Search results for "Representation theory"

showing 10 items of 197 documents

Kac-Moody group representations and generalization of the Sugawara construction of the Virasoro algebra

1988

We discuss the dynamical structure of the semidirect product of the Virasoro and affine Kac-Moody groups within the framework of a group quantization formalism. This formalism provides a realization of the Virasoro algebra acting on Kac-Moody Fock states which generalizes the Sugawara construction. We also give an explicit construction of the standard Kac-Moody group representations associated with strings on SU(2) and recover, in particular, the ‘renormalization’ β factor of L(z)

Quantum affine algebraPure mathematicsSemidirect productCurrent algebraStatistical and Nonlinear PhysicsUniversal enveloping algebraGroup algebraN = 2 superconformal algebraAlgebraHigh Energy Physics::TheoryMathematics::Quantum AlgebraAlgebra representationVirasoro algebraMathematics::Representation TheoryMathematical PhysicsMathematicsLetters in Mathematical Physics
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Quantum deformations of singletons and of free zero-mass fields

1993

We consider quantum deformations of the real symplectic (or anti-De Sitter) algebra sp(4), ℝ ≅ spin(3, 2) and of its singleton and (4-dimensional) zero-mass representations. For q a root of −1, these representations admit finite-dimensional unitary subrepresentations. It is pointed out that Uq(sp(4, ℝ)), unlike Uq(su(2, 2)), contains Uq(sl2) as a quantum subalgebra.

Quantum mechanicsSubalgebraGeneral Physics and AstronomyQuantum algebraLie groupQuantum field theoryMathematics::Representation TheorySL2(R)QuantumMathematicsSpin-½Symplectic geometryMathematical physicsFoundations of Physics
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On Associative Rings with Locally Nilpotent Adjoint Semigroup

2003

Abstract The set of all elements of an associative ring R, not necessarily with a unit element, forms a semigroup R ad under the circle operation r ∘ s = r + s + rs for all r, s in R. This semigroup is locally nilpotent if every finitely generated subsemigroup of R ad is nilpotent (in sense of A. I. Mal'cev or B. H. Neumann and T. Taylor). The ring R is locally Lie-nilpotent if every finitely generated subring of R is Lie-nilpotent. It is proved that R ad is a locally nilpotent semigroup if and only if R is a locally Lie-nilpotent ring.

Reduced ringDiscrete mathematicsPure mathematicsAlgebra and Number TheoryMathematics::Rings and AlgebrasLocally nilpotentUnipotentSubringMathematics::Group TheoryNilpotentBicyclic semigroupNilpotent groupMathematics::Representation TheoryUnit (ring theory)MathematicsCommunications in Algebra
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Module categories of finite Hopf algebroids, and self-duality

2017

International audience; We characterize the module categories of suitably finite Hopf algebroids (more precisely, $X_R$-bialgebras in the sense of Takeuchi (1977) that are Hopf and finite in the sense of a work by the author (2000)) as those $k$-linear abelian monoidal categories that are module categories of some algebra, and admit dual objects for "sufficiently many" of their objects. Then we proceed to show that in many situations the Hopf algebroid can be chosen to be self-dual, in a sense to be made precise. This generalizes a result of Pfeiffer for pivotal fusion categories and the weak Hopf algebras associated to them.

Self-duality[ MATH ] Mathematics [math]Finite tensor categoryGeneral MathematicsDuality (mathematics)Representation theory of Hopf algebrasBimodulesQuasitriangular Hopf algebra01 natural sciencesMonoidal CategoriesMathematics::Category TheoryMathematics::Quantum Algebra0103 physical sciencesRings0101 mathematicsAlgebra over a fieldAbelian group[MATH]Mathematics [math]Fusion categoryHopf algebroidMSC: Primary 16T99 18D10SubfactorsMathematicsQuantum groupApplied Mathematics010102 general mathematicsMathematics::Rings and AlgebrasTensor CategoriesTheorem16. Peace & justiceHopf algebraDual (category theory)Algebra010307 mathematical physicsWeak Hopf algebra
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The Kp Hierarchy

1989

As an application of the theory of infinite-dimensional Grassmannians and the representation theory of gl1 we shall study in this chapter certain nonlinear “exactly solvable” systems of differential equations. Exactly solvable means here that the nonlinear system can be transformed to an (infinite-dimensional) linear problem. A prototype of the equations is the Korteweg-de Vries equation $$\frac{{\partial u}}{{\partial t}} = \frac{3}{3}u\frac{{\partial u}}{{\partial x}} + \frac{1}{4}\frac{{{\partial ^3}u}}{{\partial {x^3}}}$$ . It turns out that it is more natural to consider an infinite system of equations like that above, for obtaining explicit solutions. The set of equations is called th…

Set (abstract data type)Pure mathematicsNonlinear systemNonlinear Sciences::Exactly Solvable and Integrable SystemsHierarchy (mathematics)Differential equationGrassmannianKdV hierarchySystem of linear equationsRepresentation theoryMathematics
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Harmonic maps and singularities of period mappings

2015

We use simple methods from harmonic maps to investigate singularities of period mappings at infinity. More precisely, we derive a harmonic map version of Schmid’s nilpotent orbit theorem. MSC Classification 14M27, 58E20

Simple (abstract algebra)Applied MathematicsGeneral Mathematicsmedia_common.quotation_subjectMathematical analysisHarmonic mapNilpotent orbitGravitational singularityMathematics::Representation TheoryInfinityPeriod (music)media_commonMathematicsProceedings of the American Mathematical Society
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The Dunkl–Williams constant, convexity, smoothness and normal structure

2008

Abstract In this paper we exhibit some connections between the Dunkl–Williams constant and some other well-known constants and notions. We establish bounds for the Dunkl–Williams constant that explain and quantify a characterization of uniformly nonsquare Banach spaces in terms of the Dunkl–Williams constant given by M. Baronti and P.L. Papini. We also study the relationship between Dunkl–Williams constant, the fixed point property for nonexpansive mappings and normal structure.

Smoothness (probability theory)Applied MathematicsMathematical analysisStructure (category theory)Banach spaceMathematics::Classical Analysis and ODEsCharacterization (mathematics)Fixed-point propertyJames constantSmoothnessNormal structureConvexityPhysics::History of PhysicsDunkl–Williams constantConvexityMathematics::Quantum AlgebraConstant (mathematics)Mathematics::Representation TheoryAnalysisMathematicsJournal of Mathematical Analysis and Applications
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Locally convex quasi $C^*$-normed algebras

2012

Abstract If A 0 [ ‖ ⋅ ‖ 0 ] is a C ∗ -normed algebra and τ a locally convex topology on A 0 making its multiplication separately continuous, then A 0 ˜ [ τ ] (completion of A 0 [ τ ] ) is a locally convex quasi ∗-algebra over A 0 , but it is not necessarily a locally convex quasi ∗-algebra over the C ∗ -algebra A 0 ˜ [ ‖ ⋅ ‖ 0 ] (completion of A 0 [ ‖ ⋅ ‖ 0 ] ). In this article, stimulated by physical examples, we introduce the notion of a locally convex quasi C ∗ -normed algebra, aiming at the investigation of A 0 ˜ [ τ ] ; in particular, we study its structure, ∗-representation theory and functional calculus.

Strong commutatively quasi-positive elementNormed algebraPure mathematicsApplied MathematicsRegular locally convex topologyRegular polygonStructure (category theory)Mathematics - Operator AlgebrasFOS: Physical sciencesLocally convex quasi C∗-normed algebraMathematical Physics (math-ph)Representation theoryquasi *-algebras C*-normsFunctional calculusMathematics::LogicCommutatively quasi-positive elementSettore MAT/05 - Analisi MatematicaFOS: MathematicsMultiplicationAlgebra over a fieldElement (category theory)Operator Algebras (math.OA)AnalysisMathematical PhysicsMathematics
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Maximal Operators with Respect to the Numerical Range

2018

Let $\mathfrak{n}$ be a nonempty, proper, convex subset of $\mathbb{C}$. The $\mathfrak{n}$-maximal operators are defined as the operators having numerical ranges in $\mathfrak{n}$ and are maximal with this property. Typical examples of these are the maximal symmetric (or accretive or dissipative) operators, the associated to some sesquilinear forms (for instance, to closed sectorial forms), and the generators of some strongly continuous semi-groups of bounded operators. In this paper the $\mathfrak{n}$-maximal operators are studied and some characterizations of these in terms of the resolvent set are given.

Strongly continuous semi-groupsPure mathematicsCayley transformSesquilinear form01 natural sciencesSettore MAT/05 - Analisi MatematicaMaximal operator0103 physical sciencesFOS: Mathematics0101 mathematicsMathematics::Representation TheoryNumerical rangeMathematics47A20 47A12 47B44 47A07Resolvent setApplied Mathematics010102 general mathematicsRegular polygonOperator theoryFunctional Analysis (math.FA)Mathematics - Functional AnalysisComputational MathematicsComputational Theory and MathematicsBounded functionDissipative systemSectorStrip010307 mathematical physicsNumerical rangeComplex Analysis and Operator Theory
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Annihilators of tensor density modules

2007

Abstract We describe the two-sided ideals in the universal enveloping algebras of the Lie algebras of vector fields on the line and the circle which annihilate the tensor density modules. Both of these Lie algebras contain the projective subalgebra, a copy of sl 2 . The restrictions of the tensor density modules to this subalgebra are duals of Verma modules (of sl 2 ) for Vec ( R ) and principal series modules (of sl 2 ) for Vec ( S 1 ) . Thus our results are related to the well-known theorem of Duflo describing the annihilating ideals of Verma modules of reductive Lie algebras. We find that, in general, the annihilator of a tensor density module of Vec ( R ) or Vec ( S 1 ) is generated by …

Tensor density modulesPure mathematicsVerma moduleAlgebra and Number TheorySubalgebraMathematics::Rings and AlgebrasUniversal enveloping algebraGeneralized Verma moduleAffine Lie algebraLie conformal algebraAnnihilating idealsMathematics::Quantum AlgebraTensor product of modulesTensor densityMathematics::Representation TheoryMathematicsJournal of Algebra
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