Search results for "Quark"

showing 10 items of 2905 documents

Meson-Baryon s-wave Resonances with Strangeness -3

2006

Starting from a consistent SU(6) extension of the Weinberg-Tomozawa (WT) meson-baryon chiral Lagrangian (Phys. Rev. D74 (2006) 034025), we study the s-wave meson-baryon resonances in the strangeness S=-3 and negative parity sector. Those resonances are generated by solving the Bethe-Salpeter equation with the WT interaction used as kernel. The considered mesons are those of the 35-SU(6)-plet, which includes the pseudoscalar (PS) octet of pions and the vector (V) nonet of the rho meson. For baryons we consider the 56-SU(6)-plet, made of the 1/2+ octet of the nucleon and the 3/2+ decuplet of the Delta. Quantum numbers I(J^P)=0(3/2^-) are suggested for the experimental resonances Omega*(2250)-…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsRho mesonMesonNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFísicaFOS: Physical sciencesStrangenessPentaquarkBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNucleonNuclear Experiment
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Quarkonium spectral functions with complex potential

2011

Abstract We study quarkonium spectral functions at high temperatures using a potential model with complex potential. The real part of the potential is constrained by the lattice QCD data on static quark anti-quark correlation functions, while the imaginary part of the potential is taken from perturbative calculations. We find that the imaginary part of the potential has significant effect on quarkonium spectral functions, in particular, it leads to the dissolution of the 1S charmonium and excited bottomonium states at temperatures about 250 MeV and melting of the ground state bottomonium at temperatures slightly above 450 MeV.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsSpectral representationHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryLattice QCDQuarkoniumCorrelation function (statistical mechanics)Excited stateHigh Energy Physics::ExperimentGround stateNuclear Physics A
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Spontaneous CP violation and Non-Abelian Family Symmetry in SUSY

2004

We analyse the properties of generic models based on an SU(3) family symmetry providing a full description of quark charged lepton and neutrino masses and mixing angles. We show that a precise fit of the resulting fermion textures is consistent with CP being spontaneously broken in the flavour sector. The CP violating phases are determined by the scalar potential and we discuss how symmetries readily lead to a maximal phase controlling CP violation in the quark sector. In a specific model the CP violation to be expected in the neutrino sector is related to that in the quark sector and we determine this relation for two viable models. In addition to giving rise to the observed structure of q…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsSpontaneous symmetry breakingHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesSupersymmetrySupersymmetry breakingBottom quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics::ExperimentNeutrinoParticle Physics - Phenomenology
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HighpThadrons as probes of the central region of Au-Au collisions atSNN=200GeV

2006

The energy loss of high ${p}_{T}$ partons propagating through a hot and dense medium is regarded as a valuable tool to probe the medium created in ultrarelativistic heavy-ion collisions. The angular correlation pattern of hadrons associated with a hard trigger in the region of ${p}_{T}~1\text{\ensuremath{-}}2$ GeV which exhibits a dip in the expected position of the away side jet has given rise to the idea that energy is lost predominantly to propagating collective modes (`Mach cones'). Recent measurements by the STAR Collaboration have shown that for a high ${p}_{T}g8$ GeV trigger the angular pattern of associate hadrons for ${p}_{T}g4$ GeV shows the emergence of the expected away side pea…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsStar (game theory)HadronPartonJet (particle physics)GluonNuclear physicsQuark–gluon plasmaHigh Energy Physics::ExperimentNuclear ExperimentEnergy (signal processing)Physical Review C
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Perturbative quark mass corrections to the tau hadronic width

1998

15 páginas, 3 figuras, 2 tablas.-- arXiv:hep-ph/9804462v1

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsStrange quarkNLO computationsSeries (mathematics)High Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesOrder (ring theory)FísicaQCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::Experiment
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Measurement of the t-channel single top quark production cross section

2009

The D0 collaboration reports direct evidence for electroweak production of single top quarks through the t-channel exchange of a virtual W boson. This is the first analysis to isolate an individual single top quark production channel. We select events containing an isolated electron or muon, missing transverse energy, and two, three or four jets from 2.3 fb^-1 of ppbar collisions at the Fermilab Tevatron Collider. One or two of the jets are identified as containing a b hadron. We combine three multivariate techniques optimized for the t-channel process to measure the t- and s-channel cross sections simultaneously. We measure cross sections of 3.14 +0.94 -0.80 pb for the t-channel and 1.05 +…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsTop quark010308 nuclear & particles physicsHadronElectroweak interactionTevatronFOS: Physical sciences01 natural scienceslaw.inventionStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciencesExperimental High Energy Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysics Letters B
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Resummation prediction on top quark transverse momentum distribution at largepT

2012

We study the factorization and resummation of t-channel top quark transverse momentum distribution at large pT in the SM at both the Tevatron and the LHC with soft-collinear effective theory. The cross section in the threshold region can be factorized into a convolution of hard, jet and soft functions. In particular, we first calculate the NLO soft functions for this process, and give a RG improved cross section by evolving the different functions to a common scale. Our results show that the resummation effects increase the NLO results by about 9%-13% and 4%-9% when the top quark pT is larger than 50 and 70 GeV at the Tevatron and the 8 TeV LHC, respectively. Also, we discuss the scale inde…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsTop quarkHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyElectroweak interactionTevatronFOS: Physical sciencesRenormalization groupNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Soft-collinear effective theoryHigh Energy Physics::ExperimentSymmetry breakingResummationPhysical Review D
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Measurement of the top quark mass andpp¯→tt¯cross section in the all-hadronic mode with the CDF II detector

2010

We present a measurement of the top quark mass and of the top-antitop pair production cross section using p-pbar data collected with the CDFII detector at the Tevatron Collider at the Fermi National Accelerator Laboratory and corresponding to an integrated luminosity of 2.9 fb-1. We select events with six or more jets satisfying a number of kinematical requirements imposed by means of a neural network algorithm. At least one of these jets must originate from a b quark, as identified by the reconstruction of a secondary vertex inside the jet. The mass measurement is based on a likelihood fit incorporating reconstructed mass distributions representative of signal and background, where the abs…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsTop quarkMass distribution010308 nuclear & particles physicsHadronTevatron01 natural sciencesBottom quarkNuclear physicsPair production0103 physical sciencesMass spectrumHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Search for pair production of the scalar top quark in the electron-muon final state

2010

We report the result of a search for the pair production of the lightest supersymmetric partner of the top quark ($\tilde{t}_1$) in $p\bar{p}$ collisions at a center-of-mass energy of 1.96 TeV at the Fermilab Tevatron collider corresponding to an integrated luminosity of 5.4 fb$^{-1}$. The scalar top quarks are assumed to decay into a $b$ quark, a charged lepton, and a scalar neutrino ($\tilde{\nu}$), and the search is performed in the electron plus muon final state. No significant excess of events above the standard model prediction is detected, and improved exclusion limits at the 95% C.L. are set in the the ($M_{\tilde{t}_1}$,$M_{\tilde{\nu}}$) mass plane.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsTop quarkMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciences01 natural sciences7. Clean energyStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pair production0103 physical sciencesExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentNeutrino010306 general physicsLepton
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Three-body final state interaction in η→ 3π updated

2017

In view of the recent high-statistic KLOE data for the η→π+π−π0 decay, a new determination of the quark mass double ratio has been done. Our approach relies on a dispersive model that takes into account rescattering effects between three pions via subenergy unitarity. The latter is essential to reproduce the Dalitz plot distribution. A simultaneous description of the KLOE and WASA-at-COSY data is achieved in terms of just two real parameters. From a global fit, we determine Q=21.6±1.1. The predicted slope parameter for the neutral channel α=−0.025±0.004 is in reasonable agreement with the PDG average value.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsUnitarity010308 nuclear & particles physicsDalitz plotValue (computer science)State (functional analysis)01 natural scienceslcsh:QC1-999Nuclear physicsPionDistribution (mathematics)0103 physical sciences010306 general physicsDispersion (water waves)lcsh:PhysicsPhysics Letters B
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