Search results for "SCALAR"

showing 10 items of 1002 documents

Chiral unitary approach to eta'N scattering at low energies

2010

We study the \eta' N interaction within a chiral unitary approach which includes \pi N, \eta N and related pseudoscalar meson-baryon coupled channels. Since the SU(3) singlet does not contribute to the standard interaction and the \eta' is mostly a singlet, the resulting scattering amplitude is very small and inconsistent with experimental estimations of the \eta' N scattering length. The additional consideration of vector meson-baryon states into the coupled channel scheme, via normal and anomalous couplings of pseudoscalar to vector mesons, enhances substantially the \eta' N amplitude. We also exploit the freedom of adding to the Lagrangian a new term, allowed by the symmetries of QCD, wh…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeNuclear Theory01 natural sciencesQuantum mechanics0103 physical sciencesMesons (Nuclear physics)Mesons (Física nuclear)010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsUnitarityReaccions nuclears010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaCromodinàmica quàntica Partícules (Física nuclear)Scattering lengthBaryonPseudoscalarScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNuclear reactionsQuantum chromodynamics
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Scalar spectrum in a graviton soft wall model

2020

In this study we present a unified phenomenological analysis of the scalar glueball and scalar meson spectra within an AdS/QCD framework in the bottom up approach. For this purpose we generalize the recently developed graviton soft-wall (GSW) model, which has shown an excellent agreement with the lattice QCD glueball spectrum, to a description of glueballs and mesons with a unique energy scale. In this scheme, dilatonic effects, are incorporated in the metric as a deformation of the AdS space. We apply the model also to the heavy meson spectra with success. We obtain quadratic mass equations for all scalar mesons while the glueballs satisfy an almost linear mass equation. Besides their spec…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeScalar (mathematics)FOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Spectrum0103 physical sciencesAdS/CFT010306 general physicsScalar mesonQuantum chromodynamicsPhysics010308 nuclear & particles physicsGlueballHigh Energy Physics::PhenomenologyGravitonLattice QCDMesonMass formulaHigh Energy Physics - PhenomenologyGlueballHigh Energy Physics::Experiment
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Peripheral transverse densities of the baryon octet from chiral effective field theory and dispersion analysis

2017

The baryon electromagnetic form factors are expressed in terms of two-dimensional densities describing the distribution of charge and magnetization in transverse space at fixed light-front time. We calculate the transverse densities of the spin-1/2 flavor-octet baryons at peripheral distances b = O(M_\pi^{-1}) using methods of relativistic chiral effective field theory (\chi EFT) and dispersion analysis. The densities are represented as dispersive integrals over the imaginary parts of the form factors in the timelike region (spectral functions). The isovector spectral functions on the two-pion cut t > 4 M_\pi^2 are calculated using relativistic \chi EFT including octet and decuplet baryons.…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryIsoscalarHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)PionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesVector meson010306 general physicsNuclear ExperimentPhysicsIsovector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)HyperonForm factor (quantum field theory)BaryonHigh Energy Physics - PhenomenologyQuantum electrodynamicsHigh Energy Physics::Experiment
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Nature of the light scalar mesons

2005

Despite the apparent simplicity of meson spectroscopy, light scalar mesons cannot be accommodated in the usual $q\bar q$ structure. We study the description of the scalar mesons below 2 GeV in terms of the mixing of a chiral nonet of tetraquarks with conventional $q\bar q$ states. A strong diquark-antidiquark component is found for several states. The consideration of a glueball as dictated by quenched lattice QCD drives a coherent picture of the isoscalar mesons.

Nuclear and High Energy PhysicsParticle physicsMesonNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]IsoscalarHigh Energy Physics::Latticemeson massquark confinementLattice field theoryNuclear TheoryFOS: Physical sciencessparticles01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesquantum chromodynamics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsGlueballHigh Energy Physics::PhenomenologyScalar (physics)lattice field theory12.39.-x 12.38.-tFísicaLattice QCDDiquarkHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentchiral symmetries
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Charmed hadrons in nuclear medium

2010

5th International Conference on Quarks and Nuclear Physics (QNP09).Inst High Energy Phys Chinese Acad Sci, Beijing, PEOPLES R CHINA, SEP 21-25, 2009

Nuclear and High Energy PhysicsParticle physicsMesondynamically-generated baryonic resonancesNuclear TheoryHadronScalar (mathematics)Nuclear TheoryFOS: Physical sciencesspectral functionCharmed and hidden charmed scalar resonances01 natural sciences7. Clean energyNuclear Theory (nucl-th)symbols.namesakePauli exclusion principleHigh Energy Physics - Phenomenology (hep-ph)charmed and hidden charmed scalar resonances0103 physical sciencesNuclear Experiment (nucl-ex)Open-charm mesons010306 general physicsNuclear ExperimentInstrumentationNuclear ExperimentPhysics010308 nuclear & particles physicsBlocking (radio)Dynamically-generated baryonic resonancesHigh Energy Physics::PhenomenologyFísicaAstronomy and AstrophysicsSpectral functionBaryonHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentDense matterRESONANCESMATTERopen-charm mesons
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A dispersive estimate of scalar contributions to hadronic light-by-light scattering

2021

We consider the contribution of scalar resonances to hadronic light-by-light scattering in the anomalous magnetic moment of the muon. While the $f_0(500)$ has already been addressed in previous work using dispersion relations, heavier scalar resonances have only been estimated in hadronic models so far. Here, we compare an implementation of the $f_0(980)$ resonance in terms of the coupled-channel $S$-waves for $\gamma^*\gamma^*\to \pi\pi/\bar K K$ to a narrow-width approximation, which indicates $a_\mu^{\text{HLbL}}[f_0(980)]=-0.2(2)\times 10^{-11}$. With a similar estimate for the $a_0(980)$, the combined effect is thus well below $1\times 10^{-11}$ in absolute value. We also estimate the …

Nuclear and High Energy PhysicsParticle physicsNuclear Theory530 PhysicsQC1-999Scalar (mathematics)HadronFOS: Physical sciencesAbsolute value01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Dispersion relation0103 physical sciences010306 general physicsPhysicsMuonAnomalous magnetic dipole moment010308 nuclear & particles physicsScatteringPhysicsHigh Energy Physics - Lattice (hep-lat)ResonanceHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentPhysics Letters B
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Neutrino-nucleus quasi-elastic and 2p2h interactions up to 10 GeV

2013

We extend to 10 GeV results from a microscopic calculation of charged-current neutrino-nucleus reactions that do not produce a pion in the final state. For the class of events coming from neutrino interactions with two nucleons producing two holes (2p2h), limiting the calculation to three-momentum transfers less than 1.2 GeV produces a two-dimensional distribution in momentum and energy transfer that is roughly constant as a function of energy. The cross section for 2p2h interactions approximately scales with the number of nucleons for isoscalar nuclei, similar to the quasi-elastic cross section. When limited to momentum transfers below 1.2 GeV, the cross section is 26% of the quasi-elastic…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryIsoscalarFOS: Physical sciences01 natural sciences7. Clean energyScatteringNuclear Theory (nucl-th)Nuclear physicsMomentumCross section (physics)High Energy Physics - Phenomenology (hep-ph)Pion0103 physical sciencesNuclear Experiment010306 general physicsNeutrino oscillationPhysicsMeson-exchange currents010308 nuclear & particles physicsMomentum transferHigh Energy Physics - PhenomenologyFísica nuclearHigh Energy Physics::ExperimentNeutrinoNucleonPhysical Review D
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Charm and Hidden Charm Scalar Resonances in Nuclear Matter

2009

18th Particles and Nuclei International Conference (PANIC08). Eilat, ISRAEL, NOV 09-14, 2008

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryMesonD(s0)(2317)Nuclear TheoryFOS: Physical sciencesD(2400)Nuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)medicineNuclear ExperimentNuclear theoryPhysicsHyperonScalar (physics)FísicaNuclear matterX(3700)Charmed baryonsHigh Energy Physics - Phenomenologymedicine.anatomical_structureDynamically-generated resonanceScalar mesonsMESON RESONANCESscalar mesonsD-s0(2317)dynamically-generated resonanceNucleonNucleus
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Strangeness and charm in nuclear matter

2012

The properties of strange (K, (K) over bar and (K) over bar*) and open-charm (D, (D) over bar and D*) mesons in dense matter are studied using a unitary approach in coupled channels for meson-baryon scattering. In the strangeness sector, the interaction with nucleons always comes through vector-meson exchange, which is evaluated by chiral and hidden gauge Lagrangians. For the interaction of charmed mesons with nucleons we extend the SU(3) Weinberg-Tomozawa Lagrangian to incorporate spin-flavor symmetry and implement a suitable flavor symmetry breaking. The in-medium solution for the scattering amplitude accounts for Pauli blocking effects and meson self-energies. On one hand, we obtain the …

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesStrangeness01 natural sciences7. Clean energyNuclear Theory (nucl-th)Nuclear physicsStrange mesonsTransparency ratioHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesVector mesonSymmetry breakingNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDynamically-generated baryon resonancesFísicaNuclear matterOpen charm in matterPseudoscalarBaryonD-mesic nucleiHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNucleon
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Probing Novel Scalar and Tensor Interactions from (Ultra)Cold Neutrons to the LHC

2012

Scalar and tensor interactions were once competitors to the now well-established V-A structure of the Standard Model weak interactions. We revisit these interactions and survey constraints from low-energy probes (neutron, nuclear, and pion decays) as well as collider searches. Currently, the most stringent limit on scalar and tensor interactions arise from 0+ -> 0+ nuclear decays and the radiative pion decay pi -> e nu gamma, respectively. For the future, we find that upcoming neutron beta decay and LHC measurements will compete in setting the most stringent bounds. For neutron beta decay, we demonstrate the importance of lattice computations of the neutron-to-proton matrix elements t…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryLattice field theoryFOS: Physical sciences01 natural sciencesNuclear physicsNuclear Theory (nucl-th)PionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesRadiative transferNeutronNuclear Experiment010306 general physicsCharged currentPhysicsLarge Hadron ColliderMissing energy010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Scalar (physics)High Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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