Search results for "Dispersion"

showing 10 items of 1101 documents

A microscopic approach to Casimir and Casimir-Polder forces between metallic bodies

2014

We consider the Casimir-Polder interaction energy between a metallic nanoparticle and a metallic plate, as well as the Casimir interaction energy between two macroscopic metal plates, in terms of the many-body dispersion interactions between their constituents. Expressions for two- and three-body dispersion interactions between the microscopic parts of a real metal are first obtained, both in the retarded and non-retarded limits. These expressions are then used to evaluate, a compare each other, the overall two- and three-body contributions to the macroscopic Casimir-Polder and Casimir force, by summing up the contributions from the microscopic constituents of the bodies (metal nanoparticle…

PhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsFOS: Physical sciencesGeneral Physics and AstronomyNanoparticlemany-body interactionsCasimir-Polder interactionInteraction energyCasimir effectMetalCasimir effectClassical mechanicsvisual_artMesoscale and Nanoscale Physics (cond-mat.mes-hall)Dispersion (optics)Convergence (routing)visual_art.visual_art_mediumRapidityQuantum Physics (quant-ph)Metal nanoparticles
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Electric quantum walks in two dimensions

2015

We study electric quantum walks in two dimensions considering Grover, Alternate, Hadamard, and DFT quantum walks. In the Grover walk the behaviour under an electric field is easy to summarize: when the field direction coincides with the x or y axes, it produces a transient trapping of the probability distribution along the direction of the field, while when it is directed along the diagonals, a perfect 2D trapping is frustrated. The analysis of the alternate walk helps to understand the behaviour of the Grover walk as both walks are partially equivalent; in particular, it helps to understand the role played by the existence of conical intersections in the dispersion relations, as we show th…

PhysicsQuantum PhysicsField (physics)DiagonalFOS: Physical sciences01 natural sciences010305 fluids & plasmasDiscrete Fourier transform (general)Hadamard transformQuantum mechanicsDispersion relationElectric field0103 physical sciencesProbability distributionQuantum walkStatistical physics010306 general physicsQuantum Physics (quant-ph)
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N-dimensional alternate coined quantum walks from a dispersion-relation perspective

2013

We propose an alternative definition of an N-dimensional coined quantum walk by generalizing a recent proposal [Di Franco et al., Phys. Rev. Lett. 106, 080502 (2011)]. This N-dimensional alternate quantum walk, AQW_N, in contrast with the standard definition of the N-dimensional quantum walk, QW_N, requires only a coin-qubit. We discuss the quantum diffusion properties of AQW_2 and AQW_3 by analyzing their dispersion relations that reveal, in particular, the existence of diabolical points. This allows us to highlight interesting similarities with other well known physical phenomena. We also demonstrate that AQW_3 generates genuine multipartite entanglement. Finally we discuss the implementa…

PhysicsQuantum PhysicsN dimensionalFOS: Physical sciencesQuantum diffusion01 natural sciencesMultipartite entanglementAtomic and Molecular Physics and OpticsÒptica quàntica010305 fluids & plasmasPerspective (geometry)Standard definitionQubitQuantum mechanicsDispersion relation0103 physical sciencesQuantum walkQuantum Physics (quant-ph)010306 general physicsPhysical Review A
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Casimir-Polder interatomic potential between two atoms at finite temperature and in the presence of boundary conditions

2007

We evaluate the Casimir-Polder potential between two atoms in the presence of an infinite perfectly conducting plate and at nonzero temperature. In order to calculate the potential, we use a method based on equal-time spatial correlations of the electric field, already used to evaluate the effect of boundary conditions on interatomic potentials. This method gives also a transparent physical picture of the role of a finite temperature and boundary conditions on the Casimir-Polder potential. We obtain an analytical expression of the potential both in the near and far zones, and consider several limiting cases of interest, according to the values of the parameters involved, such as atom-atom d…

PhysicsQuantum Physicsdispersion interactionFOS: Physical sciencesInteratomic potentialLimitingAtomic and Molecular Physics and OpticsCasimir effectCavity quantum electrodynamictemperature effects.Lennard-Jones potentialQuantum mechanicsElectric fieldPhysics::Atomic and Molecular ClustersBoundary value problemPhysics::Atomic PhysicsQuantum field theoryQuantum Physics (quant-ph)
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The pion quasiparticle in the low-temperature phase of QCD

2017

We extend our previous studies [PhysRevD.90.054509, PhysRevD.92.094510] of the pion quasiparticle in the low-temperature phase of two-flavor QCD with support from chiral effective theory. This includes the analysis performed on a finite temperature ensemble of size $20\times 64^3$ at $T\approx 151$MeV and a lighter zero-temperature pion mass $m_{\pi} \approx 185$ MeV. Furthermore, we investigate the Gell-Mann--Oakes-Renner relation at finite temperature and the Dey-Eletsky-Ioffe mixing theorem at finite quark mass.

PhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::LatticePhysicsQC1-999Nuclear TheoryHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyCharge densityFOS: Physical sciences01 natural sciencesHigh Energy Physics - LatticePionDispersion relationQuantum electrodynamicsLattice (order)0103 physical sciencesEffective field theoryQuasiparticleHigh Energy Physics::Experiment010306 general physicsNuclear ExperimentEPJ Web of Conferences
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What can be learned from the Belle spectrum for the decay τ−→ντKSπ−

2008

Abstract A theoretical description of the differential decay spectrum for the decay τ − → ν τ K S π − , which is based on the contributing Kπ vector and scalar form factors F + K π ( s ) and F 0 K π ( s ) being calculated in the framework of resonance chiral theory (R χ T), additionally imposing constraints from dispersion relations as well as short distance QCD, provides a good representation of a recent measurement of the spectrum by the Belle Collaboration. Our fit allows to deduce the total branching fraction B [ τ − → ν τ K S π − ] = 0.427 ± 0.024 % by integrating the spectrum, as well as the K ∗ resonance parameters M K ∗ = 895.3 ± 0.2 MeV and Γ K ∗ = 47.5 ± 0.4 MeV , where the last t…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsBranching fractionDispersion relationQuantum mechanicsScalar (mathematics)Decays of tausAtomic physicsCurvatureChiral symmetriesDispersion relationsShort distancePhysics Letters B
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The pion quasiparticle in the low-temperature phase of QCD

2015

We investigate the properties of the pion quasiparticle in the low-temperature phase of two-flavor QCD on the lattice with support from chiral effective theory. We find that the pion quasiparticle mass is significantly reduced compared to its value in the vacuum, by contrast with the static screening mass, which increases with temperature. By a simple argument, near the chiral limit the two masses are expected to determine the quasiparticle dispersion relation. Analyzing two-point functions of the axial charge density at non-vanishing spatial momentum, we find that the predicted dispersion relation and the residue of the pion pole are simultaneously consistent with the lattice data at low m…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryThermal quantum field theoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Charge densityFOS: Physical sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - LatticePionHigh Energy Physics - Phenomenology (hep-ph)Dispersion relationQuantum electrodynamicsLattice (order)QuasiparticleEffective field theory
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Finite-energy sum rules and finite dispersion relations for K*→Kππ transitions

1977

PhysicsQuantum mechanicsDispersion relationGeneral Physics and AstronomySum rule in quantum mechanicsEnergy (signal processing)Lettere Al Nuovo Cimento Series 2
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Resonant atom-field interaction in large-size coupled-cavity arrays

2011

We consider an array of coupled cavities with staggered inter-cavity couplings, where each cavity mode interacts with an atom. In contrast to large-size arrays with uniform-hopping rates where the atomic dynamics is known to be frozen in the strong-hopping regime, we show that resonant atom-field dynamics with significant energy exchange can occur in the case of staggered hopping rates even in the thermodynamic limit. This effect arises from the joint emergence of an energy gap in the free photonic dispersion relation and a discrete frequency at the gap's center. The latter corresponds to a bound normal mode stemming solely from the finiteness of the array length. Depending on which cavity …

PhysicsQuantum opticsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsBand gapCavity quantum electrodynamicsFOS: Physical sciencesMolecular physicsAtomic and Molecular Physics and OpticsNormal modeExcited stateDispersion relationThermodynamic limitAtomMesoscale and Nanoscale Physics (cond-mat.mes-hall)coupled cavities quantum opticsQuantum Physics (quant-ph)
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Higher Order Polarizabilities of the Proton

1999

Compton scattering results are used to probe proton structure via measurement of higher order polarizabilities. Values for $\alpha_{E2}^p,\beta_{E2}^p,\alpha_{E\nu}^p,$ $\beta_{E\nu}^p$ determined via dispersion relations are compared to predictions based upon chiral symmetry and from the constituent quark model. Extensions to spin-polarizabilities are also discussed.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsChiral symmetryProtonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyCompton scatteringFOS: Physical sciencesOrder (ring theory)Constituent quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dispersion relationAtomic physicsSpin-½
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