The flow of a heuristic antigravity-related radial (rotational) acceleration, may often help work to allow, for the consequentially incurred flow, of a heuristic antigravity-related transversal acceleration. SAM ROACH.
Showing posts with label antigravity. Show all posts
Showing posts with label antigravity. Show all posts
Thursday, April 14, 2022
Tuesday, July 2, 2019
Neilson-Kolosh Cohomology And Gravity
Neilson-Kolosh cohomology, that tends to generate an Anti-De-Sitter/De-Sitter gravitational mode -- tends to work to be most directly involved with a tense of gravity, -- whereas, -- Neilson-Kolosh cohomology, that tends to degenerate an Anti-De-Sitter/De-Sitter gravitational mode -- tends to work to be most directly involved with a tense of anti gravity. Sincerely, Samuel!
Wednesday, April 24, 2013
A Little Bit More As To Gravity
When the directoral-basis of the wave-tug/wave-pull of the Rarita Structure via the Ricci Scalar is reversed in terms of the corresponding holomorphic-based direction of the correponding Hamiltonian operation through a reltively superconformally invariant field that beares a minimal scalar projection in terms of the basis of the Lagrangian that this is happening in, then, the said eigenstate of Rarita Structure is applying its fractal of angular momnetum in the opposite tense of holomorphic directoral permittivity in basically a static-based equilibrium manner, to where, this is said to be an example of antigravity.
When the motion of the Rarita Structure as a kinematic wholeistic entity is reversed in terms of the direction that it is moving -- when the Hamiltonian operation here happens through a relatively more variant basis of Lagrangian when in terms of the corresponding scalar projection of the eluded to general locus, then, one is said to have a condition of reverse-gravity.
This is apart from the concepts of Ante-De-Sitter and De-Sitter gravitational modes.
Simple is best. I will continue with the suspense later! Sincerely, Samuel David Roach.
When the motion of the Rarita Structure as a kinematic wholeistic entity is reversed in terms of the direction that it is moving -- when the Hamiltonian operation here happens through a relatively more variant basis of Lagrangian when in terms of the corresponding scalar projection of the eluded to general locus, then, one is said to have a condition of reverse-gravity.
This is apart from the concepts of Ante-De-Sitter and De-Sitter gravitational modes.
Simple is best. I will continue with the suspense later! Sincerely, Samuel David Roach.
Thursday, January 7, 2010
More About Gravity
Reverse gravity is a reversal in the direction of the flow of gravitational particles as a unit. Antigravity, on the other hand, is a reversal in the directoralization of the Ricci Scalar. Gravitational particles are gravitons and gravitinos. Gravitational particles are gravitons and gravitinos. Gravitational force, as entailed by the Ricci Scalar, is a metric-gauge, that, via the Rarita Structure, acts also as a type of gauge-action. Every phenomenon that's physical is is involved with gravity of some sorts or another. So, although not everything has mass, every phenomenon in terms of superstrings and gauge-bosons has a mass index. This is because every superstring has some subtending upon gravitational particles via Ricci Scalar eigenstates that act through the respective Rarita Structure eigenstates. A string that appertains to mass is a superstring that is Yau-Exact in terms of its surrounding substringular singularities, and bears a light-cone-gauge topology that is Kaluza-Klein. A Kaluza-Klein topology is a light-cone-gauge topology is a light-cone-gauge topology that is abelian per the Laplacian conditions respectively at BRST. Phenomena that bear singularities in adjacent substringular Gliossi tangency that is both hermitian and non-perturbative per iteration is said to be Yau-Exact in the associated instanton. If the given superstring differentiates along a toroidal mapping upon detection, then this superstring of mass is in a state of conformal invariance that bears mass-on-shell, since all of the Majorana-Weyl charge of a discrete unit of permittivity's Ward field is at the periphery of its Ward Neumman bounds. The condition of a superstring that is a vibrating hoop or a vibrating strand that is detected, though as toroidal, is the basis of M-Theory.
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.
Subscribe to:
Posts (Atom)