Search results for "Correlation function"

showing 10 items of 164 documents

Vibrational dephasing of νs(OH) in 2,6-dichloro-4-nitrophenol

1988

Abstract A detailed analysis of the infrared bandshape of ν s (OH) in intramolecularly hydrogen-bonded 2,6-dichloro-4-nitrophenol in a series of solvents is presented. A distinct dependence of the bandshape and relaxation parameters on the polarity of solvent molecules has been found. The band shifts to lower wavenumbers, broadens and becomes more Gaussian with increasing solvent polarity; correspondingly, the correlation function decays faster and the correlation time decreases. The results are compared with those of previously studied systems. Factors determing the bandshape are discussed.

Quantitative Biology::Biomolecules2 6 dichloro 4 nitrophenolInfraredChemistryPolarity (physics)DephasingOrganic ChemistryRelaxation (NMR)Analytical ChemistryInorganic ChemistrySolventCorrelation functionComputational chemistryPhysical chemistryMoleculePhysics::Chemical PhysicsSpectroscopyJournal of Molecular Structure
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Towards a consistent estimate of the chiral low-energy constants

2006

Guided by the large-N_C limit of QCD, we construct the most general chiral resonance Lagrangian that can generate chiral low-energy constants up to O(p^6). By integrating out the resonance fields, the low-energy constants are parametrized in terms of resonance masses and couplings. Information on those couplings and on the low-energy constants can be extracted by analysing QCD Green functions of currents both for large and small momenta. The chiral resonance theory generates Green functions that interpolate between QCD and chiral perturbation theory. As specific examples we consider the VAP and SPP Green functions.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsChiral perturbation theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísica01 natural sciencesQCD[PHYS.HPHE] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Low energyCorrelation function[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quantum electrodynamicsQuantum mechanics0103 physical sciences1/NC expansion010306 general physicsChiral lagrangians
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Violation of quark-hadron duality and spectral chiral moments in QCD

2010

We analyze the spectral moments of the V - A two-point correlation function. Using all known short-distance constraints and the most recent experimental data from tau decays, we determine the lowest spectral moments, trying to assess the uncertainties associated with the so-called violations of quark-hadron duality. We have generated a large number of acceptable spectral functions, satisfying all conditions, and have used them to extract the wanted hadronic parameters through a careful statistical analysis. We obtain accurate values for the chi PT couplings L-10 and C-87, and a realistic determination of the dimension six and eight contributions in the operator product expansion, O-6 = (-5.…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHadronDimension (graph theory)Duality (optimization)FísicaFOS: Physical sciencesElementary particleCorrelation function (quantum field theory)Particle decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentOperator product expansion
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Pinched weights and duality violation in QCD sum rules: A critical analysis

2010

We analyze the so-called pinched weights, that are generally thought to reduce the violation of quarkhadron duality in finite-energy sum rules. After showing how this is not true in general, we explain how to address this question for the left-right correlator and any particular pinched weight, taking advantage of our previous work [1], where the possible high-energy behavior of the left-right spectral function was studied. In particular, we show that the use of pinched weights allows to determine with high accuracy the dimension six and eight contributions in the operator-product expansion, O-6 = (-4.3(-0.7)(+0.9)) x 10(-3) GeV6 and O-8 = (-7.2(-5.3)(+4.2)) x 10(-3) GeV8.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsQCD sum rulesDimension (graph theory)FísicaFOS: Physical sciencesDuality (optimization)Correlation function (quantum field theory)CombinatoricsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentOperator product expansionQuantum field theorySeries expansionPhysical Review D
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Bottomonium precision tests from full lattice QCD: Hyperfine splitting, ϒ leptonic width, and b quark contribution to e+e−→hadrons

2021

We calculate the mass difference between the $\mathrm{\ensuremath{\Upsilon}}$ and ${\ensuremath{\eta}}_{b}$ and the $\mathrm{\ensuremath{\Upsilon}}$ leptonic width from lattice QCD using the highly improved staggered quark formalism for the $b$ quark and including $u$, $d$, $s$ and $c$ quarks in the sea. We have results for lattices with lattice spacing as low as 0.03 fm and multiple heavy quark masses, enabling us to map out the heavy quark mass dependence and determine values at the $b$ quark mass. Our results are ${M}_{\mathrm{\ensuremath{\Upsilon}}}\ensuremath{-}{M}_{{\ensuremath{\eta}}_{b}}=57.5(2.3)(1.0)\text{ }\text{ }\mathrm{MeV}$ (where the second uncertainty comes from neglect of …

Quantum chromodynamicsPhysicsQuarkParticle physicsMuonAnomalous magnetic dipole moment010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHadronLattice QCDCorrelation function (quantum field theory)01 natural sciencesBottom quark0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Incommensurate phases of a bosonic two-leg ladder under a flux

2016

A boson two--leg ladder in the presence of a synthetic magnetic flux is investigated by means of bosonization techniques and Density Matrix Renormalization Group (DMRG). We follow the quantum phase transition from the commensurate Meissner to the incommensurate vortex phase with increasing flux at different fillings. When the applied flux is $\rho \pi$ and close to it, where $\rho$ is the filling per rung, we find a second incommensuration in the vortex state that affects physical observables such as the momentum distribution, the rung-rung correlation function and the spin-spin and charge-charge static structure factors.

Quantum phase transitionBosonizationBosonisation[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]IncommensurationsFOS: Physical sciencesGeneral Physics and Astronomychamps de jauge artificiels01 natural sciences010305 fluids & plasmasPhysics and Astronomy (all)Condensed Matter - Strongly Correlated ElectronsCorrelation functionGauge fieldsCondensed Matter::Superconductivity0103 physical sciencesBosonizationtranstion commensurable-incommensurable010306 general physicsCommensurate-Incommensurate transitions[PHYS.COND.CM-MSQHE]Physics [physics]/Condensed Matter [cond-mat]/Mesoscopic Systems and Quantum Hall Effect [cond-mat.mes-hall]BosonPhysicsCondensed Matter::Quantum GasesStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsartificial gauge fieldsDensity matrix renormalization groupGauge fields; Incommensurations; Meissner to vortex transition; Physics and Astronomy (all)Vortex stateMagnetic fluxVortexQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality.Quantum Gases (cond-mat.quant-gas)Meissner to vortex transitionCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum GasesQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality
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Growth, percolation, and correlations in disordered fiber networks

1997

This paper studies growth, percolation, and correlations in disordered fiber networks. We start by introducing a 2D continuum deposition model with effective fiber-fiber interactions represented by a parameter $p$ which controls the degree of clustering. For $p=1$, the deposited network is uniformly random, while for $p=0$ only a single connected cluster can grow. For $p=0$, we first derive the growth law for the average size of the cluster as well as a formula for its mass density profile. For $p>0$, we carry out extensive simulations on fibers, and also needles and disks to study the dependence of the percolation threshold on $p$. We also derive a mean-field theory for the threshold ne…

Random graphPhysicsStatistical Mechanics (cond-mat.stat-mech)Degree (graph theory)Continuum (topology)FOS: Physical sciencesPair distribution functionStatistical and Nonlinear PhysicsPercolation threshold01 natural sciences010305 fluids & plasmasCorrelation function (statistical mechanics)Percolation0103 physical sciencesCluster (physics)Statistical physics010306 general physicsCondensed Matter - Statistical MechanicsMathematical Physics
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An ergodic wideband MIMO channel simulator based on the geometrical T-junction scattering model for vehicle-to-vehicle communications

2010

In this paper, a wideband multiple-input multiple-output (MIMO) simulation model for vehicle-to-vehicle (V2V) channels in T-junction propagation environments is proposed. This simulation model takes the exact relationship between the angle-of-arrival (AOA) and the angle-of-departure (AOD) into account. In order to determine the parameters of the simulation model, the Riemann sum method (RSM) is applied. Furthermore, the statistical and ergodic properties of the simulation model are studied. Closed-form solutions are derived for the space-time-frequency cross-correlation function (STF-CCF), the two-dimensional (2D) spatial cross-correlation function (CCF), the temporal autocorrelation functi…

Scatteringbusiness.industryComputer scienceAutocorrelationMIMOFunction (mathematics)Correlation function (quantum field theory)TopologyAngle of arrivalFadingWidebandTelecommunicationsbusinessCommunication channelInternational Conference on Communications and Electronics 2010
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Determination of the chiral couplingsL10andC87from semileptonicτdecays

2008

Using recent precise hadronic {tau}-decay data on the V-A spectral function, and general properties of QCD such as analyticity, the operator product expansion, and chiral perturbation theory, we get accurate values for the QCD chiral order parameters L{sub 10}{sup r}(M{sub {rho}}) and C{sub 87}{sup r}(M{sub {rho}}). These two low-energy constants appear at order p{sup 4} and p{sup 6}, respectively, in the chiral perturbation theory expansion of the V-A correlator. At order p{sup 4} we obtain L{sub 10}{sup r}(M{sub {rho}})=-(5.22{+-}0.06)x10{sup -3}. Including in the analysis the two-loop (order p{sup 6}) contributions, we get L{sub 10}{sup r}(M{sub {rho}})=-(4.06{+-}0.39)x10{sup -3} and C{s…

Semileptonic decayQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsCrystallographyChiral perturbation theoryQuantum mechanicsHadronOrder (ring theory)Operator product expansionCorrelation function (quantum field theory)Perturbation theoryPhysical Review D
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Suppression of the speckle noise in solid polymer samples: a light scattering study

1994

The speckle effect disturbs the measurement of spatial correlation functions in solid polymer samples by light scattering. To be able to extract the desired correlations from the measurements, the speckle noise must be suppressed. This is possible by moving the sample during the measurement. In this paper we demonstrate that a sufficient reduction of speckle contrast can be achieved even in samples of restricted dimensions or with a preferential direction.

Spatial correlationMaterials scienceScatteringbusiness.industryGeneral EngineeringSpeckle noiseNoise (electronics)Atomic and Molecular Physics and OpticsLight scatteringSpeckle patternCorrelation function (statistical mechanics)BruitOpticsmedicinemedicine.symptombusinessOptical Engineering
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