Search results for "Field Theory"

showing 10 items of 1188 documents

Nonlinear Relaxation in Population Dynamics

2001

We analyze the nonlinear relaxation of a complex ecosystem composed of many interacting species. The ecological system is described by generalized Lotka-Volterra equations with a multiplicative noise. The transient dynamics is studied in the framework of the mean field theory and with random interaction between the species. We focus on the statistical properties of the asymptotic behaviour of the time integral of the i-th population and on the distribution of the population and of the local field.

education.field_of_studyDistribution (number theory)Statistical Mechanics (cond-mat.stat-mech)Applied MathematicsPopulationFOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksMultiplicative noiseQuantitative BiologyNonlinear systemMean field theoryModeling and SimulationFOS: Biological sciencesQuantitative Biology::Populations and EvolutionGeometry and TopologyRelaxation (approximation)Statistical physicseducationFocus (optics)Local fieldCondensed Matter - Statistical MechanicsQuantitative Biology (q-bio)Mathematics
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Opinion dynamics and stubbornness through mean-field games

2013

This paper provides a mean field game theoretic interpretation of opinion dynamics and stubbornness. The model describes a crowd-seeking homogeneous population of agents, under the influence of one stubborn agent. The game takes on the form of two partial differential equations, the Hamilton-Jacobi-Bellman equation and the Kolmogorov-Fokker-Planck equation for the individual optimal response and the population evolution, respectively. For the game of interest, we establish a mean field equilibrium where all agents reach epsilon-consensus in a neighborhood of the stubborn agent's opinion.

education.field_of_studyPartial differential equationControl and OptimizationDifferential equationMulti-agent systemPopulationComputer Science::Social and Information NetworksControl and Systems Engineering; Modeling and Simulation; Control and OptimizationInterpretation (model theory)Computer Science::Multiagent SystemsStochastic partial differential equationMean field theoryComputer Science::Systems and ControlControl and Systems EngineeringModeling and Simulationopinion dynamicseducationMathematical economicsGame theoryMathematics
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Complete One-Loop Renormalization of the Higgs-Electroweak Chiral Lagrangian

2018

The electroweak sector of the Standard Model can be formulated in a way similar to Chiral Perturbation Theory (ChPT), but extended by a singlet scalar. The resulting effective field theory (EFT) is called Higgs-Electroweak Chiral Lagrangian (EWCh$\mathcal{L}$) and is the most general approach to new physics in the Higgs sector. It solely assumes the pattern of symmetry breaking leading to the three electroweak Goldstone bosons (i.e. massive $W$ and $Z$) and the existence of a Higgs-like scalar particle. The power counting of the EWCh$\mathcal{L}$ is given by a generalization of the momentum expansion of ChPT. It is connected to a loop expansion, making the theory renormalizable order by ord…

effective Lagrangian: chiralNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryelectroweak interaction: symmetry breakingHigh Energy Physics::LatticeScalar (mathematics)standard modelFOS: Physical sciencesTechnicolorsinglet: scalarHiggs particleexpansion: higher-order01 natural sciencesHiggs sectorStandard ModelrenormalizationRenormalizationTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)effective field theoryfluctuation: scalar0103 physical sciencesEffective field theorylcsh:Nuclear and particle physics. Atomic energy. RadioactivityLimit (mathematics)010306 general physicsPhysicselectroweak interaction010308 nuclear & particles physicsnew physicsElectroweak interactionHigh Energy Physics::Phenomenologyhigher-order: 1perturbation theory: chiralGoldstone particleHiggs fieldHigh Energy Physics - Phenomenologyscalar particlebackground field[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Goldstone bosonHiggs bosonHiggs modellcsh:QC770-798expansion: heat kernelfield theory: renormalizableexpansion: momentum
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First measurement of proton's charge form factor at very low $Q^2$ with initial state radiation

2017

We report on a new experimental method based on initial-state radiation (ISR) in e-p scattering, in which the radiative tail of the elastic e-p peak contains information on the proton charge form factor ($G_E^p$) at extremely small $Q^2$. The ISR technique was validated in a dedicated experiment using the spectrometers of the A1-Collaboration at the Mainz Microtron (MAMI). This provided first measurements of $G_E^p$ for $0.001\leq Q^2\leq 0.004 (GeV/c)^2$.

experimental methodsProtonelastic scattering01 natural sciencesHigh Energy Physics - ExperimentLamb shiftHigh Energy Physics - Experiment (hep-ex)Initial state radiation ; Proton ; Form factor ; Radiative correctionsRadiative transfer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentMicrotronElastic scatteringPhysicsForm factor (quantum field theory)beam: currentRadiative correctionslcsh:QC1-9993. Good healthPRIRODNE ZNANOSTI. Fizika.ProtonNuclear and High Energy PhysicsFOS: Physical sciencesBethe-Heitler25.30.BfRadiation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear physicselectron p: scatteringMainz Linac[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]12.20.-m0103 physical sciencesradiation: initial-state interaction010306 general physicsnumerical calculationsform factor: charge41.60.-m010308 nuclear & particles physicsScatteringp: chargeNATURAL SCIENCES. Physics.microtronForm factorLamb shiftspectrometerInitial state radiationlcsh:Physicsexperimental results
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Remarks on strange-quark simulations with Wilson fermions

2020

Physical review / D 102(7), 074506 (1-10) (2020). doi:10.1103/PhysRevD.102.074506

fermion: WilsonStrange quarkParticle physicsWilson [fermion]High Energy Physics::Latticefermion: determinantdeterminant [fermion]FOS: Physical sciencesLattice QCD12.38.GcComputer Science::Digital Libraries01 natural sciences5303 [flavor]High Energy Physics - Lattice0103 physical sciencesquantum chromodynamicsflavor: 3ddc:530010306 general physicsMonte CarloMonte Carlo algorithmsQuantum chromodynamicsPhysicsCondensed Matter::Quantum Gases010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)lattice field theoryFermionLattice field theories lattice QCDHigh Energy Physics::Experiment
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Leading isospin breaking effects in the HVP contribution to $a_{\mu}$ and to the running of $\alpha$

2021

The 38th International Symposium on Lattice Field Theory, LATTICE2021, Zoom/Gather@Massachusetts Institute of Technology, USA, 26 Jul 2021 - 30 Jul 2021; Proceedings of Science / International School for Advanced Studies (LATTICE2021), 106 (2021). doi:10.22323/1.396.0106

fermion: WilsonWilson [fermion]muon: magnetic momentHigh Energy Physics::Latticevacuum polarization: hadronicHigh Energy Physics::Phenomenologylattice field theorynonperturbative530isospinHigh Energy Physics - Latticeelectromagnetic [coupling]coupling: electromagneticmagnetic moment [muon]quantum chromodynamicshadronic [vacuum polarization]quantum electrodynamicsddc:530High Energy Physics::Experimentcorrelation function
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Transverse momentum distributions for exclusive $\varrho^{0}$ muoproduction

1992

We have studied transverse momentum distributions for exclusive rho(0) muoproduction on protons and heavier nuclei at 2 < Q2 < 25 GeV2. The Q2 dependence of the slopes of the p(t)2 and t' distributions is discussed. The influence of the non-exclusive background is investigated. The p(t)2-slope for exclusive events is 4.3 +/- 0.6 +/- 0.7 GeV-2 at large Q2. The p(t)2 spectra are much softer than inclusive p(t)2 spectra of leading hadrons produced in deep inelastic scattering.

forward spectrometer: experimental resultsPhysics and Astronomy (miscellaneous)Nuclear Theorymuon nucleus: nuclear reactionchemistry.chemical_elementElementary particlemuon deuteron: nuclear reaction530Nuclear physicsmass spectrum: two-pionmomentum transfer: slopespectrum: transverse momentumField theory (psychology)Quantum field theoryNuclear Experimentrho(770)0: electroproductionEngineering (miscellaneous)muon p: exclusive reactionPhysicspomeron: exchangecalciumtwo-pion: mass spectrumbackgroundelectroproduction: rho(770)0carbon200 GeVCERN SPSDeep inelastic scatteringParticle accelerationexchange: pomeronchemistrytransverse momentum: spectrumQuantum electrodynamicsTransverse momentumHigh Energy Physics::ExperimentCarbonParticle Physics - Experimentmuon p --> rho(770)0 nucleon
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Pants complex, TQFT and hyperbolic geometry

2021

We present a coarse perspective on relations of the $SU(2)$-Witten-Reshetikhin-Turaev TQFT, the Weil-Petersson geometry of the Teichm\"uller space, and volumes of hyperbolic 3-manifolds. Using data from the asymptotic expansions of the curve operators in the skein theoretic version of the $SU(2)$-TQFT, as developed by Blanchet, Habegger, Masbaum and Vogel, we define the quantum intersection number between pants decompositions of a closed surface. We show that the quantum intersection number admits two sided bounds in terms of the geometric intersection number and we use it to obtain a metric on the pants graph of surfaces. Using work of Brock we show that the pants graph equipped with this …

geometryasymptotic expansiongraph theory[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]Geometric Topology (math.GT)[PHYS.MPHY] Physics [physics]/Mathematical Physics [math-ph]field theory: topologicalMathematics::Geometric Topologygroup: representationMathematics - Geometric TopologySU(2)FOS: Mathematicssurfacespace: noncompact
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Forward light-by-light scattering and electromagnetic correction to hadronic vacuum polarization

2023

Lattice QCD calculations of the hadronic vacuum polarization (HVP) have reached a precision where the electromagnetic (e.m.) correction can no longer be neglected. This correction is both computationally challenging and hard to validate, as it leads to ultraviolet (UV) divergences and to sizeable infrared (IR) effects associated with the massless photon. While we precisely determine the UV divergence using the operator-product expansion, we propose to introduce a separation scale $\Lambda\sim400\;$MeV into the internal photon propagator, whereby the calculation splits into a short-distance part, regulated in the UV by the lattice and in the IR by the scale $\Lambda$, and a UV-finite long-di…

hadronic contributionsNuclear and High Energy Physicsfusionmassless530 PhysicsFOS: Physical sciences[PHYS.HLAT] Physics [physics]/High Energy Physics - Lattice [hep-lat]operator product expansionhadronicHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)vacuum polarizationultravioletquantum electrodynamicstree approximationphoton photonlattice[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]effectscatteringphotonscattering amplitudeHigh Energy Physics - Lattice (hep-lat)lattice field theory530 Physikradiative correctionssum rule[PHYS.HPHE] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics - Phenomenologyelectromagneticfinite size[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]infrareddispersionlight-by-light scatteringpropagatorcorrectionJournal of High-Energy Physics
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Quarkonium suppression in heavy-ion collisions: an open quantum system approach

2016

We address the evolution of heavy-quarkonium states in an expanding quark-gluon plasma by implementing effective field theory techniques in the framework of open quantum systems. In this setting we compute the nuclear modification factors for quarkonia that are $S$-wave Coulombic bound states in a strongly-coupled quark-gluon plasma. The calculation is performed at an accuracy that is leading-order in the heavy-quark density expansion and next-to-leading order in the multipole expansion. The quarkonium density-matrix evolution equations can be written in the Lindblad form, and, hence, they account for both dissociation and recombination. Thermal mass shifts, thermal widths and the Lindblad …

heavy ion: scatteringNuclear TheoryHigh Energy Physics::Latticequarkonium: productionhiukkasfysiikka01 natural sciences7. Clean energyHigh Energy Physics - ExperimentOpen quantum systemHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Bound stateEffective field theory[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]quark gluon: plasmaPhysicsLindblad equationquarkonium: suppressionopen quantum systemsQuarkoniumHigh Energy Physics - PhenomenologyQuantum electrodynamicsquarkoniummomentum: diffusion[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencesdissociationMomentum diffusionNuclear Theory (nucl-th)[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]Quantum mechanics0103 physical sciencesplasma: expansionparticle physics010306 general physicsheavy quark: momentumta114010308 nuclear & particles physicsHigh Energy Physics::Phenomenologynuclear matter: effectrecombinationUpsilon(10020)evolution equation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quark–gluon plasma[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentMultipole expansionUpsilon(9460)
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