A Little Bit Of Knowledge To Help You

---

                   

Hello, this is Sam Roach here. I am about to ellaborate as to the discussion that I wrote about the other time that I was on linkedin. I am sorry that the computer elliminated my explaination that I went out of my way to initially type. Well, anyhow, here goes a redo and I sure hope that no hacker takes this one away! The actual motion of gluons causes the existence of the Wick Action. The Wick Action is an arbitrary example of a Hausendorf Projection. The activity of the Wick Action causes the Landau-Gisner-Action to move in such a manner so as to produce the leverage operation known as the Fischler-Suskind-Mechanism. The Fischler-Suskind-Mechansim moves the Higgs Action in the proper directoralization so as to move Klein Bottle eigenstates to the proper loci so as to allow for the Kaeler Metric. The Kaeler Metric allows for Gaussian Transformations. Gaussian Transformations allow for changes in norm-conditions that are necessary for the spontaneous kinematic differention of Fourier Transformations. Gaussian Transformations that directly involve the activity of Njenhuis tensors that act upon these in the process of the covariant translation of phenomena that are going through an arbitrary Gaussian Tranformation always involve the scattering of electromagnetic energy and/or the activity of entropy. Such Gaussian Transformations are known of as gauge-transformations. So, whenever there is a change of physical state and/or wherever light strikes something, there is a gauge-transformation.The Kaeler Metric allows for superstrings to reatain discrete energy permittivity, as well as allowing the field trajectory of the mentioned superstrings to reatain discrete energy impedance. If the directly prior did not happen, discrete energy would not exist. The Kaeler Metric always involves a Gaussian Transformation. The activity of the reatainment of discrete energy permittivity and the activity of the reatainment of discrete energy impedance produces alterations in the covariant displacement that are involved in the kinematic Fourier Translation of superstrings so that the sequential series of the integrated redisplacements of superstrings may differentiate among each other without interfering with other of such activities of other superstrings. So, the Higgs Action is not only essential for the interaction of E.M. with other phenomena and the existence and kinematic differentiation of entropy, yet, the Higgs Action also allows for the covariant redistribution of superstrings among each other without the condition of superstrings interfering with each other's space.
God Bless You, and you have a great day! Sincerely, Sam Roach.        

More About the Activity of the Kaeler Metric

More About the Activity of the Kaeler Metric


                
The Kaeler Metric is active over the course of 191 iterations of Ultimon Flow. The iterations of the Kaeler Metric, when it is active, are right after a superstring or a set of superstrings falls into the Klein Bottle, which is right after instanton. When the Kaeler Metric is active, it also happens right before the Regge Action. The Kaeler Metric happens in a minimum of two cycles, with 191 iterations of Ultimon Flow before it is interactive with the shaking of superstrings in the Klein Bottle & 191 iterations of Ultimon Flow after it is interactive with the shaking of superstrings in the Klein Bottle. This means that a Kaeler Metric provides a process of recreating enough permittivity in superstrings for a minimum of two sets of superstrings (at least one superstring per set). So, the overall activity of a Higgs Action eigenstate is interactive upon a specific substringular local region for a minimum of 764 iterations of Ultimon Flow. This is because the kinematic interaction of a Higgs Action eigenstate upon a specific local region in the substringular has its 382nd iteration (which is in-between instantons) at one Planck Length from where it started, while yet needing another group eigenmetric of iterations (again, in-between instantons) to go back to the same locus from where it started. Yet, Gaussian Transformations are always happening somewhere in the substringular at many substringular neighborhoods that are adjacent. So, Higgs Action eigenstates are constantly busy. The more perturbative the substringular region, the more busy the local Higgs Action eigenstates are.in that region. The Hausendorf Projections that happen right before the Wick Action help Higgs Action eigenstates to commute to the proper settings where these may be used as the "force" that transports the Klein Bottle eigenstates to allow the Kaeler Metric to allow superstrings to reattain their permittivity.

                                                                    

About the Metrical Activity That Occurs During the Kaeler-Metric

When a superstring is to go into a Kaeler Metric, its instanton prior to an eigenmetric of Kaeler Metric is at the same rate as usual (based on the present rate of instanton of 10^(-43) seconds), yet the metric-gauge of a given superstring that is to undergo the given Kaeler Metric is to be topologically indiscrete immediately after the described instanton. Immediately after the given instanton, the described superstring takes 1/240th of an h bar time to fall at a 22.5 degree angle into an eigenstate of a Klein Bottle. The superstring described is then shaken back-and-forth 8 times (for a total of 16 sways) at as even rate to help make an eigenstate of the associated superstring's metric-gauge to be discrete. The overall given metric of eight back-and-forth sways takes 1/240th h bar time. The described superstring then goes into the Regge Action for 1/240th h bar time. The associated superstring, then, takes 79/80th h bar time to circle its set of parallel universes that it belongs to before falling into an eigenstate of one of the Main Heterotic Strings that work to interconnect the three sets of parallel universes that I have recently mentioned. Regge Action normally takes 1/80th h bar time to happen. (Regge Action is the beginning of Ultimon Flow in-between iterations.) When a superstring is fully contracted, the Polyakov Action simplly permutates the arrangement of the said superstring's first-ordered point particles, yet, since the associated counterstring permutates the same way with the same multiplicit holomorphicity, the Grassman Constant may be maintained when during Bette Action, allowing a superstring in Noether Flow to remain orientable and thus non-tachyonic. 




By Samuel Roach, Blogger at SamsPhysicsWorld                    
                          

Extra On The Higgs Action

When a Higgs Action reverses in relative directoralization, the “vacuumed pouch”

                    
that is Dirac relative to the Higgs Action hermitianly changes in its second derivative. It

will reverse the concavity of the mini-loop hermitian singularities that exist as the gauge-

action field sub-quantum that exist between a superstring and its associated light-cone-

gauge eigenstate. Look. As Kaeler metric happens, gauge bosons pluck the assocaitaed

second-ordered light-cone-gauge eigenstates, as is always the case during BRST. The

scattering of the norm-conditions in the Klein Bottle, also seeing that a superstring in the

substringular (fully contracted here) has a length (1-D) or circumference (2-D) of 10^

(-43) meters, inverts the vibratory holomorphicity of the associated Schwinger Index

away from the Rarita Structure. Such an inverted vibration increases the impedance of

a Fadeev-Popov-Trace while it allows for the increase in permittivity of the associated

superstring. Again, gauge-bosons have twice the circumference of a two-dimensional

regular superstring. Each Kaeler metric in a superconformal Fourier Klein Bottle

transformation during a Gaussian Transformation equally increases the metric-gauge

potential of the superstrings, while increasing the metric-impedance potential of the

superstrings’ associated Fadeev-Popov-Trace or Planck phenomenon related phenomena.                   

Part One of the Second Session of Course 9

There are discrepencies in the normalizations between Planck phenomenon related phenomena.  Planck phenomenon related phenomena of our universe are normal with a discrepency of ~1.104735878*10^(-81)i degrees.  Such stated phenomena of the furthest parallel universe in our set of parallel      universes are normal to ours with a discrepency of 32piI degrees.  I can imagine that some people are thinking, "Any charge that is divisible by piI degrees is zero!", yet, if such a number involves the scalar of a charge that  is linearly delineated through a transversal Lagrangian, then, instead, it bears a discrete and definetive value and thereby a discrete and definitive charge.  This means that the parallel universe that is farthest from ours has Planck phenomenon related phenomena normal to ours when one discounts a 32 dimensional separation from our universe.  Each parallel universe has such mentioned phenomena that are normal to each other with a discrepency due to a wobble during each successive instanton of ~1.104735878*10(-81)i degrees.  This corresponds to the wobble of the mentioned related phenomena from within their iterations and reiterations.  So, Planck phenomenon related phenomena that are adjacent to each other and are of the same universe are basically normal (meaning to have an orphoganol relationship in terms of corresponding differential geometry) -- except for the fact that such mentioned related phenomena  wobble during iteration not only by the angle that was previously described, yet, also through the gauge-metrical activity of  close to 100,000 back-and-forth motions per each successive instanton.  The operation of the space-hole  that helps to set the condition of an ensuing Kaeler Metric is involved with the fact that the mentioned related phenomena do not always wobble back-and-forth exactly 100,000 times during the successive course of each multiplicit instanton.  If Planck phenomenon related phenomena were to wobble more than these should during the course of an arbitrary individual instanton in an arbitrary locus, this could form a fissure in space-time-fabric -- since during the successive series of a Kaeler Metric, Planck phenomenon related phenomena must wobble half as much so as to allow for the gauge-activities of the Kaeler Metric eigenstate and the Regge Action eigenstates to both happen right before Ultimon Flow.  I will explain why that is right here.  When the Kaeler Metric is happening in a given locus over the course of sets of 191 instantons per group eigenmetric at the substringular neighborhood where the mentioned Metric is operational at, the duration that would normally occur for just the Regge Action is split into two durations of equal scalar "tempos" -- one for each Kaeler Metric eigenstate and one for each Regge Action eigenstate.  The reorganization of the Gaussian Matrices that happens over the duration in which the "space-hole" and the Basis of Light is kinematic right before instanton-quaternionic-field-impulse works to cause the Wick Action to be brought into motion when the Jacobian eigenbasis of an orbifold or when the Jacobian eigenbasis of an orbifold eigenstate is to change in terms of general Norm Ward Conditions.  The 100,000 back-and-forth wobbling motions of a Planck Phenomon related phenomena happens specifically during BRST to help prepare for the general duration of the Regge Action -- and the Regge Action is what converts the Hamiltonian Operation of the light-cone-gauge during BRST into the multiplicit group wave-tug permittivity that causes superstrings to cycle the Ultimon in-between each instanton.  So, if a Regge Action eigenstate is prepared to operate in half of its normal duration, then, the Planck phenomenon related phenomena that act as the local discrete units of energy impedance must thereby wobble half as much during BRST so as to allow for the added kinematic "drive" that allows for the necessary related Kaeler Metric eigenstate to happen at the latter part of the duration of an arbitrary instanton eigenstate that happens in a given arbitrary locus where a Gaussian Transformation is taking place.  This means that the wobble of the described discrete units of energy impedance here would transpire with half the sub-frequency that it would otherwise occur at so as to allow the initial activity of the light-cone-gauge to bring into motion both the here necessary Kaeler Metric eigenstate and the here necessary Regge Action eigenstate.  How does the wobbling slow down so as to allow what I just said to happpen?  When a Gaussian Transformation is to occur -- whether such a transformation is to be a gauge-transformation or not -- their is a fractor of a multiplicit dipole moment that mainly operates between what is encoded to form two orbifolds and/or that mainly operates between what is encoded to form two orbifold eigenstates.  This is so as to allow for a minimum of two local Gaussian Transformations that will consequently change the Norm Ward Conditions of a minimum of two orbifolds and/or will consequently change the Norm Ward Conditions of a minimum of two orbifold eigensets.  Such a fractor of a dipole moment at such a small scale slows the wobbling of the directly associated Planck phenomenon related phenomena that still sway over a common duration of BRST. (Although, over the last close to 13.7 billion "terrestrial" years, instanton duration has mildly slowed.)  Consequently, the less back-and-forth wobbling of the described discrete units of energy impedance allows for the motion of the light-cone-gauge during BRST to be able to bear the duration of an arbitrary Kaeler Metric eigenstate while allowing an equal duration in a relatively quicker Regge Action.  I am only able to explain so much at once.  I really appreaciate your reading!  God Bless You in the name of Yahweh!  Sincerely, Sam.                                                                                                                  

A Little Bit More Of AN Explanation For Contractions

During Polyakov Action, a superstring seperates its first-ordered point particles in an overall      homeomoriphic manner so that the given superstring is uncontracted into the size that it must appear as as according to the associated Lorentz-Four-Contractions.  So, when a superstring related to a form of electromagnetic energy (the superstring here being of itself bosonic) is to go through Polyakov Action, its mild amount of dissociation is a mere yet relatively local disconbobulation in the Ward Newmann Conditions of the described superstring -- yet without any expansion in the holonimic "tapestry" of the associated string.  So, the increased sub-dimensional volume that exists in-between the first-ordered part particles that comprise a superstring is to the extent of a reverse-engineering of the apparent size of the superstring based on the present Lorentz-Four-Contractions that are here acting upon the described string.   Such Polyakov Action, the Bette Action, and the Imaginary Exchange of Real Residue all happen during  instanton as well as during BRST, while the Kaeler Metric and the Regge Action happen immediately after instanton.  So, if a superstring is to go into an eigenmetric of a Kaeler Metric metric-gauge-eigencondition, then the gauge-metrics of the associated eigenaction of the Kaeler Metric happens at the same overall rate as the ensuing Regge Action.  If the Kaeler Metric is not kinematic during a set of substringular instantons, then the Regge Action happens during half of the duration that it would undertake if it were not for the activity of the local eigenstate of Kaeler Metric.  So, when without Kaeler Metric, Regge Action happens in the duration of half of its otherwise speed  When  superstrings enter a Klein Bottle eigenstate-like metric-gauge, these upon contact with the topology of the top of the associated Schotky Construction, recontract to the extent of a fully contracted superstring.
Gotta Run!  I hope you have a phenomenal day!  Sincerely, Sam.    

A Little About Sam Roach

Hello. My name is Samuel David Roach. I have been writing string theory since 1992.

I wrote and compilesd 32 courses on string theory between March of 2001 and August of 2008.

I have written many addendums on those courses since.

I wrote a lot of string theory in-between 1992 and 2001.

I have come up with a lot of inventions since 2000. I had a patent lawyer named James M.Deimen whom I saw between 2000 and 2007.

I first came up with an idea on cold fusion by the beginning of 1998, yet, I did not actually see a patent lawyer until September of 2000.

I have a post already on my blog that mathematically proves the dangers of the Hadron colliding experiment. I am here to serve.

Please read my writings carefully, and feel free to comment on them.

Dialogue to me means "I'm wrong, you're wrong, I'm right, you're right, let's talk."

I perceive that I am getting closer and closer to the truth over the years.

The Higgs Action is a gauge-action/metric-gauge-like phenomena that is smaller than a superstring yet bigger than a point particle. It may be extrapolated, yet it may never be illucidated. Please read my writings for further detail, and may the "force" (the Higgs Action) be with you! (Serious play on words). If you have any questions, please ask these in the comment section. Without the Higgs Action, there would be no superstrings, since the Higgs Action turns Hamiltonian momentum that lacks permittivity into superstrings via the Kaeler Metric. Please read more to learn. My website is samsphysicsworld@blogspot.com.

Sincerely,

Samuel David Roach