum of energy -- both the discrete quantum of electromagnetic energy that I have just mentioned, as well as the discrete quantum of energy that it had just scattered upon, will then proceed to become Yukawa to the Kahler-Metric in an eminent manner, -- over the course of the immediately ensuing 384 group-related instantons. The last three of such so-eluded-to 384 consecutve iterations of group-related instanton, are involved with a re-orientation -- by which the correlative Kahler-Metric eigenstate is to be re-positioned, in order to be functioning at a mildly different proximal locus.  In pretty much the central 191 consecutive iterations of group-related instanton -- that are to be from within the said 384 consecutive correlative instantons, the Kahler-Metric is to be Gliosis to both of the discrete quanta of energy that are to be undergoing the so-eluded-to gauge-transformation.  When such an eminent Yukawa-based inter-relationhip is to be of a Gliosis-based manner with the Kahler-Metric, the directly corresponding discrete fractals of energy, that are needed for the said discrete quanta of energy to both continue to exist and persist as discrete energy, are to be re-attained by both of the individually taken quanta of energy of this respective case.  Furthermore -- just as any Gaussian Transformation that is to act in an eminent Yukawa manner, when in relationship to the Kahler-Metric, is to go through its directly corresponding 384 consecutive iterations -- before such an eminent Ward-Caucy relationship is to be relaxed, -- this is as well to be true with that genus of a Gaussian Transformation that is known of as as a gauge-transformation.  I will more intensely describe the process of both the mentioned 384 consecutive iterations and the mentioned 191 consecutive iterations in Course 24 -- as to Conformally Invariant And Superconformally Invariant Phenomenology.  Please bear with me with any potential grammatical errors.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

More As To Gaussian Transformations Versus Gauge-Transformations

With a Gaussian Transformation that is here to not be a gauge-tranformation, as the directly corresponding discrete energy quanta that are to here be most Yukawa to the correlative Kahler-Metric manifold -- as the correlative directly corresponding holonomic substrate of the pertinent Klein Bottle eigenstate, that is to be made Gliosis to the just mentioned discrete energy quanta, is to shake in a significant manner, this shaking is to only happen in the general direction of the holomorphic directorial-based Lagrangian-based Hamiltonian operand, that is in the path of holomorphic wave-tug of the correlative set of discrete energy quanta, where the correlative set of superstrings of discrete energy permittivity are to ensue, right after the then metric-wise iteration of BRST is to then be happening.  Yet -- with a Gaussian Transformation that IS here to be a gauge-transformation, as the directly corresponding discrete energy quanta that are to here be most Yukawa to the correlative Kahler-Metric manifold -- as the correlative directly corresponding holonomic substrate of the pertinent Klein Bottle eigenstate, that is to be made Gliosis to the just mentioned discrete energy quanta, is to shake in a significant manner, this shaking is to happen in both the general direction of the holomorphic directorial-based Lagrangian-based Hamiltonian operand, as well as in the Njenhuis-to-holomorphic directorial-based Lagrangian-based Hamiltonian operand, that is in the path of the holomorphic wave-tug of the correlative set of discrete energy quanta, where the correlative set of superstrings of discrete energy permittivity are to ensue, right after the then metric-wise iteration of BRST is to then be happening.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Effect Of Added Dimensions Upon The Force Of Gravity

When one has an isomorphism that is comprised of multiple superstrings that are relatively separated from being in the same general locus, yet, such superstrings are all within an Angstrom of each other, then, one has to consider the condition as to whether or not such extrapolated superstrings, over a time-wise differential association, are under a state of static equilibrium, or, if such a set of superstrings are more along the lines of behaving in both a perturbative and also in a relatively divergent manner. If one has two given arbitrary sets of superstrings that are proximal -- microscopically -- yet, are not of the same general locus, and, if the two said sets of superstrings are under a condition of superconformal invariance, as these said superstrings are non-trivially isomorphic the one set relative to the other, then, these superstrings would need to be acted upon in order to become diverged away from the eluded to condition of static equilibrium. If there happened to be a ghost inhibitor that acted as a buffer in-between the two eluded to general loci of each set of such superstrings that are here of the same universe, then, if some sort of norm-state projection that were to act upon both of the said sets of superstrings via the holonomic substrate of the said ghost inhibitor that were to be in-between the two eluded to orbifolds (physically-based spaces) were able to possibly work to produce an alteration or a perturbation in the said condition of static equilibrium that was here to initially be kinematic in-between the two said sets of superstrings that are in this case initially in a symmetry of non-trivial isomorphism, then, this would then make it possible to end the eluded to condition of static equilibrium. Such an alteration from what was here a given arbitrary case of superconformal invariance would tend to diverge the two sets of superstrings in such a manner in so that the directoral-based wave-tug/wave-pull of each individual set of superstrings would reverse in terms of their holomorphic permittivity. Such a reverse in directoral flow would then here indirectly cause the production of a Wick Action eigenstate, which would consequently cause the activity of a Gaussian Transformation that would act upon the general locus of part of the initial region in which the orbifolds, or, the physical spaces, that are here represented by the two sets of superstrings, so stated, that here work to perform two different functions that are Gliossi upon the holonomic substrate of the same universe. This is a general example as to that activity that may often work to allow for the need for the changes in certain norm-based conditions. Again, norm-conditions need to change often in order for room to be made for the essential operations of space-time-fabric.

A Little As To The Relationship Of The Higgs Field To Photons

Most superstrings of discrete energy permittivity and their directly corresponding counterparts -- in conjunction with their correlative Fadeev-Popov-Trace eigenstates of discrete energy impedance and their correlative light-cone-gauge eigenstates -- in order to remain as discrete energy, must routinely undergo the Kaeler-Metric, via the correlative activity of the guidance of the directly corresponding Higgs Boson eigenstates --these of which move the directly corresponding Klein Bottle eigenstates, in so as to allow for the here needed correlative Gaussian Transformations, that work to allow substringular spaces to both persist and exist, over time.  This works to mean, that most superstrings of discrete energy are routinely put through the immediate influence of what is termed of as the Higgs Field.  The exception is photons.  Photons both have no mass, as well as the condition that photons are comprised of what would otherwise be completely Lorentz-Four-Contracted superstrings of discrete energy permittivity.  This Ward-Caucy-based condition works to allow for photons -- that are Not being lagged-down by Calabi-based interactions, to just slide-out of the so-stated immediate influence of the genus of that Yukawa Coupling, that is known of as the said Higgs Field.  Yet, during the first 384 directly corresponding group-related instantons that happen -- right after any given arbitrary respective photon has struck another superstring of discrete energy permittivity in a Gliosis-based manner -- since this works to form discrete increments of entropy -- this will be the only exception as to a photon, instead, being directly influenced by the Yukawa-based pull of the Higgs Field.  This exception that I have just stated here, is when even a photon, that is normally not directly tugged by the Higgs Field, will be put into a situation -- in which it needs to re-attain its discrete fractals of energy -- in order to both persist and thereby exist as energy.  I will continue with the suspense later!  To Be Continued!  Sam Roach.

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

The norm-state-projections that will then here be trapped inside of the Ward-Neumman bounds of any specific respective given arbitrary Klein Bottle eigenstate -- as well as those superstrings, that act as indices that are placed in the Ward-Neumman bounds of the so-stated Klein Bottle eigenstate in a cyclical-based manner, per each individual group-related instanton, over the course of one relatively local group metrical-based duration of one set Kaeler Metric-based translation -- act as a set of a holonomic substrate of substringular phenomenology, that moves, per each relative transition of group instanton, in both a holomorphic and an antiholmorphic-based manner do to the "shaking" that is here involved, in so as to work to form a fractal of an electromagnetic resonation, that would here tend to be proximal to the said respective given arbitrary Klein Bottle eigenstate of any of such case scenarios.  This is particularly the case, when such a given arbitrary correlative Kaeler Metric is of the general manner of being as an example of a gauge-transformation.  As I will explain later in my writings, whenever there is a Calabi-based interaction that is of the metrical-based mode of being in the process of a Kaeler Metric, the directly corresponding Gaussian Transformation that then is here to follow will always tend to be of a gauge-transformation.  The norm-state-projections that work to comprise the initial interior of any of such so-stated Klein Bottle eigenstates, are harmonically ordered in a spatial manner, as is here in accordance with the Reimman scattering that is here to initially bring an order to the so-eluded-to substringular composition of the said given arbitrary Klein Bottle eigenstate.  The superstrings of discrete energy permittivity that act in so as to enter the interior of such a said composition of such an eigenstate, are here to initially re-contract to a maximum-based contraction, and, after such superstrings of discrete are pulled-out of the interior of such a said Klein Bottle eigenstate -- per each individually taken respective part of each of such iterations of group-related instanton, as is here right before each of such correlative individually taken iterations of the directly corresponding Regge Action eigenstates -- these are pulled out of such a said contractive mode, into their fully uncontracted shape, at each of such individually taken loci in which the Regge Slope is to be Gliossi to the topological substrate of each of such individually taken superstrings of discrete energy permittivity -- that may here be considered in any of such respective given arbitrary case scenarios.  During the metrical endpoint of each directly corresponding iterations of BRST -- that are to here be considered as happening before each individually taken iteration of the mode of one eigenmetric of one specific given arbitrary Kaeler Metric, any superstring of discrete energy that may be considered here, will -- at this point -- be Lorentz-Four-Contracted to the inverse of as to how it is encoded to be expanded in a Clifford-based manner, after the initial instant in which such a directly corresponding mode of BRST is here to be initially commenced.
Superstrings Tend To Always Be Lorentz-Four-Contracted To Their Encoded Degree Of Contraction, At The End Of Each Correlative Iteration Of BRST.
To Be Continued!  I will continue with the suspense later!  Sincerely, Sam Roach.

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

When there is a Gaussian Transformation that is happening during the period in which the Kaeler Metric is going on -- in such a manner in so as to act as a gauge-transformation -- there is one genus of a difference between this general category of a Gaussian-based Transformation and the rest of this general category of a Gaussian-based Transformation.  This one genus of a difference, is that, during a gauge-transformation,  the directly corresponding Klein Bottle eigenstate of any one individual specific respective given arbitrary cite, in which such a Kaeler Metric is undergoing its general format of activity -- will work to bear an additive side-to-side torsioning,  that would here be applied to both the relatively reverse holomorphic end and the relatively forward holomorphic end of such a so-stated respective given arbitrary Klein Bottle eigenstate.  This general genus of activity, will then tend to increase the tendency of a relative lack of such a holonomic substrate as a given arbitrary Klein Bottle eigenstate -- from appearing to  be anything that is even similar in morphology to an open-top parallelepiped, in this case.  So, when one is to work to extrapolate the mappable tracing of any respective given arbitrary Klein Bottle eigenstate, that is here to be undergoing a correlative gauge-transformation -- there will be an additional torsional-based cohomological-based twisting of the here directly corresponding ghost-based indices -- to where the resultant homotopic-based physical memory of both the existence and the activity of such a so-stated Klein Bottle eigenstate, will give the appearance of a somewhat membronous morphology, that, in a way, may appear as looking at the trippy "innards" of a microscopic organism.  Most Gaussian Transformations are gauge-transformations, as I will explain later in the future.  To Be Continued!  I will continue with the suspense later!  Sincerely, Sam Roach.

Questions To The Last Test of Course 18 -- the Ricci Scalar and Kaeler Differentiation

1) What is a Regge Transformation?

2)  What is a Kaeler Manifold?

3)  What is the relationship of a Klein Bottle eigenstate, toward the relatively local dilatons and dilatinos -- when there is a Yakawa-based tendency of Noether Flow?

4)  What is the relationship of a Klein Bottle eigenstate toward the relatively local dilatons and dilatinos -- when there is a Yakawa-based tendency of tachyonic-flow?

5)  What is a Bette Manifold?

6)  What is the Bianchi Identity?

7)  What is the Klein-Gordan Theorem?

8)  How may a perturbation in a relatively local Kaeler-Metric eigenmetric work to effect the tendency of the relatively neighboring Gaussian Transformation eigenmetrics?

The Kaeler Relationship To Ghost Annhilation

When a Gliossi-Sherk-Olive ghost-based cohomology of any significant scalar magnitude of Hodge-based index is scattered annharmonically by relatively reverse-holomorphic norm-state projections -- there is a correlative Nielson-Kollosh ghost-based cohomololgy of a significant scalar magnitude of Hodge-based index that is, as well, scattered annharmonically by relatively reverse-holomophic norm-state projections, off of the relative Real Reimmanian Plane.  There is, at this general group metrical point in activity, a complementary-based group attractor that works to pull the residue of the so-eluded-to annharmonically scattered Neilson-Kollosh-based cohomological pattern out of the relatively Njenhuis Plane -- from which the so-stated Neilson-Kollosh ghost-based pattern was formed by gravitons and gravitinos -- into the relative Real Reimmanian Plane, where the so-stated Gliossi-Sherk-Olive ghost-based cohomological pattern that I have here eluded-to was initially both formed and scattered into a certain quantum of Fock Space residue.  Likewise, there is, simultaneously, via the vantage-point of a central conipoint, a complementary-based group attractor that works to pull the residue of the so-eluded-to annharmonically scattered Gliossi-Sherk-Olive ghost-based pattern -- out of the relatively Real Reimmanian Plane and into the correlative Njenhuis Plane, where the so-stated Neilson-Kollosh ghost-based cohomological pattern that I have eluded-to was initially both formed and scattered into a certain quantum of Fock Space residue.  It is, in both just eluded-to cases, one covariant, codifferentiable, and codeterminable ghost-inhibitor for each of such so-stated cases, when taken individually, per case, that works to act upon both of the so-eluded-to genus-based formats of group attractor indices -- in so as to cause such an exchange of the residue of the so-stated ghost-based cohomological indices.  When such a significant quantum, as I have here eluded-to, of the residue of ghost-based cohomological indices, is recycled in the manner that I have just mentioned -- this genus of activity will here work to form an antiholomorphic Kaeler conidition -- via the affect that such a genus of activity works to bear upon the relatively local Rarita Structure eigenstates.  This so-stated affect works to involve the Ricci Scalar -- since the Ricci Scalar happens along the topological surface of the activity of the correlative Rarita Structure eigenstates.  Such an eluded-to initialization of an antiholomorphic Kaeler condition works to cause what is known of as the Kaeler Metric -- at the here given arbitrary local substringular neighborhood.  This will then work to initiate the Wick Action -- which will ensue to cause a Gaussian Transformation, in so as to allow for both the continued kinematic differentiation of active superstrings, as well as causing discrete energy to reattain their correlative multiplets of the fractal of such discrete energy.  To Be Continued!  I will continue with the suspense later!  Sam Roach.

How Gauge-Bosons Fit-In With Gauge-Transformations, A Heads-Up to Courses 18 and 19

When a substringular cohomology reverses in its directoral-based holomorphicity, there is a reversal in the applicable Kaeler conditions, and, this works to form a Wick Action eigenstate -- of which works to initiate the process of a Gaussian Transformation, which involves the activity of a Kaeler-Metric eigenstate.  When this happens, the directly corresponding gauge-bosons reverse in their holomophic-directoral basis.  What this means, is that the gauge-bosons will here go from "plucking" their respective second-ordered light-cone-gauge eigenstates from one Laplacian-based direction of wave-tug/wave-pull -- to "plucking' their respective second-ordered light-cone-gauge eigenstates in the opposite Laplacian-based direction of wave-tug/wave-pull.  When such a Gaussian Transformation here involves the scattering of electromagnetic energy, this is called a gauge-transformation.  In relation to the gauge-bosons, this works to not only reverse the basis of their correlative holomorphic directoral tense, yet, it also works to reverse the parity of the vibrations that are formed by their plucking of their correlative second-ordered light-cone-gauge eigenstates -- the directly corresponding second-ordered Schwinger-Indices are here then reversed in the arrangement of their indical-based holonomic substrate.  This is a beginning of an explanation as to the relationship between the activity of a gauge-transformation -- with the activity of the correlative gauge-bosons, that are here of the same respective given arbitrary basis of phenomenology.
To Be Continued!  I will continue with the suspense later!  Sam.

Part Three of the Eleventh Session of Course 16

A Njenhuis Klein-Gordan mechanism is an interaction that happens when transversel, radial, and/or spin-orbital tensors that are off of the Real Reimmanian Plane interact with a given arbitrary superstring of discrete energy permittivity at a tangent of normalcy that is orphoganal to the extra dimensionality of the Imaginary-based subspaces that are directly correlative to any pertainent given arbitrary case scenario.  For instance, let us say that a given arbitrary superstring has just become non-orientable.  The so-stated superstring is not able to be orientable during both the directly corresponding Bette Action eigenstate and the directly corresponding Regge Action eigenstate.  Under the just stated conditions, the said given arbitrary superstring will become tachyonic over the course of the ensuing iteration of group instanton that the so-stated superstring will be flowing into -- for over the course of one or more instantons. Since the superstring is to now become at least temporarily tachyonic in this case scenario, the ensuing one or more eigenmetrics of the Regge Action eigenstates that will be directly involved with the interaction of the said given arbitrary superstring with its envronment over a sequential series of instantons will be initially scattered annharmonically at the initial stage of such a perturbation of the so-stated superstring -- due to the said superstring that is here being discussed going from a Noether-based flow into a tahchyonic-based flow.  Those tensors that act upon the said superstring -- in the form of norm-state projections -- in so as to allow for the superstring to be able to succeed at its needed path at becoming tachyonic, will bear a subtended directoral basis that is Njenhuis in nature.  When the said superstring that is here becoming at least temporarily tachyonic is also undergoing a change in norm conditions -- known of as a Gaussian Transformation -- then, the activity of that substringular scattering that is involved with the eluded-to genus of the added condition of the Kaeler Metric being introduced into the activity of the here tachyonic superstring will be of an annharmonic nature. This annharmonic nature is involved with the here local intrusion of a Klein Bottle eigenstate, along with a geometrical-based need for a perturbation of that indistinguishably different Regge Action eigenstate that will need to "fidget" in order to accomodate the altered genus -- as to the format of how the directly associated superstring will move over the ensuing increment of time that is here correlative.  It is when a tachyonic condition that is directly involved with a superstring that is also entering into an eigenstate of the Kaeler Metric that is when there are both norm-state projections that are Njenhuis that interact upon the correlative superstring, as well as that there will here be a "fidgeting" of the directly corresponding indistinguishably different Regge Action eigenstate that is to take the "brunt" of the motion of the here newly developed tachyonic nature of the so-stated superstring that has just left from being of a Noether-based nature.  Yet, when a superstring remains, instead, of a Noether-based nature, then, when a Kaeler-Metric is introduced to a superstring that is to undergo a Gaussian Transformation, the directly corresponding scattering of the correlative Regge Action eigenstate is instead of a harmonic nature, since, here, the general nature of the flow of the so-stated superstring is, in this case, not perturbated out of this here said condition.  This scattering is directly related to the nature of the flow of the correlative superstring as it is projected through a Regge Slope eigenstate.  If the kinematic projection through such a slope is hermitian, then, it is being harmonically scattered.  Yet, if the kinematic projection through such a slope is Chern-Simmons in its basic nature, then, it is being annharmonically scattered.  I will continue with the suspense later!  Sincerely, Sam Roach.

A Little Bit of a Heads Up as to the Ensuing Portion of Course 16

When there are many world-sheets differentiating upon a relatively general locus -- that would here involve, in this given arbitrary scenario, different sets of world-sheets that would here correspond to individual sets of world-sheets that each involve kinematic mappings of different parallel universes that are of the same set of parallel universes -- then, what would work to entail the individual antiholomorphic Kaeler conidtions that apply to one antiholomorphic Kaeler condition per set of world-sheets that each directly correspond to different universe-based conditions per stratum of the said individual antiholomorphic Kaeler conditionality, would involve what is here to be the substringular status of different respective Gaussian Transformations that are to occur -- one Gaussian Transformation per each set of world-sheets that would each concur to different parallel universes, per each of the so-stated individual sets of world-sheets that work to form cohomological ghost anomalies that work to map out the tracing as to the existence and the activity of superstrings that act upon the stratum of the here eluded to indices of the here respective universes that comply to one universe per set of world-sheets that I have eluded to here at the said general locus of activity.  So, in this given arbitrary case, one has each individual set of world-sheets that each bear an antiholomorphic Kaeler condition, of which works to activate an individual Wick Action eigenstate for each of the said bases of cohomological index -- in so as to indirectly work to cause the activity of an ensuing Gaussian Transformation.  There is at least one index of holonomic substrate for each universe of one set of parallel universes that is kinematic from within the Ward-Caucy bounds from within -- say one to three millimeters from wherever one may extrapoltate these to be at.  So, it is possible for one to have, at a general locus, many sets of world-sheets -- that each form a viable bearing for one parallel universe that is unique to all of the other respective individual sets of world-sheets that are here kinematically being traced as a mappble  holonomic substrate as ghost anomaly-based indices -- in so as to allow for a conglomerate set of individual set of Wick Action eigenstates that each work to indirectly form what is here to be the respective sets of individual sets of respective Gaussian Transformation eigenstates that are all happening in a general locus.  Yet, individual eigenstates of Gaussian Transformation that are proximal, yet, are of different  universal settings, are not Gliossi in terms of cohomological index in any Yakawa manner that is viable to any abelian format of direct wave-tug/wave-pull leveraging -- in so long as none of the eluded to superstrings that are directly involved here do not synchronize in their intrinsic vibrations.  Superstrings that synchronize in their intrinsic vibrations become of the same universal settings when and if this is done.  Either way, each respective antiholomorphic Kaeler conditon that is to happen works to form one individual Wick Action eigenstate -- that indirectly works to form one individual Gaussian Transformation eigenstate.  Such an activity works to form the respective individual basis of specific Landau-Gisner Action eigenstates, as well as the respective individual basis of specific Fischeler-Suskind Mechanism eigenstaes, as well as each set of Gaussain Transformations that comply to unique universal settings that each work to involve different respective Higgs Boson eigenstates and different respective Klein Bottle eigenstates. So, in such a genus of a general locus that would here involve the changing of norm conditons of different indices of universal settings that are proixmal at the Poincaire level would here involve different individual Kaeler Metric eigenstates each, respectively.  I will continue with the suspense later!  Sincerely, Samuel David Roach.

Ensuing Kaeler Metric Eigenstates

As I will discuss in much more detail over the course 24 about conformal and superconformal invariance, a specific discrete Gaussian Transformation eigenstate is directly effectual over the course of 384 consecutive group instantons -- the discrete Kaeler Metric portion of which is comprised of 191 consecutive of the so-stated 384 consecutive group instantons.  When a substringular region bears relatively little need for a change in norm conditions in its local substringular neighborhood -- due to a relatively mild genus of a here given arbitrary antiholomorphic Kaeler condition -- then, immediately after one discrete format of a local Gaussian Transformation, the activity of the directly corresponding Fischler Suskind-Mechanism eigenstate will be varied to an ensuing spatial delineation, that would here operate upon superstrings that are of a different universe. Again, all of the universes of one given arbitrary set of parallel universes are within about 3 millimeters of each other.  The activity of the genus of the angling of the directly involving Fischler-Suskind-Mechanism eigenstate is what functions in so as to propagate the motion of the so-stated mechanism-based eigenstate towards the eluded to "new" locus, that here works to form a bearing upon a different universal setting.  Yet, if a given arbirtary substringular locus needs a more vast alteration in norm conditions, then, there may be up to many consecutive discrete eigenstates of Gaussian Transformation that are Gliossi upon the same universal setting at the Poicaire level over time.  Again, different universes are not Real Reimmanian -- when this is considered relative to one another.  This basis of relativistic Gaussian Format is based upon the directly correlative basis of substringular angling of vibration.  I will continue with the suspense later!  Sincerely, Samuel David Roach.

Part Five of the Third Session of Course 16

The ability of a specific region of a world-sheet that works to form ghost anomalies may be either propagated in the relatively forward-holomorphic directoral Hamiltonian path-integral, or, are propagated in the relatively reverse-holomorphic directoral Hamiltonian path integral, or, are propagated in a relatively antiholomorphic directoral Hamiltonian path integral -- given the tense of the directly associated kinematic-based flow of the accompanying Lagrangian that the said world-sheet is being propagated through over time -- in relation to the general directoral-based-flow of the eluded to Hamiltonian holomorphicity.  This is when in terms of the genus of the said condition, that could thence be called a Kaeler condition.  So, if a world-sheet of a given arbitrary scenario is moving in either a reverse-holomorphic directoral Hamiltonian-based path flow, or, in an antiholomorphic directoral Hamiltonian-based path flow -- in terms of the given arbitrary  Sterling approximation of the kinematic mappable tracing of the respective local divergence-based covariance or local scattering-based covariance.  Such formats of covariant-based modes are often Yakawa to the eluded to perturbation of one given arbitrary world-sheet relative to its immediately surrounding world-sheets, that are propagated in a metrical-based Dirac manner -- that is either euclidean-based in expansion mode or Clifford-based in expansion mode.  On account of what I just mentioned, this may be a Kaeler condition of an antiholomorphic divergence that may be extrapolated by the mapping of either a perturbative reverse-based covariance and/or a perturbative scattering-based covariance of the directly associated ghost anomalies -- that act here as physical memories of both the existence and the activity of the directly corresponding superstrings that behave in the format of the said manner.  If the given arbitrary world-sheets of a general locus are all kinematically covariant in terms of the genus of a convergent-based mode, then, the corresponding condition of holomorphicity may be considered as a holomorphic Kaeler condition. If a Kaeler condition is of a relatively antiholomorphic mode, and/or is of a relatively reverse-holomorphic mode, then, such a format of either a respective perturbative scattering-based condition or of a perturbative divergent-based condition is of a Kaeler condition that works upon the activity of a unique set of specific Njenhuis Rarita Structure indical projection eigenstates -- to form the metrical-gauge eigencondition of a Wick Action eigenstate.  The Wick Action is multiplicitly performed by a genus of a Hausendorf Projection that is applied through a mechanism of corroborative norm-state projections, that operates in such a manner in so as to activate the activity of Gaussian Transformations -- via the general basis of the operation of the Kaeler Metric.  The Kaeler Metric is applied by the interaction of a local Higgs Boson eigenstate with a local Klein Bottle eigenstate.  Please read my previous writings for some more detail about this.  I will continue with the suspense later!  Sincerely, Samuel David Roach.

How Gauge-Bosons Move

As the Polyakov Action occurs multiplicitly, in a simultaneous manner that hereby coincides with the activity of the Bette Action -- that is also here multiplicit in operational index --, the directly corresponding gauge-bosons that work at plucking second-ordered light-cone-gauge eigenstates in so that the corresponding second-ordered Schwinger-Indices may form, bear both a relatively "steady-state" kinematic topological sway & a sort of "back-and-forth" kinematic wave-tug/wave-pull, that works to unleash those vibrations from the light-cone-gauge that fuel those ghost inhibitors of the Rarita Structure -- so that there may be a direct relationship between discrete phenomena of both energy permittivity and energy impedance & discrete phenomena of metrical-based-Gliossi gravitational Hodge Index.  The so-stated "steady-state" kinematic operation is a mobility that topologically sways outward -- in functional parity with that given arbitrary genus of Clifford Expansion that happens to a first-ordered light-cone-gauge eigenstate, when a Polyakov Action eigenmetric occurs -- in an ellipto-inverse-hyperbollic curvature-based motim.  This happens as the so-stated gauge-bosons move "anatomically" in a sort of "back-and-forth" manner, in so as to pull the directly related second-ordered light-cone-gauge eigenstates -- in so as to form discrete vibrations that are known of as second-ordered Schwinger-Indices.  These just stated indices come together in multivarious combinations, in order to work to trigger the motion and the mobility of the Rarita Stucture.  Schinger-Indices -- as well as forming the link between discrete energy of detectible motion & discrete gravitational Hamiltonian operation, in that collaboration that works to form Ricci Scalar eigenstates, also form a tying of substringular fields that functions as an operational group attractor, that bears the mobility to work to activate the operation of the multiplicit Wick Action.  The Wick Action is the phenomena-based Hamiltonian operator that initiates Gaussian Transformations.  This functions in so that any shear reversal in the holomorphic-based directoral-pull of a substringular region puts the neighboring Wick Action eigenstates into motion, so that norm-conditions of substringular holonomic substrate may be able to alter in genus -- so that the flow of the kinematics of the substringular may perpetuate in the process of re-establishing the Jacobian eigenbasis of the mappable extrapolation of continual substringular energy.  I will continue with the suspense later!
To Be Continued.  Sincerely, Sam Roach.

Certain Means of Yakawa Coupling

When a given arbitrary Wick Action eigenstate initiates a Gaussian Transformation via its Yakawa interaction with its directly corresponding Landau-Gisner Action eigenstate, the just mentioned Yakawa interaction is of a Gliossi nature.  As the just so-stated Landau-Gisner Action eigenstate initiates the activity of the directly corresponding Fischler-Suskind Mechanism, the initial locus of the eluded to and affiliated wave-tug/wave-pull is of a Gliossi manner, at the Poincaire level of kinematic interaction.  As the leveraging of the just mentioned Fischler-Suskind Mechanism is occurring -- in so as to produce that activity of a Kaeler-Metric eigenstate that works to allow for a directly associated Gaussian Transformation, the activity of the so-stated leveraging is of a Yakawa nature that is not Gliossi at the relatively central framework of such a genus of substringular "mechanics."  Yet, at the Poincaire level as to the interaction of the said Fischler-Suskind Mechanism upon the directly affiliated Higgs Action eigenstate, such a leveraging is here actually of a Gliossi manner.  The activity of a given arbitrary Higgs Action eigenstate upon its directly affiliated Klein Bottle eigenstate is a Yakawa Coupling that is of a Gliossi manner.  The activity of superstrings of discrete energy permittivity interacting with a Klein Bottle eigenstate -- in so as to undergo a Kaeler Metric eigenmetric -- is Gliossi with the contents of the said Klein Bottle eigenstate, yet, it is not Gliossi to the "chasis" of that part of the Shotky Construction that acts as the structure of the Ward-Neumman bounds of the directly affiliated Klein Bottle eigenstate.  The Yakawa interaction of superstrings of discrete energy permittivity -- entering their respective Klein Bottle eigenstates -- is what works to re-initiate the said superstrings with those critical cusps of discrete energy perimttitivity that are needed so that superstrings may sustain the drive that these need, so that discrete energy may be able to persist at all.

I will continue with the suspense later!  Sincerely, Samuel David Roach.

Tachyonic Versus Noether Flow

A superstring that is orientable differentiates kinematically via Noether Flow.  A superstring that is not orientable differentiates kinematically via a tachyonic flow.  A superstring is orientable when the substringular field eigenstates that are first-ordered and supplementally norm between a given superstring and its corresponding counterstring are trivially isomorpphic in terms of the connections in-between the associated superstring and its corresponding counterstring as caused by the Bette Action, and if the delineatory amplitudes of these said connections have the same scalar distribution when considering all of the said first-ordered substringular field eigenstates, even if the Hodge distribution among the said field eigenstates is not homogeneous and therefore not integrably hermitian during the Laplacian condition of the given instanton in which the associated Bette Action is occurring through its described gauge-metric.  If a superstring is not orientable during the Bette Action, the superstring described will attempt to become orientable during the subsequent gauge-metric of a given Regge Action eigenmetric via a Regge Slope eigenstate that "totters" the associated superstring in an attempt to obtain the multiplicit trivial isomorphism and a common homogeneous and delineatory amplitude that bears a supplementally norm abelian nature that retains the Noether Condition of the said superstring's wave-tug.  (This is via a simultaneous internal push-and pull that is exterially projected along the Ultimon.)  If a superstring is still orientable during the said Regge Action eigenmetric, then the associated superstring becomes tachyonic.  This is an example of how a lack of substringular super-symmetry may effect the differential operation of that superstring over a simple sub-Fourier-based Transformationm which, if such a condition is integrable over a sequential series of iterations that is non-trivial gauge-metric-wise, will form a Fourier Transformation over time that involves a superstring that is tachyonic and thereby perturbative relative to its general condition of Noether Flow.  Such a perturbation effects the matrix of the delineatory index of the involved orbifolds that are directly effected by this tachyonic multiplicitly integrable distribution.  Since the anharmonic multiplicit redistribution of a kinematically unorientable superstring flows differently then the surrounding Noether Conditions, and Noether Conditions are the kinematic delineatory means of maintaining the norm conditions that allow for a sustained covariant Gaussian Symmetry, the Fourier Transformaion involved with a tachyonic flow will produce change in Gaussian Symmetry either via a regular Gaussian Transformation or via a gauge-transformation, the latter of which is the substringular cause of entropy.
Sincerely, Samuel David Roach.  samsphysicsworld@blogspot.com.

Some More Stough About The Dangers Of Colliding Gluons

Gluons are hadrons whose metrical activity directly causes leptons and/or quarks to "glue" together in so that protons, electrons, and nuetrons may be formed.
Gluons put the directly prior mentioned subatomic particles to be brought together via an Ante-De-Sitter/De-Sitter gravitational mode.
The metrical activity of gluons as these interbind leptons and/or quarks in such a manner so that the said larger sub-atomic particles may exist -- so that matter may exist in any organized reasonable fashion -- indirectly works, via the extensions of the Rarita Structure, to allow for that delineation of a Hausendorf Projection that is known of as a Wick Action to move through time in a way that it may apply a certain general type of pressure upon a gauge-action that is known of as a Landau-Gisner-Action.  The pressure applied to the just stated Landau-Gisner-Action works upon a field of mini-string via a stratum that is known of as the Fischler-Suskind-Mechanism in such a manner so that leverage may be applied to a small boson that is known of as the Higgs Boson.  The just stated boson acts to raise the Klein Bottle in order for the Kaeler-Metric to occur in the general neighborhood of superstrings that need to soon undergo a Gaussian Transformation. Gaussian Transformations are needed in order for superstrings to regain the permittivity that these need so that the related superstrings may remain as discrete units of energy permittivity -- so that energy may exist at all.
So, bombarding gluons is potentially dangerous to the proper formation and delineation of the Wick Action -- such activity can possibly steer the stated Hausendorf projection in a manner that may veer Gaussian Transformations from doing what these need to do.  Such a corresponding mis-allignment may potentially dominoe in a manner that could keep superstrings from re-obtaining their permittivity, and thus, such a veering may work to cause certain superstrings to not be able to remain as discrete units of energy.
You don't want that.  You want energy to remain as energy so that space-time-fabric may remain safe.
Please end the Hadron Colliding Experiment.
Thank You.
I will continue with the suspense later!
Sincerely,
Sam Roach.

About Certain Assymetric Needed Delineation

Hello, my name is Samuel David Roach. When you consider the condition that E(6)XE(6) strings that are adjacent are to spin assymetrically, then photons are not to collide head on.

Photons tend to propagate in the direction of their permittivity, such as the inertial nature of all phenomena related to superstrings. Given the construction of the discrete energy permittivity and the construction of the discrete energy impedance of a photon in the Lagrangian Fourier propagation of an arbitrary photon as it is propagated through space-time-fabric, the direct collision of photons head-on would potentially jeapordize the condition of the E(6)XE(6) strings that are directly affiliated with the said arbitrary photons in terms of the natural tendency of such named heterotic strings to spin assymetrically.
E(8)XE(8) strings are to spin assymtrically. So, the bombardment of orbifolds head-on in terms of the related E(8)XE(8) strings invading each others direct Gaussian sub-space would infringe upon the inertial tendency of the mentioned heterotic strings to spin assymetrically.
So, colliding the holomoriphiclly Laplacian-based ends of heterotic strings that are of a substringular nature in our kinematic-based region of space-time-fabric over the course of the Fourier activity of the propagation of such superstrings would infringe upon some basic Pauli-Exclusion-like conditions that are essential for the continued protection of local space-time-fabric. Saying silly things like, "Well, it only creates a fissure!" is like saying, "Well, we only put a little hole in the damm!" When one understands what I am trying to say, it becomes painfully clear that the collision of such hadrons in any such manner is shear foolishness.
Also, the Higgs Action is essential for the continued existence of Gaussian Transformations.
Gaussian Transformations are essential for the spontaneous existence of kinematically-based energy and thus for the continued existence of reality. I dare you to do the math that I prepared back in 2009 as to the dangers of illucidating the Higgs Action. Every eigenstate of such a basis of Action is differentially kinematic for the continued motion of each minute subspace that involves the spontaneously kinematic translation of energy. Without such a translation, energy would be unable to correlate in the manners that allow for covariant Fourier differentiation that is time-wise related, not to mention that the translation of changing norm-conditions allows for the differential reconfigurations that allow for commutations that even allow for the flow of different Laplacian configurations. Therefore, illucidating the Higgs Action should not happen, and the Hadron Colliding Experiment should be shut down for even the simple fact that the continued exsitence of Gaussian Transformations is essential for perpetual change and thus for the continued existence of unfrayed space-time-fabric.
Finally, the strong force is the gluonic force that interbinds leptons and/or quarks -- given what particle you are talking about. Gluons metrical activity are the source of the Wick Action. Am I talking to the wall! My Gosh, the Wick Action is essential for the proper Fourier Translation of the Higgs Action so that the Higgs Action may do its job in allowing the conditon of Gaussian Transformations to happen at all! So, learn all you can, and we will all agree that we need to end the Hadron Colliding Experiment! God Bless You, and so long!
Sincerely,
Samuel David Roach.