Search results for "dispersion relation"

showing 10 items of 140 documents

Wellentypen in Helium II-Schichten

1968

In liquid helium two wave modes are possible. Their properties may be analysed by solving the thermohydrodynamical equations under the condition that the tangential component of the normal fluid velocity is vanishing on the walls. In the present paper, these two types of wave propagation are determined for a plane-parallel capillary with the heat conduction and the thermal expansion being neglected and with the width of the capillary being much smaller than the penetration depth of a viscous wave. In particular, the dispersion relations of both, the so called fourth sound and an overdamped mode are calculated. (This overdamped mode may be called fifth wave mode.) The velocity fields can be …

PhysicsNuclear and High Energy PhysicsCondensed matter physicsWave propagationCapillary actionLiquid heliumThermal conductionlaw.inventionPhysics::Fluid DynamicslawDispersion relationParticle velocityPenetration depthTangential and normal componentsZeitschrift für Physik A Hadrons and nuclei
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Double pion photoproduction in nuclei

1995

The inclusive A(gamma,pi+ pi-)X reaction is studied theoretically. A sizeable enhancement of the cross section is found, in comparison with the scaling of the deuteron cross section (sigma_deuteron * A/2). This enhancement is due to the modifications in the nuclear medium of the gamma N ----> pi pi N amplitude and the pion dispersion relation. The enhancement is found to be bigger than the one already observed in the (pi,pi pi) reaction in nuclei.

PhysicsNuclear and High Energy PhysicsNuclear TheoryFOS: Physical sciencesFísicaSigmaNuclear Theory (nucl-th)Nuclear physicsCross section (physics)AmplitudePionDeuteriumCIENCIA DE LOS MATERIALES E INGENIERIA METALURGICADispersion relationPiScalingNuclear Physics A
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Dispersion relations and the spin polarizabilities of the nucleon

1997

A forward dispersion calculation is implemented for the spin polarizabilities $\gamma_1, ... ,\gamma_4$ of the proton and the neutron. These polarizabilities are related to the spin structure of the nucleon at low energies and are structure-constants of the Compton scattering amplitude at ${\cal O}(\omega^3)$. In the absence of a direct experimental measurement of these quantities, a dispersion calculation serves the purpose of constraining the model building, and of comparing with recent calculations in heavy baryon chiral perturbation theory.

PhysicsNuclear and High Energy PhysicsNuclear TheoryHeavy baryon chiral perturbation theoryProtonNuclear TheoryCompton scatteringFOS: Physical sciencesSpin structureNuclear Theory (nucl-th)Nuclear physicsDispersion relationNeutronNuclear ExperimentNucleonSpin-½Physics Letters B
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Dispersion relation formalism for virtual Compton scattering of the proton

2001

We present in detail a dispersion relation formalism for virtual Compton scattering (VCS) off the proton from threshold into the $\Delta(1232)$-resonance region. Such a formalism can be used as a tool to extract the generalized polarizabilities of the proton from both unpolarized and polarized VCS observables over a larger energy range. We present calculations for existing and forthcoming VCS experiments and demonstrate that the VCS observables in the energy region between pion production threshold and the $\Delta(1232)$-resonance show an enhanced sensitivity to the generalized polarizabilities.

PhysicsNuclear and High Energy PhysicsParticle physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyCompton scatteringFOS: Physical sciencesComputer Science::Software EngineeringObservableHigh Energy Physics - PhenomenologyFormalism (philosophy of mathematics)High Energy Physics - Phenomenology (hep-ph)PionQuantum electrodynamicsDispersion relationComputer Science::Networking and Internet ArchitectureEnhanced sensitivitySDG 7 - Affordable and Clean Energy
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Exploring the intrinsic Lorentz-violating parameters at DUNE

2018

Neutrinos can push our search for new physics to a whole new level. What makes them so hard to be detected, what allows them to travel humongous distances without being stopped or deflected allows to amplify Planck suppressed effects (or effects of comparable size) to a level that we can measure or bound in DUNE. In this work we analyze the sensitivity of DUNE to CPT and Lorentz-violating interactions in a framework that allows a straightforward extrapolation of the bounds obtained to any phenomenological modification of the dispersion relation of neutrinos.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelLorentz transformationExtrapolationFOS: Physical sciences01 natural sciencesMeasure (mathematics)Partícules (Física nuclear)lcsh:QC1-999High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Dispersion relation0103 physical sciencessymbolsSensitivity (control systems)NeutrinoPlanck010306 general physicslcsh:PhysicsPhysics Letters B
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Spectral distribution for the decay τ→ντKπ

2006

Abstract With the newly available data sets on hadronic τ decays from the B -factories BaBar and BELLE, and future data from BESIII, precise information on the decay distributions will soon become available. This calls for an improvement of the decay spectra also on the theoretical side. In this work, the distribution function for the decay τ → ν τ K π will be presented with the relevant Kπ vector and scalar form factors being calculated in the framework of the resonance chiral theory, also taking into account additional constraints from dispersion relations and short-distances. As a by-product the slope and curvature of the vector form factor F + K π ( s ) are determined to be λ + ′ = 25.6…

PhysicsNuclear and High Energy PhysicsParticle physicsBranching fractionPartial wave analysisHadronScalar (mathematics)ResonanceDecays of tausNuclear physicsDistribution functionDispersion relationHigh Energy Physics::ExperimentB mesonChiral symmetriesDispersion relationsPhysics Letters B
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Universal Bounds for SU(3) Low Energy Constants

2008

In this paper bounds for L_1, L_2 and L_3 are obtained in Chiral Perturbation Theory with three flavours. At the same time we test the compatibility of this theory with axiomatic principles. Following a recent paper we use dispersion relations to write positivity conditions that translate into bounds for the chiral low energy constants. As a first approach we consider the exact SU(3)_V limit and notice that if a common mass of the order of that of the kaon is adopted for the octet of pseudo-Goldstone bosons the bounds have very large O(p^6) corrections. Once the positivity conditions are adapted to account for different masses, we correct the previous bounds for a physical kaon mass and fin…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryOctetFOS: Physical sciencesHigh Energy Physics - PhenomenologyLow energyHigh Energy Physics - Phenomenology (hep-ph)Dispersion relationGoldstone bosonAxiomMathematical physicsBoson
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Dispersion Theory in Electromagnetic Interactions

2018

We review various applications of dispersion relations (DRs) to the electromagnetic structure of hadrons. We discuss the way DRs allow one to extract information on hadron structure constants by connecting information from complementary scattering processes. We consider the real and virtual Compton scattering processes off the proton, and summarize recent advances in the DR analysis of experimental data to extract the proton polarizabilities, in comparison with alternative studies based on chiral effective field theories. We discuss a multipole analysis of real Compton scattering data, along with a DR fit of the energy-dependent dynamical polarizabilities. Furthermore, we review new sum rul…

PhysicsNuclear and High Energy PhysicsParticle physicsField (physics)Nuclear Theory010308 nuclear & particles physicsScatteringHadronCompton scatteringFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PolarizabilityDispersion relation0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNucleonMultipole expansionNuclear Experiment
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Radiative pion capture by a nucleon

2000

The differential cross sections for $\pi^- p \to \gamma n$ and $\pi^+ n \to \gamma p$ are computed up to $O(p^3)$ in heavy baryon chiral perturbation theory (HBChPT). The expressions at $O(p)$ and $O(p^2)$ have no free parameters. There are three unknown parameters at $O(p^3)$, low energy constants of the HBChPT Lagrangian, which are determined by fitting to experimental data. Two acceptable fits are obtained, which can be separated by comparing with earlier dispersion relation calculations of the inverse process. Expressions for the multipoles, with emphasis on the p-wave multipoles, are obtained and evaluated at threshold. Generally the results obtained from the best of the two fits are i…

PhysicsNuclear and High Energy PhysicsParticle physicsHeavy baryon chiral perturbation theoryNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInverseFOS: Physical sciences01 natural sciencesJNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Dispersion relation0103 physical sciencesRadiative transfersymbolsddc:530010306 general physicsNucleonLagrangianFree parameter
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Precise determination of resonance pole parameters through Pad\'e approximants

2014

In this work, we present a precise and model--independent method to extract resonance pole parameters from phase-shift scattering data. These parameters are defined from the associated poles in the second Riemann sheet, unfolded by the analytic continuation to the complex pole using Pad\'e approximants. Precise theoretical parameterizations of pion-pion scattering phase shifts based on once-- and twice-- subtracted dispersion relations are used as input, whose functional form allows us to show the benefit and accuracy of the method. In particular, we extract from these parametrization the pole positions of the $f_0(500)$ at $\sqrt{s}=(453\pm 15) - i(297 \pm 15)$ MeV, the $\rho(770)$ at $\sq…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryScatteringAnalytic continuationResonanceRiemann hypothesissymbols.namesakeHigh Energy Physics - PhenomenologyPionHigh Energy Physics - LatticeQuantum electrodynamicsDispersion relationsymbolsPadé approximantNuclear Experiment
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