On the universal Chamseddine–Connes action. I. Details of the action computation

DOI10.1063/1.531927zbMath0906.58004arXivhep-th/9607158OpenAlexW2013637234MaRDI QIDQ4379243

Bruno Iochum, Thomas Schücker, Daniel Kastler

Publication date: 31 January 1999

Published in: Journal of Mathematical Physics (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/hep-th/9607158

zbMATH Keywords

noncommutative geometryphysicsbosonic actionChamseddine-Connes models

Mathematics Subject Classification ID

Noncommutative topology (46L85) Noncommutative differential geometry (46L87) Spinor and twistor methods applied to problems in quantum theory (81R25) Spinor and twistor methods in general relativity and gravitational theory; Newman-Penrose formalism (83C60)

Related Items (12)

Noncommutative geometry and the standard model vacuum ⋮ INTERNAL SPACE FOR THE NONCOMMUTATIVE GEOMETRY STANDARD MODEL AND STRINGS ⋮ The Einstein–Hilbert–Yang–Mills–Higgs action and the Dirac–Yukawa operator ⋮ Chiral asymmetry and the spectral action ⋮ Discrete Kaluza–Klein from scalar fluctuations in noncommutative geometry ⋮ The spectral action for Dirac operators with skew-symmetric torsion ⋮ Noncommutative geometry and fundamental physical interactions: The Lagrangian level—Historical sketch and description of the present situation ⋮ A DARK SECTOR EXTENSION OF THE ALMOST-COMMUTATIVE STANDARD MODEL ⋮ Disctances in finite spaces from noncommutative geometry ⋮ STRINGS, NONCOMMUTATIVE GEOMETRY AND THE SIZE OF THE TARGET SPACE ⋮ A nonperturbative form of the spectral action principle in noncommutative geometry ⋮ Field theories on deformed spaces

Cites Work

• The action functional in non-commutative geometry
• Gravity, non-commutative geometry and the Wodzicki residue
• Noncommutative geometry and reality

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