The multiplicity of the general interaction, of entropic tachyon-related photons (which tend to bear the combination, of having both a Khovanov geometry, along with a Kaluza-Klein light-cone-gauge topology), with discrete energy quanta, that are here of the nature of working to bear a tachyon-related tense of kinetic energy (which tend to bear the combination, of having both a Khovanov geometry, along with a Yang-Mills light-cone-gauge topology), — works to facilitate the general processes, by which the “wear-and-tear,” that is here to be attributable, to what may often tend to happen to a worm-hole, when it has been utilized enough times, is often thereby to be able to happen to such a space-time-related “shortcut,” if it has been exacerbated, over the potential combination of both a lot of usage, along With a long duration that it may have been present, at some given arbitrary covariant region of space. Sincerely, SAMUEL DAVID ROACH.
Showing posts with label geometry. Show all posts
Showing posts with label geometry. Show all posts
Saturday, December 26, 2020
“Wear-And-Tear” Upon A Worm-Hole
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geometry,
Kaluza-Klein,
light-cone-gauge,
photons,
space,
tachyon,
time,
topology,
wear-and-tear,
worm-hole,
Yang-Mills
Friday, December 18, 2020
A Charged Diffeomorphic Field
A charged diffeomorphic field tends to work to form a more harmonic tense of magnetism, than a similar charged field, that is, instead, to not work to bear a diffeomorphic geometry. Sincerely, SAM ROACH.
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charged,
diffeomorphic,
field,
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magnetism,
work
Thursday, May 21, 2020
Second-Order Light-Cone-Gauge Eigenstates And Slippage
Just as those cohomology-related eigenstates, that are directly corresponding to the proximal local presence of a symplectic geometry -- are to tend to work to bear less slippage, at a level that is Poincare to the topological surface of such a respective superstring of discrete energy permittivity, that is here to work to bear such an inferred tense of a symplectic geometry -- than what often tends to be the case for those cohomology-related eigenstates, that are, instead, to be directly corresponding to the general tendency as to what is here to occur, with the correlative grouping of those cohomology-related eigenstates, that are here to be appertaining to the proximal local presence of a Khovanov geometry; it then tends to follow, that any second-order light-cone-gauge eigenstate that is here to be directly corresponding to a given arbitrary discrete quantum of energy, that is of an abelian light-cone-gauge topology, will tend to bear less of a tense of a scalar amplitude of slippage upon a Gliosis-based contact, -- than those bearings of a relative tense of a general scalar amplitude of slippage, that would otherwise occur, for any second-order light-cone-gauge eigenstate, that is here to instead to be directly corresponding to a given arbitrary discrete quantum of energy, that is of a non abelian light-cone-gauge topology. This is why any given arbitrary second-order light-cone-gauge eigenstate, that is of a non abelian topology, will eminently have a set intrinsic tense of sinusoidal standing waves -- of which are internally like a tense of a minute fractal of a soliton-related nature, at a level that is Poincare to the Gliosis-based topological surface of such a herein stated second-order light-cone-gauge eigenstate, since such sinusoidal waves are here to be Like a non-rippling "standing wave" at an internal reference-frame, while these are here to be in the process of being shifted around very quickly at an immediately external reference-frame. This acts, in so as to help to work to compensate for the so-inferred tense of slippage.; Whereas, -- any given arbitrary second-order light-cone-gauge eigenstate, that is of an abelian topology, will eminently have a set intrinsic tense of a More "supplemental" nature at a level that is Poincare to the Gliosis-based topological surface of such a herein stated second-order light-cone-gauge eigenstate, since the condition of a lesser tense of a scalar amplitude of slippage, tends to work to allow for the relinquishment of the eminent need for such sinusoidal "divots," that would Otherwise be necessary for the correlative gauge-bosons of such a given arbitrary quantum of energy, to be able to go into the act of plucking such stated light-cone-eigenstates, in so as to work to produce those Schwinger-Indices that are "proliferated," in so as to work to help to form the countless eigenstates of the various basic forces of nature. Sam Roach.
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abelian,
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Gliosis,
Khovanov
Monday, May 4, 2020
Some More Stuff, As To Isotropically Stable Superstrings
When a superstring of discrete energy permittivity -- whether such a said superstring is to be of either a symplectic geometry or of a Khovanov geometry, is to be working to generate as much cohomology as it is here to be degenerating, -- over the course of some discrete evenly-gauged Hamiltonian eigenmetric, -- and if, as well, there is here to be the Ward-Cauchy-related condition physical present here, in which the said superstring is to basically act as "one unit," as it is to be undergoing the general course of its translation through space over time, -- to where the topological surface of such an implied string, when this is here to be taken at a level that is Poincare to the general region that is "barely" external to the holonomic substrate of the here mentioned topological surface of this said superstring, is to bear a relatively consistently minimal topological "rippling" of its inherent homotopic indices of vibrational oscillation, then, one may say that such a said superstring of discrete energy permittivity, will consequently tend to bear an isotropically stable nature, that is known to act as being of a Floer (co)homology. Sam Roach.
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cohomology,
energy,
geometry,
Khovanov,
superstring
Monday, December 23, 2019
Vibration And Permutations
As any given arbitrary Noether-based mass-bearing orbifold eigenset, is to smoothly increase in its relative velocity, when this is here to be taken in its relationship to both the presence and the motion of light, it is accordingly to tend to consequently increase in its relative vibration-related pulsation, over a given arbitrary proscribed time, -- in which such an inferred acceleration of a respective orbifold eigenset, is here to be transferred through the fabric of time and space. Furthermore -- as any given arbitrary mass-bearing Noether-based orbifold eigenset, is to smoothly increase in its relative velocity, when in its relationship to both the presence and the motion of light, its composite superstrings of discrete energy permittivity that work to comprise such an inferred respective eigenset, are then to accordingly to tend to consequently smoothly decrease in the number of those partition-based discrepancies, that are here to tend to help at working to allow for the conservation of homotopic residue -- via the codifferentiable kinematic activity of what I term of as being the "i*PI(del) Action." Consequently -- if any given arbitrary mass-bearing orbifold eigenset, is to be undergoing a cycle, -- in which such an inferred set of discrete quanta of energy that operate in so as to perform a specific function, are here to go "back-and-forth" from initially accelerating smoothly in relation to both the presence and the motion of light To then subsequently decelerating smoothly in relation to both the presence and the motion of light, And son on and so forth, -- then, this general reverberation-related process, will therefore work to form a Ward-Cauchy-related process, which will here work to involve both a tense of metric-based cyclic permutations, as well working to involve a tense of Calabi-based cyclic permutations -- over a sequential series of group-related instantons, of which may be estimated with a relatively decent expectation value, via the determination of a potentially stipulated evenly-gauged Hamiltonian eigenmetric. Since the orbifold eigenset of such a case, is cyclical in the directly corresponding pattern of its rate of dimensional-related pulsation, this general condition, will consequently tend to work to form a tense of metric-based cyclical permutations. Furthermore -- since the superstrings of discrete energy permittivity, that work to comprise such an inferred orbifold eigenset of such a case, is cyclical in its directly corresponding pattern of those partition-based discrepancies, that are here to work to comprise part of the holonomic substrate of the topological surface of such said composite superstrings of discrete energy permittivity, that work to comprise the respective orbifold eigenset of such a general case, what will thence unfold, is that this will consequently tend to work to form a tense of Calabi-related cyclical permutations. This is a dual condition of cyclic permutations, that are here to work together, in so as to work to allow for such a general geometric example of a cyclical attribution for such a case. Later! To Be Continued! I will continue with the suspense later! Samuel David Roach.
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geometry,
permittivity,
strings,
Ward-Cauchy
Friday, December 13, 2019
Cohomology And Tense Of Substringular Flow
When a mass-bearing superstring of discrete energy permittivity is moving via a Noether-based flow, it will tend to bear a cohomology -- that is shaped in the nature of being as a euclidean toroidal-related geometric tense of a structural genus. Furthermore -- when a mass-bearing superstring of discrete energy permittivity is moving via a tachyonic-based flow, it will tend to bear a cohomology -- that is shaped in the nature of being as a hyperbolic toroidal-related geometric tense of a structural genus. I will continue with the suspense later! To Be Continued! Samuel David Roach.
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cohomology,
euclidean,
geometry,
hyperbolic,
Noether-based for,
structural genus,
superstring,
toroidal
Friday, September 13, 2019
Asymmetry Among Adjacent Cohomology-Related Eigenstates
The adjacent cohomology-related eigenstates, -- that are of those individually taken superstrings of discrete energy permittivity, that are here to be in the process of working to comprise one given arbitrary orbifold eigenset, -- tend to bear a tense of asymmetry, in order to act in so as not to infringe upon the space of the inferred adjacent cohomology-related eigenstates.
Those adjacent cohomology-related eigenstates -- that work to be as appertaining to the cohomology of those superstrings, that work to comprise one given arbitrary respective orbifold eigneset, that are here to be appertaining to the workings of a symplectic geometry, -- tend to work to bear a trivially isometric asymmetry. Whereas, -- those adjacent cohomology-related eigenstates -- that work to be as appertaining to the cohomology of those superstrings, that work to comprise one given arbitrary respective orbifold eigenset, that are here to be appertaining to the workings of a Khovanov geometry, -- tend to work to bear a non-trivially isometric asymmetry. To Be Continued! Sam.
Those adjacent cohomology-related eigenstates -- that work to be as appertaining to the cohomology of those superstrings, that work to comprise one given arbitrary respective orbifold eigneset, that are here to be appertaining to the workings of a symplectic geometry, -- tend to work to bear a trivially isometric asymmetry. Whereas, -- those adjacent cohomology-related eigenstates -- that work to be as appertaining to the cohomology of those superstrings, that work to comprise one given arbitrary respective orbifold eigenset, that are here to be appertaining to the workings of a Khovanov geometry, -- tend to work to bear a non-trivially isometric asymmetry. To Be Continued! Sam.
Saturday, October 13, 2018
Homologies And Norm-State-Projection Strike
A superstring that works to bear a symplectic homology -- tends to form a Yukawa Coupling upon those norm-state-projections that these are to strike in a Gliosis-related manner, that is of more of an orthogonal manner, than the general tense of a Yukawa-based Coupling that a superstring that works to bear a Legendre homology is to bear upon those norm-state-projections that these are to strike in a Gliosis-related manner, -- because superstrings that work to bear a symplectic homology, tend to interact with less topological slippage upon the stratum that these are to work to bear a Yukawa-related coupling upon, than superstrings that are to instead to work to bear a Legendre homology are to tug upon the correlative topological stratum that these are to come into a direct contact with. This is, in part, because, superstrings that are of a symplectic homology, are of a closed-looped nature, that thereby work to interact with the norm-state-projections that these are to interact with, in a manner that is to tend to bear a stronger direct wave-tug-related angular drive in their directly corresponding holomorphic direction, whereas, superstrings that are of a Legendre homology, are of an open-looped nature, that thereby work to bear a stronger indirect wave-tug-related angular drive in their directly corresponding holomorphic direction. This helps at working to describe as to why phenomenologies that are of abelian geometries, tend to form cohomology entities around the topological region of closed-looped superstrings of discrete energy permittivity -- whereas, phenomenologies that are of non abelian geometries, tend to form around the topological stratum of superstrings of discrete energy permittivity, -- that are of either of an open-looped or of an open-stand-related nature.
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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angular drive,
cohomologies,
entities,
geometry,
Gliosis,
Legendre,
norm-state-projections,
superstrings,
symplectic homology,
topology,
Yukawa
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