Showing posts with label Neumman bounds. Show all posts
Showing posts with label Neumman bounds. Show all posts
Tuesday, May 20, 2014
As To The Configurations of World-Sheets
If a given arbitrary world-sheet is of a toroidal-shaped-nature, then, the physical ends of the Ward-Neumman boudaries of those ghost anomalies that work to trace the mapped-out extrapolation as to the trajectory of the projection of the directly corresponding superstrings -- that worked to form the so-stated ghost anomalies -- via the physical evidence of the directly corresponding world-sheets, bear cap-like permutations that act as critical cusps that are due to the just-eluded-to cyclic permutation of those cross-sections of the so-stated external format of first-ordered point particles that bear a chirality, which is relative to the other of such so-stated critical cusps, that may be either symmetrically fashioned or assymetrically fashioned -- in relation to the directly corresponding trivially isomorphic alterior end caps of that toroidal-based pointal-construction of the mentioned ghost-based configuration -- that bears a mappable tracing that is shaped like a "doughnut" that bears a central anuulus that contains a non-time-oriented Lagrangian that is Gliossi to the so-stated pointal configuration of the world-sheet, which is relatively hermitian in unitary flow, as one were to map the coniaxions that work to indicate the relative vacuum that would here be at the Poincaire level of the center of the so-stated world-sheet. If the so-stated end caps in this case are symmetrically arranged, any given arbitrary superstring that may be potentially caught in the said anuulus -- during any given arbitrary group metric in which the said ghost anomaly configuration is not yet annharmonically scattered -- will propagate out of the Ward-Neumman bounds of the so-eluded-to ghost-based configuration, in a forward-holomorphic-based directoral flow of the given topological sway. If one of the so-stated end caps is arranged symmetrically, with its so-eluded-to counterpart, yet, the other end Lagrangian-based mapping of end caps is arranged antisymmetrically with its counterpart, then, the chirality of the so-stated Lagrangian will bear Chern-Simmons singularities. Also, with the past format of scenario, over time, such a situation will work to form metrical-based singularities -- with the kinematic flow of its external-based enviorenment. This metrical dissonance would then work to pull any given arbitrary superstring that is within the region of the so-stated anuulus of the toroidal-based world-sheet configuration in the reverse-holomorpohic directoral flow of topological sway. If two or more of such sets of end caps is annharmonic -- in terms of the non-time-oriented mapping of the chirality of their counterpart -- as taken via a trivially isomorphic extrapolation, then, any given superstring caught within this genus of construction will rebound between the end caps per iteration. Yet, this is given the general space-time-curvature-based considerations. So, ironically yet logically enough, if the end caps of this general format of scenario are only harmonically chiral, via the extrapolation of a Wilson-based linearity, then, the so-stated rebounding of superstrings that would be caught-up in a configuration such as this would rebound in a manner that would work to reattain fractals of discrete energy permittivity in superstrings. Hint: the Schotky Construction and the Klein Bottle. I will continue with the suspense later! To Be Continued. Sam Roach.
Wednesday, July 27, 2011
How the Bases of Light Are Fractored By the Planck-Related-Phenomena
When the Bases of Light are retied -- via the quaternionic-instanton-field-impulse-mode -- the same basic type of morphological nature of each Basis of Light taken individually is fractored by the corresponding Planck-Related-Phenomena. Aside from the 159,000 different types of Planck-Related-Phenomena morphologies that may be generalized by what I had discussed in my previous post, there are close to one trillion manners in which the hyperbolically concave up morphologies of the "Chi" shapes of the given mini-traces may formulate in terms of the intensity of such a prior mentioned type of curvature that may be mapped out under any given Laplacian condition of such Planck-Related-Phenomena that involves forward moving time during BRST. Likewise, there are also close to one trillion manners in which the hyperbolically concave down morphologies of the "Chi" shapes of the given mini-traces may formulate in terms of the intensity of such a prior mentiones type of curvature that may be mapped out under any given Laplacian condition of such Planck-Related-Phenomena that involves backward moving time during BRST. In the region to where the Bases of Light moves primarily forward, there is one Basis of Light that involves forward and backward moving time equally. In the region to where the Bases of Light moves primarily backward, there is one Basis of Light that involves forward and backward moving time equally. So, one not only has the 159,000 basic variations of Planck-Related-Phenomena as I described in my previous post, yet, there are three different general types of intensity in terms of the hyperbollic nature of the basic curvature of the "Chi" shapes that are an integral part of the mentioned Bases of Light as may be determined by the detection of the corresponding mini-traces. Regular mini-traces bear a hyperbollic concave curvature along the mapping out of the "Chi" shapes under Laplacian conditions that is strictly eucildean and hermitian.
Virtual mini-traces bear a hyperbollic concave curvature along the mapping ot of the "Chi" shapes under Laplacian conditions that is determined via a power series of observed extension. While Planck-phenemenoa visages bear a Laplacian tracing that is exponential in terms of how one may map it out from the center of a mini-trace to its exterior Ward Neumman bounds. Likewise, for every Regular-Planck-Phenomena, or, RPP, there are 10,000 times as many total RPP and virtual PP combined, and, for every RPP, there are 100,000,000 total virtual PRP, visage PRP and RPP combined. Virtual visage Planck-Related-Phenomena, or, VVPRP, bear an exponential mapping as before, except, the related traces bear a Laplacian condion of extended sub-mini-string in-between the second-ordered point particles that comprise the traces that comprise the mentioned "Chi" shapes. Again, for every RPP, there are one trillion total RPP, virtual PRP, visage PRP, and VVPRP. You have a phenomenal day, and I will continue with the suspence later! Sincerely, Sam Roach.
Virtual mini-traces bear a hyperbollic concave curvature along the mapping ot of the "Chi" shapes under Laplacian conditions that is determined via a power series of observed extension. While Planck-phenemenoa visages bear a Laplacian tracing that is exponential in terms of how one may map it out from the center of a mini-trace to its exterior Ward Neumman bounds. Likewise, for every Regular-Planck-Phenomena, or, RPP, there are 10,000 times as many total RPP and virtual PP combined, and, for every RPP, there are 100,000,000 total virtual PRP, visage PRP and RPP combined. Virtual visage Planck-Related-Phenomena, or, VVPRP, bear an exponential mapping as before, except, the related traces bear a Laplacian condion of extended sub-mini-string in-between the second-ordered point particles that comprise the traces that comprise the mentioned "Chi" shapes. Again, for every RPP, there are one trillion total RPP, virtual PRP, visage PRP, and VVPRP. You have a phenomenal day, and I will continue with the suspence later! Sincerely, Sam Roach.
Thursday, November 4, 2010
Course 6, Session 5, Part 3, The Toroidal Nature Of Superstrings
Well hello again world, this is Samuel Roach here! I hope that you are doing great, and that you are following along!
So, although there are 32 spacial dimensions per set of parallel universes, and there are three sets of parallel universes, the basis of spacial dimensionality is a three-dimensional world -- such as is perceived by an observer in the globally distinguishable. When you look within the dimensions of a main world-sheet or a main world-tube, and one consequently observes a volume here, you are observing a three-dimensionality within another dimensionality. The perceived "volume" you are observing is three-dimensional on a fundamental basis, because volume taken to where you can form an i/j/k (hat) directorallized field has a relative up-down-right-left-side-to-side basis of Neumman boundary conditions. When you bring a field into observation to where you can dellineate these said basis of directorals -- you have globalized this field into an observers perspective. Yet, since there are a total of 96 spacial dimensions in the physical portion of the Continuum, directorals that help to describe the delineation of space-time-fabric may be described by ihat, jhat, khat...isub2hat...lsub2hat, msub2hat, to nsub2hat. The function of the globally distinguishable manner in which there is a basis in direcoralzation of ihat, jhat, and khat, acts according to the substringular, yet one is here able to detect indices within a smaller region. Substringular globalizations arae smaller than the general Bases of Light are directly involved with the perceptions here, yet one is able to make computerized drawings of what is going on here based on what one knows of the activity here within specific moments of Lapalacian and Fourier Transformations. Moments that are made up of simultaneous metric sequencial series (theoretical) are actually known as based on what we already understand, combined with experiment. One knows the value of hbar by looking at a physics table which describes this. When one is accurate to what is actual within the course of Planck Bar Time, then at least the accuracy of energy is within discreteness of one unit of energy. When the curvature between two adjacent tori-sector-ranges relative to a central one is completely flush over the sub-metric that happens during the Bases of Light (which is in-between instantons and right before instanton-quaternionic-field-impulse-mode), then the curvature is within one tense of a globalization of curvature as may be perceived by a living being. Remember, substringular string is composed of many minit superstring, and mini-string forms the field of superstrings. So, discrete energy permittivity is always perceived during instanton, and discrete energy impedance is always perceived during instanton. Here's more as to why.: it is the mutually interaction of discrete energy permittivity with discrete energy impedance that allows the activity of the light-cone-gauge to be able to fascilitate the "springing" into action of superstrings and their corresponding Planck phenomenon related phenomena through the course of the generally unperceived activity that happens in-between instantons. Why do I write "Planck phenomenon related phenomena" instead of just "Planck phenomena?" Because what I term of as just "Planck phenomena" is the smoothest curvature in terms of topological hermicity that is possible, given the general curvature of the corresponding Basis of Light that converts into that phenomena that interacts with superstrings so to create the basic fields of discrete energy permittivity and discrete energy impedance that form a disrete unit of energy that may be transversally described as an eigenstate of Planck energy, and also, that has discrete radial motion that may be describe of as an eigenstate of Planck Bar energy. I would just love to hear some education responses. I will leave with a question.: How does the condition of the substringular's toroidal nature that is often exhibited as a unit fractor down to the toroidal nature that is often exhibited by superstrings? I will begin to answer some of this question later. Until then, I will continue with the suspense later, and you have a phenomenal day! Sincerely, Sam.
So, although there are 32 spacial dimensions per set of parallel universes, and there are three sets of parallel universes, the basis of spacial dimensionality is a three-dimensional world -- such as is perceived by an observer in the globally distinguishable. When you look within the dimensions of a main world-sheet or a main world-tube, and one consequently observes a volume here, you are observing a three-dimensionality within another dimensionality. The perceived "volume" you are observing is three-dimensional on a fundamental basis, because volume taken to where you can form an i/j/k (hat) directorallized field has a relative up-down-right-left-side-to-side basis of Neumman boundary conditions. When you bring a field into observation to where you can dellineate these said basis of directorals -- you have globalized this field into an observers perspective. Yet, since there are a total of 96 spacial dimensions in the physical portion of the Continuum, directorals that help to describe the delineation of space-time-fabric may be described by ihat, jhat, khat...isub2hat...lsub2hat, msub2hat, to nsub2hat. The function of the globally distinguishable manner in which there is a basis in direcoralzation of ihat, jhat, and khat, acts according to the substringular, yet one is here able to detect indices within a smaller region. Substringular globalizations arae smaller than the general Bases of Light are directly involved with the perceptions here, yet one is able to make computerized drawings of what is going on here based on what one knows of the activity here within specific moments of Lapalacian and Fourier Transformations. Moments that are made up of simultaneous metric sequencial series (theoretical) are actually known as based on what we already understand, combined with experiment. One knows the value of hbar by looking at a physics table which describes this. When one is accurate to what is actual within the course of Planck Bar Time, then at least the accuracy of energy is within discreteness of one unit of energy. When the curvature between two adjacent tori-sector-ranges relative to a central one is completely flush over the sub-metric that happens during the Bases of Light (which is in-between instantons and right before instanton-quaternionic-field-impulse-mode), then the curvature is within one tense of a globalization of curvature as may be perceived by a living being. Remember, substringular string is composed of many minit superstring, and mini-string forms the field of superstrings. So, discrete energy permittivity is always perceived during instanton, and discrete energy impedance is always perceived during instanton. Here's more as to why.: it is the mutually interaction of discrete energy permittivity with discrete energy impedance that allows the activity of the light-cone-gauge to be able to fascilitate the "springing" into action of superstrings and their corresponding Planck phenomenon related phenomena through the course of the generally unperceived activity that happens in-between instantons. Why do I write "Planck phenomenon related phenomena" instead of just "Planck phenomena?" Because what I term of as just "Planck phenomena" is the smoothest curvature in terms of topological hermicity that is possible, given the general curvature of the corresponding Basis of Light that converts into that phenomena that interacts with superstrings so to create the basic fields of discrete energy permittivity and discrete energy impedance that form a disrete unit of energy that may be transversally described as an eigenstate of Planck energy, and also, that has discrete radial motion that may be describe of as an eigenstate of Planck Bar energy. I would just love to hear some education responses. I will leave with a question.: How does the condition of the substringular's toroidal nature that is often exhibited as a unit fractor down to the toroidal nature that is often exhibited by superstrings? I will begin to answer some of this question later. Until then, I will continue with the suspense later, and you have a phenomenal day! Sincerely, Sam.
Tuesday, September 29, 2009
GUFT, Additional Addendum
When a superstring goes thru a Kaeler metric, the angling of the associated superstrings as a unit going into the given Klein bottle is 22 and a half degrees as subtended from a supplemental arc going in the direction of the ultimon's curvature pointing directly downward with the same ultimon curvature. One superstring usually undergoes 191 (96+95) iterations thru a Klein metric until it has completely regained the permittivity that it needs to be the energy that it's to be by the holomorphic/antiholomorphic shaking of the Kaeler metric. If the associated superstring still hasn't regained its permittivity after this, it will move reverse holomorphicly 95 iterative positions (one per core of BRST instantons), while then spinning at the same iterative locus for 80 iterations while then undergoing 10 spin-orbital/roll superconformal invariance modes at that locus. When this is the case, the associated superstring at this point will move into the core norm Ward boundaries of the Klein bottle directly transversally the 19th iteration hereafter this at the associated 22+(1/2) degree subtended angle. At this point, the first iteration of the next set of Kaeler metric iterations will happen to allow for the associated superstring to regain the permittivity that it needs to be the energy that it is to be. Each Klein bottle is 768 Planck Lengths long. Its exterior Neumman conditions consist of two normalized sets of orientifolds that allow the Klein bottle to be 384*768 Planck Lengths. This half cube's Neumman exterior boundaries consist of mini-string or superstringular fields that are hermitianly supplementally norm to form a fabric that is the equivalent of one Planck Length thick. This hermitianly supplementally norm field type exists at all four sides and the bottom of each Klein bottle. The interior of the Klein bottle consists of negative-norm first-ordered point particles that vibrate in the associated Schotky construction at 45 degrees from positive-norm first-ordered point particles. The difference between these negative norm states and positive norm states is that negative norm states initially go in the opposite direction of the Klein bottles And in the general transversal dirction in a forward moving time frame when the Klein bottle has absorbed superstrings, while positive norm states initially go in the same general transversal direction of the Klein bottle during a forward moving time-frame when superstrings are in the Klein bottle. In a backward moving time-frame, positive norm states go in the opposite general transversal direction of the Klein bottle, while negative norm states move in the same gereral transversal direction of the Klein bottle when superstrings are in the Klein bottle. The then associated fields of the norm states in the Klein bottle, these fields being mini-string subtended from the norm states that are interconnected in one fashion or another. So, the less metric-gauge that a superstring has as it goes into the Schotky construction, the more the skuperstring gets shuck to reattain permittivity in the form of metric-gauge. This "reverse proportionality" obeys a tangential Dirac function as a locus of superstrings changes the Jacobian eigenbasis of an orbifold or an orbifold eigenset thru a Clifford algebra that form a perturbative Fourie Transformation known as a Gaussian Transformation. When such a Gaussian Transformation alters the elasticity per hermicity of the associated light-cone-gauge eigenstates the associated light-cone-gauge eigenstates alters in abelian nature. This happens when norm conditions form a Yakawa Coupling with the associated superstrings.
Friday, September 25, 2009
GUFT, The New Addition
A Higgs-Action is an example of a tiny particle that is smaller than a superstring. A one-dimensional superstring is
3*10^(-35) meters long when fully uncontracted and is 10^(-43) meters long when fully contracted. A regular two-dimensional superstring, besides gauge-bosons, has a circumference of 3*10^(-35) meters around when fully uncontracted and has a circumference of 10^(-43) meters around when it is fully contracted. A superstring is 10^(-43) meters long when it is one-dimensional in the substringular and a regular two-dimensional superstring besides gauge-bosons has a circumference of
10^(-43) meters around in the substringular. A Higgs-Action or an eigenstate of the Higgs-Action has a length when fully uncontracted, which is in the globally distinguishable, of 10^(-43) meters. A Higgs-Action or an eigenstate of the Higgs-Action has a length when fully contracted, which is in the substringular, of 3 and one-third * 10^(-52) meters. An eigenstate of the Higgs-Action is an oval type point particle-like structure that is conical at both ends while hermitianly curving from its center of 10^(-43) meters in the globally distinguishable and 3 and one-third * 10(-52) meters in the substringkular to its respective apexes at both ends of 3*10^(-78) meters in the globally distinguishable in thickness and 10^(-86) meters in the substringular. The associated hermitian-like quality involves a parabollic shape that exists in central locus of the associated Higgs-Action eigenstate at an equal theta and phi, at the same initial rho as the length of the associated Higgs-Action eigenstate, while the parabollic shape given smoothly curves in all 32 first derivatives to a shaft on either end of the associated parabollic structure to the given thickness. (3*10^(-78) meters thick in the globally distinguishable and 10^(-86) meters thick in the substringular.) The mini-string or field that comprises the construction of the Fischler-Suskind-Mechanism is 10^(-129) meters thick in the substringular and 3*10^(-121) meters thick in the globally distinguishable. The Shotcky construction of the Klein bottle has outer Neumman boundaries that are 3*10(-35) meters thick in the globally distinguishable and 10^(-43) meters thick in the substringular. The norm conditions in the Klien bottle are interconnected by mini-string, or, in other words, by subsringular fields, in such a way that the Klein bottle bears a subtended Ricci Scalar metric-gauge that is equal to 6.25*10^(18) in both the globally distinguishable and in the substringular. The associated Higgs-Action eigenstate bears a Hodge-Index in terms of Poincaire interelation of the overall first-ordered-point-particles that could fit in the given Higgs-Action eigenvalue. The structure here allows for just the leverage needed for the lifting of the given Klein bottle. The "top", or norm to holomorphic end of a Higgs-Action eigenstate, bears a borne tangency with the "bottom", or norm to antiholomorphic end of the associated Klein bottle via a supplementally norm mesh of mini-string, or, in other words, substringular fields.
3*10^(-35) meters long when fully uncontracted and is 10^(-43) meters long when fully contracted. A regular two-dimensional superstring, besides gauge-bosons, has a circumference of 3*10^(-35) meters around when fully uncontracted and has a circumference of 10^(-43) meters around when it is fully contracted. A superstring is 10^(-43) meters long when it is one-dimensional in the substringular and a regular two-dimensional superstring besides gauge-bosons has a circumference of
10^(-43) meters around in the substringular. A Higgs-Action or an eigenstate of the Higgs-Action has a length when fully uncontracted, which is in the globally distinguishable, of 10^(-43) meters. A Higgs-Action or an eigenstate of the Higgs-Action has a length when fully contracted, which is in the substringular, of 3 and one-third * 10^(-52) meters. An eigenstate of the Higgs-Action is an oval type point particle-like structure that is conical at both ends while hermitianly curving from its center of 10^(-43) meters in the globally distinguishable and 3 and one-third * 10(-52) meters in the substringkular to its respective apexes at both ends of 3*10^(-78) meters in the globally distinguishable in thickness and 10^(-86) meters in the substringular. The associated hermitian-like quality involves a parabollic shape that exists in central locus of the associated Higgs-Action eigenstate at an equal theta and phi, at the same initial rho as the length of the associated Higgs-Action eigenstate, while the parabollic shape given smoothly curves in all 32 first derivatives to a shaft on either end of the associated parabollic structure to the given thickness. (3*10^(-78) meters thick in the globally distinguishable and 10^(-86) meters thick in the substringular.) The mini-string or field that comprises the construction of the Fischler-Suskind-Mechanism is 10^(-129) meters thick in the substringular and 3*10^(-121) meters thick in the globally distinguishable. The Shotcky construction of the Klein bottle has outer Neumman boundaries that are 3*10(-35) meters thick in the globally distinguishable and 10^(-43) meters thick in the substringular. The norm conditions in the Klien bottle are interconnected by mini-string, or, in other words, by subsringular fields, in such a way that the Klein bottle bears a subtended Ricci Scalar metric-gauge that is equal to 6.25*10^(18) in both the globally distinguishable and in the substringular. The associated Higgs-Action eigenstate bears a Hodge-Index in terms of Poincaire interelation of the overall first-ordered-point-particles that could fit in the given Higgs-Action eigenvalue. The structure here allows for just the leverage needed for the lifting of the given Klein bottle. The "top", or norm to holomorphic end of a Higgs-Action eigenstate, bears a borne tangency with the "bottom", or norm to antiholomorphic end of the associated Klein bottle via a supplementally norm mesh of mini-string, or, in other words, substringular fields.
Subscribe to:
Posts (Atom)