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The aim of this contribution is to explain how Connes derives the standard model of electromagnetic, weak and strong forces from noncommutative geometry. The reader is supposed to be aware of two other derivations in fundamental physics:…

High Energy Physics - Theory · Physics 2007-05-23 Thomas Schucker

Connes' noncommutative approach to the standard model of electromagnetic, weak and strong forces is sketched as well as its unification with general relativity.

High Energy Physics - Theory · Physics 2009-11-10 Thomas Schucker

The restrictions imposed on the strong force in the `non-commutative standard model' are examined. It is concluded that given the framework of non-commutative geometry and assuming the electroweak sector of the standard model many details…

High Energy Physics - Theory · Physics 2009-10-28 Becca Asquith

We briefly sketch the noncommutative geometry approach to the Standard Model, with attention to what can be inferred about particle masses.

High Energy Physics - Theory · Physics 2008-02-03 Jose M. Gracia-Bondia

Connes' notion of non-commutative geometry (NCG) generalizes Riemannian geometry and yields a striking reinterepretation of the standard model of particle physics, coupled to Einstein gravity. We suggest a simple reformulation with two key…

High Energy Physics - Theory · Physics 2015-06-18 Latham Boyle , Shane Farnsworth

This is a brief review where some basic elements of non-commutative geometry are given. The rules and ingredients that enter in the construction of the standard model and grand unification models in non-commutative geometry are summarized.…

High Energy Physics - Theory · Physics 2015-03-10 A. H. Chamseddine

Noncommutative geometry allows to unify the basic building blocks of particle physics, Yang-Mills-Higgs theory and General relativity, into a single geometrical framework. The resulting effective theory constrains the couplings of the…

High Energy Physics - Phenomenology · Physics 2013-05-15 Christoph A. Stephan

The Standard Model of particle physics can be deduced from a small number of axioms within Connes' noncommutative geometry (NCG). Boyle and Farnsworth [New J. Phys. 16 (2014) 123027] proposed to interpret Connes' approach as an algebra…

High Energy Physics - Theory · Physics 2015-06-08 Christian Brouder , Nadir Bizi , Fabien Besnard

The derivation of the full Standard Model from noncommutative geometry has been a promising sign for possible applications of the latter in High Energy Physics. Many believe, however, that the Standard Model cannot be the final answer. We…

High Energy Physics - Theory · Physics 2015-06-12 Thijs van den Broek , Walter D. van Suijlekom

A noncommutative version of the usual electro-weak theory is constructed. We discuss how to overcome the two major problems: 1) although we can have noncommutative U(n) (which we denote by $U_{\star}(n)$) gauge theory we cannot have…

High Energy Physics - Theory · Physics 2010-05-28 M. Chaichian , P. Presnajder , M. M. Sheikh-Jabbari , A. Tureanu

Our aim in this review article is to present the applications of Connes' noncommutative geometry to elementary particle physics. Whereas the existing literature is mostly focused on a mathematical audience, in this article we introduce the…

High Energy Physics - Theory · Physics 2012-10-16 Koen van den Dungen , Walter D. van Suijlekom

Connes' non-commutative geometry (NCG) is a generalization of Riemannian geometry that is particularly apt for expressing the standard model of particle physics coupled to Einstein gravity. In a previous paper, we suggested a reformulation…

High Energy Physics - Theory · Physics 2015-06-22 Shane Farnsworth , Latham Boyle

Noncommutative geometry applied to the standard model of electroweak and strong interactions was shown to produce fuzzy relations among masses and gauge couplings. We refine these relations and show then that they are exhaustive.

High Energy Physics - Theory · Physics 2009-10-30 Lionel Carminati , Bruno Iochum , Thomas Schucker

The Standard Model of elementary particles is a theory unifying three of the four basic forces of the Nature: electromagnetic, weak, and strong interactions. In this paper we consider the Standard Model in the presence of a classical…

Differential Geometry · Mathematics 2007-05-23 Ruslan Sharipov

We render a thorough, physicist's account of the formulation of the Standard Model (SM) of particle physics within the framework of noncommutative differential geometry (NCG). We work in Minkowski spacetime rather than in Euclidean space.…

High Energy Physics - Theory · Physics 2008-11-26 C. P. Martin , Jose M. Gracia-Bondia , Joseph C. Varilly

Alain Connes' noncommutative theory led to an interesting model including both Standard Model of particle physics and Euclidean Gravity. Nevertheless, an hyperbolic version of the gravitational part would be necessary to make physical…

Mathematical Physics · Physics 2013-06-11 Nicolas Franco

We review the noncommutative approach to the standard model. We start with the introduction if the mathematical concepts necessary for the definition of noncommutative spaces, and manifold in particular. This defines the framework of…

High Energy Physics - Theory · Physics 2018-05-02 Fedele Lizzi

Unification of electromagnetic, weak, and strong coupling constants is studied in the extension of standard model with additional fermions and scalars. It is remarkable that this unification in the supersymmetric extension of standard model…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ling-Fong Li , Feng Wu

We review the construction of particle physics models in the framework of non-commutative geometry. We first give simple examples, and then progress to outline the Connes-Lott construction of the standard Weinberg-Salam model and our…

High Energy Physics - Theory · Physics 2007-05-23 A. H. Chamseddine , J. Fröhlich

A new geometry, called General geometry, is constructed. It is proven that its the most simplest special case is geometry underlying Electromagnetism. Another special case is Riemannian geometry. Action for electromagnetic field and Maxwell…

General Physics · Physics 2007-05-23 Shervgi Shahverdiyev
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