Search results for "quantization"

showing 10 items of 253 documents

Analysis of Optimal High Resolution and Fixed Rate Scalar Quantization

2009

In 2001, Hui and Neuhoff proposed a uniform quantizer with overload for the quantization of scalar signals and derived the asymptotically optimal size of the quantization bins in the high-bitrate limit. The purpose of the present paper is to prove a quantitatively more precise version of this result which, at the same time, is valid for a more general, quite natural class of probability distributions that requires only little regularity and includes, for instance, positive Lipschitz-continuous functions of unit integral.

Discrete mathematicsAsymptotically optimal algorithmScalar quantizationQuantization (signal processing)Applied mathematicsHigh resolutionProbability distributionLibrary and Information SciencesInformation theoryNatural classComputer Science ApplicationsInformation SystemsMathematicsIEEE Transactions on Information Theory
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Scattering Matrix and Observables in Scattering and Decays

2013

As an interlude in the analysis of canonical field quantization, this section describes important concepts of scattering theory for Lorentz covariant quantum field theories that will be needed for the calculation of observables such as scattering cross sections and decay probabilities.

Elastic scatteringScattering amplitudePhysicsTheoretical physicsQuantization (physics)ScatteringScattering lengthScattering theoryMott scatteringInelastic scattering
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The electromagnetic and Proca fields revisited: A unified quantization

1997

Quantizing the electromagnetic field with a group formalism faces the difficulty of how to turn the traditional gauge transformation of the vector potential, Aμ(x) → Aμ(x) + ∂μφ(x), into a group law. In this paper, it is shown that the problem can be solved by looking at gauge transformations in a slightly different manner which, in addition, does not require introducing any BRST-like parameter. This gauge transformation does not appear explicitly in the group law of the symmetry but rather as the trajectories associated with generalized equations of motion generated by vector fields with null Noether invariants. In the new approach the parameters of the local group, U(1)(x, t), acquire dyn…

Electromagnetic fieldPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsPhotonQuantization (signal processing)Equations of motionFOS: Physical sciencesAstronomy and AstrophysicsMatemática AplicadaCampos electromagnéticosCampos electromagnéticos ProcaAtomic and Molecular Physics and OpticsCuantización unificadasymbols.namesakeHigh Energy Physics - Theory (hep-th)Proca Cuantización unificadasymbolsVector fieldGauge theoryNoether's theoremMathematical physicsVector potential
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Vacuum induced berry phase: Theory and experimental proposal

2003

We investigate quantum effects in geometric phases arising when a two-level system is interacting with a quantized electromagnetic field. When the system is adiabatically driven along a closed loop in the parameter space, signatures of the field quantization are observable in the geometric phase. We propose a feasible experiment to measure these effects in cavity QED and also analyse the semi-classical limit, recovering the usual Berry phase results.

Electromagnetic fieldPhysicsJaynes–Cummings modelVacuumGround stateMathematical transformationObservableParameter spaceComputational geometryAtomic and Molecular Physics and OpticsClosed loop control systemQuantization (physics)Mathematical operatorGeometric phaseConvergence of numerical methodQuantum electrodynamicsQuantum mechanicsElectromagnetic fieldBerry connection and curvatureFunctionClosed loopLight polarizationJournal of Modern Optics
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The electromagnetic group: Bosonic BRST charge

1990

Abstract We give an infinite-dimensional Lie group from which a group approach to quantization (GAQ) derives a Gupta-Bleuler-like quantization for the electromagnetic field. The incorporation into the group law of the gauge transformation properties of Aμ(x), Aμ(x) → Aμ(x) + ∂μφ, requires a non-conventional generator which is related to the BRST charge.

Electromagnetic fieldPhysicsNuclear and High Energy PhysicsQuantization (physics)Quantum groupQuantum electrodynamicsLie algebraLie groupGauge theoryPolarization (waves)BRST quantizationMathematical physicsPhysics Letters B
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Second quantization and atomic spontaneous emission inside one-dimensional photonic crystals via a quasinormal-modes approach

2004

An extension of the second quantization scheme based on the quasinormal-modes theory to one-dimensional photonic band gap (PBG) structures is discussed. Such structures, treated as double open optical cavities, are studied as part of a compound closed system including the electromagnetic radiative external bath. The electromagnetic field inside the photonic crystal is successfully represented by a new class of modes called quasinormal modes. Starting from this representation we introduce the Feynman's propagator to calculate the decay rate of a dipole inside a PBG structure, related to the density of modes, in the presence of the vacuum fluctuations outside the one-dimensional cavity.

Electromagnetic fieldPhysicsPhysics::OpticsPropagatorSecond quantizationDipolesymbols.namesakeQuantum mechanicsQuantum electrodynamicssymbolsFeynman diagramSpontaneous emissionQuantum fluctuationPhotonic crystal
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Nonlocal properties of dynamical three-body Casimir-Polder forces

2005

We consider the three-body Casimir-Polder interaction between three atoms during their dynamical self-dressing. We show that the time-dependent three-body Casimir-Polder interaction energy displays nonlocal features related to quantum properties of the electromagnetic field and to the nonlocality of spatial field correlations. We discuss the measurability of this intriguing phenomenon and its relation with the usual concept of stationary three-body forces.

Electromagnetic fieldPhysicsQuantum PhysicsGeneral Physics and AstronomyFOS: Physical sciencesSpatial field correlationsRelativistic quantum mechanicsCasimir effectQuantization (physics)Open quantum systemQuantum nonlocalityClassical mechanicsQuantum mechanicsNonlocalityThree-body forcePhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsQuantum dissipationQuantum Physics (quant-ph)Introduction to quantum mechanics
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Berry's phase in Cavity QED: proposal for observing an effect of field quantization

2002

Geometric phases are well known in classical electromagnetism and quantum mechanics since the early works of Pantcharatnam and Berry. Their origin relies on the geometric nature of state spaces and has been studied in many different systems such as spins, polarized light and atomic physics. Recent works have explored their application in interferometry and quantum computation. Earlier works suggest how to observe these phases in single quantum systems adiabatically driven by external classical devices or sources, where, by classical, we mean any system whose state does not change considerably during the interaction time: an intense magnetic field interacting with a spin 1/2, or a birefringe…

Electromagnetic fieldPhysicsQuantum PhysicsVacuumFOS: Physical sciencesSemiclassical physicsAtomic and Molecular Physics and OpticsQuantization of the electromagnetic fieldQuantization (physics)Quantum electrodynamicsQuantum mechanicsfield quantizationAtomQuantum systemBerry connection and curvatureQuantum field theoryQuantum Physics (quant-ph)
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Gigahertz Single-Electron Pumping Mediated by Parasitic States

2018

In quantum metrology, semiconductor single-electron pumps are used to generate accurate electric currents with the ultimate goal of implementing the emerging quantum standard of the ampere. Pumps based on electrostatically defined tunable quantum dots (QDs) have thus far shown the most promising performance in combining fast and accurate charge transfer. However, at frequencies exceeding approximately 1 GHz, the accuracy typically decreases. Recently, hybrid pumps based on QDs coupled to trap states have led to increased transfer rates due to tighter electrostatic confinement. Here, we operate a hybrid electron pump in silicon obtained by coupling a QD to multiple parasitic states, and achi…

Electron capturePhysics::OpticsFOS: Physical sciencesBioengineering02 engineering and technologyElectron7. Clean energy01 natural sciencesQuantization (physics)0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)Quantum metrologyGeneral Materials Science010306 general physicsQuantumQCPhysicsta214Condensed Matter - Mesoscale and Nanoscale Physicsta114business.industryMechanical EngineeringQuantum dotsiliconGeneral Chemistry021001 nanoscience & nanotechnologyCondensed Matter PhysicsSemiconductorQuantum dotquantum electrical metrologysingle-electron pumpOptoelectronicsElectric current0210 nano-technologybusinessNANO LETTERS
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Ideas in the History of Nano/Miniaturization and (Quantum) Simulators: Feynman, Education and Research Reorientation in Translational Science

2015

Cultural history of nanominiaturization, computing, quantum computing and simulating is necessary to comprehend human character and place it in the whole of living beings. Ideas in the history of physics by Feynman, etc. are valued by the questions that generate. A series of questions, answers and hypothesis introduces the nature of the history of nanominiaturization, providing facts. Nanotechnology adds a third dimension to the periodic table of the elements. Thinking about computers was useful. It must do with learning computers possibilities and physics potential. Provisional conclusions follow. (1) Nature (space–time) is not classical but discrete; quantization is a different kind of ma…

Engineeringbusiness.industryProbabilistic logicQuantum simulatorDeterminismEpistemologyQuantization (physics)symbols.namesakeTheoretical physicssymbolsFeynman diagramHistory of physicsDimension (data warehouse)businessQuantum computerProceedings of The 19th International Electronic Conference on Synthetic Organic Chemistry
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