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Yang-Mills Interactions and Gravity in Terms of Clifford Algebra
General Physics · Submitted 31 Jul 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A model of Yang-Mills interactions and gravity in terms of the Clifford algebra Cl(0,6) is presented.
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The abstract, sentence by sentence
A model of Yang-Mills interactions and gravity in terms of the Clifford algebra Cl(0,6) is presented. The gravity and Yang-Mills actions are formulated as different order terms in a generalized action. The feebleness of gravity as well as the smallness of the cosmological constant and theta terms are discussed at the classical level. The invariance groups, including the de Sitter and the Pati-Salam SU(4) subgroups, consist of gauge transformations from either side of an algebraic spinor. Upon symmetry breaking via the Higgs fields, the remaining symmetries are the Lorentz SO(1,3), color SU(3), electromagnetic U(1)_EM, and an additional U(1). The first generation leptons and quarks are identified with even and odd parts of spinor idempotent projections. There are still several shortcomings with the current model. Further research is needed to fully recover the standard model results.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A model of Yang-Mills interactions and gravity in terms of the Clifford algebra Cl(0,6) is presented. | contribution 1.00 | 0.91 | 0.25 | asserted 1.00 |
| s1 | The gravity and Yang-Mills actions are formulated as different order terms in a generalized action. | contribution 0.52 | 0.89 | 0.21 | asserted 1.00 |
| s2 | The feebleness of gravity as well as the smallness of the cosmological constant and theta terms are discussed at the classical level. | interpretation 0.51 | 0.73 | 0.08 | asserted 0.82 |
| s3 | The invariance groups, including the de Sitter and the Pati-Salam SU(4) subgroups, consist of gauge transformations from either side of an algebraic spinor. | result 0.65 | 0.78 | 0.10 | asserted 1.00 |
| s4 | Upon symmetry breaking via the Higgs fields, the remaining symmetries are the Lorentz SO(1,3), color SU(3), electromagnetic U(1)_EM, and an additional U(1). | result 0.96 | 0.82 | 0.13 | asserted 1.00 |
| s5 | The first generation leptons and quarks are identified with even and odd parts of spinor idempotent projections. | result 0.64 | 0.83 | 0.12 | asserted 1.00 |
| s6 | There are still several shortcomings with the current model. | limitation 1.00 | 0.55 | 0.03 | asserted 1.00 |
| s7 | Further research is needed to fully recover the standard model results. | future work 1.00 | 0.15 | 0.06 | asserted 0.75 |
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The paper
Original abstract
A model of Yang-Mills interactions and gravity in terms of the Clifford algebra Cl(0,6) is presented. The gravity and Yang-Mills actions are formulated as different order terms in a generalized action. The feebleness of gravity as well as the smallness of the cosmological constant and theta terms are discussed at the classical level. The invariance groups, including the de Sitter and the Pati-Salam SU(4) subgroups, consist of gauge transformations from either side of an algebraic spinor. Upon symmetry breaking via the Higgs fields, the remaining symmetries are the Lorentz SO(1,3), color SU(3), electromagnetic U(1)_EM, and an additional U(1). The first generation leptons and quarks are identified with even and odd parts of spinor idempotent projections. There are still several shortcomings with the current model. Further research is needed to fully recover the standard model results.
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How the literature uses it
3 arXiv papers cite this in 11 sentences
Papers citing it · 7 sentences without a confident label
Uses its method or tool 1 paper
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Our approach is based on the framework of six-dimensional Clifford algebra $Cℓ_0,6$ [ref] .
A Clifford Algebra Approach to Chiral Symmetry Breaking and Fermion Mass Hierarchies · Introduction · 0.87
Cites it as background 1 paper
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We begin with a review of Clifford algebra $Cℓ_0,6$ [ref] .
Electroweak and Majorana Sector Higgs Bosons and Pseudo-Nambu-Goldstone Bosons · Leptons, Quarks, and Projection Operators · 0.86
What it cites · 13 sentences without a confident label
Compares with 4 papers
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This is different from all previous approaches [ref] .
Gauge Gravity and Electroweak Theory · Introduction · 0.92
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This is different from all previous approaches [ref] .
A Geometric Approach to the Standard Model · Introduction · 0.92
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The similarities between these two cases are more salient here than the conventional formulation [ref] .
Yang-Mills analogues of the Immirzi ambiguity · The Curvature and Gauge Action · 0.82
Cites as background 5 papers
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Thus a tiny effective mass is generated for the left-handed neutrino, known as the seesaw mechanism [ref] .
Fermion masses, neutrino oscillations, and proton decay in the light of SuperKamiokande · The Gauge Fields and Spinor Action · 0.82
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[ref] for attempts to construct a Higgs sector for gravity.], neither do we know how the Higgs fields acquire the rather ad hoc VEVs, nor do we know how the gauge bosons with broken symmetries are suppressed by acquiring large masses.
The Higgs sector of gravitational gauge theories · Conclusion · 0.84
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The geometrical meaning of MacDowell-Mansouri gravity is discussed in the context of the Cartan geometry [ref] .].
AdS Taub-Nut Space and the O(N) Vector Model on a Squashed 3-Sphere · The Curvature and Gauge Action · 0.96
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