Search results for "bracket"

showing 10 items of 99 documents

On the canonical structure of higher-derivative field theories. The gravitational WZW-model

1992

Abstract A general expression for the symplectic structure of a higher-derivative lagrangian field theory is given. General relativity and the gravitational WZW-model are considered in this framework. In the second case we work out explicitly the Poisson bracket for both chiral solutions giving rise, in two different ways, to the classical exchange algebra of the SL q (2) group.

GravitationPhysicsNuclear and High Energy PhysicsPoisson bracketField (physics)General relativityGroup (mathematics)Structure (category theory)Field theory (psychology)Mathematics::Symplectic GeometryGeneral Theoretical PhysicsMathematical physicsSymplectic geometryPhysics Letters B
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The Principles of Canonical Mechanics

2010

Canonical mechanics is a central part of general mechanics, where one goes beyond the somewhat narrow framework of Newtonian mechanics with position coordinates in the three-dimensional space, towards a more general formulation of mechanical systems belonging to a much larger class. This is the first step of abstraction, leaving behind ballistics, satellite orbits, inclined planes, and pendulum-clocks; it leads to a new kind of description that turns out to be useful in areas of physics far beyond mechanics. Through d’Alembert’s principle we discover the concept of the Lagrangian function and the framework of Lagrangian mechanics that is built onto it. Lagrangian functions are particularly …

Hamiltonian mechanicsLegendre transformationsymbols.namesakePoisson bracketPhase spaceLagrangian mechanicssymbolsCanonical transformationMechanicsAnalytical dynamicsHamiltonian systemMathematics
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Spin texture motion in antiferromagnetic and ferromagnetic nanowires

2017

We propose a Hamiltonian dynamics formalism for the current and magnetic field driven dynamics of ferromagnetic and antiferromagnetic domain walls in one dimensional systems. To demonstrate the power of this formalism, we derive Hamilton equations of motion via Poisson brackets based on the Landau-Lifshitz-Gilbert phenomenology, and add dissipative dynamics via the evolution of the energy. We use this approach to study current induced domain wall motion and compute the drift velocity. For the antiferromagnetic case, we show that a nonzero magnetic moment is induced in the domain wall, which indicates that an additional application of a magnetic field would influence the antiferromagnetic do…

Hamiltonian mechanicsPhysicsDrift velocityCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsMagnetic momentFOS: Physical sciences02 engineering and technologyPhysik (inkl. Astronomie)021001 nanoscience & nanotechnology01 natural sciencesMagnetic fieldTransverse planePoisson bracketsymbols.namesakeFerromagnetism0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)symbolsAntiferromagnetismCondensed Matter::Strongly Correlated Electrons010306 general physics0210 nano-technology
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The damped harmonic oscillator in deformation quantization

2005

We propose a new approach to the quantization of the damped harmonic oscillator in the framework of deformation quantization. The quantization is performed in the Schr\"{o}dinger picture by a star-product induced by a modified "Poisson bracket". We determine the eigenstates in the damped regime and compute the transition probability between states of the undamped harmonic oscillator after the system was submitted to dissipation.

High Energy Physics - TheoryDeformation quantization[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Canonical quantizationGeneral Physics and AstronomyFOS: Physical sciences01 natural sciences[ PHYS.HTHE ] Physics [physics]/High Energy Physics - Theory [hep-th]Poisson bracket[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Quantum mechanics0103 physical sciencesdissipative systems010306 general physicsNonlinear Sciences::Pattern Formation and Solitonsquantum mechanics.Harmonic oscillatorEigenvalues and eigenvectorsPhysicsQuantum Physics010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Quantization (signal processing)quantum mechanicsPACS numbers: 03.50.-z 03.50.De 11.10.-z 03.65.DbLandau quantization16. Peace & justiceSecond quantizationClassical mechanicsHigh Energy Physics - Theory (hep-th)Schrödinger pictureQuantum Physics (quant-ph)
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Algebraic and Differential Star Products on Regular Orbits of Compact Lie Groups

2000

In this paper we study a family of algebraic deformations of regular coadjoint orbits of compact semisimple Lie groups with the Kirillov Poisson bracket. The deformations are restrictions of deformations on the dual of the Lie algebra. We prove that there are non isomorphic deformations in the family. The star products are not differential, unlike the star products considered in other approaches. We make a comparison with the differential star product canonically defined by Kontsevich's map.

High Energy Physics - TheoryGeneral MathematicsSimple Lie groupLie groupFOS: Physical sciencesRepresentation theoryLie Grups deAlgebraPoisson bracketCompact groupHigh Energy Physics - Theory (hep-th)Star productMathematics::Quantum AlgebraMathematics - Quantum AlgebraLie algebraFOS: MathematicsQuantum Algebra (math.QA)Astrophysics::Earth and Planetary AstrophysicsÀlgebraDifferential (mathematics)Mathematics
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Topics on n-ary algebras

2011

We describe the basic properties of two n-ary algebras, the Generalized Lie Algebras (GLAs) and, particularly, the Filippov (or n-Lie) algebras (FAs), and comment on their n-ary Poisson counterparts, the Generalized Poisson (GP) and Nambu-Poisson (N-P) structures. We describe the Filippov algebra cohomology relevant for the central extensions and infinitesimal deformations of FAs. It is seen that semisimple FAs do not admit central extensions and, moreover, that they are rigid. This extends the familiar Whitehead's lemma to all $n\geq 2$ FAs, n=2 being the standard Lie algebra case. When the n-bracket of the FAs is no longer required to be fully skewsymmetric one is led to the n-Leibniz (or…

High Energy Physics - TheoryHistoryPure mathematicsAnticommutativityAlgebraic structureInfinitesimalFOS: Physical sciencesEducationQuantitative Biology::Subcellular ProcessesMathematics::K-Theory and HomologySimple (abstract algebra)Mathematics - Quantum AlgebraLie algebraFOS: MathematicsQuantum Algebra (math.QA)Mathematical PhysicsMathematicsLemma (mathematics)Quantitative Biology::Molecular NetworksMathematics::Rings and AlgebrasMathematical Physics (math-ph)Mathematics - Rings and AlgebrasCohomologyComputer Science ApplicationsBracket (mathematics)High Energy Physics - Theory (hep-th)Rings and Algebras (math.RA)Journal of Physics: Conference Series
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The Schouten - Nijenhuis bracket, cohomology and generalized Poisson structures

1996

Newly introduced generalized Poisson structures based on suitable skew-symmetric contravariant tensors of even order are discussed in terms of the Schouten-Nijenhuis bracket. The associated `Jacobi identities' are expressed as conditions on these tensors, the cohomological contents of which is given. In particular, we determine the linear generalized Poisson structures which can be constructed on the dual spaces of simple Lie algebras.

High Energy Physics - TheoryMathematics - Differential GeometryPhysicsPure mathematicsSchouten–Nijenhuis bracketFOS: Physical sciencesGeneral Physics and AstronomyOrder (ring theory)Statistical and Nonlinear PhysicsPoisson distributionCohomologysymbols.namesakeBracket (mathematics)High Energy Physics - Theory (hep-th)Differential Geometry (math.DG)Simple (abstract algebra)Mathematics - Quantum AlgebraLie algebraFOS: MathematicssymbolsCovariance and contravariance of vectorsQuantum Algebra (math.QA)Mathematics::Symplectic GeometryMathematical PhysicsJournal of Physics A: Mathematical and General
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Quantum deformation of the Poincare supergroup and kappa -deformed superspace

1994

The classical $r$-matrix for $N=1$ superPoincar{\'e} algebra, given by Lukierski, Nowicki and Sobczyk is used to describe the graded Poisson structure on the $N=1$ Poincar{\'e} supergroup. The standard correspondence principle between the even (odd) Poisson brackets and (anti)commutators leads to the consistent quantum deformation of the superPoincar{\'e} group with the deformation parameter $q$ described by fundamental mass parameter $\kappa \quad (\kappa^{-1}=\ln{q})$. The $\kappa$-deformation of $N=1$ superspace as dual to the $\kappa$-deformed supersymmetry algebra is discussed.

High Energy Physics - TheoryPhysicsGroup (mathematics)General Physics and AstronomyStatistical and Nonlinear PhysicsSuperspacePoisson bracketPoisson manifoldCorrespondence principleSupergroupQuantumMathematical PhysicsMathematical physicsSupersymmetry algebraJournal of Physics A: Mathematical and General
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Supersymmetry in non commutative superspaces

2003

Non commutative superspaces can be introduced as the Moyal-Weyl quantization of a Poisson bracket for classical superfields. Different deformations are studied corresponding to constant background fields in string theory. Supersymmetric and non supersymmetric deformations can be defined, depending on the differential operators used to define the Poisson bracket. Some examples of deformed, 4 dimensional lagrangians are given. For extended superspace (N>1), some new deformations can be defined, with no analogue in the N=1 case.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsFOS: Physical sciencesFísicaSupersymmetrySuperspaceString theoryDifferential operatorNoncommutative geometryPoisson bracketQuantization (physics)High Energy Physics::TheoryNonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics - Theory (hep-th)Commutative propertyComputer Science::DatabasesParticle Physics - TheoryMathematical physics
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On the physical contents of q-deformed Minkowski spaces

1994

Some physical aspects of $q$-deformed spacetimes are discussed. It is pointed out that, under certain standard assumptions relating deformation and quantization, the classical limit (Poisson bracket description) of the dynamics is bound to contain unusual features. At the same time, it is argued that the formulation of an associated $q$-deformed field theory is fraught with serious difficulties.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsTheoretical physicsQuantization (physics)Poisson bracketHigh Energy Physics - Theory (hep-th)Minkowski spaceFOS: Physical sciencesClassical limitPhysics Letters B
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