Search results for "Effective Field Theory"

showing 10 items of 212 documents

Effective Field Theory for Jet Processes

2015

Processes involving narrow jets receive perturbative corrections enhanced by logarithms of the jet opening angle and the ratio of the energies inside and outside the jets. Analyzing cone-jet processes in effective field theory, we find that in addition to soft and collinear fields their description requires degrees of freedom which are simultaneously soft and collinear to the jets. These collinear-soft particles can resolve individual collinear partons, leading to a complicated multi-Wilson-line structure of the associated operators at higher orders. Our effective field theory provides, for the first time, a factorization formula for a cone-jet process, which fully separates the physics at …

PhysicsJet (fluid)Wilson loop010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaDegrees of freedom (physics and chemistry)FOS: Physical sciencesGeneral Physics and AstronomyPartonRenormalization group01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationQuantum electrodynamics0103 physical sciencesEffective field theoryHigh Energy Physics::ExperimentResummation010306 general physicsPhysical Review Letters
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Weak Interactions at Low Energy

1985

In this series of lectures, I would like to discuss the basic aspects of the standard electroweak theory, as well as some alternatives. The phenomenology associated with charged and neutral currents weak interaction will show the success of the standard theory in giving a quantitative account of the existing data. The framework of most of our considerations will be that of an effective theory at low momentum transfer, low with respect to the masses of the intermediate vector bosons, 80–90 GeV. As an extension of the standard theory for the leptonic sector, I will contemplate the possibility of massive neutrinos being described by Majorana fields, leading to exotic phenomena induced by lepto…

PhysicsMAJORANAParticle physicsHigh Energy Physics::PhenomenologyElectroweak interactionEffective field theoryHigh Energy Physics::ExperimentNeutrinoWeak interactionPhenomenology (particle physics)Lepton numberVector boson
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A one-loop study of matching conditions for static-light flavor currents

2012

Heavy Quark Effective Theory (HQET) computations of semi-leptonic decays, e.g. B -> pi l nu, require the knowledge of the parameters in the effective theory for all components of the heavy-light flavor currents. So far non-perturbative matching conditions have been employed only for the time component of the axial current. Here we perform a check of matching conditions for the time component of the vector current and the spatial component of the axial vector current up to one-loop order of perturbation theory and to lowest order of the 1/m-expansion. We find that the proposed observables have small higher order terms in the 1/m-series and are thus excellent candidates for a non-perturbat…

PhysicsMatching (statistics)Nuclear and High Energy PhysicsCurrent (mathematics)010308 nuclear & particles physicsComponent (thermodynamics)ComputationHigh Energy Physics - Lattice (hep-lat)Mathematical analysisHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservable01 natural sciencesHigh Energy Physics - Lattice0103 physical sciencesEffective field theoryddc:530Perturbation theory (quantum mechanics)010306 general physicsPseudovector
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Dispersive evaluation of the Lamb shift in muonic deuterium from chiral effective field theory

2020

We merge the dispersive relation approach and the ab initio method to compute nuclear structure corrections to the Lamb shift in muonic deuterium. We calculate the deuteron response functions and corresponding uncertainties up to next-to-next-to-next-to-leading order in chiral effective field theory and compare our results to selected electromagnetic data to test the validity of the theory. We then feed response functions calculated over a wide range of kinematics to the dispersion-theory formalism and show that an improved accuracy is obtained compared to that with the use of available experimental data in the dispersive analysis. This opens up the possibility of applying this hybrid metho…

PhysicsNuclear Theory010308 nuclear & particles physicsNuclear structureAb initioFOS: Physical sciencesExperimental dataKinematicsAtomic spectroscopy7. Clean energy01 natural sciences3. Good healthComputational physicsLamb shiftNuclear Theory (nucl-th)Deuterium0103 physical sciencesEffective field theoryPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysical Review C
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Recent developments in effective field theory

2007

We will give a short introduction to the one-nucleon sector of chiral perturbation theory and will address the issue of a consistent power counting and renormalization. We will discuss the infrared regularization and the extended on-mass-shell scheme. Both allow for the inclusion of further degrees of freedom beyond pions and nucleons and the application to higher-loop calculations. As applications we consider the chiral expansion of the nucleon mass to order O(q^6) and the inclusion of vector and axial-vector mesons in the calculation of nucleon form factors.

PhysicsNuclear and High Energy PhysicsChiral perturbation theoryMesonNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryDegrees of freedom (statistics)FOS: Physical sciencesRenormalizationNuclear Theory (nucl-th)Theoretical physicsPionRegularization (physics)Effective field theoryNucleonNuclear Experiment
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The polarizability of the pion: no conflict between dispersion theory and chiral perturbation theory

2008

Recent attempts to determine the pion polarizability by dispersion relations yield values that disagree with the predictions of chiral perturbation theory. These dispersion relations are based on specific forms for the absorptive part of the Compton amplitudes. The analytic properties of these forms are examined, and the strong enhancement of intermediate-meson contributions is shown to be connected with spurious singularities. If the basic requirements of dispersion relations are taken into account, the results of dispersion theory and effective field theory are not inconsistent.

PhysicsNuclear and High Energy PhysicsChiral perturbation theorynucl-thNuclear TheoryFOS: Physical scienceshep-phnucl-exChirality (electromagnetism)Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)SingularityPionPolarizabilityQuantum electrodynamicsDispersion relationEffective field theoryNuclear Experiment (nucl-ex)Perturbation theoryNuclear Experiment
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Electromagnetic transition form factors of the Roper resonance in a phenomenological field theory

2014

We analyze the form factors of the electromagnetic nucleon-to-Roper-resonance transition in the framework of a low-energy phenomenological field theory. A systematic power-counting procedure is generated by applying the complex-mass scheme. Within this power counting we calculate the form factors to next-to-next-to-leading order and fit the results to empirical data.

PhysicsNuclear and High Energy PhysicsEmpirical dataTheoretical physicsRoper resonanceTransition (fiction)Quantum electrodynamicsEffective field theoryOrder (ring theory)Field theory (psychology)Nuclear theoryPower (physics)Physical Review C
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Factorization and NNLL Resummation for Higgs Production with a Jet Veto

2012

Using methods of effective field theory, we derive the first all-order factorization theorem for the Higgs-boson production cross section with a jet veto, imposed by means of a standard sequential recombination jet algorithm. Like in the case of small-q_T resummation in Drell-Yan and Higgs production, the factorization is affected by a collinear anomaly. Our analysis provides the basis for a systematic resummation of large logarithms log(m_H/p_T^veto) beyond leading-logarithmic order. Specifically, we present predictions for the resummed jet-veto cross section and efficiency at next-to-next-to-leading logarithmic order. Our results have important implications for Higgs-boson searches at the…

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesWeierstrass factorization theoremHiggs bosonsymbolsEffective field theoryHigh Energy Physics::ExperimentResummationAnomaly (physics)010306 general physics
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Factorization and resummation for jet broadening

2011

Jet broadening is an event-shape variable probing the transverse momenta of particles inside jets. It has been measured precisely in e+e- annihilations and is used to extract the strong coupling constant. The factorization of the associated cross section at small values of the broadening is afflicted by a collinear anomaly. Based on an analysis of this anomaly, we present the first all-order expressions for jet-broadening distributions, which are free of large perturbative logarithms in the two-jet limit. Our formulae reproduce known results at next-to-leading logarithmic order but also extend to higher orders.

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physicsLogarithm010308 nuclear & particles physicsElectron–positron annihilationFOS: Physical sciences01 natural sciencessymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationQuantum electrodynamics0103 physical sciencesWeierstrass factorization theoremEffective field theorysymbolsAnomaly (physics)Resummation010306 general physicsPHYSICS LETTERS B
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The magnetic moment of the ρ-meson

2014

The magnetic moment of the \rho-meson is calculated in the framework of a low-energy effective field theory of the strong interactions. We find that the complex-valued strong interaction corrections to the gyromagnetic ratio are small leading to a value close to the real leading tree level result, g_\rho = 2. This is in a reasonably good agreement with the available lattice QCD calculations for this quantity.

PhysicsNuclear and High Energy PhysicsMesonMagnetic moment010308 nuclear & particles physicsHigh Energy Physics::LatticeGyromagnetic ratioStrong interactionLattice QCDReal tree01 natural sciencesHigh Energy Physics - PhenomenologyQuantum electrodynamics0103 physical sciencesEffective field theoryddc:530010306 general physicsValue (mathematics)
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