Showing posts with label Gauge-Transformations. Show all posts
Showing posts with label Gauge-Transformations. Show all posts
Monday, November 27, 2017
Part Of As To Why Gauge-Transformations Are Thus Called
When a photon is to strike the externalized core-field-density of a given arbitrary light-cone-gauge eigenstate, that is of another discrete quantum of energy, in a Gliosis-based manner -- the said respective photon that had just been scattered by coming into a direct contact with another discrete quantum of energy, over the immediately ensuing 384 consecutive iterations of group-related instanton, is to go from working to bear a Yang-Mills light-cone-gauge topology, into working to bear a Kaluza-Klein light-cone-gauge topology, while then, after the completion of the so-mentioned 384 consecutive iterations of group-related instanton, the so-stated photon is to return to then bearing a Yang-Mills light-cone-gauge topology. This general tendency is to happen, every time that a photon is to scatter upon another discrete quantum of energy. The directly corresponding genus of Gaussian Transformation, that is related to that type of Fourier Transformation, that is here to be involved with any given arbitrary scattering of light that is to happen when discrete energy is Gliosis to the Kahler-Metric, is known of as a gauge-transformation. In the process of such a general genus of activity, that is here to act in so as to work to remold second-ordered light-cone-gauge eigenstates -- into more of an innate Yukawa inter-relattionship with their directly corresponding gauge-bosons, the multiplicit discrete quantum of energy impedance, that is directly correlative, is here, to then act in so as to re-attain those fractals of discrete energy impedance that these need to re-attain, so that discrete energy impedance may both persist and exist, over time. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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energy,
Gauge-Bosons,
Gauge-Transformations,
impedance,
instanton,
Kaluza-Klein,
light-cone-gauge eigenstates,
superstrings,
Yang-Mills
Tuesday, June 6, 2017
As To Different Genre Of Gauge-Transformations
When different forms of electromagnetic energy are to strike either any given arbitrary Calabi-Yau space, Calabi-Wilson-Gordan space, or any Calabi-Calabi space manifold-type of phenomenology -- a different given arbitrary genre of a gauge-transformation is to happen. Different genre of gauge-transformations, work to help at forming different tenses of a shimmering -- of those directly corresponding light-cone-gauge eigenstates, that are to be struck by such so-eluded-to photons in a Gliosis-based manner, over time. Such different tenses of gauge-tranformation, tend to work to help at causing different tenses of metrical-based Chern-Simons singularities, over time. This just mentioned tendency, tends to work at forming different genre of the consequently formed Schwinger-Indices -- by which such Schwinger-Indices are to here to act as gravity waves. Such a unique set of gravity waves, tend to act to make the multiplicit Calabi-based spaces -- to behave in their unique correlative ways -- as such gravity waves are to here to be propagated along the directly corresponding multiplicit Rarita Structure eigenstates, over time.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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Calabi-Yau,
Chern-Simons,
eigenstates,
Gauge-Transformations,
gravity waves,
light-cone-gauge,
metrical-based,
Rarita Structure,
Schwinger-Indices
Friday, May 26, 2017
Gaussian Transformations Versus Gauge-Transformations
When there is to be a Gaussian Transformation anywhere in the substringular realm-- to where this of which, what I mean of here in this case -- is when a given arbitrary set of one or more superstrings of discrete energy permittivity is most Yukawa to the Kahler-Metric, -- then, the said respective given arbitrary set of superstrings that are to here be undergoing such a Gaussian Transformation -- are to here both be working to re-attain their needed fractals of discrete energy quanta in order to both exist and persist as discrete energy quanta, as well as to here be working in so as to move in the qualitative direction of having the Ward-Caucy-based conditions of a more ordered proximal localized spatial tense, over the directly correlative and applicable sequential series of group-related instantons, through which such a so-stated set of one or more superstrings are to be undergoing such a said Transformation. Furthermore -- a gauge-tranformation, as I describe it, is general genus of a given arbitrary Gaussian Transformation -- that is to here be directly involving those eigenindices of discrete energy quanta, that are to be most Yukawa to the process of the scattering of electromagnetic energy, over time.
Later in this course as to the nature of Calabi-based interactions, I will explain further -- the differences as to how the respective proximal local eigenindices of the correlative group-metrics of certain Fourier-based Transformations -- that are to here be most directly related to the Kahler-Metric -- are to behave differently in the case of a gauge-transformation, versus how such so-eluded-to eigenindices are to behave in more of a case of a more preverbial translation of other of such Gaussian Transformations that are to happen in the substringular elsewhere, over time.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
Later in this course as to the nature of Calabi-based interactions, I will explain further -- the differences as to how the respective proximal local eigenindices of the correlative group-metrics of certain Fourier-based Transformations -- that are to here be most directly related to the Kahler-Metric -- are to behave differently in the case of a gauge-transformation, versus how such so-eluded-to eigenindices are to behave in more of a case of a more preverbial translation of other of such Gaussian Transformations that are to happen in the substringular elsewhere, over time.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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Calabi,
eigenindices,
Fourier,
Gauge-Transformations,
Gaussian Transformations,
Kahler-Metric,
substringular,
superstrings,
Ward-Caucy,
Yukawa
Friday, July 26, 2013
A Little Dittie To Help Explain Some Stuff
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 differentiation 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 re-attain 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 re-attainment of discrete energy permittivity and the activity of the re-attainment 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 re-displacements 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
God Bless You, and you have a great day! Sincerely, Sam Roach
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Gauge-Transformations,
Kaeler-Metric,
Njenhuis
Thursday, March 21, 2013
A Little Bit Of An Explaination of discrete permittivity and impedance
As superstrings differentiate over time, their discrete permittivity begins to "wear-out." When the discrete permittivity of superstrings starts to wear-out, the discrete impedance of their directly corresponding Fadeev-Popov-Trace eigenstates begins to wear-out over the course of the same general group metric. When such an initial loss of discrete permittivity and such a loss of discrete impedance in superstrings and their directly corresponding Fadeev-Popov-Trace eigenstates respecitively happens to the point that such metric-gauge is almost fully depleted, then, the said superstrings and their corresponding Fadeev-Popov-Trace eigenstates go through what is known of as a Kaeler-Metric so that both superstrings may reattain discrete permittivity and so that their field trajectory (PLP) may reattain their discrete impedance. As this happen, the Kaeler-Metric happens in such a manner so that -- not only will the substringular phenomena that I have just mentioned will reattain their respective permttivity and impedance, yet, also so that norm-conditions may change over the course of Gaussian Transformation-based metrical activity. Gaussian Transformations that involve the scattering of light are known of as gauge-transformations. Gauge-Transformations work to allow for entropy -- which is essential so that physical states may change. The arena of the knowledge of gauge-transformations will be more thoroughly discussed in course 20 about Calabi-Interactions. The discrete energy permittivity and the discrete energy impedance that the substringular reattains bears the prior mentioned geni of fractaled Njenhuity that is based upon the condition that certain phenomena sometimes may be able to travel to different sets of parallel universes. Also, this bears upon the condition of what happens during Ultimon Flow. This way, phenomena may bear some sort of association with all of the other phenomena in space-time-fabric -- so that such a "fabric" may be of a space-time-continuum. Enough for now! Sincerely, Samuel David Roach.
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Gauge-Transformations,
Gaussian Transformations,
Njenhuity
Thursday, March 8, 2012
What makes Gauge-Transformations So Special
Gauge-Transformations are an arbitrary example of Gaussian Transformations. Gauge-Transformations happen when electromagnetic energy scatters. Gauge-Transformations are what in general produces entropy. The physical activity that differentiates gauge-transformations from other Gaussian Transformations is that, during a gauge-transformation, not only do superstrings "shake" from within an eigenstate of the Klein Bottle, yet, the holonomic entity of the said Klein Bottle eigenstate here shakes through the Lagrangian of a bilateral coniaxial that may be mapped in a Laplacian manner at the center of the conipoint of the said holonomic entity of the said Klein Bottle eigenstate. Yet, with other Gaussian Transformations, as the superstrings that "skake", so as to reattain the permittivity that these need to be discrete energy, from within a here given arbitrary Klein Bottle eigenstate, the holonomic entity of the here mentioned Klein Bottle eigenstate remains covariantly stationary per each metric in which the correlative superstrings that are here reattaining permittivity are "shook" so as to regain the said permittivity that these need so that the related superstrings may remain as discrete units of energy permittivity. So, the individual eigenmetrics of Kaeler-Metric in gauge-transformations involve a bilateral wobble through a tightly-knit Lagrangian that may be mapped in the general locus of where the said Klein Bottle eigenstate is at during each of such described eigenmetrics, while the individual eigenmetrics of Kaeler-Metric in other Gaussian Transformations involve no covariantly viable shaking in the holonomic entity of the related Klein Bottle during the individual eigenmetrics that involve their respective Kaeler-Metric eigenstates. The shaking of the given Klein Bottle eigenstates that happens during gauge-transformations produces an anharmonic shift in loci of Rarita Structure eigenstates that causes enough lack of discrete order so as to allow for those perturbations that cause the potentially needed reorganizations of the related Campbell, Hausendorf, and Campbell-Hausendorf Projections that increase the expectation value as to the ability of substringular subspaces to be able to maximize their agility in terms of their ability to help handle any given arbitrary alterations in norm-conditons. These perturbations may spontaneously be needed so that the kinematic translations of norm-conditions, that may be necessary so that Fourier Transformations will not be bogged up, may be able to happen. Sincerely, Sam Roach.
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bilateral coniaxial,
Campbell index,
Campbell-Hausendorf Profections,
eigenmetrics,
Fourier,
Gauge-Transformations,
Gaussian,
Hilbert Lagrangian,
holonomic,
Kaeler-Metric,
Klein Bottle,
Laplacian
Saturday, February 12, 2011
Course #9 -- Course One on Fock Space and the Light-Cone-Gauge, Session One
Well hello again world, this is Sam Roach here! I am here today to provide an introduction to my first course on Fock Space and the Light-Cone-Gauge. Here we go!
Point particles do a vast amount of their kinematic differentiation in-between the durations of individual instantons. The duration of an instanton is what I call an iteration of the substringular as a unit. First-Ordered point particles may be explained by a Gaussian set per the successive series of the Laplacian conditions that work to define the Ward Norm conditions of both the substringular differential geometries through multiplicitly arrayed Fourier Transformations, as well as helping to determine the Ward Norm conditons of the norm-state differential geometries which are also multiplicitly arrayed through Fourier Transformations. The interacion of the multiplicit Fourier Transformations of ground-states along with and including the multiplicit Fourier Transformations of norm-states forms the basis of kinematics, whereby, through a successive series of instantons, forms the procession of the activities of space via the integrable variations of time. First-Ordered point particles of our set of parallel universes are associated with Imaginary (as opposed to Real Reimmanian) indices in the Gaussian positions ranging just over 0 to 32piI. First-Ordered point particles of the central set of parallel universes may be explained relative to our universe with numbers in the Gaussian positions ranging from just over 32piI to 64piI. First-Ordered point particles relating to the opposite side of the Ultimon in terms of this set of parallel universes may be explained relative to our universe with numbers in the Gaussian positions ranging from just over 64piI to 96piI. This corresponds to the condition that our Overall-Physical-Portion of space and time has 96 spacial dimensions plus time, & imaginary charge may be up to 96piIev per BTU that it associates with. Any added imaginary charge density is automatically scattered from whatever source that the holonomic radiation that is being expelled is interacting with. The Gaussian format of any particular space -- here we are talking about any particular orbifold -- must be the same, unless there is a Gaussian Transformation that alters the mentioned format. The interaction of the countless Fourier Transformations causes the constantly inevitable conditions that cause Gaussian Transformations to happen all the time at various places over time. Gauge-Transformations are the most common form of Gaussian Transformations. Gauge-Transformations happen when the light-cone-gauge topology changes. This happens (gauge-transformations) whenever photons scatter upon anything. I hope that this is a good start to my ninth course! Bless You, One and All! Sincerely, Sam.
Point particles do a vast amount of their kinematic differentiation in-between the durations of individual instantons. The duration of an instanton is what I call an iteration of the substringular as a unit. First-Ordered point particles may be explained by a Gaussian set per the successive series of the Laplacian conditions that work to define the Ward Norm conditions of both the substringular differential geometries through multiplicitly arrayed Fourier Transformations, as well as helping to determine the Ward Norm conditons of the norm-state differential geometries which are also multiplicitly arrayed through Fourier Transformations. The interacion of the multiplicit Fourier Transformations of ground-states along with and including the multiplicit Fourier Transformations of norm-states forms the basis of kinematics, whereby, through a successive series of instantons, forms the procession of the activities of space via the integrable variations of time. First-Ordered point particles of our set of parallel universes are associated with Imaginary (as opposed to Real Reimmanian) indices in the Gaussian positions ranging just over 0 to 32piI. First-Ordered point particles of the central set of parallel universes may be explained relative to our universe with numbers in the Gaussian positions ranging from just over 32piI to 64piI. First-Ordered point particles relating to the opposite side of the Ultimon in terms of this set of parallel universes may be explained relative to our universe with numbers in the Gaussian positions ranging from just over 64piI to 96piI. This corresponds to the condition that our Overall-Physical-Portion of space and time has 96 spacial dimensions plus time, & imaginary charge may be up to 96piIev per BTU that it associates with. Any added imaginary charge density is automatically scattered from whatever source that the holonomic radiation that is being expelled is interacting with. The Gaussian format of any particular space -- here we are talking about any particular orbifold -- must be the same, unless there is a Gaussian Transformation that alters the mentioned format. The interaction of the countless Fourier Transformations causes the constantly inevitable conditions that cause Gaussian Transformations to happen all the time at various places over time. Gauge-Transformations are the most common form of Gaussian Transformations. Gauge-Transformations happen when the light-cone-gauge topology changes. This happens (gauge-transformations) whenever photons scatter upon anything. I hope that this is a good start to my ninth course! Bless You, One and All! Sincerely, Sam.
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Fourier Transformations,
Gauge-Transformations,
Gaussian set,
instantons,
orbifolds,
second-ordered point particles,
Ultimon Flow,
Ward Norm conditions
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