Search results for "Quantum algebra"

showing 10 items of 117 documents

Quantum and Braided Integrals

2001

We give a pedagogical introduction to integration techniques appropriate for non-commutative spaces while presenting some new results as well. A rather detailed discussion outlines the motivation for adopting the Hopf algebra language. We then present some trace formulas for the integral on Hopf algebras and show how to treat the $\int 1=0$ case. We extend the discussion to braided Hopf algebras relying on diagrammatic techniques. The use of the general formulas is illustrated by explicitly worked out examples.

High Energy Physics - TheoryPure mathematicsQuantum affine algebraQuantum groupFOS: Physical sciencesRepresentation theory of Hopf algebrasMathematical Physics (math-ph)Quasitriangular Hopf algebraHopf algebraFiltered algebraAlgebraHigh Energy Physics - Theory (hep-th)Mathematics::Quantum AlgebraMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)QuantumMathematical PhysicsMathematicsProceedings of Corfu Summer Institute on Elementary Particle Physics — PoS(corfu98)
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The $q$-calculus for generic $q$ and $q$ a root of unity

1996

The $q$-calculus for generic $q$ is developed and related to the deformed oscillator of parameter $q^{1/2}$. By passing with care to the limit in which $q$ is a root of unity, one uncovers the full algebraic structure of ${{\cal Z}}_n$-graded fractional supersymmetry and its natural representation.

High Energy Physics - TheoryPure mathematicsRoot of unityAlgebraic structureFOS: Physical sciencesGeneral Physics and AstronomyFractional supersymmetryHigh Energy Physics - Theory (hep-th)Mathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Limit (mathematics)Representation (mathematics)Mathematics
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Instanton Counting, Quantum Geometry and Algebra

2020

The aim of this memoir for "Habilitation \`a Diriger des Recherches" is to present quantum geometric and algebraic aspects of supersymmetric gauge theory, which emerge from non-perturbative nature of the vacuum structure induced by instantons. We start with a brief summary of the equivariant localization of the instanton moduli space, and show how to obtain the instanton partition function and its generalization to quiver gauge theory and supergroup gauge theory in three ways: the equivariant index formula, the contour integral formula, and the combinatorial formula. We then explore the geometric description of $\mathcal{N} = 2$ gauge theory based on Seiberg-Witten geometry together with it…

High Energy Physics - TheoryQuiver gauge theoryThéorie de jauje de carquoisHigh Energy Physics::Lattice[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]FOS: Physical sciencesQuiver W-algebraqq-characterW-algébre de carquoisHigh Energy Physics::TheorySupergroupgauge theory[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]InstantonMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Representation Theory (math.RT)Algébre vertexComputingMilieux_MISCELLANEOUSMathematical PhysicsSeiberg–Witten geometryIntegrable systemqq-caractéreVertex operator algebra[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics::PhenomenologyMathematical Physics (math-ph)Localization équivarianteGéométrie de Seiberg–WittenHigh Energy Physics - Theory (hep-th)Théoriede jauje de supergroupe[PHYS.HTHE] Physics [physics]/High Energy Physics - Theory [hep-th]Systèmes intégrablesEquivariant localizationMathematics - Representation Theory
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Spin Chains with Non-Diagonal Boundaries and Trigonometric SOS Model with Reflecting End

2011

In this paper we consider two a priori very different problems: construction of the eigenstates of the spin chains with non parallel boundary magnetic fields and computation of the partition function for the trigonometric solid-on-solid (SOS) model with one reflecting end and domain wall boundary conditions. We show that these two problems are related through a gauge transformation (so-called vertex-face transformation) and can be solved using the same dynamical reflection algebras.

High Energy Physics - TheorySOS modelsspin chainsDiagonalFOS: Physical sciencesBoundary (topology)algebraic Bethe ansatzMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Boundary value problemGauge theoryMathematical PhysicsEigenvalues and eigenvectorsMathematicsSpin-½Partition function (statistical mechanics)Nonlinear Sciences - Exactly Solvable and Integrable Systemslcsh:MathematicsMathematical analysisMathematical Physics (math-ph)lcsh:QA1-939dynamical reflection algebraTransformation (function)High Energy Physics - Theory (hep-th)Geometry and TopologyExactly Solvable and Integrable Systems (nlin.SI)AnalysisSymmetry, Integrability and Geometry: Methods and Applications
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Deformation quantization of covariant fields

2002

After sketching recent advances and subtleties in classical relativistically covariant field theories, we give in this short Note some indications as to how the deformation quantization approach can be used to solve or at least give a better understanding of their quantization.

High Energy Physics - Theory[MATH.MATH-QA] Mathematics [math]/Quantum Algebra [math.QA][ MATH.MATH-QA ] Mathematics [math]/Quantum Algebra [math.QA][PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]010102 general mathematicsFOS: Physical sciences01 natural sciences[ PHYS.HTHE ] Physics [physics]/High Energy Physics - Theory [hep-th]MSC: 53D55 81T70 81R20 35G25deformation quantizationnonlinear representationsHigh Energy Physics - Theory (hep-th)53D55 81T70 81R20 35G250103 physical sciencesMathematics - Quantum Algebra[MATH.MATH-QA]Mathematics [math]/Quantum Algebra [math.QA]FOS: MathematicsQuantum Algebra (math.QA)[PHYS.HTHE] Physics [physics]/High Energy Physics - Theory [hep-th]010307 mathematical physics0101 mathematicsquantum field theory
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Integrating over quiver variety and BPS/CFT correspondence

2019

We show the vertex operator formalism for the quiver gauge theory partition function and the $qq$-character of highest-weight module on quiver, both associated with the integral over the quiver variety.

High Energy Physics - Theorypartition function[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]FOS: Physical sciencesalgebraSupersymmetric gauge theoryQuiver variety[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Mathematics - Quantum AlgebraInstantonFOS: MathematicsQuantum Algebra (math.QA)Representation Theory (math.RT)Mathematics::Representation Theoryfield theory: conformalVertex operator algebra[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]W-algebraMathematics::Rings and Algebras[PHYS.MPHY] Physics [physics]/Mathematical Physics [math-ph]operator: vertexgauge field theory: quiverConformal field theoryHigh Energy Physics - Theory (hep-th)BPS[PHYS.HTHE] Physics [physics]/High Energy Physics - Theory [hep-th]instantonsMathematics - Representation Theory
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About Leibniz cohomology and deformations of Lie algebras

2011

We compare the second adjoint and trivial Leibniz cohomology spaces of a Lie algebra to the usual ones by a very elementary approach. The comparison gives some conditions, which are easy to verify for a given Lie algebra, for deciding whether it has more Leibniz deformations than just the Lie ones. We also give the complete description of a Leibniz (and Lie) versal deformation of the 4-dimensional diamond Lie algebra, and study the case of its 5-dimensional analogue.

Leibniz algebraPure mathematicsAlgebra and Number TheoryMathematics::Rings and AlgebrasInfinitesimal deformationK-Theory and Homology (math.KT)17A32 17B56 14D15CohomologyMathematics::K-Theory and HomologyLie algebraMathematics - Quantum AlgebraMathematics - K-Theory and HomologyFOS: MathematicsQuantum Algebra (math.QA)Mathematics
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Back to the Amitsur-Levitzki theorem: a super version for the orthosymplectic Lie superalgebra osp(1, 2n)

2003

We prove an Amitsur-Levitzki type theorem for the Lie superalgebras osp(1,2n) inspired by Kostant's cohomological interpretation of the classical theorem. We show that the Lie superalgebras gl(p,q) cannot satisfy an Amitsur-Levitzki type super identity if p, q are non zero and conjecture that neither can any other classical simple Lie superalgebra with the exception of osp(1,2n).

Lie superalgebraType (model theory)17B2001 natural sciencesInterpretation (model theory)CombinatoricsIdentity (mathematics)Simple (abstract algebra)Mathematics::Quantum Algebra0103 physical sciencesFOS: Mathematics0101 mathematicsRepresentation Theory (math.RT)Classical theoremMathematics::Representation TheoryMathematical PhysicsPhysicsConjecture[MATH.MATH-RT]Mathematics [math]/Representation Theory [math.RT]010308 nuclear & particles physics010102 general mathematicsMathematics::Rings and AlgebrasStatistical and Nonlinear Physics16. Peace & justice17B56[ MATH.MATH-RT ] Mathematics [math]/Representation Theory [math.RT]17B20; 17B56Mathematics - Representation Theory
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The HOMFLY-PT polynomials of sublinks and the Yokonuma–Hecke algebras

2016

We describe completely the link invariants constructed using Markov traces on the Yokonuma-Hecke algebras in terms of the linking matrix and the HOMFLYPT polynomials of sublinks.

MSC: Primary 57M27: Invariants of knots and 3-manifolds Secondary 20C08: Hecke algebras and their representations 20F36: Braid groups; Artin groups 57M25: Knots and links in $S^3$Pure mathematicsMarkov chainGeneral Mathematics010102 general mathematicsYokonuma-Hecke algebrasGeometric Topology (math.GT)Linking numbers01 natural sciencesMathematics::Geometric TopologyMatrix (mathematics)Mathematics - Geometric TopologyMarkov tracesMathematics::Quantum Algebra[MATH.MATH-GT]Mathematics [math]/Geometric Topology [math.GT]0103 physical sciencesMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)010307 mathematical physics0101 mathematicsRepresentation Theory (math.RT)Link (knot theory)Mathematics - Representation TheoryMathematics
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Deformations of semisimple Poisson pencils of hydrodynamic type are unobstructed

2015

We prove that the bihamiltonian cohomology of a semisimple pencil of Poisson brackets of hydrodynamic type vanishes for almost all degrees. This implies the existence of a full dispersive deformation of a semisimple bihamiltonian structure of hydrodynamic type starting from any infinitesimal deformation.

Mathematics - Differential GeometryFOS: Physical sciencesPoisson distribution01 natural sciencessymbols.namesakePoisson bracketMathematics::Quantum Algebra0103 physical sciencesFOS: Mathematics0101 mathematicsMathematics::Representation TheoryMathematics::Symplectic GeometryMathematical PhysicsPencil (mathematics)MathematicsAlgebra and Number TheoryNonlinear Sciences - Exactly Solvable and Integrable Systems010102 general mathematicsMathematical analysisInfinitesimal deformationMathematical Physics (math-ph)Cohomology[ MATH.MATH-DG ] Mathematics [math]/Differential Geometry [math.DG]Nonlinear Sciences::Exactly Solvable and Integrable SystemsDifferential Geometry (math.DG)[MATH.MATH-DG]Mathematics [math]/Differential Geometry [math.DG]symbols010307 mathematical physicsGeometry and TopologyExactly Solvable and Integrable Systems (nlin.SI)Analysis
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