Search results for "NONCOMMUTATIVE GEOMETRY"

showing 10 items of 36 documents

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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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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Multiple Noncommutative Tori and Hopf Algebras

2001

We derive the Kac-Paljutkin finite-dimensional Hopf algebras as finite fibrations of the quantum double torus and generalize the construction for quantum multiple tori.

PhysicsPure mathematicsAlgebra and Number TheoryFOS: Physical sciencesTorusMathematics - Rings and AlgebrasMathematical Physics (math-ph)Hopf algebraNoncommutative geometry16W30 57T05Rings and Algebras (math.RA)Mathematics::Quantum AlgebraMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Mathematics::Symplectic GeometryQuantumMathematical PhysicsCommunications in Algebra
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Probing Models of Extended Gravity using Gravity Probe B and LARES experiments

2014

We consider models of Extended Gravity and in particular, generic models containing scalar-tensor and higher-order curvature terms, as well as a model derived from noncommutative spectral geometry. Studying, in the weak-field approximation, the geodesic and Lense-Thirring processions, we impose constraints on the free parameters of such models by using the recent experimental results of the Gravity Probe B and LARES satellites.

PhysicsSPECTRAL ACTION; NONCOMMUTATIVE GEOMETRY; NEWTONIAN DYNAMICSHigh Energy Physics - TheoryNuclear and High Energy PhysicsGravity (chemistry)Cosmology and Nongalactic Astrophysics (astro-ph.CO)GeodesicNEWTONIAN DYNAMICSSpectral geometryFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)CurvatureSPECTRAL ACTIONNoncommutative geometryGeneral Relativity and Quantum CosmologyNewtonian dynamicsTheoretical physicsTheory of relativityClassical mechanicsHigh Energy Physics - Theory (hep-th)NONCOMMUTATIVE GEOMETRYPhysics::Space PhysicsFree parameterAstrophysics - Cosmology and Nongalactic Astrophysics
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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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Defining relations of the noncommutative trace algebra of two 3×3 matrices

2006

The noncommutative (or mixed) trace algebra $T_{nd}$ is generated by $d$ generic $n\times n$ matrices and by the algebra $C_{nd}$ generated by all traces of products of generic matrices, $n,d\geq 2$. It is known that over a field of characteristic 0 this algebra is a finitely generated free module over a polynomial subalgebra $S$ of the center $C_{nd}$. For $n=3$ and $d=2$ we have found explicitly such a subalgebra $S$ and a set of free generators of the $S$-module $T_{32}$. We give also a set of defining relations of $T_{32}$ as an algebra and a Groebner basis of the corresponding ideal. The proofs are based on easy computer calculations with standard functions of Maple, the explicit prese…

Polynomial (hyperelastic model)Defining relationsTrace (linear algebra)Trace algebrasApplied MathematicsSubalgebraCenter (category theory)Free moduleNoncommutative geometryRepresentation theoryAlgebraGröbner basisGeneric matricesMatrix invariants and concomitantsGröbner basisMathematicsAdvances in Applied Mathematics
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Central Polynomials of Algebras and Their Growth

2020

A polynomial in noncommutative variables taking central values in an algebra A is called a central polynomial of A. For instance the algebra of k × k matrices has central polynomials. For general algebras the existence of central polynomials is not granted. Nevertheless if an algebra has such polynomials, how can one measure how many are there?

PolynomialPure mathematicsExponential growthCodimensionAlgebra over a fieldMeasure (mathematics)Noncommutative geometryMathematics
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Two-dimensional Noncommutative Swanson Model and Its Bicoherent States

2019

We introduce an extended version of the Swanson model, defined on a two-dimensional noncommutative space, which can be diagonalized exactly by making use of pseudo-bosonic operators. Its eigenvalues are explicitly computed and the biorthogonal sets of eigenstates of the Hamiltonian and of its adjoint are explicitly constructed.We also show that it is possible to construct two displacement-like operators from which a family of bi-coherent states can be obtained. These states are shown to be eigenstates of the deformed lowering operators, and their projector allows to produce a suitable resolution of the identity in a dense subspace of \(\mathcal{L}^\mathrm{2}\, (\mathbb{R}^\mathrm{2})\).

Pseudo-bosonPhysicsSwanson modelNoncommutative geometrylaw.inventionsymbols.namesakeProjectorlawBiorthogonal systemsymbolsMathematics (all)Coherent statesHamiltonian (quantum mechanics)Coherent stateEigenvalues and eigenvectorsSubspace topologyMathematical physics
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Extensions of the Noncommutative Integration

2016

In this paper we will continue the analysis undertaken in Bagarello et al. (Rend Circ Mat Palermo (2) 55:21–28, 2006), Bongiorno et al. (Rocky Mt J Math 40(6):1745–1777, 2010), Triolo (Rend Circ Mat Palermo (2) 60(3):409–416, 2011) on the general problem of extending the noncommutative integration in a *-algebra of measurable operators. As in Aiena et al. (Filomat 28(2):263–273, 2014), Bagarello (Stud Math 172(3):289–305, 2006) and Bagarello et al. (Rend Circ Mat Palermo (2) 55:21–28, 2006), the main problem is to represent different types of partial *-algebras into a *-algebra of measurable operators in Segal’s sense, provided that these partial *-algebras posses a sufficient family of pos…

Pure mathematicsApplied MathematicsGeneral problem010102 general mathematicsMeasurable operatorOperator theory01 natural sciencesNoncommutative geometryNoncommutative integrationPartial algebras of operator010101 applied mathematicsComputational MathematicsComputational Theory and MathematicsSettore MAT/05 - Analisi MatematicaComputational Theory and MathematicComputational Mathematic0101 mathematicsAlgebra over a fieldCommutative propertyMathematicsComplex Analysis and Operator Theory
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Locally convex quasi C*-algebras and noncommutative integration

2015

In this paper we continue the analysis undertaken in a series of previous papers on structures arising as completions of C*-algebras under topologies coarser that their norm and we focus our attention on the so-called {\em locally convex quasi C*-algebras}. We show, in particular, that any strongly *-semisimple locally convex quasi C*-algebra $(\X,\Ao)$, can be represented in a class of noncommutative local $L^2$-spaces.

Pure mathematicsClass (set theory)Series (mathematics)General Mathematicsnoncommutative integrationRegular polygonFOS: Physical sciencesMathematical Physics (math-ph)Noncommutative geometrySettore MAT/05 - Analisi MatematicaNorm (mathematics)quasi C*-algebrasPrimary 46L08 Secondary 46L51 47L60Focus (optics)Mathematical PhysicsMathematics
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