Static Equilibrium And The Generation Of The Wick Action

 The more that a cohesive set of discrete energy quanta, is to tend to be in the process of working to remain in a state of a kinetic tense of static equilibrium, the more that there will consequently tend to be a continual generation, of a set of the proximal regional presence of both Wick Action eigenstates and the correlative Landau-Gisner Action eigenstates.  I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.

Part 7 Of Session 1 Of Course 20 -- Calabi Manifolds And Calabi Interactions

Just as any respective given arbitrary electron drops an energy level, this general tense of activity -- of which works to bear an antiholomorphic Kahler condition -- will, at this point in activity, work to initiate a directly corresponding Wick Action eigenstate.  This said Wick Action eigenstate will then ensue to work to form a correlative Landau-Gisner Action eigenstate.  The holonomic substrate of what is to here act in so as to work to perform the so-stated Landau-Gisner Action eigenstate, will then work to cause what may be called of here as an eigenstate of the here proximal local Fischler-Suskind-Mechanism.  The just mentioned Fischler-Suskind-Mechanism, will then work to push the directly corresponding holonomic substrate of the correlative Klein Bottle eigenstate -- in so as to move this just mentioned eigenstate -- in what will here be in the relative norm-to-forward-holomorphic direction, in so as to work to move the so-stated holonomic substrate of the said Klein Bottle eigenstate -- into that general region of the relative Real Reimmanian Plane, so that those discrete quanta of energy, that are to here be in the need of re-attaining their fractals of discrete energy quanta, will be in such a substringular position, in so as to be facilitated to be able to then undergo their respective Gliosis-based interaction with the said holonomic substrate of the correlative eigenstate of the Klein Bottle.  This so-stated activity of the Kahler-Metric eigenstate, will happen just after the said electron that is to here be releasing its spare kinetic energy, has to have then just dropped that correlative energy level, that is here being discussed.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Re-Adjustment Of Fischler-Suskind-Mechanism

Whenever there is an antiholomorphic Kahler condition happening in the substringular, there is consequently an ensuing Wick Action eigenstate -- of which indirectly works to form what may be termed of here as the Kahler-Metric -- from within the general region in which such a so-stated antiholomorphic Kahler condition had just recently happened.  The said antiholomorphic Kahler condition, works to initiate a directly corresponding Wick Action eigenstate -- in so as to work to apply a physical torsioning of what may be termed of here as the directly corresponding Landau-Gisner Action, in so as to work to cause the consequent leveraging upon the directly corresponding Fischler-Suskind-Mechanism, that is here to be most proximal localized to the initial said Fourier-based activity of the said Wick Action eigenstate, that is to here be of such a respective given arbitrary case scenario.  Upon the 96th consecutive iteration of the applied torque that is to exist, that is of the directly corresponding Fischler-Suskind-Mechanism of such a case -- that is to happen upon the directly corresponding holonomic substrate of the local proximal Klein Bottle eigenstate -- the Gliosis-based interactions of the correlative and local discrete quanta of energy with the said respective Klein Bottle eigenstate, is to then be initiated -- and is to continue for a total of 191 consecutive iterations of group-related instanton, for the correlative respective given arbitrary case scenario.  In the process of the correlative Fourier-based activity that is of the so-eluded-to Gliosis-based interactions of discrete energy quanta, with the so-mentioned respective and correlative Klein Bottle eigenstate -- the discrete quanta of energy that have then interacted in such a manner with the said Klein Bottle eigenstate, will have then re-attained those fractals of discrete energy that these need, to have then built-back into the Ward-Neumman bounds of their physical composition -- to have then be brought in such a condition, to where these are to now be properly refurbished.  After the said 191 consecutive Gliosis-based interactions of the said discrete quanta of energy with the said Klein Bottle eigenstate -- the so-stated Klein Bottle eigenstate is to then exit from the general Ward-Caucy bounds of the directly associated discrete energy quanta, while then re-adjusting over the course of three additional iterations of group-related instanton, to then be primed in so as to work to help in the course of the Gaussian-based transformation of a relatively adjacent substringular cite, to where the respective adjacent discrete quanta of energy that are to have a need of re-attaining their fractals of discrete energy, will have then been put into such a position in so as to need to be "operated upon" by an ensuing Fourier-based activity of the Kahler-Metric.  The multiplicit Klein Bottle does not repeat at one specific spot, over the span in which it is iterated over the course of one specific Kahler-Metric-based activity.  This overall so-eluded-to process, that is directly applicable to the correlative motion of any given arbitrary respective Klein Bottle eigenstate -- when including the re-adjustment -- lasts for 384 consecutive iterations of group-related instantons.   I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Some Ideas As To The Effect Of The Higgs Field

When a given arbitrary photon that is of one orbifold eigenset of electromagnetic energy, strikes another superstring of discrete energy permittivity in a Glioisi-based manner -- over a sequential series of group-related instantons, -- the so-stated given arbitrary individual photons, of which will always (as photons) be of a bosonic nature (closed-loop and two-dimensional), will tend to "bounce" from one general directoral tense of a relative holomorphic motion, to a reversal of its said directoral tense of relative holomorphic motion, -- until the so-mentioned respective given photons of which had just scattered upon a topological-based holonomic substrate, are re-quantized back into its ensuing correlative orbifold eigenset of electromagnetic energy, that the said photon is to then be incorporated into next.  When a superstring of discrete energy permittivity perturbates -- in so as to go from one general holomorphic-based directoral flow into a relatively reversed general holomorphic-based directoral flow -- this general genus of activity works to form what is known of as an antiholomorphic Kahler condition.  The region in which  such a Kahler condition is to happen, may be viewed of or called a Kahler Manifold.  When an antiholomorphic Kahler condition happens, the so-eluded-to Fourier-based activity of such a condition -- works to initiate what may be viewed of as an eigenstate of the Wick Action.  Any respective given arbitrary Wick Action eigenstate that happens, acts as a gauge-action -- that works to act upon what may be termed of as a metric-gauge that may be viewed of as a Landau-Gisner-Action.  The Landau-Gisner-Action acts upon a Laplacian-based leveraging of norm-state-projection -- of which may be termed of as the Fischler-Suskind-Mechanism.  The Fischler-Suskind-Mechanism works to mobilize a respective given arbitrary Klein Bottle eigenstate -- via the wave-tug/wave-pull of what would here be a respective given arbitrary Higgs Boson eigenstate -- in so as to allow for the activity of what may be termed of as the Kahler-Metric.  This just-mentioned general genus of activity, works to allow for the kinematic activity of what may be termed of as Gaussian Transformations -- in so as to allow for the continued persistence and the continued existence of both substringular spaces and discrete substringular energy.
So, when any respective given arbitrary photon scatters upon any superstring, in a Gliosis-based manner -- the said photon will then tend to work to be involved in an antiholomorphic Kahler condition.  This will work -- as I have described of on this page -- in so as to cause the ensuing activity of a Kahler-Metric eigenbase.  This will then work to utilize the mobilization of the respective given Higgs-Boson eigenstate -- that would be correlative to any one given arbitrary case.  This is why any given arbitrary individual photons, that had just been scattered -- within the first 384 instantons after such so-stated discrete individual photons have just struck another superstring of discrete energy permittivity in a Gliosis-based manner -- will, over the relatively quite transient duration in which such an exception for photons is the case, only then tend to be directly under the influence of the Higgs Field.
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.

The Reason As To How Gravity Exists

Gravity happens because of the amplitude due to the Ricci Scalar, and the Ricci Scalar happens via the multiplicit activity and the multiplicit distributions of Rarita Structure eigenstates. Gauge-Bosons throughout space and time pluck the second-ordered-light-cone-gauge eigenstates that comprise first-ordered-light-cone-gauge eigenstates -- first-orderd-light-cone-gauge eigenstates exist in-between superstrings and their respective Fadeev-Popov-Traces -- to form Schwinger-Indices. (The corresponding vibrations of first-ordered-light-cone-gauge eigenstates form first-ordered Schwinger Indices, while, the corresponding vibrations of second-ordered-light-cone-gauge eigenstates form second-ordered Schwinger-Indices.) Schwinger-Indices propagate to form a kinematic relationship between gravitational particles and superstrings that are discrete units of energy permittivity so that gravity may take effect. The residue of Schwinger-Indices that exist over the course of the perpetuation of gravity are used to bring Wick Action eigenstates into the general regions of the Landau-Gisner Action eigenstates in order to indirectly cause the activity of Gaussian Transformations. You may learn more about this by reading my blog. My blogcite is samsphysicsworld@blogspot.com.

A Little About The Norm-Projections That Help Start Gaussian Transformations

The Wick Action is put into play by the activity of gluons. The activity of gluons by which certain sub-atomic particles are stuck together is known of as the strong force.  Gluons work to stick the respective sub-atomic particles together that the said gluons are most directly associated with via the help of a perturbation in the Ricci Scalar that involves an Anti-De-Sitter/De-Sitter gravitational alteration.  Just as the quaternionic-instanton-field-impulse begins to happen directly before instanton, what are to be gluons during the ensuing respective instanton undergo an Anti-De-Sitter gravitational pull that initially "flaps" the concavity of what are to be the Hausendorf Projections that will form Wick Action eigenstates, during the same general region during the same duration of instanton, from being directly concave toward each other toward being directly concave away from each other.  The relatively simultaneous activity of the mentioned Anti-De-Sitter gravitational directoralization of the Ricci Scalar initially -- as the ends of the corresponding mentioned Hausendorf states are flapping -- works to hold the related Hausendorf norm-states in a relatively and covariant still position until the beginning of the ensuing local instanton.  Just as the said ensuing instanton that we are arbitrarily dealing with here begins, the ends of the Hausendorf norm state eigenstates  that are to work together to form a projection known of as a Wick Action "flap" back into a condition of being concave toward each other on account of the alteration of the Ricci Scalar in regards with the relatively local gluonic force from going back into a De-Sitter gravitational mode.  At this point, the respective Hausendorf eigenstates that are to integrate in so as to form the Wick Action are relatively loosened from a localized covariant-based virtual standstill into being thence pulled into the direction of a Campbell-Hausendorf projection that is known of as a Landau-Gisner Action.  The end of the initially touched eigenstate of the mentioned Landau-Gisner Action Action overall eigenstate is of a planar configuration that bears a Hodge volume that is 6.25*10^18 times the Hodge volume of a fully contracted Higgs Action eigenstate.  At the respective relatively norm-to-reverse-holomorphic end of the said Landau-Gisner Action that we are arbitrarily discussing in this given case at the relatively holomorphic end of where the said Action is undergoing a Fischler-Suskind-Mechanism eigenmetric, the end of the Campbell-Hausendorf projection here is correspondingly concave-up.  Directly to the relatively reverse holomorphic end of the just mentioned relatively concave-up holonomic geometry -- connected via mini-string -- is another of such prior mentioned planar Hodge-based volumes that also consist of tightly-knit and integrated first-ordered-point particles.  Such an interconnectioin continues as such until a planar end of a Campbell-Hausendorf norm-state is avainable to lift a respective Klein Bottle eigenstate via its corresponding Higgs Action eigenstate.  Any given arbitrary well-functioning Wick Action eigenstate touches its corresponding Landau-Gisner Action eigenstate in a Gliossi manner at 22.5 degrees from a Wilson Line that one may subtend as colinear -- in a Laplacian manner -- in delineation across the relatively norm-to-holomorphic end of the most holomorphically-placed end of the said Landau-Gisner Action that is to undergo its associated Fischler-Suskind-Mechanism.  This -- via the particular twining and motion of that mini-string that binds the whole said Mechanism -- causes the flush leveraging of the Higgs Action to move the Klein Bottle, while also causing the respective Higgs Action eigenstate involved in any given particular case to angle at 22.5 degrees  from straight up-and-down holomorphically in such a manner so as to move the corresponding Klein Bottle eigenstate to the left -- while causing the same Higgs Action eigenstate to angle at 22.5 degrees from straight up-and-down reverse-holomorphically in such a manner so as to move the corresponding Klein Bottle to the right.  Enough for now!  Sam Roach.        

A Little Clarification As To The Light-Cone-Gauge

The last three Planck-based motions of the Klein Bottle in any given arbitrary Kaeler-Metric eigen-based activity is a positional readjustment that allows the Klein Bottle -- via the Higgs Action -- to be able to move to a locally-based different general spot so that a Gaussian Transformation may occur at a slightly different location during an ensuing Kaeler-Metric eigen-based activity in terms of the utilization of the same Klein Bottle eigenstate.  This way, the same Klein Bottle eigenstate is able to be used for local Gaussian Transformations that are not of the same holonomic substrate in the same general region.
There are countless Klein Bottle eigenstates that multiplicitly move via the Kaeler-Metric eigencondition via one Higgs Action eigenstate per Klein Bottle eigenstate.  This way, relatively localized Higgs Action eigenstates are able to form relatively localized Gaussian Transformations indirectly so that local changes in norm-conditions that are essential for the freeing up of space in a general region may be more directly associated so that there is no chance for the inability of superstrings -- that are in need of reattaining permittivity so that the said strings may be the energy that these need to be so that superstrings and thus discrete reality may exist -- to lack the kinematic interchanges that are necessary so that Gaussian Transformations may happen to the said superstrings so that the said here given arbitrary norm conditions may occur so that such a reattaining of permittivity in discrete units of holonomic-based energy may occur.  The implied Klein Bottle eigenstates thence exist all over the place in their respective world-tubes so that wherever superstrings are relatively at, there is a basis of substrate in which the respective Higgs Acion eigenstates may be able to move the respective Klein Bottle eigenstates in such a manner so that Gaussian Transformations may occur for the reasons mentioned before.  Therefore, Wick Action eigenstates, Landau-Gisner Action eigenstates, and the holonomic substrate of Fischler-Suskind-Mechanism eigenstates also are multiplicitly displaced around the general world-tubes so that there may be a definitive basis for the ability of the Kaeler-Metric eigenconditions to happen in such a manner so that the necessary Gaussian Transformations may occur.  I will continue with the suspence later!  Sincerely, Sam.

How Gauge-Bosons Indirectly Cause The Kaeler-Metric

Gauge-bosons pluck second-ordered light-cone-gauge eigenstates like a harp, so as to form vibrations known of as second-ordered Schwinger Indices.  These Indices ripple throughout the respective substringular regions through a topological webbing known of as the Rarita Structure.  Schwinger Indices fork to both gravitational particles, norm-projections, and also to superstrings of discrete energy permittivity so that there may be a covariant correspondance between the basis of  gravity and the substringular regions that are from the Real Reimmanian Plane.  So, when norm projections that interact in a Gliossi manner upon the related substringular substrates so as to start to become spurious and Chern-Simmons over a brief Fourier Transformation, this said activity which here exists in any particular arbitrary given case, is the activity that pulls the Wick Action -- which is an arbitrary form of a Hausendorf Projection -- into the local field of the Landau-Gisner Action through a cohomology that forms between the said Wick Action and the Landau-Gisner Action that angles the mentioned Wick Action from a horizontally mapped Wilson Line in 22.5 degrees that may be subtended from four of the six dimensions that the Wick Action exists in so as to form a pseudo 90 degree relationship that works to initiate the Kaeler-Metric.  Such an activity causes a change in the Jacobian eigenbasis of any arbitrary given orbifold and/or orbifold eigenstate that alters the configuration of the norm-conditions of a given local region of superstrings.
A Hausendorf norm-state may occasionally form reverse chirality in their concavities that involve either one end being concave down and one end of the said given arbitrary projection being concave up under one type of circumstance, or, a Hausendorf norm-state may occasionally form reverse chirality in their concavities that involve the initial relative end being concave up and one end of the said given arbitary projection being concave up (given the same holomorphic Laplacian-Based mapping), or, a Hausendorf norm-state may occasionally form the same chirality in their concavities -- whether the ends under the same holomorphic Laplacian-Baed mapping are both concave up or both cocave down.  Yet, a Hausendorf Projection may only bear two ends that are of opposite concave-based chirality in a manner in so that the amplitude of the interior of what one would map in a Laplacian-Based manner would curve upward toward the general direction of what one would define of as the relative center of such a projection.  Such a condition is due to the situation that such parity helps to maintain the fractal modulae of the said type of projection in so that the projection will not fly apart over its course of helping in the continuous structuring and restructuring  of norm-conditions.  Again, norm-conditions in orbifolds and norm-conditions in orbifold eigenstates are changed over the course of any prolonged Fourier Transformations that are covariant so that energy may be freed up enough so that energy may kinematically interact so that energy may exist.  This condtion as to what Hausendorf Projections are is just a fact of life that is neither dangerous nor is it secret.
Campbell-Hausendorf Projections are less kinematically interactive with the rest of the substringular. This is due to the condition that such just stated projections, when taken individually, are far more limited in the amplitude of the Lagrangians that these differentiate through over any time-wise mapping of any covariant sequential series of Fourier Transformations that may be extrapolated over time.  Again, this is just the way things are.  I will begin the work of Course Ten tommorrow.  Again, I will continue with the suspence later!  Sincerely, Samuel Roach.    

About The Cohomologies During The Kaeler-Metric

When the Wick Action -- which is an arbitrary example of a Hausendorf Projection -- moves upon the Landau-Gisner Action, the subtended angling that a corelative Wick Action eigenstate bears upon its corresponding Landau-Gisner Action eigenstate when extrapolating it in the relative reverse- holomorphic general direction is 22.5 degrees in all of the local dimensions that may be described by the related Ward Neumman conditions from a Wilson Line that one would here map linearly horizontal from the norm-to-forward-holomorphic end of the respective Landau-Gisner Action eigenstate.  The Landau-Gisner Action is an arbitrary example of a Campbell/Hausendorf Projection.  As a Wick Action eigenstate acts upon a Landau-Gisner Action eigenstate to begin the process of a Kaeler-Metric eigenduration, the first-ordered point particles that comprise both norm-projection eigenstates that are here respectively mentioned are relatively uncompactified when in comparison to the first-ordered point particles that comprise superstrings during BRST.  The holonomic substringular topological "substance" that comprises the first-ordered point particles of both a Wick Action eigenstate and a Landau-Gisner eigenstate meshes torsion-wise to form a genus of cohomology.  This is so as to allow for the appropriate Gliossi interaction that allows the related Wick Action eigenstate and its corresponding Landau-Gisner Action eigenstate to directly interact so as to provide the proper type of leveraging of the Fischler-Suskind-Mechanism eigenstate that is here involved.  This is so that the related Klein Bottle eigenstate may be moved via the respective Higgs Action eigenstate.  Just as the related Wick Action eigenstate meshes at one end with the respective Landau-Gisner eigenstate here, the reverse-norm-to-forward-holomorphic end of the Landau-Gisner Action acts upon the Fischler-Suskind-Mechanism to form an overall cohomology that begins Rham while then becoming Doubolt at the reverse-norm-to-forward-holomorphic end of the relative Real Reimmanian Plane that is involved in this given arbitrary case.  The relative pulse of the Real Reimmanian Plane at the described "bottom" of the associated Plane causes the change in the Laplacian Ward Neumman topological norm conditions that causes the cohomological structure that is locally mapped here to convert from Rham to Doubolt at the singularity that may be described by where the associated Fischler-Suskind-Mechanism eigenstate initially reaches the said "bottom" of the related Real Reimmanian Plane eigencondition.  After an equal Laplacian-Based mapping delineation in the initial change of the norm-conditions of the Ward Neumman distribution of the respective Fischler-Suskind-Mechanism eigenstate, the associated Doubolt cohomological tracing of the said mechanism's eigenstate changes in displacement from going in the relative reverse-holomorphic direction to being displaced in the relative norm-to-forward-holomorphic direction.  As kinematic pressure is applied to the related Wick Action eigenstate as we begin here to describe how the Kaeler-Metric eigenduration happens here through time, the Landau-Gisner Action eigenstate here is pulled in the relative norm-to-reverse-holomorphic direction so as -- via the described Doubolt-related changes in norm translation -- to move the related Higgs Action eigenstate that is described here so as to move the related Klein Bottle eigenstate in the relative norm-to-forward-holomorphic direction so that the respective Klein Bottle eigenstate may move in the direction as to where the Kaeler-Metric is to kinematically interact with superstrings so that :  1)  The associated superstrings may reattain permittivity; 2)  The corresponding Fadeev-Popov-Traces may reattain impedance;  & 3)  Also so that, during gauge-transformations, the appropriate entropy may occur so that light may scatter in such a manner so that the related photons may not only requantize, yet, also so that there may be enough necessary chaos so that there may be changes in physical state.  I have more to discuss on this point, yet, my time is limited.  I will continue with the suspence later!  Sincerely, Sam Roach.      

More As To The Nature Of The Higgs Action

The Higgs Action is a general gauge-action that is multiplicitly existent througout the entirety of space-time-fabric. Each individual eigenstate of the Higgs Action is a closed string that bears an abelian wave-tug upon each individual Klein Bottle eigenstate. The field of each Higgs Action eigenstate is part of what one would think of as the whole state of any arbitrarily mentioned Higgs Action eigenstate. The Higgs Action is comprised of a two-dimensional superstring that comes to a smooth-curved-like edge that approaches being as an apex-shaped bosonic superstring as one follows the Laplacian delinieation of the interconnection in-between a given Higgs Action eigenstate and its corresponding Klein Bottle eigenstate -- which bears a rho, phi, and a theta Laplacian differentiation of a field that works to form a twelve-dimensional substringular/pointal-like field that is smaller in length that a two-dimensional string, yet larger than a first-ordered point particle. Such a bosonic-like field-networking of phenomena exists in a majorized Hilbert Space in the Laplacian conditions that exist per each individual instanton, while yet being transferred through a given arbitrary Lagrangian that is involved with the direction-based operation of the motion of the mentioned Higgs Action eigestate as a Gaussian Transformation is to be performed. The perturbation in the surrounding substringular fields that exist in the region near a given Higgs Action eigenstate form Njenhuis Tensors that interact with the surrounding Schwinger Indices so as to interact with the metrical activity of hadrons such as gluons so as to allow for the operation of the Wick Action. The operation of the Wick Action causes the Landau-Gisner Action to cause the Fischler-Suskind Mechanism so that the given Higg Action eigenstate may be leveraged to move the given Klein Bottle eigenstate so that a Kaeler-Metric may occur so that Gaussian Transformations may happen. Gaussian Transformations are essential so that norm-conditions may be kinematic so that energy may continue spontaneously and kinematically. So, undoing the Higgs Action or illucidating it would undo discrete charge, since 6.25*10^(18) = 1/1.6^(19).                                                      


So, please help to end the Hadron Colliding Experiment so that we may have a world.

Sincerely,

Sam.

A Description Of Campbell-Hausendorf Ghosts

A Campell-Hausendorf ghost is like a Campbell ghost except that it involves Campbell-Hausendorf norm-states. A Campbell-Hausendorf norm-state is comprised of a first-ordered point particle that is supplementally norm to what could arbitrarily be either a concave up half-parabollic shell of first-ordered point particles or a concave down half-parabollic shell of first-ordered point particles. The initial first-ordered point particle that I have recently mentioned would be considered to be in the norm to forward holomorphic positioning relative to the type of half-parabollic shell that the prior said first-ordered point particle is supplementally norm to. There are 191 mini-string interconnections that interconnect the originally stated arbitrary first-ordered point particle to the given half-parabollic shell -- whether the given shell is relatively concave up or concave down relative to such a shell being considered in the forward norm to antiholomorphic position. What I am describing is over the course of a basic Laplacian Transform, so that I am not here discussing how such configurations exist over periods that involve time. With Hausendorf norm-states, there are 191 mini-string interconnections that bind the two given shells of an arbitrary Hausendorf norm-state to each other. Yet, with a Campbell-Hausendorf norm-state, the mini-string interconnections are apexed at the norm to forward holomorphic described first-ordered point particle, while, with a Hausendorf norm-state, the described mini-string interconnections are evenly spaced along the Laplacian topology that interbinds the associated shells. So, Campbell-Hausendorf states tend to obey more of an abelian field nature than Hausendorf states. This is why the Wick Action causing the Landau-Gisner Action causing the Fischler-Suskind Mechanism is an arbitrary example of a progression of more and more abelian geometry that is used to leverage an ability of force. At this, such an "arbitrary" example is actually a the most primal example. So, the Higgs Action, acted upon by the Fischler-Suskind Mechanism, is the primal source of the abelian nature which acts as the "force" whereupon energy may recycle back into primal energy so that energy may exist.
Sincerely,
Sam.

More On The Importance Of Not Colliding Hadrons

E(8)XE(8) strings that are adjacent have a spin-orbital-momentum that is covariantly assymetric. This assymetric spin-orbit allows for this type of superstring to not collide with other of such superstrings. Hadrons of any sort are the bases of the holding together of orbifolds and orbifold eigenstates. Counterpart pairing hadrons have a Laplacian delineation that bears a symmetrism that is trivially isomorphic in terms of orbifolds and orbifold eigensets that comprise electromagnetic energy and in terms of kinetic energy, and is non-trivially isomorphic in terms of orbifolds and orbifold eigensets that comprise mass. So, the colliding of hadrons would cause an attempt to produce a contradiction to a fractor of the Pauli Exclusion Principle that could undue the ability of the Wick Action in such a way as to undue the operation of the Landau-Gisner Action. Such an undoing of the operation of the Landau-Gisner Action could cause a lack in the ability of the gauge-metrical activity of the Higgs Acton, thereby inhibiting the activity of the Kaeler Metric in a set regional locus. Detracting from the necessary Kaeler Metric eigenstates has the potential to undo the ability of the local superstrings that are in the region of the Hadron Colliding Experiment to regain the necessary permittivity to remain as the energy that these need to be so that such strings may even exist. Yet, the tendency of superstrings, since these operate over the delineation of homotopy, is to exist as discrete units of energy permittivity. Such a juxtaposition has the potential of fraying local sections of space-time that could form a black-hole or black-holes that have the potential of damaging earth. Local space-time fabric is to remain unfrayed, since black-holes have the ability of spreading rather quickly. So, please end the Hadron Colliding Experiment so that our planet may last. I am writing this out of a love for mankind. God Bless You, and you have a phenomenal day!
Sincerely,
Sam.

About E(8)xE(8) Gauge bosons

An orbifold is a structure that contains one basic set of superstrings. An orbifold bears a fractor of magnetism that is induced by the Majorana-Weyl covariance of the superstrings that it contains. An orbifold eigenset is a basic set of orbifolds. An orbifold eigenset bears a discrete magnetism that is induced by the Majorana-Weyl covariance of the orbifolds that is contains. A Majorana-Weyl  covariance is the codifferentiation of the magnetic indices of a subatomic phenomenon. Magnetic indices are Campbell norm and Hausendorf norm states that generate gauge-metric via the action of spin-orbit. So, as superstrings obtain a translation of spin-orbit, an orbifold bears a set of Campbell and/or Hausendorf indices that are generated through space to obtain a magnetic effect. The Campbell and Hausendorf indices here that are thence generated are Majorana-Weyl indices, and the codifferentiation of these magnetic indices is an example of Majorana-Weyl covariance. Likewise, as orbifolds obtain a translation of spin-orbit an orbifold bears a set of Campbell norm and/or Hausendorf norm indices that are generated through space to obtain a magnetic effect. These norm indices here that are thence generated are Majorana-Weyl indices, and the codifferentiation of these magnetic indices is an example of Majorana-Weyl covariance. The Majorana-Weyld indices of an orbifold are a fractor of the Majorana-Weyl indices of an orbifold eigenset. When an orbifold is connected to one or more orbifolds of an orbifold eigenset, there is a buffer connection between these orbifolds that is at the conicenter of the substringular field, made of mini-string, that helps to trigger the Wick Action. When an orbifold and/or and orbifold eigenset is "backgammoned" into a change of norm conditions in terms of the conformal invariance of the given orbifold and/or orbifold eigenset, this buffer connection known as an E(8)xE(8) gauge boson will torsion to pull/push to induce the Landau-Gisner Action to work through the Fischler-Suskind mechanism to trigger the Higgs Action to raise the Klein Bottle to the locus of superstrings that are running out of permittivity so that the Kaeler metric may happen to bring metric-gauge back to the discussed superstrings so that these may have the permittivity that these need to be the energy that these are so that energy may exist. The Kaeler metric also settles the vibration level of Fadeev-Popov-Ghosts so that these may have the impedence that these need to have so that the world will not be charred by an Imaginary Supercharge. Each time that the Kaeler metric goes through an iteration, at the time (metric) that the superstrings that were in the Klein bottle go into Regge Slope, the E(8)xE(8) gauge bosons are undone of torsion to allow for the associated superstrings to go through ultimon flow. Once the discussed superstrings are done with the Kaeler metric, the E(8)xE(8) superstrings not only stop having torsion, yet these become completely hermitian until Gaussian Transformation is to happen again. A Hausendorf Projection may be a Wick Action in terms of gauge-action when it is localied and directoralized toward the effecting of a Landau-Gisner Action during a metric when this effect is to occur. A Wick Action is always a Hausendorf Projection, yet a Hausendorf Projection is not always a Wick Action.

More On Mini-Loops

The mini-loops have a minimal diameter of 3*10^(-78) meters in the globally distinguishable, which amounts to a minimal diameter of 10^(-86) meters in the substringular. The mini-loops are evenly spaced between the bottom eighth theoretical potential from the bottoom of a one-dimensional superstring to the top eighth theoretical potential from the top of a one-dimensional superstring. The mini-loops are evenly spaced between the eighth from the antiholomorphic side taken counterclockwise of a two-dimensional superstring's theoretical position to the eighth theoretical position from the holomorphic side taken clockwise of a two-dimensional superstring. The mini-loops exist as a hermitianly torsioned hoop that acts as a majorized substringular field. The mini-loops begin relatively large, and decrease in size as the metric-gauge is generally depleated from an associated superstring to conform to (e^((del C)-iG))/# of mini-loops =~Multiplicative factor for mini-loops of one-d superstrings

or 2*((e^((del C)-iG))/# of mini-loops) =~The multiplicative factor for mini-loops of two-d strings
The mini-loops are depleted as metric-gauge is depleted. The distribution divergence of the said mini-loops is Diracly increased or maintained as the number of mini-loops decreases, with the exception of when a one or two-dimensional string has 100 mini-loops, respectively. This is since mini-loops act as the gauge-action which enables the metric-gauge to exist in superstrings, not including the fact that one-d strings have one spatial partition, and two-d strings have two spatial partitions, and two-d strings have partition at (width (at 90 degrees)), & (thickness (at 270 degrees)). These allow for the Polyakov Action which is group caused by the partitions, and the superstrings area brought along ultimon flow because of the metric-gauge brought about by the gauge-action gauge-metrics of the mini-loops.

There is always a relative spuriousness to a superstring that has 100 mini-loops of the substance of metric-gauge before the associated superstring undergoes a Kaeler metric. ((e^0/1)-iG) then equals 1-i. This "1-i" is a multiplicative factor here.

This is due to that the borne tangency of the Gliossi-Indices are then the "life-support" (metaphorical) of the remaining permittivity of the associated superstring. This is since Cassimer Invariance is maximized during the Wick action that causes the Landau-Gisner Action that works through the Fischler-Suskind Mechanism that works the Higgs Action to move the Klein Bottle to allow the Kaeler Metric to happen. This latter activity is known as the substringularly natural mechanism of a Gaussian Transformation.

FTAAN, Session 13

When a superstring is superconformally invariant it is limited in its sway of differentiation. Let us consider the differentiation of the superconformal superstrings of a gluon. The superstrings of a gluon are two-dimensional. These superstrings do not transversally differentiate in a relatively transient period of time, nor do these superstrings kinematically differentiate off of the Real Reimmanian plane after a quantum metric per iteration after the core of BRST has begun in terms of any Kaeler metric outside of the activity that transpires during the instanton-quaternionic-field-impulse that associates here directly with the given gluon. Yet, per iteration the given two-dimensional superstrings differentiate at different radial loci that may be mapped out by considering the Planck associated tendencies that accompany the gauge-metric wave-tug pressures that pull the given superstrings toward or away from the neighborhood of the superstring's field. The two-dimensional superstrings will begin in a polarized to holomorphic position that is pure Gaussian relative to the field of orbifold eigenset differentiation. The given superstrings will then turn counterclockwise one radian relative to the holomorphic position at the next iteration. The given superstrings will then turn clockwise one radian relative to the holomorphic position at the next iteration. The given superstrings will then pull clockwise as before one more radian at the next iteration. The given superstrings will then turn counterclockwise one radian at the next iteration relative to the holomorphic position. The given superstrings will then tip holomorphically one radian in the next iteration. Then, per iteration, the given superstrings will tip antiholomorphically twice one radian at a time per iteration. Then, the given superstring will tip holomorphically one radian at the next iteration This happens after many iterations at the core of BRST. This will happen until the Landau-Gisner action in automated by a change of Gaussian that happens via a physical perturbation to the given gluon.

FTAAN, Session 4

Physical phenomena may be perturbative or it may be non-perturbative. When a superstring and/or its singularity that binds the given superstring to another superstrings, or when an orbifold and/or its singularities that bind this orbifold to other orbifolds is perturbative, the vibration of these perturbative phenomena is Cevita energy. The vibration of perturbative substringular phenomena is the perturbation itself taken on a kinematic basis. This type of vibration is not just the Cevita world-sheet mapping of the anharmonic motion of a substringular phenomenon, yet this type of vibration is the non-linear/inexact redistribution/redifferentiation of the point particles that surround the given Cevita kinematism. The Cevita kinematism is a Chern-Simmons metric-gauge that is altered in its inertial flow by the Wick Action of the given holonomy in its euclidean or euler Ward time-oriented differential conditions. This metric-gauge is therefore altered in holonomity and holomorphism through a change in the Lagrangian conditions of the Dirac or Clifford substringular Hamiltonian basis. As the Hamiltonian matrix is altered in terms of the kinematism of the physical Gaussian basis, the Jacobian eigenbasis is altered just as the metric-gauge is altered to form a reverse holomorphicity as the Wick Action indicates. The alteration in the Jacobian eigenbasis signals the Landau-Gisner Action via mini-string to produce the activity of the action that moves the Klein Bottle to allow the Ricci Scalar to bring superstrings that lack metric-gauge to perform the Kaeler metric. The Kaeler metric is performed via the 22and1/2 degree rock-sway/45 degree 2-D/90 degree 3-D integrated into 12 dimensions sway of the Klein bottle to the superstrings that allows a holomorphic/antiholomorphic sway to allow the superstrings to be given metric-gauge within this Schotky Construction. The amount of need for Kaeler metric is provided for by the degree of Higgs Action. The degree of Higgs Action is provided for by the degree of Landau-Gisner Action. The Landau-Gisner Action degree is provided by the light-cone-gauge eigenbasis differential kinematic mini-strings that are activated proportionably to the perturbation for the Gaussian norm eigenbasis.