0000000000318436

AUTHOR

P Teixeira Dias

showing 9 related works from this author

Search for anomaly-mediated supersymmetry breaking with the ATLAS detector based on a disappearing-track signature in $pp$ collisions at $\sqrt{s}=7$…

2012

In models of anomaly-mediated supersymmetry breaking (AMSB), the lightest chargino is predicted to have a lifetime long enough to be detected in collider experiments. This letter explores AMSB scenarios in pp collisions at s√=7 TeV by attempting to identify decaying charginos which result in tracks that appear to have few associated hits in the outer region of the tracking system. The search was based on data corresponding to an integrated luminosity of 1.02 fb[superscript −1] collected with the ATLAS detector in 2011. The pT spectrum of candidate tracks is found to be consistent with the expectation from Standard Model background processes and constraints on the lifetime and the production…

Physics and Astronomy (miscellaneous)01 natural sciencesmediation: anomasymmetry breaking [supersymmetry]MASS-DEGENERATElaw.inventionHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Charginolawscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]GENERATORSanoma [mediation]supersymmetry: symmetry breakingDetectors de radiacióPhysicsddc:539Luminosity (scattering theory)PIONSSettore FIS/01 - Fisica SperimentaleSUPERGAUGE TRANSFORMATIONSATLASSupersymmetry breakingmedicine.anatomical_structurePhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCParticle Physics - ExperimentParticle physicsp p: scatteringCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Standard ModelCHARGINOSNuclear physicsPionAtlas (anatomy)0103 physical sciencesmedicineFysikddc:530High Energy Physics010306 general physicsColliderEngineering (miscellaneous)Science & Technology010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaATLAS detector; anomaly-mediated supersymmetry breakingMODELCol·lisions (Física nuclear)Experimental High Energy PhysicsHigh Energy Physics::ExperimentAnomaly (physics)
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Measurement of Ab_FB using inclusive b-hadron decays

2001

Based on a sample of four million events collected by ALEPH from 1991 to 1995, a measurement of the forward-backward asymmetry in Z -> b-barb decays using inclusive final states is presented. High-performance tagging of b-barb events in a wide angular range is achieved using neural network techniques. An optimal hemisphere charge estimator is built by merging primary and secondary vertex information, leading kaon identification and jet charge in a neural network. The average charge asymmetry, the flavour tagging efficiencies and mean b-hemisphere charges are measured from data and used to extract the pole b asymmetry in the Standard Model A^{0,b}_{FB} = 0.1009 +- 0.0027 (stat) +- 0.0015 …

PhysicsParticle physicsAlephPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsmedia_common.quotation_subjectHadronEstimatorFOS: Physical sciencesCharge (physics)Jet (particle physics)01 natural sciencesAsymmetryVertex (geometry)Standard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsEngineering (miscellaneous)Particle Physics - Experimentmedia_common
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Searches for rare or forbidden semileptonic charm decays

2011

We present searches for rare or forbidden charm decays of the form $X_c^+\to h^\pm\ell^\mp\ell^{(\prime)+}$, where $X_c^+$ is a charm hadron ($D^+$, $D^+_s$, or $\Lambda_c^+$), $h^\pm$ is a pion, kaon, or proton, and $\ell^{(\prime)\pm}$ is an electron or muon. The analysis is based on $384 fb^{-1}$ of $e^+e^-$ annihilation data collected at or close to the $\Upsilon(4S)$ resonance with the BaBar detector at the SLAC National Accelerator Laboratory. No significant signal is observed for any of the 35 decay modes that are investigated. We establish 90% confidence-level upper limits on the branching fractions between $1 \times 10^{-6}$ and $44 \times 10^{-6}$ depending on the channel. In most…

Semileptonic decayNuclear and High Energy PhysicsParticle physicsforbiddenMesonElectron–positron annihilationFOS: Physical sciencessemileptonic charm decays01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decayPion0103 physical sciencessemileptonic[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment010306 general physicsPhysicsMuon010308 nuclear & particles physicsBranching fractionParticle physicsBABAR detectorrareHEPcharm decays3. Good healthCharmed baryonsBaBarPACS: 11.30.Fs 11.30.Hv 13.20.Fc 13.30.CeHigh Energy Physics::Experimentrare; forbidden; semileptonic; charm decaysFísica de partículesExperiments
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Study of radiative bottomonium transitions using converted photons

2011

We use 111+/-1 million Upsilon(3S) and 89+/-1 million Upsilon(2S) events recorded by the BaBar detector at the PEP-II B-factory at SLAC to perform a study of radiative transitions between bottomonium states using photons that have been converted to e+e- pairs by the detector material. We observe Upsilon(3S) -> gamma chi_b0,2(1P) decay, make precise measurements of the branching fractions for chi_b1,2(1P,2P) -> gamma Upsilon(1S) and chi_b1,2(2P) -> gamma Upsilon(2S) decays, and search for radiative decay to the eta_b(1S) and eta_b(2S) states.

Nuclear and High Energy PhysicsParticle physicsMesonElectron–positron annihilationHadronbottomoniumFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decayBaBar detector at SLAC; radiative bottomonium transitions0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Radiative transfer010306 general physicsPACS: 13.20.Gd 14.40.PqPhysics010308 nuclear & particles physicsBranching fractionParticle physicsQuarkoniumHEPconverted photons3. Good healthbottomonium; converted photonsPair productionradiative bottomonium transitionsBaBarBaBar detector at SLACFísica de partículesExperimentsPhysical Review D
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Test of Colour Reconnection Models using Three-Jet Events in Hadronic Z Decays

2006

Hadronic Z decays into three jets are used to test QCD models of colour reconnection (CR). A sensitive quantity is the rate of gluon jets with a gap in the particle rapidity distribution and zero jet charge. Gluon jets are identified by either energy-ordering or by tagging two b-jets. The rates predicted by two string-based tunable CR models, one implemented in JETSET (the GAL model), the other in ARIADNE, are too high and disfavoured by the data, whereas the rates from the corresponding non-CR standard versions of these generators are too low. The data can be described by the GAL model assuming a small value for the R_0 parameter in the range 0.01-0.02.

Particle physicsPhysics and Astronomy (miscellaneous)Electron–positron annihilationAstrophysics::High Energy Astrophysical PhenomenaANNIHILATIONSW-BOSONFOS: Physical sciencesElementary particleJet (particle physics)MASS01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decaySEARCH0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Rapidity010306 general physicsParton showerEngineering (miscellaneous)PhysicsQuantum chromodynamics010308 nuclear & particles physicsLEPQCDGLUON JETSGluonQUARK JETSHigh Energy Physics::ExperimentFRAGMENTATIONParticle Physics - ExperimentGENERATION
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Studies of the performance of the ATLAS detector using cosmic-ray muons

2011

Muons from cosmic-ray interactions in the atmosphere provide a high-statistics source of particles that can be used to study the performance and calibration of the ATLAS detector. Cosmic-ray muons can penetrate to the cavern and deposit energy in all detector subsystems. Such events have played an important role in the commissioning of the detector since the start of the installation phase in 2005 and were particularly important for understanding the detector performance in the time prior to the arrival of the first LHC beams. Global cosmic-ray runs were undertaken in both 2008 and 2009 and these data have been used through to the early phases of collision data-taking as a tool for calibrat…

:Mathematics and natural science: 400::Physics: 430 [VDP]ATLAS detector; cosmic-ray muonsPhysics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and Detectors:Mathematics and natural science: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]Tracking (particle physics)01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Naturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesPhysicsLarge Hadron ColliderDetectorSettore FIS/01 - Fisica SperimentaleInstrumentation and Detectors (physics.ins-det)ATLASRadiación cósmicamedicine.anatomical_structureComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCNatural SciencesCiências Naturais::Ciências FísicasInstrumentationAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesmedicineCalibrationddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Aerospace engineering010306 general physicsEngineering (miscellaneous)Ciencias ExactasEvent generatorCalorimeterScience & TechnologyCalorimeter (particle physics)ATLAS detectorbusiness.industry010308 nuclear & particles physicsPhysics and Astronomy (miscellaneous); Engineering (miscellaneous)FísicaExperimental High Energy PhysicsHigh Energy Physics::Experimentbusiness
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Measurement of the W boson Mass and Width in $e^{+}e^{-}$ Collisions at LEP

2006

The mass of the W boson is determined from the direct reconstruction of W decays in WW→qq̄qq̄ and WW→ℓνqq̄ events in e+e- collisions at LEP. The data sample corresponds to an integrated luminosity of 683 pb-1 collected with the ALEPH detector at centre-of-mass energies up to 209 GeV. To minimise any effect from colour reconnection a new procedure is adopted in which low energy particles are not considered in the mass determination from the qq̄qq̄ channel. The combined result from all channels is mW=80.440±0.043(stat.)±0.024(syst.)±0.009(FSI)±0.009(LEP)GeV/c2,where FSI represents the possible effects of final state interactions in the qq̄qq̄ channel and LEP indicates the uncertainty in the b…

Particle physicsPhysics and Astronomy (miscellaneous)Electron–positron annihilationFOS: Physical sciencesElementary particle01 natural sciencesSystematic UncertaintyHigh Energy Physics - ExperimentNuclear physicsParticle decayHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massInvariant Mass010306 general physicsNuclear ExperimentEngineering (miscellaneous)Monte CarloBosonPhysicsMuonAnnihilation010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPair productionBoson MassTime Projection ChamberHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsParticle Physics - Experiment
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Measurement of the Michel parameters and the nu(tau) helicity in tau lepton decays

2001

A measurement of the Michel parameters and the average $\nu_\tau$ helicity in $\tau$ lepton decays is described. The data was collected with the ALEPH detector at LEP during the years 1991 to 1995. A total integrated luminosity of 155\,$\text{pb}^{-1}$ is analysed. The Michel parameters $\rho_l$, $\xi_l$, $(\xi\delta)_l$ ($l=e,\mu$), and $\eta_\mu$ are determined for the leptonic deca ys, and the chirality parameters $\xi_\pi$, $\xi_\rho$, and $\xi_{a_1}$ for the hadronic final states. Under the assumptions of $e$\bis $\mu$ universality and $\xi_\pi=\xi_\rho=\xi_{a_1}$, the values $\rho_l=0.742\pm 0.016, \eta_l=0.01 2\pm 0.026,\break (\xi\delta)_l=0.776\pm 0.051, \xi_l=0.986\pm 0.074$, and …

PhysicsParticle physics[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]Physics and Astronomy (miscellaneous)010308 nuclear & particles physicsElectron–positron annihilationHadronParity (physics)Weak interaction01 natural sciencesHelicity0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Michel parametersHigh Energy Physics::Experiment010306 general physicsEngineering (miscellaneous)Particle Physics - ExperimentLepton
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Performance of the ATLAS detector using first collision data

2010

More than half a million minimum-bias events of LHC collision data were collected by the ATLAS experiment in December 2009 at centre-of-mass energies of 0.9 TeV and 2.36 TeV. This paper reports on studies of the initial performance of the ATLAS detector from these data. Comparisons between data and Monte Carlo predictions are shown for distributions of several track- and calorimeter-based quantities. The good performance of the ATLAS detector in these first data gives confidence for successful running at higher energies.

Nuclear and High Energy PhysicsParticle physicsAtlas detectorPhysics::Instrumentation and DetectorsMonte Carlo methodFOS: Physical sciencesddc:500.253001 natural sciences7. Clean energySettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)LHC ; ATLAS ; Minimum-bias ; 900 GeV ; 2.36 TeV ; PerformanceAtlas (anatomy)0103 physical sciencesmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy PhysicsDetectors and Experimental Techniques010306 general physicsCiencias ExactasDetectors de radiacióPhysicsHadron-Hadron ScatteringLarge Hadron Collider010308 nuclear & particles physicsATLAS DetectorSettore FIS/01 - Fisica SperimentaleATLAS experimentFísicaATLASCollisionmedicine.anatomical_structureExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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