Search results for "Goldstone"

showing 6 items of 36 documents

Resonance saturation of the chiral couplings at next-to-leading order in 1/N-C

2009

9 páginas, 3 figuras.-- ISI article identifier:000266408300099.-- ArXiv pre-print avaible at:http://arxiv.org/abs/0903.2440

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)ResonanceRenormalizationQuantum mechanicsGoldstone bosonSaturation (graph theory)Perturbation theory (quantum mechanics)Mathematical physics
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The A5 and the pion field

2005

In this talk, an SU(Nf)xSU(Nf)Yang-Mills model with a compact extra-dimension is used to describe the spin-1 mesons and pions of massless QCD in the large-Nc. The right 4D symmetry and symmetry-breaking pattern is produced by imposing appropriate boundary conditions. The Goldstone boson fields are constructed using a Wilson line. We derive the low-energy limit (chiral lagrangian), discuss rho-meson dominance, sum rules between resonance couplings and the relation with the QCD high-energy behavior. Finally, we provide an analytic expression for the two-point function of vector and axial currents.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMesonField (physics)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesAtomic and Molecular Physics and OpticsSymmetry (physics)High Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosonChiral symmetry breaking
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Proton Spin in Chiral Quark Models

1997

The spin and flavor fractions of constituent quarks in the proton are obtained from their chiral fluctuations involving Goldstone bosons. SU(3) flavor symmetry breaking suggested by the mass difference between the strange and up, down quarks is included, and this improves the agreement with the data markedly.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryProtonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyAstronomy and AstrophysicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosonProton spin crisisHigh Energy Physics::ExperimentSymmetry breakingFlavorSpin-½Modern Physics Letters A
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Finite Volume Scaling of Pseudo Nambu-Goldstone Bosons in QCD

2008

We consider chiral perturbation theory in a finite volume and in a mixed regime of quark masses. We take N_l light quarks near the chiral limit, in the so-called epsilon-regime, while the remaining N_h quarks are heavier and in the standard p-regime. We compute in this new mixed regime the finite-size scaling of the light meson correlators in the scalar, pseudoscalar, vector and axial vector channels.Using the replica method, we easily extend our results to the partially quenched theory. With the help of our results, lattice QCD simulations with 2+1 flavors can safely investigate pion physics with very light up and down quark masses even in the region where the pion's correlation length ove…

QuarkQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesDown quarkLattice QCDPseudoscalarPionHigh Energy Physics - LatticeGoldstone bosonHigh Energy Physics::Experiment
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Molecular dynamics in low-molar and polymeric ferroelectric liquid crystals

1991

Broadband dielectric spectroscopy covering the frequency range from 10−1 Hz to 109 Hz was employed to study the molecular dynamics in low-molar and polymeric ferrroelectric liquid crystals. At frequencies below 106 Hz the ferroelectric modes, soft and Goldstone mode are observed. In the frequency regime from 106 Hz to 109 Hz a fast relaxation process is found, which is assigned to the hindered rotation of the mesogens around their long molecular axis. It turns out that the molecular dynamics is not principally different between low-molar and polymeric systems.

Range (particle radiation)Materials sciencePolymers and PlasticsOrganic ChemistryMolecular axisCondensed Matter PhysicsRotationFerroelectricityMolecular physicsMolecular dynamicsNuclear magnetic resonanceLiquid crystalvisual_artMaterials Chemistryvisual_art.visual_art_mediumGoldstoneBroadband dielectric spectroscopyMakromolekulare Chemie. Macromolecular Symposia
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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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