Search results for "Particle physics"

showing 10 items of 6826 documents

THE POSSIBLE DI-OMEGA DIBARYON IN QUARK CLUSTER MODEL

2014

The mixing of scalar mesons is introduced into the baryon-baryon system in the chiral SU(3) quark model to further dynamically investigate the Di-omega state by using the same parameters as those in reasonably describing the experimental hyperon-nucleon and nucleon-nucleon scattering data. Two different mixings of scalar mesons, the ideal mixing and 19° mixing, are discussed, and compared with no mixing. The results show that it is still deeply bound state if 19° mixing is adopted, the same as those of no mixing. However, for ideal mixing, the binding energy is reduced quite a lot, yet it is still a bound state.

QuarkPhysicsParticle physicsMesonHigh Energy Physics::PhenomenologyNuclear TheoryBinding energyBound stateQuark modelScalar (physics)Few-body systemsNuclear ExperimentOmegaInternational Journal of Modern Physics: Conference Series
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Exotic dynamically generated baryons with C=-1

2010

We follow a model based on the SU(8) symmetry for the interaction of mesons with baryons. The model treats on an equal footing the pseudo-scalars and the vector mesons, as required by heavy quark symmetry. The T-matrix calculated within an unitary scheme in coupled channels has poles which are interpreted as baryonic resonances.

QuarkPhysicsParticle physicsMesonNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particleSymmetry group01 natural sciencesSymmetry (physics)BaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsNuclear ExperimentS-matrix
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Electron and muon $g-2$ anomalies in general flavour conserving two Higgs doublets models

2020

In general two Higgs doublet models (2HDMs) without scalar flavour changing neutral couplings (SFCNC) in the lepton sector, the electron, muon and tau interactions can be decoupled in a robust framework, stable under renormalization group evolution. In this framework, the breaking of lepton flavour universality (LFU) goes beyond the mass proportionality, opening the possibility to accommodate a different behaviour among charged leptons. We analyze the electron and muon $(g-2)$ anomalies in the context of these general flavour conserving models in the leptonic sector (g$\ell$FC). We consider two different models, I-g$\ell$FC and II-g$\ell$FC, in which the quark Yukawa couplings coincide, res…

QuarkPhysicsParticle physicsMuon010308 nuclear & particles physicsElectroweak interactionScalar (mathematics)High Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesComputer Science::Digital Libraries01 natural sciencesHigh Energy Physics - Experiment3. Good healthPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLepton
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Lattice calculation of the hadronic leading order contribution to the muon g − 2

2019

The European physical journal / Web of Conferences Web of Conferences : proceedings proceedings 234, 01016 - (2020). doi:10.1051/epjconf/202023401016

QuarkPhysicsParticle physicsMuonAnomalous magnetic dipole momentComputer Science::Information RetrievalPhysics beyond the Standard ModelHigh Energy Physics::LatticePhysicsQC1-999High Energy Physics - Lattice (hep-lat)HadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDLattice QCD530Standard deviationHigh Energy Physics - LatticeLattice (order)ddc:530High Energy Physics::ExperimentEPJ Web of Conferences
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Search for New Phenomena in Final States with Two Leptons and One or No b -Tagged Jets at s=13  TeV Using the ATLAS Detector

2021

A search for new phenomena is presented in final states with two leptons and one or no $b$-tagged jets. The event selection requires the two leptons to have opposite charge, the same flavor (electrons or muons), and a large invariant mass. The analysis is based on the full Run-2 proton-proton collision dataset recorded at a center-of-mass energy of $\sqrt{s} = 13$ TeV by the ATLAS experiment at the LHC, corresponding to an integrated luminosity of 139 fb$^{-1}$. No significant deviation from the expected background is observed in the data. A four-fermion contact interaction between two quarks ($b,s$) and two leptons ($ee$ or $\mu\mu$), inspired by the $B$-meson decay anomalies, is used as a…

QuarkPhysicsParticle physicsMuonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyATLAS experimentGeneral Physics and AstronomyLambdaCoupling (probability)7. Clean energy01 natural sciences0103 physical sciencesHigh Energy Physics::ExperimentInvariant mass010306 general physicsLeptonPhysical Review Letters
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Spin on same-sign W -boson pair production

2019

We demonstrate that the LHC will be sensitive to quantum correlations between two quarks inside the proton. Same-sign W-boson pair production is the most promising channel for clear measurements of double parton scattering. The left-handed nature of the coupling between quarks and W-bosons makes it a prime probe to measure parton spin correlations. We perform a detailed analysis of double parton scattering, including relevant backgrounds. The analysis reveals that measurements comparing the rate at which two muons from W boson decays are produced in the same compared to opposite hemispheres are especially sensitive to spin correlations between two quarks inside the proton. We provide estima…

QuarkPhysicsParticle physicsMuonLarge Hadron ColliderProton010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFOS: Physical sciencesParton01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Pair production0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsSpin-½Physical Review D
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Lattice calculation of the pion transition form factor $\pi^0 \to \gamma^* \gamma^*$

2016

We calculate the $\pi^0\to \gamma^*\gamma^*$ transition form factor ${\cal F}_{\pi^0\gamma^*\gamma^*}(q_1^2,q_2^2)$ in lattice QCD with two flavors of quarks. Our main motivation is to provide the input to calculate the $\pi^0$-pole contribution to hadronic light-by-light scattering in the muon $(g-2)$, $a_\mu^{\rm HLbL;\pi^0}$. We therefore focus on the region where both photons are spacelike up to virtualities of about $1.5~$GeV$^2$, which has so far not been experimentally accessible. Results are obtained in the continuum at the physical pion mass by a combined extrapolation. We reproduce the prediction of the chiral anomaly for real photons with an accuracy of about $8-9\%$. We also com…

QuarkPhysicsParticle physicsMuonPhotonHigh Energy Physics::LatticeNuclear TheoryDegenerate energy levelsHadronLattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticePionLattice (order)High Energy Physics::ExperimentNuclear ExperimentProceedings of 34th annual International Symposium on Lattice Field Theory — PoS(LATTICE2016)
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Dipole operator constraints on composite Higgs models

2014

Flavour- and CP-violating electromagnetic or chromomagnetic dipole operators in the quark sector are generated in a large class of new physics models and are strongly constrained by measurements of the neutron electric dipole moment and observables sensitive to flavour-changing neutral currents, such as the $B\to X_s\gamma$ branching ratio and $\epsilon'/\epsilon$. After a model-independent discussion of the relevant constraints, we analyze these effects in models with partial compositeness, where the quarks get their masses by mixing with vector-like composite fermions. These scenarios can be seen as the low-energy limit of composite Higgs or warped extra dimensional models. We study diffe…

QuarkPhysicsParticle physicsNeutron electric dipole momentPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelHigh Energy Physics::LatticeFlavourElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesddc:DipoleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Composite Higgs modelsHiggs bosonHigh Energy Physics::ExperimentRegular Article - Theoretical PhysicsEngineering (miscellaneous)The European Physical Journal C
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The effect of hyperfine mixing in electromagnetic and semileptonic decays of doubly heavy baryons

2010

We consider the role played by hyperfine mixing in electromagnetic and semileptonic decays of doubly heavy baryons, which give rise to large corrections to the decay widths in both cases.

QuarkPhysicsParticle physicsNuclear TheoryHadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particleFermionBaryonNuclear Theory (nucl-th)Particle decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNuclear ExperimentHyperfine structureMixing (physics)
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Dipole model at Next-to-Leading Order meets HERA data

2021

Deep inelastic scattering (DIS) total cross section data at small-x as measured by the HERA experiments is well described by Balitsky-Kovchegov (BK) evolution in the leading order dipole picture. Recently the full Next-to-Leading Order (NLO) dipole picture total cross sections have become available for DIS, and a working factorization scheme has been devised which subtracts the soft gluon divergence present at NLO. We report our recently published work in which we make the first comparisons of the NLO DIS total cross sections to HERA data. The non-perturbative initial condition to BK evolution is fixed by fitting the HERA reduced cross section data. As the NLO results for the DIS total cros…

QuarkPhysicsParticle physicsNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesHERAhiukkasfysiikkaDeep inelastic scattering7. Clean energy114 Physical sciencesGluonMassless particleNuclear Theory (nucl-th)Cross section (physics)DipoleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationsirontaHigh Energy Physics::Experiment
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