Showing posts with label Fadeev-Popov-Ghosts. Show all posts
Showing posts with label Fadeev-Popov-Ghosts. Show all posts
Tuesday, November 19, 2013
Some Added Stuff To Say About Ghost Anomalies
Just as the Gliossi-Sherk-Olive ghosts are being formed as the physical memory of the trajectory of superstrings of discrete energy permittivity, the physical memory of the directly corresponding counterstrings, light-cone-gauge eigenstates, and the directly corresponding Planck-like phenomena are being formed by the Gliossi interaction of these said additive phenomena with the relatively forward-holomorphic-based norm-states that come into contact with the projection of the said formats of phenomena -- that are directly related to the initially mentioned discrete units of energy permittivity. The counterstrings act as a direct differential supplement to the directly corresponding discrete units of energy permittivity. The light-cone-gauge eigenstates that directly co-relate to superstrings work to spring the said superstrings into the continual activity of Ultimon Flow (aside from other functions of the light-cone-gague), and, the Fadeev-Popov-Trace eigenstates (Planck-like phenomena that work to form the Fadeev-Popov-Ghosts as their physical memories) act as discrete units of energy impedance. I will continue with the suspense later! Sincerely, Samuel David Roach.
Monday, February 18, 2013
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.
Tuesday, November 2, 2010
Course 6, Session 5, Part One, The Toroidal Nature Of Superstrings
Well hello again world, this is Samuel Roach here! I hope that you are following along with my string theory with enthouseasm!
Tori-Sector-Ranges bear relatively orphoganol norm conditions from each other on either side by a difference of the radius of the eigenstates of many point particles, since point particles always have, relativle to most other gauge-actions, small size in comaparison to superstrings, as taken in the "three-dimensional" globalizations within the substringular.
What is a "three-dimensional" globalization taken in the substringular? Picture the set of a sequence of one and two-dimensional superstrings as taken in one eigenmetric within one tori-sector-range, and the two tori-sector-ranges on two of its immediate physical sides, just as the relatively central tori-sector-range is starting to form its quaternionic-instanton-field-impulse-range. The field of the one and two-dimensional superstrings of the said central range forms a "chord" that, to its perspective, is basically straight. The main difference between the "chord" of the central said range and the "chord" of the two tori-sector-ranges that are on either relative side of the said initial range, is that the central layer of substringular holonomic reality is about to go through the process of recycling with more of a kinematic tense of permittivity -- since the tori-sector-range that I have here called central is at the given moment the layer of reality that equally involves both forward and backward moving time indices, and is thus the predominant reality over the course of the sets of the Fourier Transformations that are discribed by a sequential series of instantons over the course of a certain number of substringular iterations. Such a condition of recyclling involves Cassimer Invariance more explicitly than with the substringular activity of the other two tori-sector-ranges here described -- which will thence not be undergoing the same stage of Cassimer Invariance at that moment. All phenomena that interacts with the Bases of Light, whether we are here talking about the "mini-bases" or their corresponding Popov-Ghosts, or whether we are talking about other substringular phenomena and their corresponding ghosts, is a sense of a multiplicitly-sided tori-sector-range in the substringular -- with a variation of parameters that is used to help define a discrete gauge thickness to this. Yet, the superstrings that interact with the Popov-Trace that interconnects the Bases of Light, or, in other words, with the general Basis of Light of a predominant tori-sector-range during the sub-metric that directly precedes an instanton-quaternionic-field-impulse-mode, is considered a central toroidal Basis of Light of that said range. What is this "moment?" I will leave this first of a three part session with this question for you to ponder. In the mean while, please absorb this knowledge, and I will get back with you on this session soon so as to eleviate the sense of wonder that I am creating by the suspense here! Sincerely, Sam.
Tori-Sector-Ranges bear relatively orphoganol norm conditions from each other on either side by a difference of the radius of the eigenstates of many point particles, since point particles always have, relativle to most other gauge-actions, small size in comaparison to superstrings, as taken in the "three-dimensional" globalizations within the substringular.
What is a "three-dimensional" globalization taken in the substringular? Picture the set of a sequence of one and two-dimensional superstrings as taken in one eigenmetric within one tori-sector-range, and the two tori-sector-ranges on two of its immediate physical sides, just as the relatively central tori-sector-range is starting to form its quaternionic-instanton-field-impulse-range. The field of the one and two-dimensional superstrings of the said central range forms a "chord" that, to its perspective, is basically straight. The main difference between the "chord" of the central said range and the "chord" of the two tori-sector-ranges that are on either relative side of the said initial range, is that the central layer of substringular holonomic reality is about to go through the process of recycling with more of a kinematic tense of permittivity -- since the tori-sector-range that I have here called central is at the given moment the layer of reality that equally involves both forward and backward moving time indices, and is thus the predominant reality over the course of the sets of the Fourier Transformations that are discribed by a sequential series of instantons over the course of a certain number of substringular iterations. Such a condition of recyclling involves Cassimer Invariance more explicitly than with the substringular activity of the other two tori-sector-ranges here described -- which will thence not be undergoing the same stage of Cassimer Invariance at that moment. All phenomena that interacts with the Bases of Light, whether we are here talking about the "mini-bases" or their corresponding Popov-Ghosts, or whether we are talking about other substringular phenomena and their corresponding ghosts, is a sense of a multiplicitly-sided tori-sector-range in the substringular -- with a variation of parameters that is used to help define a discrete gauge thickness to this. Yet, the superstrings that interact with the Popov-Trace that interconnects the Bases of Light, or, in other words, with the general Basis of Light of a predominant tori-sector-range during the sub-metric that directly precedes an instanton-quaternionic-field-impulse-mode, is considered a central toroidal Basis of Light of that said range. What is this "moment?" I will leave this first of a three part session with this question for you to ponder. In the mean while, please absorb this knowledge, and I will get back with you on this session soon so as to eleviate the sense of wonder that I am creating by the suspense here! Sincerely, Sam.
Tuesday, November 3, 2009
Glossary for FTAAN
1) Njenhuis Tensor -- An added tensor that operates off of the given Real Reimmanian plane.
2) Neilson-Collosh-Ghosts -- Ghost anomalies of gravitational particles.
3) Fadeev-Popov-Ghosts -- Ghost anomalies of Planck phenomenon related phenomena.
4) Positive-Norm-States -- Forward holomorphically based ghost anomalic annihilating loci that begin as point particles of the first-order that are supplementally norm to a relatively small number of other first-ordered point particles.
5) Negative-Norm-States -- Reverse holomorphically based ghost anomalic forming loci that begin as point particles of the first-order that are supplementally norm to a relatively small number of other first-ordered point particles. Negative-Norm-States form the Gaussian topology of Fadeev-Popov-Ghosts and other ghost anomalies.
6) Substringular-Resolution -- To be able to resolve down to (3and1/3)*10^(-37) meters. You may do this via a procedure of antigravity.
7) Antigravity -- A synergy of antigravitational particles that makes the given gauge-symmetry partially abelian. It is thus a Yau-Exact translation of Chern-Simmons directorals. Antigravity is a reversal in the directoralization of the Ricci-Scalar via the Rarita-Structure.
8) Reverse Gravity -- Gravitational particle kinematism that reverses the flow of gravity and does not change the given light-cone-gauge nature in and of itself. Reverse gravity, in and of itself, maintains the directoralization of the Ricci-Scalar.
9) Abelian Topology -- Jointal topology that has a direct wave-tug at its holonomic end through a Lagrangian.
10) Non-Abelian Topology -- Sinusoidal or smooth-curved topology that bears no direct wave-tug at its holonomic end though a Lagrangian.
11) Yang-Mills Topology -- Light-Cone-Gauge topology that is nonabelian.
12) Kaluza-Klein Topology -- Light-Cone-Gauge topology that is abelian.
13) Abelian-Gauge Topology -- Light-Cone-Gauge topology that is supplemental.
14) Non-Abelian Topology -- Light-Cone-Gauge topology that is sinusoidal.
15) Partially-Abelian Topology -- In terms of the light-cone-gauge, a partially-abelian topology is a topology of a gauge-symmetry that is based on the light-cone-gauge being Yang-Mills at one locus and Kaluza-Kleing at another location. In terms of an anomalous alterior topology besides the prior mentioned situation, a partially-abelian topology is a topology that goes from a jointal structure with a direct wave-tug at its holonomic end through a Lagrangian to a sinusoidal or smooth-curved topology that bears no direct wave-tug at its holonomic end through a Lagrangian.
16) Chern-Simmons Differentiation -- Differentiation that is either non-hermitian and/or perturbative.
2) Neilson-Collosh-Ghosts -- Ghost anomalies of gravitational particles.
3) Fadeev-Popov-Ghosts -- Ghost anomalies of Planck phenomenon related phenomena.
4) Positive-Norm-States -- Forward holomorphically based ghost anomalic annihilating loci that begin as point particles of the first-order that are supplementally norm to a relatively small number of other first-ordered point particles.
5) Negative-Norm-States -- Reverse holomorphically based ghost anomalic forming loci that begin as point particles of the first-order that are supplementally norm to a relatively small number of other first-ordered point particles. Negative-Norm-States form the Gaussian topology of Fadeev-Popov-Ghosts and other ghost anomalies.
6) Substringular-Resolution -- To be able to resolve down to (3and1/3)*10^(-37) meters. You may do this via a procedure of antigravity.
7) Antigravity -- A synergy of antigravitational particles that makes the given gauge-symmetry partially abelian. It is thus a Yau-Exact translation of Chern-Simmons directorals. Antigravity is a reversal in the directoralization of the Ricci-Scalar via the Rarita-Structure.
8) Reverse Gravity -- Gravitational particle kinematism that reverses the flow of gravity and does not change the given light-cone-gauge nature in and of itself. Reverse gravity, in and of itself, maintains the directoralization of the Ricci-Scalar.
9) Abelian Topology -- Jointal topology that has a direct wave-tug at its holonomic end through a Lagrangian.
10) Non-Abelian Topology -- Sinusoidal or smooth-curved topology that bears no direct wave-tug at its holonomic end though a Lagrangian.
11) Yang-Mills Topology -- Light-Cone-Gauge topology that is nonabelian.
12) Kaluza-Klein Topology -- Light-Cone-Gauge topology that is abelian.
13) Abelian-Gauge Topology -- Light-Cone-Gauge topology that is supplemental.
14) Non-Abelian Topology -- Light-Cone-Gauge topology that is sinusoidal.
15) Partially-Abelian Topology -- In terms of the light-cone-gauge, a partially-abelian topology is a topology of a gauge-symmetry that is based on the light-cone-gauge being Yang-Mills at one locus and Kaluza-Kleing at another location. In terms of an anomalous alterior topology besides the prior mentioned situation, a partially-abelian topology is a topology that goes from a jointal structure with a direct wave-tug at its holonomic end through a Lagrangian to a sinusoidal or smooth-curved topology that bears no direct wave-tug at its holonomic end through a Lagrangian.
16) Chern-Simmons Differentiation -- Differentiation that is either non-hermitian and/or perturbative.
Thursday, October 8, 2009
FTAAN, Session 3
Anti-Cevita energy is energy that causes a perturbative physical substringular state to become non-perturbative. A Wess-Zumino conditions is a condition of a substringular state that is non-perturbative. A Cevita condition is a physical condition of a substringular state that is perturbative. A Cevita conditions is mapped via the multi-dimensional euclidean cartesian tying together of the substringular Poincaires that define the substringular region that is given. The given Cevita energy is varied through the region of the neighborhood of the differentiation of the given substringular phenomena that acts as the given substringular states. The Ward conditions of the Ceivita energy that are referred to here are the topological vibrations of where the substringular states were defines the ghost anomallies related to the differential existence of the substringular states. These ghosts may be mapped as I referred to before by Poincaire extrapolation, and one may then define the existence and neighborhood of light-cone-gauge ghosts, ghosts of singularities, ghosts of world-sheets, ghosts of Planck phenomenon related phenomena, ghosts counterstrings, and/or ghost of superstrings. Ghosts of Planck phenomena related phenomena are mapped out as Fadeev-Popov-Ghosts and there are ghosts of superstrings. Fadeev-Popov-Ghosts are more easily measurable during Wess-Zumino conditions since strings here are non-perturbative. When substringular states are under conformal invariance, the superstrings given are steady state, and one may detect a Fadeev-Popov-Ghost by mapping it and then by going convex to concave to discern a set of iterations of a substriingular phenomenon that appears torroidal because of the set of vibrations that define the detection of that given substringular phenomena.
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