Search results for "chiral [model]"

showing 10 items of 83 documents

Photoproduction of scalar mesons on protons and nuclei

1999

We study the photoproduction of scalar mesons close to the threshold of f_0(980) and a_0(980) using a unitary chiral model. Peaks for both resonances show up in the invariant mass distributions of pairs of pseudoscalar mesons. A discussion is made on the photoproduction of these resonances in nuclei, which can shed light on their nature, a subject of continuous debate.

PhysicsNuclear and High Energy PhysicsParticle physicsMeson productionMesonUnitarityNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryScalar (physics)FOS: Physical sciencesFísicaNuclear Theory (nucl-th)Nuclear physicsPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Chiral modelBibliographyInvariant massHigh Energy Physics::ExperimentNuclear Experiment
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Exploring the D* rho system within QCD sum rules

2013

We present a study of the D* rho system made by using the method of QCD sum rules to determine the mass of possible resonances generated in the same system. Using isospin and spin projectors, we investigate the different configurations and obtain evidences for three D* mesons with isospin I = 1/2, spin S = 0, 1, 2 and with masses 2500 +/- 67, 2523 +/- 60, and 2439 +/- 119 MeV, respectively. The last state can be associated with D-2*(2460) ( spin 2) listed by the Particle Data Group, while one of the first two might be related to D* (2640), with unknown spin parity. In the case of I = 3/2 we also find evidences of three states with spin 0, 1, and 2, respectively, with masses 2467 +/- 82, 242…

PhysicsNuclear and High Energy PhysicsParticle physicsQCD sum rulesNuclear TheoryField (physics)Meson010308 nuclear & particles physicsNuclear TheoryFísicaParticle Data GroupCharmed mesonsQuantum number01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyIsospin0103 physical sciencesEffective field theoryChiral dynamicsNuclear Experiment010306 general physicsSpin-½
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Axial resonances in the open and hidden charm sectors

2007

13 pages, 2 figures.-- PACS nrs.: 11.10.St, 11.80.Gw, 12.39.Hg, 12.39.Fe.-- ISI Article Identifier: 000249271600001.-- ArXiv pre-print available at: http://arxiv.org/abs/0704.2314

PhysicsNuclear and High Energy PhysicsParticle physics[PACS] Chiral LagrangiansChiral-symmetryMeson resonancesHeavy mesons[PACS] Heavy quark effective theoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísica[PACS] Bound and unstable states; Bethe-Salpeter equationsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)[PACS] Multichannel scatteringBethe-Salpeter equationsHigh Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment[PACS] Bound and unstable states
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Latest Results for the Antikaon-Nucleon Optical Potential

2010

The key question of this letter is whether the K-nucleus optical potential is deep, as it is prefered by the phenomenological fits to kaonic atoms data, or shallow, as it comes out from unitary chiral model calculations. The current experimental situation is reviewed.

PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciences01 natural sciencesUnitary stateOptical potentialAtomic and Molecular Physics and OpticsNuclear Theory (nucl-th)Chiral model0103 physical sciencesKey (cryptography)Physics::Atomic PhysicsCurrent (fluid)010306 general physicsNucleonNuclear Experiment
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Oblique S and T Constraints on Electroweak Strongly-Coupled Models with a Light Higgs

2014

Using a general effective Lagrangian implementing the chiral symmetry breaking SU(2) L ⊗ SU(2) R → SU(2) L+R , we present a one-loop calculation of the oblique S and T parameters within electroweak strongly-coupled models with a light scalar. Imposing a proper ultraviolet behaviour, we determine S and T at next-to-leading order in terms of a few resonance parameters. The constraints from the global fit to electroweak precision data force the massive vector and axial-vector states to be heavy, with masses above the TeV scale, and suggest that the W + W − and ZZ couplings of the Higgs-like scalar should be close to the Standard Model value. Our findings are generic, since they only rely on so…

PhysicsParticle physicsNuclear and High Energy PhysicsHiggs PhysicsElectroweak interactionScalar (mathematics)High Energy Physics::PhenomenologyOrder (ring theory)Oblique caseFOS: Physical sciencesTechnicolor and Composite ModelsResonance (particle physics)Standard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Beyond Standard ModelHiggs bosonChiral symmetry breakingChiral lagrangians
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Towards a determination of the chiral couplings at NLO in 1/N-C: L-8(r)(μ) and C-38(r)(μ)

2007

14 pages.-- ISI Article Identifier: 000244120200039.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0610290

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeScalar (mathematics)ResonanceOrder (ring theory)FísicaFOS: Physical sciences1/N ExpansionRenormalizationPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum Chromodynamics (QCD)High Energy Physics::ExperimentPion decay constantChiral lagrangians
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V-us determination from hyperon semileptonic decays

2005

16 páginas, 9 tablas.-- arXiv:hep-ph/0509045v2

PhysicsQuarkSystematic errorNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyHyperonFOS: Physical sciencesFísica1/N ExpansionFirst orderQCDHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSymmetry breakingChiral lagrangiansMixing (physics)Quark masses and SM parameters
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Crystal structure of (1S,2R,4S)-1-[(morpholin-4-yl)methyl]-4-(prop-1-en-2-yl)cyclohexane-1,2-diol

2014

Besides intra­molecular O—H⋯N hydrogen bonds, the crystal structure displays inter­molecular O—H⋯O and C—H⋯O hydrogen bonds linking the mol­ecules into undulating layers parallel to the (01) plane.

Quantitative Biology::Biomoleculescrystal structureCrystallographyHydrogen bondDiolCyclohexane conformationAbsolute configurationGeneral ChemistryCrystal structureCondensed Matter Physicschiral ligand for catalytic enantioselective transformationsResearch CommunicationsHexaneCrystalchemistry.chemical_compoundCrystallographychemistryQD901-999Morpholinehydrogen bondschiral ligand for catalytic enanti­oselective transformationsGeneral Materials SciencePhysics::Chemical Physicsamino-12-diolActa Crystallographica Section E: Crystallographic Communications
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Low-energy couplings of QCD from topological zero-mode wave functions

2003

By matching 1/m^2 divergences in finite-volume two-point correlation functions of the scalar or pseudoscalar densities with those obtained in chiral perturbation theory, we derive a relation between the Dirac operator zero-mode eigenfunctions at fixed non-trivial topology and the low-energy constants of QCD. We investigate the feasibility of using this relation to extract the pion decay constant, by computing the zero-mode correlation functions on the lattice in the quenched approximation and comparing them with the corresponding expressions in quenched chiral perturbation theory.

Quantum chromodynamicsPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsZero modeChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesParticle Physics - LatticeQuenched approximationDirac operatorTopologyPseudoscalarsymbols.namesakelattice QCDHigh Energy Physics - LatticeHigh Energy Physics - Theory (hep-th)nonperturbative effectssymbolschiral lagrangiansPion decay constantWave function
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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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