Search results for "Representation theory"

showing 10 items of 197 documents

Star Products on Coadjoint Orbits

2000

We study properties of a family of algebraic star products defined on coadjoint orbits of semisimple Lie groups. We connect this description with the point of view of differentiable deformations and geometric quantization.

PhysicsGeometric quantizationHigh Energy Physics - TheoryNuclear and High Energy PhysicsPure mathematicsLie groupFísicaFOS: Physical sciencesStar (graph theory)Atomic and Molecular Physics and OpticsHigh Energy Physics - Theory (hep-th)Mathematics::Quantum AlgebraMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Point (geometry)Differentiable functionAstrophysics::Earth and Planetary AstrophysicsAlgebraic numberMathematics::Representation Theory
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Higher-Order Differential Operators on a Lie Group and Quantization

1995

This talk is devoted mainly to the concept of higher-order polarization on a group, which is introduced in the framework of a Group Approach to Quantization, as a powerful tool to guarantee the irreducibility of quantizations and/or representations of Lie groups in those anomalous cases where the Kostant-Kirilov co-adjoint method or the Borel-Weyl-Bott representation algorithm do not succeed.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsGroup (mathematics)Quantization (signal processing)FOS: Physical sciencesLie groupAstronomy and AstrophysicsDifferential operatorAtomic and Molecular Physics and OpticsAlgebraHigh Energy Physics - Theory (hep-th)IrreducibilityOrder (group theory)Representation (mathematics)Mathematics::Representation Theory
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A star-product approach to noncompact Quantum Groups

1995

Using duality and topological theory of well behaved Hopf algebras (as defined in [2]) we construct star-product models of non compact quantum groups from Drinfeld and Reshetikhin standard deformations of enveloping Hopf algebras of simple Lie algebras. Our star-products act not only on coefficient functions of finite-dimensional representations, but actually on all $C^\infty$ functions, and they exist even for non linear (semi-simple) Lie groups.

PhysicsHigh Energy Physics - TheoryPure mathematics[MATH.MATH-RT]Mathematics [math]/Representation Theory [math.RT]010102 general mathematicsLie groupDuality (optimization)Statistical and Nonlinear Physics16. Peace & justiceHopf algebra01 natural sciences[ MATH.MATH-RT ] Mathematics [math]/Representation Theory [math.RT]Nonlinear systemSimple (abstract algebra)Product (mathematics)Mathematics::Quantum Algebra0103 physical sciencesLie algebraMathematics - Quantum Algebra010307 mathematical physics0101 mathematicsQuantumMathematical PhysicsComputingMilieux_MISCELLANEOUS
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-Poincaré supergravities from Lie algebra expansions

2012

Abstract We use the expansion of superalgebras procedure (summarized in the text) to derive Chern–Simons (CS) actions for the ( p , q ) -Poincare supergravities in three-dimensional spacetimes. After deriving the action for the ( p , 0 ) -Poincare supergravity as a CS theory for the expansion osp ( p | 2 ; R ) ( 2 , 1 ) of osp ( p | 2 ; R ) , we find the general ( p , q ) -Poincare superalgebras and their associated D = 3 supergravity actions as CS gauge theories from an expansion of the simple osp ( p + q | 2 , R ) superalgebras, namely osp ( p + q | 2 , R ) ( 2 , 1 , 2 ) .

PhysicsNuclear and High Energy PhysicsSupergravityAction (physics)High Energy Physics::Theorysymbols.namesakeSimple (abstract algebra)Mathematics::Quantum AlgebraPoincaré conjectureLie algebrasymbolsGauge theoryMathematics::Representation TheoryMathematical physicsNuclear Physics B
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Noncompact Topological Quantum Groups

1995

A star-product construction of quantum semisimple real Lie groups is performed for the noncompact case.

PhysicsQuantum groupLie groupTopological entropy in physicsSymmetry protected topological orderTheoretical physicsMathematics::Quantum AlgebraInverse scattering problemAstrophysics::Solar and Stellar AstrophysicsMathematics::Differential GeometryMathematics::Representation TheoryQuantumAstrophysics::Galaxy AstrophysicsTopological quantum number
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The Nonlinear σ Model

1989

The nonlinear (principal) σ model has been for a long time a theoretical laboratory to test different approaches for quantizing classical field theories. Here we shall discuss as an application of the current algebra representation theory a construction of the quantized σ model.

PhysicsTheoretical physicsNonlinear systemLine bundleField (physics)Current algebraClassical field theoryRepresentation theorySymplectic manifoldNon-linear sigma model
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Obtaining the Weyl tensor from the Bel-Robinson tensor

2010

The algebraic study of the Bel-Robinson tensor proposed and initiated in a previous work (Gen. Relativ. Gravit. {\bf 41}, see ref [11]) is achieved. The canonical form of the different algebraic types is obtained in terms of Bel-Robinson eigen-tensors. An algorithmic determination of the Weyl tensor from the Bel-Robinson tensor is presented.

PhysicsWeyl tensorPhysics and Astronomy (miscellaneous)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum Cosmologysymbols.namesakeGeneral Relativity and Quantum CosmologyTensor (intrinsic definition)symbolsAlgebraic data typeCanonical formAlgebraic numberMathematics::Representation TheoryMathematical physics
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Fermion Fields and Their Properties

2011

The fundamental building blocks of matter, i.e. quarks and leptons, carry spin 1/2. There are two formally different but in essence equivalent methods of describing particles with spin: The representation theory of the Poincare group, in the framework of Wigner’s classification hypothesis of particles (see e.g. [QP07], Chap. 6), and the Van der Waerden spinor calculus based on SL(2, \(\mathbb{C}\)).

Physicssymbols.namesakeFermion doublingSpinorHelical Dirac fermionDirac equationsymbolsVan der Waerden's theoremFermionRepresentation theory of the Poincaré groupSpin-½Mathematical physics
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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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The Schur property on projective and injective tensor products

2008

The problem of whether the Schur property is passed from a Banach space to its (symmetric) projective n-fold tensor product is reformu lated in the language of polynomial ideals. As a result, a very closely related question is solved in the negative. It is also proved that the injective tensor product of infrabarrelled locally convex spaces with the Schur property has the Schur property as well.

PolynomialPure mathematicsTensor product of algebrasApplied MathematicsGeneral MathematicsTensor product of Hilbert spacesBanach spaceInjective functionAlgebraTensor productLocally convex topological vector spaceTensor product of modulesMathematics::Representation TheoryMathematicsProceedings of the American Mathematical Society
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