Wednesday, November 4, 2009
More About Fujikawa Couplings
A two-dimensional superstring is formed when a one-dimensional superstring hermitianly bends via the Green Function to go from being a vibrating strand to being a vibrating hoop of discrete energy permittivity. When a one-dimensional superstring closes to form the discussed two-dimensional superstring, the relative "top" and "bottom" parts of the associated one-dimensional superstring loop their ends around each other in a holonomically homogeneous spatial manner 120 times while the given superstringular phenomenon has an equally added mini-string, or substringular field, holonomic gauge-action in terms of added condensed oscillation The added condensed oscillation that is brought to the closing one-dimensional superstring via the networking of Cassimer Invariance is equal to the minute decrease in the circumference of the associated two-dimensional superstring due to the tying of the two ends of the given one-dimensional superstring that is converting into a two-dimensional superstring via the hermitian bending and lacing together that may be partially described by the Green Function. The lacing together of the two ends of the associated one-dimensional superstring is due to the condition that the given hermitian bending bears a conipoint and a coniaxial at the center of the given one-dimensional superstring, and cos 120 degrees = .5, and that, at 120 degrees both sine and cosine are positive. So, the mini-string at both ends of the associated one-dimensional superstring in a hyperbollicaly tangent manner wrap themselves around each other for 120 looped Laplacian metrical delineations. This is also due to the fact that a Yang-Mills light-cone-gauge topological field is sinusoidal for a Laplacian delineation of 120 complete waves when during the core of BRST in-between a Fadeev-Popov-Trace and its associated superstring. When a two-dimensional superstring, the potential increase in wave homotopy is compensated by the holonomic decrease in the Hodge Index of the phenomenology of the given superstring via the networking of Cassimer Invariance in the locus of the associated substringular neighborhood. This aspect of Cassimer Invariance is due to the equal and opposite reaction in the opposite direction of the local Chern Simmons perturbations in terms of the Clifford expansion, and to the contraction of the kinematic differentiation of the local Campbell and Hausendorf projections that act upon the conicenter and coniaxial of the hermitian activity of the opening two-dimensional superstring. This is due to the local Calabi-Calabi, Calabi-Wilson-Gordan, and the local Calabi-Yau interactions that are defined by electrodynamic scattering that happens in the locus of the region of the given superstring that is changing morphology.
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.
Sunday, November 1, 2009
Notes for FTAAN
A swivel configuration appertaining to a one-dimensional superstring may be supplementally norm to the norm to holomorphic direction, or a swivel configuration appertaining to a one-dimensional superstring may be in the holomorphic direction.
A swivel configuration appertaining to a two-dimensional superstring may be supplementally norm to the norm to holomorphic direction in the general directoralization of the associated superstring's topology, or a swivel configuration appertaining to a two-dimensional superstring may be in the holomorphic direction.
Swivel configurations of a vibrating strand ( one-dimensional superstring, or of a vibrating hoop (two-dimensional superstring) do not necessarily intrinsically take away metric-gauge from a superstring in and of themself. Metric-Gauge is taken away as a decrement in a superstring's extra supply of potential permittivity by the Fourier successive utilization of the given superstring over a sequential series of iterations that define a group metric.
The difference between a swivel configuration as I have described, and a mini-loop that is a form of metric-gauge is that a mini-loop is tightly knit in a manner that makes the whole given superstring completely hermitian unless the said superstring is perturbated by a swivel configuration that has one or more Chern Simmons cusps. Such Chern Simmons cusps bear a non-discrete limit covariance relative to the topology that exists Wardwise on either sides of the cusps described.
A swivel configuration appertaining to a two-dimensional superstring may be supplementally norm to the norm to holomorphic direction in the general directoralization of the associated superstring's topology, or a swivel configuration appertaining to a two-dimensional superstring may be in the holomorphic direction.
Swivel configurations of a vibrating strand ( one-dimensional superstring, or of a vibrating hoop (two-dimensional superstring) do not necessarily intrinsically take away metric-gauge from a superstring in and of themself. Metric-Gauge is taken away as a decrement in a superstring's extra supply of potential permittivity by the Fourier successive utilization of the given superstring over a sequential series of iterations that define a group metric.
The difference between a swivel configuration as I have described, and a mini-loop that is a form of metric-gauge is that a mini-loop is tightly knit in a manner that makes the whole given superstring completely hermitian unless the said superstring is perturbated by a swivel configuration that has one or more Chern Simmons cusps. Such Chern Simmons cusps bear a non-discrete limit covariance relative to the topology that exists Wardwise on either sides of the cusps described.
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