Search results for " Quantization"

showing 10 items of 111 documents

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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The Complete Solution of the Classical SL(2,ℝ/U(1) Gauged WZNW Field Theory

1998

We prove that any gauged WZNW model has a Lax pair representation, and give explicitly the general solution of the classical equations of motion of the SL(2,R)/U(1) theory. We calculate the symplectic structure of this solution by solving a differential equation of the Gelfand-Dikii type with initial state conditions at infinity, and transform the canonical physical fields non-locally onto canonical free fields. The results will, finally, be collected in a local B\"acklund transformation. These calculations prepare the theory for an exact canonical quantization.

High Energy Physics - TheoryDifferential equationCanonical quantizationFOS: Physical sciencesEquations of motionStatistical and Nonlinear PhysicsState (functional analysis)Type (model theory)Nonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics - Theory (hep-th)Lax pairField theory (psychology)Mathematical PhysicsSymplectic geometryMathematical physicsMathematicsCommunications in Mathematical Physics
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ON THE DEFORMATION QUANTIZATION OF AFFINE ALGEBRAIC VARIETIES

2004

We compute an explicit algebraic deformation quantization for an affine Poisson variety described by an ideal in a polynomial ring, and inheriting its Poisson structure from the ambient space.

High Energy Physics - TheoryFunction field of an algebraic varietyMathematics::Commutative AlgebraGeneral MathematicsFOS: Physical sciencesFísicaAlgebraic varietyDimension of an algebraic varietyAlgebraic cycleAlgebraGröbner basisHigh Energy Physics - Theory (hep-th)DEFORMATION QUANTIZATIONMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Affine transformationAffine varietyMathematicsSingular point of an algebraic varietyInternational Journal of Mathematics
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DEFORMATION QUANTIZATION OF COADJOINT ORBITS

2000

A method for the deformation quantization of coadjoint orbits of semisimple Lie groups is proposed. It is based on the algebraic structure of the orbit. Its relation to geometric quantization and differentiable deformations is explored.

High Energy Physics - TheoryPhysicsGeometric quantizationPure mathematicsAlgebraic structureQuantization (signal processing)FOS: Physical sciencesFísicaLie groupStatistical and Nonlinear PhysicsDeformation (meteorology)Condensed Matter PhysicsHigh Energy Physics - Theory (hep-th)Mathematics::Quantum AlgebraMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Astrophysics::Earth and Planetary AstrophysicsDifferentiable functionOrbit (control theory)Mathematics::Representation TheoryInternational Journal of Modern Physics B
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Cohomological analysis of gauged-fixed gauge theories

1999

The relation between the gauge-invariant local BRST cohomology involving the antifields and the gauge-fixed BRST cohomology is clarified. It is shown in particular that the cocycle conditions become equivalent once it is imposed, on the gauge-fixed side, that the BRST cocycles should yield deformations that preserve the nilpotency of the (gauge-fixed) BRST differential. This shows that the restrictions imposed on local counterterms by the Quantum Noether condition in the Epstein--Glaser construction of gauge theories are equivalent to the restrictions imposed by BRST invariance on local counterterms in the standard Lagrangian approach.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesCohomologyBRST quantizationHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)symbolsGauge theoryNoether's theoremQuantumDifferential (mathematics)LagrangianParticle Physics - TheoryMathematical physics
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PRIME NUMBERS, QUANTUM FIELD THEORY AND THE GOLDBACH CONJECTURE

2012

Motivated by the Goldbach conjecture in Number Theory and the abelian bosonization mechanism on a cylindrical two-dimensional spacetime we study the reconstruction of a real scalar field as a product of two real fermion (so-called \textit{prime}) fields whose Fourier expansion exclusively contains prime modes. We undertake the canonical quantization of such prime fields and construct the corresponding Fock space by introducing creation operators $b_{p}^{\dag}$ --labeled by prime numbers $p$-- acting on the vacuum. The analysis of our model, based on the standard rules of quantum field theory and the assumption of the Riemann hypothesis, allow us to prove that the theory is not renormalizabl…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsPure mathematicsMathematics - Number TheoryCanonical quantizationPrime numberFOS: Physical sciencesFísicaAstronomy and AstrophysicsMathematical Physics (math-ph)Atomic and Molecular Physics and OpticsPrime (order theory)Riemann hypothesissymbols.namesakeNumber theoryHigh Energy Physics - Theory (hep-th)Goldbach's conjectureFOS: MathematicssymbolsNumber Theory (math.NT)Quantum field theoryScalar fieldMathematical PhysicsInternational Journal of Modern Physics A
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Spinor moving frame, M0-brane covariant BRST quantization and intrinsic complexity of the pure spinor approach

2007

To exhibit the possible origin of the inner complexity of the Berkovits's pure spinor approach, we consider the covariant BRST quantization of the D=11 massless superparticle (M0-brane) in its spinor moving frame or twistor-like Lorentz harmonics formulation. The presence of additional twistor-like variables (spinor harmonics) allows us to separate covariantly the first and the second class constraints. After taking into account the second class constraints by means of Dirac brackets and after further reducing the first class constraints algebra, the dynamical system is described by the cohomology of a simple BRST charge associated to the d=1, n=16 supersymmetry algebra. The calculation of …

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsPure spinorSpinorHigh Energy Physics::PhenomenologyFOS: Physical sciencesSupersymmetryCohomologyBRST quantizationHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Spinor fieldQuantum mechanicsBraneMathematical physicsSupersymmetry algebraPhysics Letters B
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D=11massless superparticle covariant quantization, pure spinor BRST charge and hidden symmetries

2007

We consider the covariant quantization of the D=11 massless superparticle (M0-brane) in the spinor moving frame or twistor-like Lorentz harmonics formulation. The action involves the set of 16 constrained 32 component Majorana spinors, the spinor Lorentz harmonics parametrizing (as homogeneous coordinates, modulo gauge symmetries) the celestial sphere S9. There presence allows us to separate covariantly the first and the second class constraints of the model. After taking into account the second class constraints by means of Dirac brackets and after further reducing the first class constraints algebra, the system is described in terms of a simple BRST charge associated to the d=1, n=16 supe…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsSpinorPure spinorSupergravityFOS: Physical sciencesBRST quantizationCohomologyTwistor theoryHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Quantum mechanicsCovariant transformationSupersymmetry algebraMathematical physicsNuclear Physics B
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Bicoherent-State Path Integral Quantization of a non-Hermitian Hamiltonian

2020

We introduce, for the first time, bicoherent-state path integration as a method for quantizing non-hermitian systems. Bicoherent-state path integrals arise as a natural generalization of ordinary coherent-state path integrals, familiar from hermitian quantum physics. We do all this by working out a concrete example, namely, computation of the propagator of a certain quasi-hermitian variant of Swanson's model, which is not invariant under conventional $PT$-transformation. The resulting propagator coincides with that of the propagator of the standard harmonic oscillator, which is isospectral with the model under consideration by virtue of a similarity transformation relating the corresponding…

High Energy Physics - TheorySwanson modelFOS: Physical sciencesGeneral Physics and AstronomyPT symmetrysymbols.namesakeFeynman diagramHarmonic oscillatorMathematical PhysicsNon-hermitian hamiltoniansMathematical physicsPhysicsQuantum PhysicsQuantization (signal processing)PropagatorMathematical Physics (math-ph)Bicoherent statesHermitian matrixIsospectralHigh Energy Physics - Theory (hep-th)Path integral quantizationPath integral formulationsymbolsPseudo-bosonsQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)
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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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