Search results for "noncommutative geometry"

showing 10 items of 36 documents

Muon physics — Survey

1992

The empirical basis of the minimal standard model has been consolidated in an impressive way, over the last seventeen years, by precision experiments at the meson factories. I illustrate this by means of selected examples of muonic weak interaction processes. I then describe an extension of Yang-Mills theory, inspired by noncommutative geometry, that yields precisely the standard model but fixes and explains some of its empirical input. In particular, this new approach yields a simple geometrical interpretation of spontaneous symmetry breaking. The algebraic framework of this approach offers a natural place for the lepton and quark matter fields and for inter-family mixing.

PhysicsHiggs fieldParticle physicsMuonMesonSpontaneous symmetry breakingSymmetry breakingQuantum field theoryNoncommutative geometryStandard Model
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Leptonic Generation Mixing, Noncommutative Geometry and Solar Neutrino Fluxes

1997

Triangular mass matrices for neutrinos and their charged partners contain full information on neutrino mixing in a most concise form. Although the scheme is general and model independent, triangular matrices are typical for reducible but indecomposable representations of graded Lie algebras which, in turn, are characteristic for the standard model in noncommutative geometry. The mixing matrix responsible for neutrino oscillations is worked out analytically for two and three lepton families. The example of two families fixes the mixing angle to just about what is required by the Mikheyev-Smirnov-Wolfenstein resonance oscillation of solar neutrinos. In the case of three families we classify a…

PhysicsNuclear and High Energy PhysicsParticle physicsSolar neutrinoHigh Energy Physics::PhenomenologyFOS: Physical sciencesNoncommutative geometryStandard Model (mathematical formulation)Matrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)Lepton
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The su(2|1) Model of Electroweak Interactions and Its Connection to NC Geometry

2002

I review the su(2|1) model of electroweak interactions which is essentially based on the super Lie algebra su(2|1), thus incorporating both usual gauge fields and Higgs fields in one generalized Yang-Mills field. Special emphasis is put on the natural appearance of spontaneous symmetry breaking and other appealing features of the model like generation mixing. Also the connection of the model to noncommutative geometry is briefly discussed.

Theoretical physicsField (physics)Quantum electrodynamicsSpontaneous symmetry breakingHigh Energy Physics::PhenomenologyElectroweak interactionLie algebraHiggs bosonNoncommutative geometrySpecial unitary groupMathematicsConnection (mathematics)
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Perturbative BF-Yang–Mills theory on noncommutative

2000

A U(1) BF-Yang-Mills theory on noncommutative ${\mathbb{R}}^4$ is presented and in this formulation the U(1) Yang-Mills theory on noncommutative ${\mathbb{R}}^4$ is seen as a deformation of the pure BF theory. Quantization using BRST symmetry formalism is discussed and Feynman rules are given. Computations at one-loop order have been performed and their renormalization studied. It is shown that the U(1) BFYM on noncommutative ${\mathbb{R}}^4$ is asymptotically free and its UV-behaviour in the computation of the $\beta$-function is like the usual SU(N) commutative BFYM and Yang Mills theories.

PhysicsNuclear and High Energy PhysicsYang–Mills existence and mass gapYang–Mills theoryNoncommutative geometryBRST quantizationRenormalizationHigh Energy Physics::Theorysymbols.namesakeFormalism (philosophy of mathematics)Mathematics::Quantum AlgebrasymbolsFeynman diagramCommutative propertyMathematical physicsNuclear Physics B
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A natural and rigid model of quantum groups

1992

We introduce a natural (Frechet-Hopf) algebra A containing all generic Jimbo algebras U t (sl(2)) (as dense subalgebras). The Hopf structures on A extend (in a continuous way) the Hopf structures of generic U t (sl(2)). The Universal R-matrices converge in A\(\hat \otimes \)A. Using the (topological) dual of A, we recover the formalism of functions of noncommutative arguments. In addition, we show that all these Hopf structures on A are isomorphic (as bialgebras), and rigid in the category of bialgebras.

Discrete mathematicsFormalism (philosophy of mathematics)Pure mathematicsRigid modelQuantum groupMathematics::Quantum AlgebraMathematics::Rings and AlgebrasStatistical and Nonlinear PhysicsHopf algebraNoncommutative geometryQuantumMathematical PhysicsMathematicsLetters in Mathematical Physics
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Mass relations in noncommutative geometry revisited

1997

We generalize the notion of the 'noncommutative coupling constant' given by Kastler and Sch"ucker by dropping the constraint that it commute with the Dirac-operator. This leads essentially to the vanishing of the lower bound for the Higgsmass and of the upper bound for the W-mass.

PhysicsCoupling constantConstraint (information theory)High Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics - Theory (hep-th)Mathematics::Operator AlgebrasFOS: Physical sciencesUpper and lower boundsNoncommutative geometryMathematical physics
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Supersymmetry in the standard model of electroweak interactions

1993

Abstract Starting from the peculiar chirality pattern of weak and electromagnetic interactions, established by experiment, we show that the minimal standard model contains supersymmetry, though in a new, unconventional, realization. It appears as an action on the fields but is not an invariance of the lagrangian. This supersymmetry which is not in conflict with experiment, is seen to be the raison d'etre of the Higgs fields and provides a geometrical understanding of spontaneous symmetry breaking. It turns out that this approach which is based on the fundamental role of left- and right-chiral spinor fields in weak interactions, has many similarities to models developed in the framework of n…

PhysicsNuclear and High Energy PhysicsParticle physicsTheoretical physicsSpinorSpontaneous symmetry breakingHigh Energy Physics::PhenomenologyElectroweak interactionHiggs bosonSupersymmetrySupersymmetry breakingNoncommutative geometryStandard ModelPhysics Letters B
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“The Important Thing is not to Stop Questioning”, Including the Symmetries on Which is Based the Standard Model

2014

New fundamental physical theories can, so far a posteriori, be seen as emerging from existing ones via some kind of deformation. That is the basis for Flato’s “deformation philosophy”, of which the main paradigms are the physics revolutions from the beginning of the twentieth century, quantum mechanics (via deformation quantization) and special relativity. On the basis of these facts we describe two main directions by which symmetries of hadrons (strongly interacting elementary particles) may “emerge” by deforming in some sense (including quantization) the Anti de Sitter symmetry (AdS), itself a deformation of the Poincare group of special relativity. The ultimate goal is to base on fundame…

Physicssymbols.namesakeQuantization (physics)Theoretical physicsClassical mechanicsPoincaré groupElectroweak interactionsymbolsHiggs bosonElementary particleAnti-de Sitter spaceEinsteinNoncommutative geometry
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A non self-adjoint model on a two dimensional noncommutative space with unbound metric

2013

We demonstrate that a non self-adjoint Hamiltonian of harmonic oscillator type defined on a two-dimensional noncommutative space can be diagonalized exactly by making use of pseudo-bosonic operators. The model admits an antilinear symmetry and is of the type studied in the context of PT-symmetric quantum mechanics. Its eigenvalues are computed to be real for the entire range of the coupling constants and the biorthogonal sets of eigenstates for the Hamiltonian and its adjoint are explicitly constructed. We show that despite the fact that these sets are complete and biorthogonal, they involve an unbounded metric operator and therefore do not constitute (Riesz) bases for the Hilbert space $\L…

PhysicsCoupling constantPure mathematicsQuantum PhysicsHilbert spacepseudo-bosoniFOS: Physical sciencesMathematical Physics (math-ph)Noncommutative geometryAtomic and Molecular Physics and Opticssymbols.namesakeOperator (computer programming)Biorthogonal systemQuantum mechanicssymbolsQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)QASettore MAT/07 - Fisica MatematicaSelf-adjoint operatorEigenvalues and eigenvectorsMathematical Physics
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Exact treatment of operator difference equations with nonconstant and noncommutative coefficients

2013

We study a homogeneous linear second-order difference equation with nonconstant and noncommuting operator coefficients in a vector space. We build its exact resolutive formula consisting of the explicit noniterative expression of a generic term of the unknown sequence of vectors. Some nontrivial applications are reported in order to show the usefulness and the broad applicability of the result.

Cauchy problemSequenceDifferential equationGeneral MathematicsOperator (physics)Mathematical analysisGeneral EngineeringExpression (computer science)Term (logic)Noncommutative geometrySettore FIS/03 - Fisica Della MateriaCauchy problem Noncommuting operators Operator difference equationsMathematicsVector space
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