Search results for "Poisson bracket"

showing 10 items of 28 documents

Statistical Mechanics of the sine-Gorden Field: Part II

1985

From the work of the Part I we are now in a position to address ourselves to the main problem posed in these lectures — the evaluation of Z, (1.11), for the s-G field after canonical transformation to the action-angle variables (4.27).

AlgebraPoisson bracketField (physics)Position (vector)Canonical transformationStatistical mechanicsSineClassical limitMathematics
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TANGENTIAL DEFORMATIONS ON FIBRED POISSON MANIFOLDS

2005

In a recent article, Cattaneo, Felder and Tomassini explained how the notion of formality can be used to construct flat Fedosov connections on formal vector bundles on a Poisson manifold $M$ and thus a star product on $M$ through the original Fedosov method for symplectic manifolds. In this paper, we suppose that $M$ is a fibre bundle manifold equipped with a Poisson tensor tangential to the fibers. We show that in this case the construction of Cattaneo-Felder- Tomassini gives tangential (to the fibers) star products.

Applied MathematicsGeneral Mathematics010102 general mathematicsMathematical analysis[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Vector bundle01 natural sciences53D15Volume formPoisson bracket53D17[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Mathematics::Quantum Algebra0103 physical sciencesHermitian manifold010307 mathematical physics[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]0101 mathematicsMathematics::Symplectic GeometryFirst class constraintMathematicsSymplectic manifoldSymplectic geometryPoisson algebra
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Quasi-Modes in Higher Dimension

2019

Recall that if a(x, ξ) and b(x, ξ) are two C1-functions defined on some domain in \({\mathbf {R}}^{2n}_{x,\xi }\), then we can define the Poisson bracket to be the C0-function on the same domain given by $$\displaystyle \{ a,b\} =a^{\prime }_\xi \cdot b^{\prime }_x-a^{\prime }_x \cdot b^{\prime }_\xi =H_a(b). $$ Here \(H_a=a^{\prime }_\xi \cdot \partial _x-a^{\prime }_x\cdot \partial _\xi \) denotes the Hamilton vector field of a. The following result is due to Zworski, who obtained it via a semi-classical reduction from the above mentioned result of Hormander. A direct proof was given in Dencker et al. and here we give a variant. We will assume some familiarity with symplectic geometry.

CombinatoricsPhysicsPoisson bracketReduction (recursion theory)Mathematics::Number TheoryDomain (ring theory)Dimension (graph theory)Direct proofPrime (order theory)Symplectic geometry
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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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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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