0000000001315153

AUTHOR

A. Pal

showing 187 related works from this author

Combination of searches for anomalous top quark couplings with 5.4 fb−1 of pp¯ collisions

2012

We present measurements of the tWb coupling form factors using information from electroweak single top quark production and from the helicity of W bosons from top quark decays in t (t) over bar events. We set upper limits on anomalous tWb coupling form factors using data collected with the DO detector at the Tevatron p (p) over bar collider corresponding to an integrated luminosity of 5.4 fb(-1).

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionTevatronTop quark condensate01 natural sciencesHelicitylaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsColliderBosonPhysics Letters B
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Search for a Fermiophobic and Standard Model Higgs Boson in Diphoton Final States

2011

Made available in DSpace on 2022-04-29T01:13:49Z (GMT). No. of bitstreams: 0 Previous issue date: 2011-10-05 National Science Foundation We present a search for the standard model Higgs boson and a fermiophobic Higgs boson in the diphoton final states based on 8.2fb-1 of pp̄ collisions at √s=1.96TeV collected with the D0 detector at the Fermilab Tevatron Collider. No excess of data above background predictions is observed and upper limits at the 95% C.L. on the cross section multiplied by the branching fraction are set which are the most restrictive to date. A fermiophobic Higgs boson with a mass below 112.9 GeV is excluded at the 95% C.L. © 2011 American Physical Society. Universidad de Bu…

PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyElementary particle01 natural sciences7. Clean energyStandard Modellaw.inventionNuclear physicslawExperimental High Energy Physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Higgs bosonGrand Unified TheoryHigh Energy Physics::ExperimentFermilab010306 general physicsColliderGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)BosonPhysical Review Letters
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Performance of jet substructure techniques for large-$R$ jets in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector

2013

This paper presents the application of a variety of techniques to study jet substructure. The performance of various modified jet algorithms, or jet grooming techniques, for several jet types and event topologies is investigated for jets with transverse momentum larger than 300 GeV. Properties of jets subjected to the mass-drop filtering, trimming, and pruning algorithms are found to have a reduced sensitivity to multiple proton-proton interactions, are more stable at high luminosity and improve the physics potential of searches for heavy boosted objects. Studies of the expected discrimination power of jet mass and jet substructure observables in searches for new physics are also presented.…

Ciencias FísicasPhysics beyond the Standard ModelHadronMonte Carlo method01 natural sciencesHigh Energy Physics - Experiment//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)Jets[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massNuclear ExperimentHADRONIC JEThadron-hadron scatteringQCPhysicsLarge Hadron ColliderAtlas (topology)Settore FIS/01 - Fisica SperimentaleObservableATLASPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGproton–proton collisionLHCCIENCIAS NATURALES Y EXACTASParticle Physics - ExperimentParticle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências Físicas530 PhysicsAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsCiencias ExactasScience & TechnologyHadron-Hadron ScatteringATLAS detector010308 nuclear & particles physicsFísica//purl.org/becyt/ford/1.3 [https]AstronomíaHADRON-HADRON COLLISIONSExperimental High Energy PhysicsSubstructureHigh Energy Physics::Experiment
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Measurement of the Effective Weak Mixing Angle inpp¯→Z/γ*→e+e−Events

2015

We present a measurement of the fundamental parameter of the standard model, the weak mixing angle, in $p\bar{p}\rightarrow Z/\gamma^{*}\rightarrow e^{+}e^{-}$ events at a center of mass energy of 1.96 TeV, using data corresponding to 9.7 fb$^{-1}$ of integrated luminosity collected by the D0 detector at the Fermilab Tevatron. The effective weak mixing angle is extracted from the forward-backward charge asymmetry as a function of the invariant mass around the Z boson pole. The measured value of $\sin^2\theta_{\text{eff}}^{\text{$\ell$}}=0.23146 \pm 0.00047$ is the most precise measurement from light quark interactions to date, with a precision close to the best LEP and SLD results.

PhysicsQuarkParticle physicsHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyCharge (physics)Weinberg angle7. Clean energyStandard ModelNuclear physicsHigh Energy Physics::ExperimentInvariant massCenter of massEnergy (signal processing)Physical Review Letters
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Search for the standard model Higgs boson in the ZH→νν¯bb¯ channel in 9.5 fb−1 of pp¯ collisions at s=1.96 TeV

2012

We present a search for the standard model Higgs boson in 9.5 fb-1 of ppbar collisions at sqrt(s) = 1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. The final state considered contains a pair of b jets and is characterized by an imbalance in transverse energy, as expected from ppbar->ZH->vvbb production. The search is also sensitive to the WH->lvbb channel when the charged lepton is not identified. The data are found to be in good agreement with the expected background. For a Higgs boson mass of 125 GeV, we set a limit at the 95% C.L. on the cross section sigma(ppbar->[Z/W]H), assuming standard model branching fractions, that is a factor of 4.3 times larger than th…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsB channelTevatronSigma01 natural sciencesStandard deviationNuclear physics0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentFermilab010306 general physicsLeptonPhysics Letters B
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Measurement of the charge asymmetry in top quark pair production in pp collisions at root s=7 TeV using the ATLAS detector

2012

A measurement of the top-antitop production charge asymmetry A[subscript C] is presented using data corresponding to an integrated luminosity of 1.04 fb[superscript −1] of pp collisions at s√=7 TeV collected by the ATLAS detector at the LHC. Events are selected with a single lepton (electron or muon), missing transverse momentum and at least four jets of which at least one jet is identified as coming from a b-quark. A kinematic fit is used to reconstruct the t[bar over t] event topology. After background subtraction, a Bayesian unfolding procedure is performed to correct for acceptance and detector effects. The measured value of A[subscript C] is A[subscript C]=−0.019±0.028 (stat.)±0.024 (s…

Top quarkPhysics and Astronomy (miscellaneous)01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massDetectors de radiacióPhysicsddc:539Luminosity (scattering theory)Large Hadron ColliderSettore FIS/01 - Fisica SperimentaleATLASmedicine.anatomical_structurePhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCParticle Physics - ExperimentParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysicsddc:500.2charge asymmetry; top quark pair production; pp collisions; ATLAS detectorComputer Science::Digital Libraries530Partícules (Física nuclear)Nuclear physicsAtlas (anatomy)0103 physical sciencesmedicineFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias Exactastop quarkAstrophysics::Galaxy AstrophysicsScience & TechnologyMuonATLAS detector010308 nuclear & particles physicsParton DistributionsFísicaPair productionHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Experimental High Energy Physicsproton-proton collisionsHigh Energy Physics::ExperimentLepton
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Measurement of directCPviolation parameters inB±→J/ψK±andB±→J/ψπ±decays with10.4  fb−1of Tevatron data

2013

We present a measurement of the direct CP-violating charge asymmetry in B-+/- mesons decaying to J/psi K-+/- and J/psi pi(+/-) where J/psi decays to mu(+)mu(-), using the full run II data set of 10.4 fb(-1) of proton-antiproton collisions collected using the D0 detector at the Fermilab Tevatron Collider. A difference in the yield of B- and B+ mesons in these decays is found by fitting to the difference between their reconstructed invariant mass distributions resulting in asymmetries of A(J/psi K) = [0.59 +/- 0.37]%, which is the most precise measurement to date, and A(J/psi pi) = [-4.2 +/- 4.5]%. Both measurements are consistent with standard model predictions.

PhysicsParticle physicsMeson010308 nuclear & particles physicsTevatronGeneral Physics and Astronomy01 natural sciencesStandard ModelJ/psi mesonNuclear physics0103 physical sciencesCP violationHigh Energy Physics::ExperimentB mesonInvariant massFermilab010306 general physicsPhysical Review Letters
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Measurement of theϕη*distribution of muon pairs with masses between 30 and 500 GeV in10.4  fb−1ofpp¯collisions

2015

We present a measurement of the distribution of the variable phi(eta)* for muon pairs with masses between 30 and 500 GeV, using the complete run II data set collected by the D0 detector at the Fermilab Tevatron proton-antiproton collider. This corresponds to an integrated luminosity of 10.4 fb(-1) at root s = 1.96 TeV. The data are corrected for detector effects and presented in bins of dimuon rapidity and mass. The variable phi(eta)* probes the same physical effects as the Z/gamma* boson transverse momentum, but is less susceptible to the effects of experimental resolution and efficiency. These are the first measurements at any collider of the phi(eta)* distributions for dilepton masses aw…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonHigh Energy Physics::PhenomenologyTevatronGluonlaw.inventionNuclear physicslawPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentRapidityFermilabResummationNuclear ExperimentColliderBosonPhysical Review D
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Search forWHassociated production inpp¯collisions ats=1.96  TeV

2012

This report describes a search for associated production of W and Higgs bosons based on data corresponding to an integrated luminosity of L approximate to 5.3 fb(-1) collected with the D0 detector at the Fermilab Tevatron p (p) over bar Collider. Events containing a W -> l nu candidate (with l corresponding to e or mu) are selected in association with two or three reconstructed jets. One or two of the jets are required to be consistent with having evolved from a b quark. A multivariate discriminant technique is used to improve the separation of signal and backgrounds. Expected and observed upper limits are obtained for the product of the WH production cross section and branching ratios and …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionTevatronParticle accelerator01 natural sciencesBottom quarklaw.inventionDiscriminantlaw0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentFermilab010306 general physicsBosonPhysical Review D
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Measurement of the top quark pair production cross-section with ATLAS in the single lepton channel

2012

A measurement of the production cross-section for top quark pairs (t[bar over t]) in pp collisions at √s = 7 TeV is presented using data recorded with the ATLAS detector at the Large Hadron Collider. Events are selected in the single lepton topology by requiring an electron or muon, large missing transverse momentum and at least three jets. With a data sample of 35 pb[superscript −1], two different multivariate methods, one of which uses b-quark jet identification while the other does not, use kinematic variables to obtain cross-section measurements of σ[subscript t bar over t] = 187 ± 11 (stat.) [+18 over −17] (syst.) ± 6 (lumi.) pb and σ[subscript t bar over t] = 173 ± 17 (stat.) [+18 ove…

high-energy collider experimentcross-sectionTop quarkPhysics::Instrumentation and DetectorsAtlas detectortop physicsHadronHigh-energy collider experimentElectron01 natural sciences7. Clean energySettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQCDetectors de radiacióPhysicsQuantum chromodynamicsAtlas (topology)Settore FIS/01 - Fisica SperimentaleATLASTop physicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsCross-sectionHigh-energy collider experiment; Cross-section; Top physicsCiências Naturais::Ciências Físicascross-section; high-energy collider experiment; top physics:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesTOP QUARK530Partícules (Física nuclear)Nuclear physics0103 physical sciencesddc:530High Energy Physics010306 general physicsScience & TechnologyPP COLLISIONS010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaPair productionHADRON-HADRON COLLISIONStop physics; high-energy collider experiment; cross-sectionCol·lisions (Física nuclear)Experimental High Energy PhysicsTEVHigh Energy Physics::ExperimentLepton
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A search for flavour changing neutral currents in top-quark decays in pp collision data collected with the ATLAS detector at root s=7 TeV

2012

A search for flavour changing neutral current (FCNC) processes in top-quark decays by the ATLAS Collaboration is presented. Data collected from pp collisions at the LHC at a centre-of-mass energy of √s = 7 TeV during 2011, corresponding to an integrated luminosity of 2.1 fb[superscript −1], were used. A search was performed for top-quark pair-production events, with one top quark decaying through the t → Zq FCNC (q = u, c) channel, and the other through the Standard Model dominant mode t → W b. Only the decays of the Z boson to charged leptons and leptonic W -boson decays were considered as signal. Consequently, the final-state topology is characterised by the presence of three isolated cha…

Top quarkFlavourHadron hadron scattering01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Hadron Hadron ScatteringQCDetectors de radiacióddc:539PhysicsLarge Hadron ColliderSettore FIS/01 - Fisica SperimentaleATLASTop PhysicsTop physicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCNeutrinoParticle Physics - ExperimentParticle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]Flavour Changing Neutral CurrentsFOS: Physical sciencesddc:500.2Hadron-hadron scattering530TOP QUARKPartícules (Física nuclear)0103 physical sciencesddc:530High Energy Physics010306 general physicsFlavour changing neutral currentsNeutral current010308 nuclear & particles physicsBranching fractionRare DecaysHigh Energy Physics::PhenomenologyFísicaRare decaysCollisionHadron Hadron Scattering; Top Physics; Rare Decays; Flavour Changing Neutral CurrentsFLAVOR CHANGING NEUTRAL CURRENTCol·lisions (Física nuclear)HADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentLepton
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Search for a fermiophobic Higgs boson in the diphoton decay channel with the ATLAS detector

2012

[Excerpt] A search for a fermiophobic Higgs boson using diphoton events produced in proton-proton collisions at a centre-of-mass energy of s√=7 TeV is performed using data corresponding to an integrated luminosity of 4.9 fb−1 collected by the ATLAS experiment at the Large Hadron Collider. A specific benchmark model is considered where all the fermion couplings to the Higgs boson are set to zero and the bosonic couplings are kept at the Standard Model values (fermiophobic Higgs model). The largest excess with respect to the background-only hypothesis is found at 125.5 GeV, with a local significance of 2.9 standard deviations, which reduces to 1.6 standard deviations when taking into account …

Physics and Astronomy (miscellaneous)Atlas detector7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Naturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]HADRON COLLIDERSNuclear ExperimentDetectors de radiacióddc:539PhysicsHIGGS BOSONPhysicsSettore FIS/01 - Fisica SperimentalePHYSICS PARTICLES & FIELDSATLASNuclear & Particles PhysicsTransverse momentumPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonFísica nuclearLHCNatural SciencesParticle Physics - ExperimentParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]STANDARD MODELFOS: Physical sciencesddc:500.2Partícules (Física nuclear)Nuclear physics0202 Atomic Molecular Nuclear Particle And Plasma Physics0103 physical sciencesddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)0206 Quantum PhysicsScience & Technology010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTRANSVERSE-MOMENTUMCol·lisions (Física nuclear)HADRON-HADRON COLLISIONSExperimental High Energy PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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Measurement of theWZandZZproduction cross sections using leptonic final states in8.6  fb−1ofpp¯collisions

2012

We study the processes p (p) over bar -> WZ -> l(+) vl(+) l(-) and p (p) over bar -> ZZ -> l(+) l(-) v (v) over bar, where l = e or mu. Using 8: 6 fb(-1) of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron collider, we measure the WZ production cross section to be 4.50(-0.66)(+0.63) pb which is consistent with, but slightly larger than, the prediction of the standard model. The ZZ cross section is measured to be 1: 64 +/- 0: 46 pb, in agreement with a prediction of the standard model. Combination with an earlier analysis of the ZZ -> l(+) l(-) l(+) l(-) channel yields a ZZ cross section of 1.44(-0.34)(+0.35) pb.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsTevatronD0 experiment01 natural scienceslaw.inventionLuminosityStandard Modellaw0103 physical sciencesProduction (computer science)Fermilab010306 general physicsColliderBar (unit)Physical Review D
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Measurement of three-jet differential cross sections dσ3jet/dM3jet in pp¯ collisions at s=1.96 TeV

2011

We present the first measurement of the inclusive three-jet differential cross section as a function of the invariant mass of the three jets with the largest transverse momenta in an event in p anti-p collisions at sqrt(s) = 1.96 TeV. The measurement is made in different rapidity regions and for different jet transverse momentum requirements and is based on a data set corresponding to an integrated luminosity of 0.7 fb^{-1} collected with the D0 detector at the Fermilab Tevatron Collider. The results are used to test the three-jet matrix elements in perturbative QCD calculations at next-to-leading order in the strong coupling constant. The data allow discrimination between parametrizations …

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaTevatronPerturbative QCDPartonJet (particle physics)7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentInvariant massRapidityNuclear Experiment010306 general physicsPhysics Letters B
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Measurement of the directCP-violating parameterACPin the decayD+→K−π+π+

2014

We measure the direct CP-violating parameter A_CP for the decay of the charged charm meson, D+ -> K-pi+pi+ (and charge conjugate), using the full 10.4 fb-1 sample of ppbar collisions at sqrt(s) = 1.96 TeV collected by the D0 detector at the Fermilab Tevatron collider. We extract the raw reconstructed charge asymmetry by fitting the invariant mass distributions for the sum and difference of charge-specific samples. This quantity is then corrected for detector-related asymmetries using data-driven methods and for possible physics asymmetries (from B -> D processes) using input from Monte Carlo simulation. We measure A_CP = [-0.16 +- 0.15 (stat.) +- 0.09 (syst.)]%, which is consistent with zer…

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsmedia_common.quotation_subjectMonte Carlo methodTevatron01 natural sciencesAsymmetryStandard ModelNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentInvariant massCharm (quantum number)Fermilab010306 general physicsmedia_commonPhysical Review D
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Measurement of the forward-backward asymmetry in the distribution of leptons intt¯events in thelepton+jetschannel

2014

We present measurements of the forward-backward asymmetry in the angular distribution of leptons from decays of top quarks and antiquarks produced in proton-antiproton collisions. We consider the final state containing a lepton and at least three jets. The entire sample of data collected by the D0 experiment during Run II of the Fermilab Tevatron Collider, corresponding to 9.7 inverse fb of integrated luminosity, is used. The asymmetry measured for reconstructed leptons is $A_{FB}^l = \big(2.9 \pm 2.1(stat.) ^{+1.5}_{-1.7}(syst.) \big)$%. When corrected for efficiency and resolution effects within the lepton rapidity coverage of $|y_l|<1.5$, the asymmetry is found to be $A_{FB}^l = \big(4.2…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsGenerator (category theory)media_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronInverse7. Clean energyAsymmetryNuclear physicsHigh Energy Physics::ExperimentRapidityNuclear ExperimentLeptonmedia_commonPhysical Review D
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Measurement of the Top Quark Mass Using the Matrix Element Technique in Dilepton Final States

2016

We present a measurement of the top quark mass in ppbar collisions at a center-of-mass energy of 1.96 TeV at the Fermilab Tevatron collider. The data were collected by the D0 experiment corresponding to an integrated luminosity of 9.7 fb-1. The matrix element technique is applied to ttbar events in the final state containing leptons (electrons or muons) with high transverse momenta and at least two jets. The calibration of the jet energy scale determined in the lepton + jets final state of ttbar decays is applied to jet energies. This correction provides a substantial reduction in systematic uncertainties. We obtain a top quark mass of mt = 173.93 +- 1.84 GeV.

Particle physicsTop quarkCOLLISIONSPAIR PRODUCTIONJET IDENTIFICATIONAstrophysics::High Energy Astrophysical PhenomenaTevatronFOS: Physical sciencesJet (particle physics)Astronomy & Astrophysics01 natural sciencesD0 EXPERIMENTlaw.inventionPhysics Particles & FieldsHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0202 Atomic Molecular Nuclear Particle And Plasma Physicslaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]HADRON COLLIDERSFermilabHigh Energy Physics010306 general physicsColliderRUN-IIDETECTOR0206 Quantum PhysicsPhysicsScience & Technology010308 nuclear & particles physicsPhysicsSEMILEPTONIC DECAYSHigh Energy Physics::PhenomenologyD0 experimentNuclear & Particles Physics0201 Astronomical And Space SciencesPair productionPhysical SciencesExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentCROSS-SECTIONLepton
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The ATLAS Simulation Infrastructure

2010

52 páginas, 10 figuras, 18 tablas.-- This article is distributed under the terms of the Creative Commons Attribution Noncommercial License.-- et al. (The ATLAS Collaboration).

LibraryPhysics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and Detectorscomputer.software_genre01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Statistical physicsDetectors and Experimental TechniquesSimulaciónphysics.ins-detDetectors de radiació/dk/atira/pure/subjectarea/asjc/2200/2201PhysicsLarge Hadron ColliderAtlas (topology)4. EducationAcceleradors de partículesATLAS experimentDetectorSettore FIS/01 - Fisica SperimentaleInstrumentation and Detectors (physics.ins-det)ATLASGridSimulation softwareTile CalorimeterPhysical SciencesMontecarlo simulationLHCReal-time computingFOS: Physical sciencesATLAS experimentddc:500.2530High-Energy Physics0103 physical sciencesFysikddc:530[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]High Energy PhysicsMonte-Carlo010306 general physicsPartonEngineering (miscellaneous)Ciencias ExactasGEANT4EventATLAS detector010308 nuclear & particles physicsFísicaATLAS experiment; Montecarlo simulation; LHCGrid computingInterfacingHigh Energy Physics::Experiment/dk/atira/pure/subjectarea/asjc/3100/3101computer
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Jet mass and substructure of inclusive jets in $ \sqrt {s} = 7\;{\text{TeV}} $ pp collisions with the ATLAS experiment

2012

Recent studies have highlighted the potential of jet substructure techniques to identify the hadronic decays of boosted heavy particles. These studies all rely upon the assumption that the internal substructure of jets generated by QCD radiation is well understood. In this article, this assumption is tested on an inclusive sample of jets recorded with the ATLAS detector in 2010, which corresponds to 35 pb-1 of pp collisions delivered by the LHC at √s = 7TeV. In a subsample of events with single pp collisions, measurements corrected for detector efficiency and resolution are presented with full systematic uncertainties. Jet invariant mass, kt splitting scales and N-subjettiness variables are…

jet algorithmsParticle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical PhenomenaHadronMonte Carlo method:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.201 natural sciences530Partícules (Física nuclear)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massddc:530High Energy Physics010306 general physicsGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Quantum chromodynamicsPhysicsddc:539Large Hadron ColliderHadron-Hadron ScatteringScience & Technology010308 nuclear & particles physicsAcceleradors de partículesATLAS experimentSettore FIS/01 - Fisica SperimentaleFísicaHERAATLASQCDHADRON-HADRON COLLISIONSExperimental High Energy PhysicsSubstructureproton-proton collisionsFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentJournal of High Energy Physics
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Search for associated Higgs boson production using like charge dilepton events inpp¯collisions ats=1.96  TeV

2011

We present a search for associated Higgs boson production in the process p (p) over bar -> W/ZH -> l(+/-)l'(+/-) + X in ee, e mu, and mu mu final states. The search is based on data collected by the D0 experiment at the Fermilab Tevatron Collider at root s = 1.96 TeV corresponding to 5.3 fb(-1) of integrated luminosity. We require two isolated leptons (electrons or muons) with the same electric charge and additional kinematic requirements. No significant excess above background is observed, and we set 95% C. L. observed (expected) upper limits on ratio of the production cross section to the standard model prediction of 6.4 (7.3) for a Higgs boson mass of 165 GeV and 13.5 (19.8) for a mass o…

PhysicsNuclear and High Energy PhysicsParticle physicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronElementary particleD0 experiment7. Clean energy01 natural sciencesStandard ModelNuclear physics0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLeptonBosonPhysical Review D
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Study ofCP-violating charge asymmetries of single muons and like-sign dimuons inpp¯collisions

2014

We measure the inclusive single muon charge asymmetry and the like-sign dimuon charge asymmetry in $p \bar{p}$ collisions using the full data set of 10.4 fb$^{-1}$ collected with the D0 detector at the Fermilab Tevatron. The standard model predictions of the charge asymmetries induced by CP violation are small in magnitude compared to the current experimental precision, so non-zero measurements could indicate new sources of CP violation. The measurements differ from the standard model predictions of CP violation in these asymmetries with a significance of 3.6 standard deviations. These results are interpreted in a framework of $B$ meson mixing within the CKM formalism to measure the relativ…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonMeson010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatron01 natural sciencesAsymmetryStandard deviationNuclear physicsBaryon asymmetry0103 physical sciencesCP violationHigh Energy Physics::ExperimentFermilab010306 general physicsmedia_commonPhysical Review D
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Measurement of the W+b-jet and W+c-jet differential production cross sections in pp¯ collisions at s=1.96 TeV

2015

We present a measurement of the cross sections for the associated production of a $W$ boson with at least one heavy quark jet, $b$ or $c$, in proton-antiproton collisions. Data corresponding to an integrated luminosity of 8.7 fb$^{-1}$ recorded with the D0 detector at the Fermilab Tevatron \ppbar Collider at $\sqrt{s}=1.96$ TeV are used to measure the cross sections differentially as a function of the jet transverse momenta in the range 20 to 150 GeV. These results are compared to calculations of perturbative QCD theory as well as predictions from Monte Carlo generators.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)Astrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronPerturbative QCDJet (particle physics)law.inventionNuclear physicslawPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilabNuclear ExperimentColliderBosonPhysics Letters B
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Measurement of the asymmetry in angular distributions of leptons produced in dileptontt¯final states inpp¯collisions ats=1.96  TeV

2013

We present measurements of asymmetries in angular distributions of leptons produced in t (t) over bar events in proton-antiproton collisions at the Fermilab Tevatron Collider. We consider final states where the W-+/- bosons from top quark and antiquark decays both decay into l nu (l = e, mu) resulting in oppositely charged dilepton final states with accompanying jets. Using 9.7 fb(-1) of integrated luminosity collected with the D0 detector, we find the asymmetries in lepton pseudorapidity compatible with predictions based on the standard model.

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatron7. Clean energy01 natural scienceslaw.inventionStandard ModelNuclear physicslawPseudorapidity0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilabNuclear Experiment010306 general physicsColliderLeptonPhysical Review D
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Search for Higgs boson production in trilepton and like-charge electron-muon final states with the D0 detector

2013

We present a search for Higgs bosons in multilepton final states in pp-bar collisions at sqrt(s)=1.96 TeV recorded with the D0 detector at the Fermilab Tevatron Collider, using the full Run II data set with integrated luminosities of up to 9.7 fb-1. The multilepton states considered are two electron plus muon, electron with two muons, muon with two hadronic tau leptons, and like-charge electron-muon pairs. These channels directly probe the HVV (V=W,Z) coupling of the Higgs boson in production and decay. The muon with two hadronic tau lepton channel is also sensitive to H to tau lepton pair decays. Upper limits at the 95% C.L on the rate of standard model Higgs boson production are derived i…

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsTevatronFOS: Physical sciences7. Clean energy01 natural scienceslaw.inventionStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderBosonPhysicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentLepton
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Measurement of spin correlation in ttbar production using a matrix element approach

2011

correlation, assuming that the spin of the top quark is either correlated with the spin of the anti-top quark as predicted by the standard model or is uncorrelated. For the first time we use a matrix-element-based approach to study ttbar spin correlation. We use {ttbar -&gt; W+bW-bbar -&gt;l+nubl-nub} final states produced in ppbar collisions at a center of mass energy sqrt(s)=1.96 TeV, where l denotes an electron or a muon. The data correspond to an integrated luminosity of 5.4 fb-1 and were collected with the dzero detector at the Fermilab Tevatron collider. The result agrees with the standard model prediction. We exclude the hypothesis that the spins of the ttbar are uncorrelated at the …

PhysicsTop quarkParticle physicsMuonLuminosity (scattering theory)010308 nuclear & particles physicsBar (music)Physics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentFermilab010306 general physicsSpin-½
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A study of the material in the ATLAS inner detector using secondary hadronic interactions

2011

The ATLAS inner detector is used to reconstruct secondary vertices due to hadronic interactions of primary collision products, so probing the location and amount of material in the inner region of ATLAS. Data collected in 7 TeV pp collisions at the LHC, with a minimum bias trigger, are used for comparisons with simulated events. The reconstructed secondary vertices have spatial resolutions ranging from ~ 200μm to 1 mm. The overall material description in the simulation is validated to within an experimental uncertainty of about 7%. This will lead to a better understanding of the reconstruction of various objects such as tracks, leptons, jets, and missing transverse momentum.

PhotonPhysics::Instrumentation and Detectorsdetector modelling and simulations i (interaction of radiation with matter; interaction; large detector systems for particle and astroparticle physics; of photons with matter; interaction of hadrons with matter; etc); particle tracking detectors (solid-state detectors); si microstrip and pad detectors01 natural sciencesparticle tracking detectors[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]of photons with matter interaction of hadrons with matter etc)InstrumentationGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Detectors de radiacióMathematical PhysicsPhysicsDetector modelling and simulations I (interaction of radiation with matter interaction of photons with matter interaction of hadrons with matter etc)Large Hadron ColliderSettore FIS/01 - Fisica SperimentaleDetectorVERTEX DETECTORSSi microstrip and pad detectorsTransition radiation detectorinteraction of hadrons with matterExperimental uncertainty analysismedicine.anatomical_structureParticle tracking detectors (Solid-state detectors)Física nuclearParticle Physics - Experimentof photons with matterParticle physicsDetector modelling and simulations I (interaction of radiation with matter interaction of photons with matter interaction of hadrons with matter etc); Particle tracking detectors (Solid-state detectors); Si microstrip and pad detectors; Large detector systems for particle and astroparticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]Detector modelling and simulations I (interaction of radiation with matter interactionDetector modelling and simulations I (interaction of radiation with matterddc:500.2530Detector Modelling and SimulationsInteraction of photons with matterNuclear physicsAtlas (anatomy)0103 physical sciencesmedicineddc:610010306 general physicsetc)Astroparticle physicsParticle Tracking DetectorsScience & Technology010308 nuclear & particles physicsLarge detector systems for particle and astroparticle physicsLarge Detector Systemsdetector modelling and simulations IFísicaCol·lisions (Física nuclear)Experimental High Energy PhysicsHigh Energy Physics::ExperimentSi Microstrip and Pad DetectorsLepton
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Evidence for a Particle Produced in Association with Weak Bosons and Decaying to a Bottom-Antibottom Quark Pair in Higgs Boson Searches at the Tevatr…

2012

Aaltonen, T. et al.

FERMILAB TEVATRON COLLIDERTop quarkParticle physics[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]Higgs-Boson decaysSTANDARD MODEL; PARTON DISTRIBUTIONS; SYMMETRIES; proton antiproton collisions; FERMILAB TEVATRON COLLIDER; Standard Model Higgs boson; HIGGS-BOSON production; Higgs-Boson decaysSTANDARD MODELGeneral Physics and AstronomyFOS: Physical sciencesElementary particleStandard Model Higgs boson7. Clean energy01 natural sciencesVector bosonStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsTEVATRONBosonStandard-model Higgs bosonsPhysicsHIGGS-BOSON productionHIGGS BOSON010308 nuclear & particles physics[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]High Energy Physics::PhenomenologyScalar bosonW and Z bosonsPARTON DISTRIBUTIONSExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonSYMMETRIESproton antiproton collisionsCDFLimits on production of particlesHigh Energy Physics::Experiment
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Measurement of the relative branching ratio ofBs0→J/ψf0(980)toBs0→J/ψϕ

2012

We present a measurement of the relative branching fraction, R-f0/phi, of B-s(0) -> J/psi f(0)(980), with f(0)(980) -> pi(+)pi(-), to the process B-s(0) -> J/psi phi, with phi -> K+K-. The J/psi f(0)(980) final state corresponds to a CP-odd eigenstate of B-s(0) that could be of interest in future studies of CP violation. Using 8 fb(-1) of data recorded with the D0 detector at the Fermilab Tevatron Collider, we find R-f0/phi = 0.275 +/- 0.041(stat) +/- 0.061(syst).

PhysicsNuclear and High Energy PhysicsParticle physicsFuture studies010308 nuclear & particles physicsBranching fraction0103 physical sciencesTevatronCP violationHigh Energy Physics::Experiment010306 general physics01 natural sciencesPhysical Review D
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Search for the rare decayBs0→μ+μ−

2013

Contains fulltext : 111249pub.pdf (Publisher’s version ) (Open Access) Contains fulltext : 111249.pdf (Author’s version preprint ) (Open Access)

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsTevatronD0 experiment01 natural scienceslaw.inventionData setNuclear physicslawExperimental High Energy Physics0103 physical sciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysical Review D
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Measurement of the cross section for top-quark pair production in pp collisions at √s = 7TeV with the ATLAS detector using final states with two high…

2012

A measurement is reported of the production cross section of top-quark pairs (tt¯) in proton-proton collisions at a center-of-mass energy of 7 TeV recorded with the ATLAS detector at the LHC. Candidate events have a signature consistent with containing two isolated leptons, large missing transverse momentum, and at least two jets. Using a data sample corresponding to an integrated luminosity of 0.70 fb−1, a tt¯ production cross section σtt¯=176±5(stat.)+14−11(syst.)±8(lum.) pb is measured for an assumed top-quark mass of mt = 172.5 GeV. This measurement is in good agreement with Standard Model predictions.

Nuclear and High Energy PhysicsTop quarkParticle physicsleptonsCiências Naturais::Ciências FísicasAtlas detector:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.253001 natural sciences7. Clean energyTOP QUARKPartícules (Física nuclear)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsNuclear Experimenthadron-hadron scatteringddc:539PhysicsHadron-Hadron ScatteringScience & TechnologyLarge Hadron Collider010308 nuclear & particles physicsAcceleradors de partículesHigh Energy Physics::PhenomenologySettore FIS/01 - Fisica SperimentaleSigmaFísicaATLASPair productionHADRON-HADRON COLLISIONSExperimental High Energy PhysicsTransverse momentumComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearHigh Energy Physics::Experimentproton-proton collisionsLHCParticle Physics - ExperimentLepton
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Measurement of the photon+b-jet production differential cross section in pp¯ collisions at s=1.96 TeV

2012

We present measurements of the differential cross section d sigma/dp(T)(gamma) for the inclusive production of a photon in association with a b-quark jet for photons with rapidities vertical bar y(gamma)vertical bar 15 GeV and rapidity vertical bar Y-jet vertical bar ) Collider at root s = 1.96 TeV. The measured cross sections are compared with next-to-leading order perturbative QCD calculations using different sets of parton distribution functions as well as to predictions based on the k(T)-factorization QCD approach, and those from the SHERPA and PYTHIA Monte Carlo event generators.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsPhoton010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyMonte Carlo methodPerturbative QCDPartonJet (particle physics)01 natural sciences7. Clean energylaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentRapidity010306 general physicsColliderPhysics Letters B
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Evidence for the associated production of a W boson and a top quark in ATLAS at √s = 7 TeV

2012

This Letter presents evidence for the associated production of a W boson and a top quark using 2.05 fb[superscript −1] of pp collision data at √s = 7 TeV accumulated with the ATLAS detector at the LHC. The analysis is based on the selection of the dileptonic final states with events featuring two isolated leptons, electron or muon, with significant transverse missing momentum and at least one jet. An approach based on boosted decision trees has been developed to improve the discrimination of single top-quark Wt events from background. A template fit to the final classifier distributions is performed to determine the cross-section. The result is incompatible with the background-only hypothes…

Top quarkPhysics::Instrumentation and DetectorsAtlas detectorSingleW Plus TATLAS; Single top-quark; Top quark; W+t01 natural sciencesSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]w bosonSingle top-quarkQAQCDetectors de radiacióPhysicsLarge Hadron ColliderCabibbo–Kobayashi–Maskawa matrixAtlas (topology)Acceleradors de partículesSettore FIS/01 - Fisica SperimentaleW plus tW+tW+tATLASTop-QuarkW+tComputingMethodologies_DOCUMENTANDTEXTPROCESSINGAtlasLHCParticle Physics - ExperimentATLAS; Top quark; W+tW+t; Single top-quarkNuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesTop Quarkddc:500.2530Partícules (Física nuclear)Nuclear physics0103 physical sciencesddc:530High Energy Physics010306 general physicsCiencias Exactastop quarkScience & TechnologyATLAS detector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicatop quark; single top-quark; atlas; w plus tPair productionHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentPhysics Letters B
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Measurements of Higgs boson production and couplings in diboson final states with the ATLAS detector at the LHC

2013

We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; ISF, MINERVA, GIF, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW, Poland; GRICES and FCT, Portu…

Standard Modeldilepton: mass spectrumCiencias Físicas01 natural sciences7. Clean energySettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHiggs particle: hadroproduction//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)vector boson: fusion[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QCBosonPhysicsHIGGS BOSONLarge Hadron Collidervector boson: pair productiontransverse energy: missing-energy4. EducationATLAS experimentSettore FIS/01 - Fisica SperimentaleATLAS3. Good healthMassless particleCERN LHC CollHiggs particle: massPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs boson7000: 8000 GeV-cmsFísica nuclearAtlasLhcNeutrinoHiggs particle: decay modesParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASp p: scatteringNuclear and High Energy PhysicsParticle physicsmass spectrum: (4lepton)530 PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2ATLASdetector; LHC; Higgsbosonproduction; diboson530Massless ParticlesNnlo QCDNuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsTransverse-MomentumCondensed Matter::Quantum GasesHiggs particle: couplingScience & Technologyhep-ex010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaQCD CorrectionsFermion//purl.org/becyt/ford/1.3 [https]Hadron CollidersDiboson ProductionAstronomíavector boson: leptonic decayHADRON-HADRON COLLISIONSProton-Proton CollisionsRoot-S=7 TevHiggs particle: hadroproduction ; Higgs particle: coupling ; vector boson: fusion ; p p: scattering ; CERN LHC Coll ; ATLAS ; Higgs particle: decay modes ; vector boson: pair production ; vector boson: leptonic decay ; mass spectrum: two-photon ; mass spectrum: (4lepton) ; dilepton: mass spectrum ; transverse energy: missing-energy ; Higgs particle: mass ; experimental results ; 7000: 8000 GeV-cmsExperimental High Energy PhysicsHigh Energy Physics::ExperimentCross-Sectionsmass spectrum: two-photonexperimental resultsLeptonBroken Symmetries
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Measurement of theZZproduction cross section and search for the standard model Higgs boson in the four lepton final state inpp¯collisions

2013

We present a measurement of Z boson pair production in p (p) over bar collisions at 1.96 TeV with 9.6 to 9.8 fb(-1) of D0 data. We examine the final states eeee, ee mu mu, and mu mu mu mu. Based on selected data, the measured cross section in the mass region M(Z/gamma*) > 30 GeV is sigma(p (p) over bar -> Z/gamma*Z/gamma*) = 1.26(-0.36)(+0.44)(stat)(-0.15)(+0.17) X (syst) +/- 0.08 (lumi) pb; after correcting for the expected ratio of sigma (p (p) over bar -> Z/gamma*Z/gamma*) to sigma(p (p) over bar -> ZZ), we derive a cross section for p (p) over bar -> ZZ production of 1.05(-0.30)(+0.37)(stat)(-0.12)(0.14)(syst) +/- 0.06 (lumi) pb. This result is combined with a previous result from the Z…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSigmaState (functional analysis)01 natural sciencesStandard ModelNuclear physicsPair production0103 physical sciencesHiggs bosonProduction (computer science)010306 general physicsLeptonBar (unit)Physical Review D
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Electron and Photon Identification in the D0 Experiment

2013

The electron and photon reconstruction and identification algorithms used by the D0 Collaboration at the Fermilab Tevatron collider are described. The determination of the electron energy scale and resolution is presented. Studies of the performance of the electron and photon reconstruction and identification are summarized.

Nuclear and High Energy PhysicsPhotonMonte Carlo methodTevatronFOS: Physical sciencesElectron01 natural sciencesHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderInstrumentationPhysics010308 nuclear & particles physicsResolution (electron density)D0 experiment3. Good healthExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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Measurement of the ratio of differential cross sectionsσ(pp¯→Z+b jet)/σ(pp¯→Z+jet)inpp¯collisions ats=1.96  TeV

2013

We measure the ratio of cross sections, sigma(p (p) over bar -> Z + b jet)/sigma(p (p) over bar -> Z + jet), for associated production of a Z boson with at least one jet. The ratio is also measured as a function of the Z boson transverse momentum, jet transverse momentum, jet pseudorapidity, and the azimuthal angle between the Z boson with respect to the highest p(T) b tagged jet. These measurements use data collected by the D0 experiment in Run II of Fermilab's Tevatron p (p) over bar Collider at a center-of-mass energy of 1.96 TeV, and correspond to an integrated luminosity of 9.7 fb(-1). The results are compared to predictions from next-to-leading order calculations and various Monte Car…

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physicsLuminosity (scattering theory)010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronD0 experiment01 natural sciences7. Clean energylaw.inventionNuclear physicslawPseudorapidity0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderBar (unit)Physical Review D
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Search for Doubly Charged Higgs Boson Pair Production inpp¯Collisions ats=1.96  TeV

2012

We present a search for pair production of doubly charged Higgs bosons in the processes $q\overline{q}\ensuremath{\rightarrow}{H}^{++}{H}^{--}$ decaying through ${H}^{\ifmmode\pm\else\textpm\fi{}\ifmmode\pm\else\textpm\fi{}}\ensuremath{\rightarrow}{\ensuremath{\tau}}^{\ifmmode\pm\else\textpm\fi{}}{\ensuremath{\tau}}^{\ifmmode\pm\else\textpm\fi{}},{\ensuremath{\mu}}^{\ifmmode\pm\else\textpm\fi{}}{\ensuremath{\tau}}^{\ifmmode\pm\else\textpm\fi{}},{\ensuremath{\mu}}^{\ifmmode\pm\else\textpm\fi{}}{\ensuremath{\mu}}^{\ifmmode\pm\else\textpm\fi{}}$. The search is performed in $p\overline{p}$ collisions at a center-of-mass energy of $\sqrt{s}=1.96\text{ }\text{ }\mathrm{TeV}$ using an integrated l…

PhysicsParticle physicsPair production010308 nuclear & particles physics0103 physical sciencesHiggs bosonGeneral Physics and Astronomy010306 general physics01 natural sciencesTellurium compoundsLower limitPhysical Review Letters
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Constraints on Models for the Higgs Boson with Exotic Spin and Parity inVH→Vbb¯Final States

2014

We present constraints on models containing non-standard-model values for the spin J and parity P of the Higgs boson H in up to 9.7 fb(-1) of p (p) over bar collisions at root s = 1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. These are the first studies of Higgs boson J(P) with fermions in the final state. In the ZH -> llb (b) over bar, WH -> l nu b (b) over barb, and ZH -> nu nu b (b) over bar final states, we compare the standard model (SM) Higgs boson prediction, J(P) = 0(+), with two alternative hypotheses, J(P) = 0(-) and J(P) = 2(+). We use a likelihood ratio to quantify the degree to which our data are incompatible with non-SM J(P) predictions for a range…

PhysicsNuclear physicsParticle physics010308 nuclear & particles physics0103 physical sciencesHiggs bosonTevatronGeneral Physics and AstronomyParity (physics)Fermion010306 general physics01 natural sciencesProduction ratePhysical Review Letters
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Characterisation and mitigation of beam-induced backgrounds observed in the ATLAS detector during the 2011 proton-proton run

2013

This paper presents a summary of beam-induced backgrounds observed in the ATLAS detector and discusses methods to tag and remove background contaminated events in data. Triggerrate based monitoring of beam-related backgrounds is presented. The correlations of backgrounds with machine conditions, such as residual pressure in the beam-pipe, are discussed. Results from dedicated beam-background simulations are shown, and their qualitative agreement with data is evaluated. Data taken during the passage of unpaired, i.e. non-colliding, proton bunches is used to obtain background-enriched data samples. These are used to identify characteristic features of beam-induced backgrounds, which then are …

Physics::Instrumentation and DetectorsAccelerator modelling and simulations; multi-particle dynamics; Analysis and statistical methods; Pattern recognition cluster finding calibration and fitting methods; Performance of High Energy Physics Detectors; single-particle dynamicsPROTON BEAMSMonte Carlo methodsingle-particle dynamics01 natural sciencesaccelerator modelling and simulations (multi-particle dynamics; single-particle dynamics)High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)MUON DETECTORcluster findingPIXEL DETECTORSNaturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]GeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)InstrumentationQCMathematical PhysicsPhysicsLarge Hadron ColliderPattern recognition cluster finding calibration and fitting methodsAccelerator modelling and simulations (multi-particle dynamics; single-particle dynamics)Settore FIS/01 - Fisica SperimentaleObservableATLAScalibration and fitting methodsAccelerator modelling and simulationsCalorimetermedicine.anatomical_structureBunchesAccelerator Modelling and Simulations (Multi-Particle Dynamics Single-Particle Dynamics)Analysis and statistical methodsLHCmulti-particle dynamicsNatural SciencesParticle Physics - ExperimentParticle physicsCiências Naturais::Ciências Físicas530 PhysicsInstrumentationCALORIMETERS:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicssingle-particle dynamics)Atlas (anatomy)Pattern recognition0103 physical sciencesmedicineAccelerator modelling and simulations (multi-particle dynamics single-particle dynamics)High Energy Physicspattern recognition; cluster finding; calibration and fitting methods; single-particle dynamics); analysis and statistical methods; accelerator modelling and simulations (multi-particle dynamics; performance of high energy physics detectorsddc:610010306 general physicsCalibration and fitting methodsScience & Technology010308 nuclear & particles physicsCluster findingFísicaAccelerator modelling and simulations (multi-particle dynamicsAccelerator modelling and simulations (multi-particle dynamics; Analysis and statistical methods; Pattern recognition cluster finding calibration and fitting methods; Performance of High Energy Physics Detectors; single-particle dynamics); Instrumentation; Mathematical PhysicsExperimental High Energy PhysicsPattern recognition; cluster finding; calibration and fitting methods; Performance of High Energy Physics Detectors; Accelerator modelling and simulations (multi-particle dynamics; single-particle dynamics); Analysis and statistical methodsPhysics::Accelerator PhysicsPerformance of High Energy Physics DetectorsEvent (particle physics)
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Search for displaced vertices arising from decays of new heavy particles in 7 TeV pp collisions at ATLAS

2012

We present the results of a search for new, heavy particles that decay at a significant distance from their production point into a final state containing charged hadrons in association with a high-momentum muon. The search is conducted in a pp-collision data sample with a center-of-mass energy of 7 TeV and an integrated luminosity of 33 pb[superscript −1] collected in 2010 by the ATLAS detector operating at the Large Hadron Collider. Production of such particles is expected in various scenarios of physics beyond the standard model. We observe no signal and place limits on the production cross-section of supersymmetric particles in an R-parity-violating scenario as a function of the neutral…

Nuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências FísicasPhysics beyond the Standard ModelHadron:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.253001 natural sciences7. Clean energyPartícules (Física nuclear)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)particulas pesadas0103 physical sciencesmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsCiencias ExactasPhysicsMuonLarge Hadron ColliderLuminosity (scattering theory)Science & TechnologyATLAS detector010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyATLAS; LHC; pp collisionsFísicaSupersymmetryATLAShadronsmedicine.anatomical_structureHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)NeutralinoExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGNEW PARTICLESHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Measurement of the DirectCP-violating Charge Asymmetry inDs±→ϕπ±Decays

2014

We present a measurement of the direct CP-violating charge asymmetry in Ds+ → ϕ π(±) decays where the ϕ meson decays to K(+)K(-), using the full Run II data set with an integrated luminosity of 10.4  fb-1 of proton-antiproton collisions collected using the D0 detector at the Fermilab Tevatron Collider. The normalized difference A(CP) in the yield of D(s)(+) and D(s)(-) mesons in these decays is measured by fitting the difference between their reconstructed invariant mass distributions. This results in an asymmetry of A(CP) = [-0.38 ± 0.27]%, which is the most precise measurement of this quantity to date. The result is consistent with the standard model prediction of zero CP asymmetry in thi…

PhysicsParticle physicsLuminosity (scattering theory)Mesonmedia_common.quotation_subjectTevatronGeneral Physics and AstronomyAsymmetryStandard Modellaw.inventionNuclear physicslawHigh Energy Physics::ExperimentInvariant massFermilabCollidermedia_commonPhysical Review Letters
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Measurement of the azimuthal ordering of charged hadrons with the ATLAS detector

2012

This paper presents a study of the possible ordering of charged hadrons in the azimuthal angle relative to the beam axis in high-energy proton-proton collisions at the Large Hadron Collider (LHC). A spectral analysis of correlations between longitudinal and transverse components of the momentum of the charged hadrons, driven by the search for phenomena related to the structure of the QCD field, is performed. Data were recorded with the ATLAS detector at center-of-mass energies of √s=900  GeV and √s=7  TeV. The correlations measured in a kinematic region dominated by low-pT particles are not well described by conventional models of hadron production. The measured spectra show features consis…

HadronNuclear TheoryParton7. Clean energy01 natural sciencesSpectral lineHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Subatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]HadronesNuclear ExperimentPhysicsQuantum chromodynamicsLarge Hadron ColliderSettore FIS/01 - Fisica SperimentaleATLASordering of charged hadrons;ComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physicsFragmentation0103 physical sciencesddc:530High Energy Physics010306 general physicsPartonScience & TechnologyATLAS detector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaQCDGluonPhase spaceHADRON-HADRON COLLISIONSQCD stringExperimental High Energy PhysicsHigh Energy Physics::ExperimentModel
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Precision measurement of the top-quark mass inlepton+jetsfinal states

2015

We measure the mass of the top quark in lepton + jets final states using the full sample of p (p) over bar collision data collected by the D0 experiment in Run II of the Fermilab Tevatron Collider at root s = 1.96 TeV, corresponding to 9.7 fb(-1) of integrated luminosity. We use a matrix element technique that calculates the probabilities for each event to result from t (t) over bar production or background. The overall jet energy scale is constrained in situ by the mass of the W boson. We measure m(t) = 174.98 +/- 0.76 GeV. This constitutes the most precise single measurement of the top-quark mass.

PhysicsNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronD0 experimentJet (particle physics)01 natural sciences7. Clean energylaw.inventionNuclear physicsPair productionlaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderLeptonPhysical Review D
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An improved determination of the width of the top quark

2012

We present an improved determination of the total width of the top quark, $\Gamma_t$, using 5.4 fb$^{-1}$ of integrated luminosity collected by the D0 Collaboration at the Tevatron $p\bar{p}$ Collider. The total width $\Gamma_t$ is extracted from the partial decay width $\Gamma(t\to Wb)$ and the branching fraction $\mathcal{B}(t\to Wb)$. $\Gamma(t\to Wb)$ is obtained from the $t$-channel single top quark production cross section and $\mathcal{B}(t\to Wb)$ is measured in $t\bar{t}$ events. For a top mass of $172.5\;\rm GeV$, the resulting width is $\Gamma_t = 2.00^{+0.47}_{-0.43}$ GeV. This translates to a top-quark lifetime of $\tau_t = (3.29^{+0.90}_{-0.63})\times10^{-25}$ s. We also extra…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsTop quarkUnitarity010308 nuclear & particles physicsBranching fractionCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFOS: Physical sciencesLambda01 natural sciences7. Clean energyBottom quarkHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Experimental High Energy Physics0103 physical sciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Production (computer science)High Energy Physics::Experiment010306 general physics
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Combined Search for the Standard Model Higgs Boson Decaying tobb¯Using the D0 Run II Data Set

2012

We present the results of the combination of searches for the standard model Higgs boson produced in association with a W or Z boson and decaying into b bbar using the data sample collected with the D0 detector in p pbar collisions at sqrt{s}=1.96 TeV at the Fermilab Tevatron Collider. We derive 95% CL upper limits on the Higgs boson cross section relative to the standard model prediction in the mass range 100 GeV <= M_H <= 150 GeV, and we exclude Higgs bosons with masses smaller than 102 GeV at the 95% CL. In the mass range 120 GeV <= M_H <= 145 GeV the data exhibit an excess above the background prediction with a global significance of 1.5 standard deviations, consistent with the expectat…

PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronGeneral Physics and Astronomy01 natural sciencesStandard deviationlaw.inventionStandard ModelNuclear physicslaw0103 physical sciencesHiggs bosonRange (statistics)High Energy Physics::ExperimentFermilabNuclear Experiment010306 general physicsColliderBosonPhysical Review Letters
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Measurement of the ratio of inclusive cross sectionsσ(pp¯→Z+2b jets /σ(pp¯→Z+2 jets)inpp¯collisions ats=1.96  TeV

2015

In this study, we measure the ratio of cross sections, σ(pp¯ → Z + 2 b jets)/σ(pp¯ → Z + 2 jets), for associated production of a Z boson with at least two jets with transverse momentum pjetT > 20 GeV and pseudorapidity |ηjet| < 2.5. This measurement uses data corresponding to an integrated luminosity of 9.7 fb–1 collected by the D0 experiment in Run II of Fermilab’s Tevatron pp¯ Collider at a center-of-mass energy of 1.96 TeV. The measured integrated ratio of 0.0236 ± 0.0032(stat) ± 0.0035(syst) is in agreement with predictions from next-to-leading-order perturbative QCD and the Monte Carlo event generators PYTHIA and ALPGEN.

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaTevatronPerturbative QCDD0 experiment01 natural sciences7. Clean energylaw.inventionNuclear physicslawPseudorapidity0103 physical sciencesHigh Energy Physics::ExperimentRapidityFermilabNuclear Experiment010306 general physicsColliderPhysical Review D
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Measurement of the differential γ+c-jet cross section and the ratio of differential γ+c and γ+b cross sections in pp¯ collisions at s=1.96 TeV

2013

We present measurements of the differential cross section $d\sigma/dp_{T}^{\gamma}$ for the associated production of a $c$-quark jet and an isolated photon with rapidity $|y^{\gamma}| 15$ GeV. The cross section ratios $\sigma(\gamma+c)/\sigma(\gamma+b)$ as a function of $p_{T}^{\gamma}$ are also presented. The results are based on data corresponding to an integrated luminosity of 8.7 fb$^{-1}$ recorded with the D0 detector at the Fermilab Tevatron $p\bar{p}$ Collider at $\sqrt{s}=$1.96 TeV. The obtained results are compared to next-to-leading order perturbative QCD calculations using various parton distribution functions, to predictions based on the $k_{T}$-factorization approach, and to pr…

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaTevatronPerturbative QCDOrder (ring theory)Parton7. Clean energy01 natural sciencesNuclear physicsDistribution function0103 physical sciencesHigh Energy Physics::ExperimentRapidityProduction (computer science)010306 general physicsPhysics Letters B
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Measurements of single top quark production cross sections and|Vtb|inpp¯collisions ats=1.96  TeV

2011

We present measurements of production cross sections of single top quarks in $\ppbar$ collisions at $\sqrt{s}=1.96\;\rm TeV$ in a data sample corresponding to an integrated luminosity of $5.4\;\rm fb^{-1}$ collected by the D0 detector at the Fermilab Tevatron Collider. We select events with an isolated electron or muon, an imbalance in transverse energy, and two, three, or four jets, with one or two of them containing a bottom hadron. We obtain an inclusive cross section of $\sigma({\ppbar}{\rargap}tb+X, tqb+X) = 3.43\pm^{0.73}_{0.74}\;\rm pb$ and use it to extract the CKM matrix element $0.79 < |V_{tb}| \leq 1$ at the 95% C.L. We also measure $\sigma({\ppbar}{\rargap}tb+X) = 0.68\pm^{0.38}…

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMuon010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHadronTevatron01 natural sciencesStandard ModelNuclear physics0103 physical sciencesProduction (computer science)010306 general physicsEnergy (signal processing)Physical Review D
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Measurement of inclusive two-particle angular correlations in pp collisions with the ATLAS detector at the LHC

2012

We present a measurement of two-particle angular correlations in proton- proton collisions at s√=900 GeV and 7 TeV. The collision events were collected during 2009 and 2010 with the ATLAS detector at the Large Hadron Collider using a single-arm minimum bias trigger. Correlations are measured for charged particles produced in the kinematic range of transverse momentum pT > 100 MeV and pseudorapidity |η| < 2.5. A complex structure in pseudorapidity and azimuth is observed at both collision energies. Results are compared to pythia 8 and herwig++ as well as to the AMBT2B, DW and Perugia 2011 tunes of pythia 6. The data are not satisfactorily described by any of these models.

Particle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências FísicasHadronMonte Carlo method:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesKinematicsddc:500.201 natural sciences530Partícules (Física nuclear)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsNuclear ExperimentPhysicsddc:539Large Hadron ColliderHadron-Hadron ScatteringScience & Technology010308 nuclear & particles physicsAcceleradors de partículesSettore FIS/01 - Fisica SperimentaleFísicaATLAS16. Peace & justiceCollisionCharged particleAzimuthPseudorapidityHADRON-HADRON COLLISIONSExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Observation of s-Channel Production of Single Top Quarks at the Tevatron

2014

We report the first observation of single-top-quark production in the s channel through the combination of the CDF and D0 measurements of the cross section in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV. The data correspond to total integrated luminosities of up to 9.7fb-1 per experiment. The measured cross section is σs=1.29-0.24+0.26pb. The probability of observing a statistical fluctuation of the background to a cross section of the observed size or larger is 1.8×10-10, corresponding to a significance of 6.3 standard deviations for the presence of an s-channel contribution to the production of single-top quarks. © 2014 American Physical Society.

P(P)OVER-BAR COLLISIONSTevatronGeneral Physics and AstronomyCHANGING NEUTRAL CURRENTS01 natural sciences7. Clean energyStandard deviationHigh Energy Physics - ExperimentCHANGING NEUTRAL CURRENTS; B-JET IDENTIFICATION; P(P)OVER-BAR COLLISIONS; FERMILAB-TEVATRON; ROOT-S=1.96 TEV; COUPLINGS; DETECTOR; SEARCH; FB(-1); DECAYSHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]SCALEPhysicsB-JET IDENTIFICATION02 Physical SciencesPhysicsSigmaCOUPLINGSROOT-S=1.96 TEVPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGProduction (computer science)Communication channelFERMILAB-TEVATRONQuarkParticle physicsGeneral PhysicsPhysics MultidisciplinaryFOS: Physical sciencesParticle Physics; Collider Physics; Top quark; Single top productionDECAYSCDF CollaborationNuclear physicsPhysics and Astronomy (all)Cross section (physics)SEARCH0103 physical sciencesParticle Physics010306 general physicsDETECTORFB(-1)Science & Technology010308 nuclear & particles physicshep-exTop quarkCollider PhysicsExperimental High Energy PhysicsSingle top productionHigh Energy Physics::ExperimentEnergy (signal processing)D0 Collaboration
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Measurement of the $W$ boson mass with the D0 detector

2012

We give a detailed description of the measurement of the $W$ boson mass, $M_W$, performed on an integrated luminosity of 4.3 fb$^{-1}$, which is based on similar techniques as used for our previous measurement done on an independent data set of 1 fb$^{-1}$ of data. The data were collected using the D0 detector at the Fermilab Tevatron Collider. This data set yields $1.68\times 10^6$ $W\rightarrow e\nu$ candidate events. We measure the mass using the transverse mass, electron transverse momentum, and missing transverse energy distributions. The $M_W$ measurements using the transverse mass and the electron transverse momentum distributions are the most precise of these three and are combined …

Nuclear and High Energy PhysicsParticle physicsTevatronGeneral Physics and AstronomyFOS: Physical sciences7. Clean energy01 natural scienceslaw.inventionStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderNuclear ExperimentBosonPhysicsLuminosity (scattering theory)010308 nuclear & particles physicsDetectorHigh Energy Physics::PhenomenologyParticle acceleratorExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::Experiment
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Measurement of the electron charge asymmetry inpp¯→W+X→eν+Xdecays inpp¯collisions ats=1.96  TeV

2015

We present a measurement of the electron charge asymmetry in $p\bar{p}\rightarrow W+X \rightarrow e\nu +X$ events at a center-of-mass energy of 1.96 TeV, using data corresponding to 9.7~fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider. The asymmetry is measured as a function of the electron pseudorapidity and is presented in five kinematic bins based on the electron transverse energy and the missing transverse energy in the event. The measured asymmetry is compared with next-to-leading-order predictions in perturbative quantum chromodynamics and provides accurate information for the determination of parton distribution functions of the prot…

PhysicsNuclear and High Energy PhysicsParticle physicsProtonmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronPartonElectron7. Clean energyAsymmetryNuclear physicsDistribution functionPseudorapidityHigh Energy Physics::ExperimentNuclear Experimentmedia_commonLeptonPhysical Review D
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Search for Neutral Higgs Bosons in Events with Multiple Bottom Quarks at the Tevatron

2012

The combination of searches performed by the CDF and D0 collaborations at the Fermilab Tevatron Collider for neutral Higgs bosons produced in association with b quarks is reported. The data, corresponding to 2.6fb -1 of integrated luminosity at CDF and 5.2fb -1 at D0, have been collected in final states containing three or more b jets. Upper limits are set on the cross section multiplied by the branching ratio varying between 44 pb and 0.7 pb in the Higgs boson mass range 90 to 300 GeV, assuming production of a narrow scalar boson. Significant enhancements to the production of Higgs bosons can be found in theories beyond the standard model, for example, in supersymmetry. The results are int…

Nuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelSTANDARD MODELP(P)OVER-BAR COLLISIONSTevatronFOS: Physical sciencesMASSLESS PARTICLES7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)Higgs particle: search for | Higgs particle: associated production | minimal supersymmetric standard model: parameter space | bottom: multiple production | cross section: branching ratio: upper limit | benchmark | DZERO | CDF | anti-p p: interaction | experimental results | Batavia TEVATRON Coll | anti-p p --> Higgs particle bottom anything | Higgs particle --> bottom anti-bottom | 1960 GeV-cms0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]BROKEN SYMMETRIESTEVATRONMASSES010306 general physicsDETECTORSUPERSYMMETRYBosonPhysicsHIGGS BOSON010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDETECTOR; SUPERSYMMETRY; MASSES; MSSM; ROOT-S=1.96 TEV; BROKEN SYMMETRIES; MASSLESS PARTICLES; STANDARD MODEL; P(P)OVER-BAR COLLISIONSSupersymmetryScalar bosonROOT-S=1.96 TEVExperimental High Energy PhysicsHiggs bosonComputingMethodologies_DOCUMENTANDTEXTPROCESSINGCDFHigh Energy Physics::ExperimentMSSMMinimal Supersymmetric Standard Model
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Study of the decayBs0→J/ψf2′(1525)inμ+μ−K+K−final states

2012

We investigate the decay $B_s^0 \rightarrow J/\psi K^+ K^-$ for invariant masses of the $K^+K^-$ pair in the range $1.35

PhysicsNuclear and High Energy PhysicsParticle physicsParticle decay010308 nuclear & particles physicsBranching fractionHigh Energy Physics::Phenomenology0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsTwo-body problem01 natural sciencesPhysical Review D
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Evidence for Zc±(3900) in semi-inclusive decays of b -flavored hadrons

2018

We present evidence for the exotic charged charmoniumlike state Zc±(3900) decaying to J/ψπ± in semi-inclusive weak decays of b-flavored hadrons. The signal is correlated with a parent J/ψπ+π- system in the invariant-mass range 4.2-4.7 GeV that would include the exotic structure Y(4260). The study is based on 10.4 fb-1 of pp collision data collected by the D0 experiment at the Fermilab Tevatron collider. © 2018 authors. Published by the American Physical Society.

PhysicsParticle physics010308 nuclear & particles physicsHadronTevatronD0 experiment01 natural scienceslaw.inventionlaw0103 physical sciencesHigh Energy Physics::ExperimentStatistical analysisFermilab010306 general physicsColliderPhysical Review D
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Measurements of inclusive W+jets production rates as a function of jet transverse momentum in pp¯ collisions at s=1.96 TeV

2011

This Letter describes measurements of inclusive W (--> e nu) + n jet cross sections (n = 1-4), presented as total inclusive cross sections and differentially in the nth jet transverse momentum. The measurements are made using data corresponding to an integrated luminosity of 4.2 fb-1 collected by the D0 detector at the Fermilab Tevatron Collider, and achieve considerably smaller uncertainties on W +jets production cross sections than previous measurements. The measurements are compared to next-to-leading order perturbative QCD (pQCD) calculations in the n =1-3 jet multiplicity bins and to leading order pQCD calculations in the 4-jet bin. The measurements are generally in agreement with pQCD…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsTevatronPerturbative QCD7. Clean energy01 natural sciencesBinNuclear physicsPhase space0103 physical sciencesHigh Energy Physics::ExperimentFermilabMultiplicity (chemistry)010306 general physicsN-jetPhysics Letters B
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Drift Time Measurement in the ATLAS Liquid Argon Electromagnetic Calorimeter using Cosmic Muons

2010

The ionization signals in the liquid argon of the ATLAS electromagnetic calorimeter are studied in detail using cosmic muons. In particular, the drift time of the ionization electrons is measured and used to assess the intrinsic uniformity of the calorimeter gaps and estimate its impact on the constant term of the energy resolution. The drift times of electrons in the cells of the second layer of the calorimeter are uniform at the level of 1.3% in the barrel and 2.8% in the endcaps. This leads to an estimated contribution to the constant term of (0.29-0.04+0.05)% in the barrel and (0.54-0.04+0.06)% in the endcaps. The same data are used to measure the drift velocity of ionization electrons …

Drift velocityPhysics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsInstrumentationFOS: Physical sciencesddc:500.2ElectronAstrophysics::Cosmology and Extragalactic AstrophysicsElectromagnetic CalorimeterATLAS; Drift Time Measurement; Cosmic Muons5307. Clean energy01 natural sciencesPartícules (Física nuclear)High Energy Physics - Experiment010305 fluids & plasmasNuclear physicsHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)Ionization0103 physical sciencesmedicineFysikddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Cosmic MuonsDetectors and Experimental Techniques010306 general physicsEngineering (miscellaneous)Ciencias ExactasDetectors de radiacióPhysicsCalorimeter (particle physics)010308 nuclear & particles physicsAcceleradors de partículesResolution (electron density)Instrumentation and Detectors (physics.ins-det)ATLASliquid argonElectromagnetic calorimetermedicine.anatomical_structureExperimental High Energy PhysicsDrift Time MeasurementPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentLHC
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Search forZγevents with large missing transverse energy inpp¯collisions ats=1.96  TeV

2012

We present the first search for new phenomena in Z gamma final states with large missing transverse energy using data corresponding to an integrated luminosity of 6.2 fb(-1) collected with the D0 experiment in p (p) over bar collisions at root s 1.96 TeV. This signature is predicted in gauge-mediated supersymmetry-breaking models, where the lightest neutralino (chi) over tilde (0)(1) is the next-to-lightest supersymmetric particle and is produced in pairs, possibly through decay from heavier supersymmetric particles. The (chi) over tilde (0)(1) can decay either to a Z boson or a photon and an associated gravitino that escapes detection. We exclude this model at the 95% C.L. for supersymmetr…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyD0 experimentLambda01 natural sciencesMomentumPair production0103 physical sciencesNeutralinoHigh Energy Physics::ExperimentGravitino010306 general physicsPhysical Review D
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Measurement of the W boson polarization in top quark decays with the ATLAS detector

2012

This paper presents measurements of the polarization of W bosons in top quark decays, derived from t¯t events with missing transverse momentum, one charged lepton and at least four jets, or two charged leptons and at least two jets. Data from pp collisions at a centre-of-mass energy of 7 TeV were collected with the ATLAS experiment at the LHC and correspond to an integrated luminosity of 1.04 fb−1. The measured fractions of longitudinally, left- and right-handed polarization are F0 = 0.67 ± 0.07, FL = 0.32 ± 0.04 and FR = 0.01 ± 0.05, in agreement with the Standard Model predictions. As the polarization of the W bosons in top quark decays is sensitive to the Wtb vertex Lorentz structure and…

Top quark7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]w bosonQAQCDetectors de radiacióBosonddc:539PhysicsLarge Hadron ColliderAtlas (topology)ATLAS experimentSettore FIS/01 - Fisica SperimentaleATLASPolarization (waves)symbolsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsCOLLISIONSANOMALOUS WTB COUPLINGSCiências Naturais::Ciências FísicasLorentz transformation:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physicssymbols.namesake0103 physical sciencesddc:530High Energy Physics010306 general physicsScience & TechnologyHadron-Hadron Scattering010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaHADRON-HADRON COLLISIONSExperimental High Energy PhysicsTEVHigh Energy Physics::ExperimentLeptonJournal of High Energy Physics
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Measurement of the top-quark mass inpp¯collisions using events with two leptons

2012

Made available in DSpace on 2022-04-29T05:11:39Z (GMT). No. of bitstreams: 0 Previous issue date: 2012-09-26 We present a measurement of the top-quark mass (m t) in pp̄ collisions at √s=1.96TeV using tt̄ events with two leptons (ee, eμ, or μμ) and accompanying jets in 4.3fb -1 of data collected with the D0 detector at the Fermilab Tevatron collider. We analyze the kinematically underconstrained dilepton events by integrating over their neutrino rapidity distributions. We reduce the dominant systematic uncertainties from the calibration of jet energy using a correction obtained from tt̄ events with a final state of a single lepton plus jets. We also correct jets in simulated events to replic…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsBar (music)Astrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFlavour01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentRapidity010306 general physicsLeptonPhysical Review D
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Measurement of the differential cross section of photon plus jet production inpp¯collisions ats=1.96  TeV

2013

We study the process of associated photon and jet production, p (p) over bar -> gamma + jet + X, using 8.7 fb(-1) of integrated luminosity collected by the D0 detector at the Fermilab Tevatron Collider at a center-of-mass energy root s = 1.96 TeV. Photons are reconstructed with rapidity vertical bar y(gamma)vertical bar 20 GeV. The highest-p(T) jet is required to be in one of four rapidity regions up to vertical bar y(jet)vertical bar 0) and opposite signs (y(gamma)y(jet) <= 0) of photon and jet rapidities. We compare the measured triple-differential cross sections, d(3)sigma/dp(T)(gamma)dy(gamma)dy(jet), to next-to-leading order (NLO) perturbative QCD calculations using different sets of p…

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physicsLarge Hadron Collider010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronPerturbative QCDPartonHERA01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentRapidity010306 general physicsColliderPhysical Review D
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Measurement of theΛb0lifetime in the exclusive decayΛb0→J/ψΛ0inpp¯collisions ats=1.96  TeV

2012

We measure the Lambda_b^0 lifetime in the fully reconstructed decay Lambda_b^0 -> J/psi Lambda^0 using 10.4 fb^-1 of ppbar collisions collected with the D0 detector at sqrt(s)=1.96 TeV. The lifetime of the topologically similar decay channel B^0 -> J/psi K^0_S is also measured. We obtain tau(Lambda_b^0) = 1.303 +- 0.075 (stat.) +- 0.035 (syst.) ps and tau(B^0) = 1.508 +- 0.025 (stat.) +- 0.043 (syst.) ps. Using these measurements, we determine the lifetime ratio of tau(Lambda_b^0)/tau(B^0) = 0.864 +- 0.052 (stat.) +- 0.033 (syst.).

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::Phenomenology0103 physical sciencesHeavy quark effective theoryHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment010306 general physicsLambda01 natural sciencesPhysical Review D
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Measurement of the jet fragmentation function and transverse profile in proton-proton collisions at a center-of-mass energy of 7 TeV with the ATLAS d…

2011

The jet fragmentation function and transverse profile for jets with 25 GeV<pT jet<500 GeV and |ηjet|<1.2 produced in proton–proton collisions with a center-of-mass energy of 7 TeV are presented. The measurement is performed using data with an integrated luminosity of 36 pb−1. Jets are reconstructed and their momentum measured using calorimetric information. The momenta of the charged particle constituents are measured using the tracking system. The distributions corrected for detector effects are compared with various Monte Carlo event generators and generator tunes. Several of these choices show good agreement with the measured fragmentation function. None of these choices reproduce both t…

Physics and Astronomy (miscellaneous)Atlas detectorMonte Carlo methodKinematics7. Clean energy01 natural sciencesScaling ViolationsHigh Energy Physics - ExperimentScatteringHigh Energy Physics - Experiment (hep-ex)jet fragmentation[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentPhysicsSettore FIS/01 - Fisica SperimentaleDetectorATLASCharged particleTransverse planePhysical SciencesQuarkFísica nuclearDistributionsLHCParticle Physics - ExperimentParticle physics530 PhysicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]jet fragmentation function; proton–proton collisions; ATLAS detectorFOS: Physical sciencesAnnihilationddc:500.2530Nuclear physicsQ2 Dependence0103 physical sciencesFragmentation functionFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias ExactasHeraScience & TechnologyATLAS detector010308 nuclear & particles physicsFísicaQCDproton-proton collisionsHigh Energy Physics::Experiment
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Search for heavy neutrinos and right-handed W bosons in events with two leptons and jets in pp collisions at √s=7 TeV with the ATLAS detector

2012

This letter reports on a search for hypothetical heavy neutrinos, N, and right-handed gauge bosons, WR, in events with high transverse momentum objects which include two reconstructed leptons and at least one hadronic jet. The results were obtained from data corresponding to an integrated luminosity of 2.1 fb−1 collected in proton–proton collisions at √s=7 TeV with the ATLAS detector at the CERN Large Hadron Collider. No excess above the Standard Model background expectation is observed. Excluded mass regions for Majorana and Dirac neutrinos are presented using two approaches for interactions that violate lepton and lepton-flavor numbers. One approach uses an effective operator framework, t…

Physics and Astronomy (miscellaneous)Atlas detector01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]w bosonNuclear ExperimentDetectors de radiacióBosonMajorana Neutrinosddc:539PhysicsRight handedSettore FIS/01 - Fisica SperimentaleHadron-Hadron Scattering; ATLAS detectorATLASParityPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCNeutrinoParticle Physics - ExperimentParticle physicsOscillationsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias ExactasLEFT-RIGHT SYMMETRYGauge bosonScience & TechnologyATLAS detectorViolation010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaParity (physics)LepMassEnergiesPair productionCol·lisions (Física nuclear)Experimental High Energy Physicsproton-proton collisionsHigh Energy Physics::ExperimentLepton
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Search for Higgs bosons decaying to τ+τ− pairs in pp¯ collisions at s=1.96 TeV

2012

Abstract We present a search for the production of neutral Higgs bosons decaying into τ + τ − pairs in p p ¯ collisions at a center-of-mass energy of 1.96 TeV. The data, corresponding to an integrated luminosity of 5.4 fb−1, were collected by the D0 experiment at the Fermilab Tevatron Collider. We set upper limits at the 95% C.L. on the product of production cross section and branching ratio for a scalar resonance decaying into τ + τ − pairs, and we interpret these limits as limits on the production of Higgs bosons in the minimal supersymmetric standard model (MSSM) and as constraints in the MSSM parameter space.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyScalar (mathematics)Tevatron7. Clean energy01 natural scienceslaw.inventionStandard ModelNuclear physicslaw0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsColliderMinimal Supersymmetric Standard ModelBosonPhysics Letters B
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Combination of CDF and D0 W-Boson mass measurements

2013

We summarize and combine direct measurements of the mass of the W boson in √s=1.96 TeV proton-antiproton collision data collected by CDF and D0 experiments at the Fermilab Tevatron Collider. Earlier measurements from CDF and D0 are combined with the two latest, more precise measurements: a CDF measurement in the electron and muon channels using data corresponding to 2.2 fb-1 of integrated luminosity, and a D0 measurement in the electron channel using data corresponding to 4.3 fb-1 of integrated luminosity. The resulting Tevatron average for the mass of the W boson is M W=80387±16 MeV. Including measurements obtained in electron-positron collisions at LEP yields the most precise value of M W…

Particle physicsNuclear and High Energy PhysicsInclusive production with identified leptonsSTANDARD MODELTevatronDecays of W bosonsFOS: Physical sciencesddc:500.201 natural sciences7. Clean energyStandard Modellaw.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]photonsFermilab010306 general physicsColliderTEVATRONNuclear ExperimentDETECTORGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)BosonPhysicsLuminosity (scattering theory)MuonLarge Hadron Collider010308 nuclear & particles physicsApplications of electroweak models to specific processesHigh Energy Physics::Phenomenologyor other nonhadronic particlesW bosonsW bosons; Applications of electroweak models to specific processes; Decays of W bosons; Inclusive production with identified leptons; photons; or other nonhadronic particlesExperimental High Energy PhysicsCDFPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentLHCSTANDARD MODEL; LHC; DETECTOR
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Improved $b$ quark jet identification at the D0 experiment

2013

The ability to identify jets which originated from $b$ quarks is an important tool of the physics program of the D0 experiment at the Fermilab Tevatron $p\bar{p}$ collider. This article describes a new algorithm designed to select jets originating from $b$ quarks while suppressing the contamination caused by jets from other quark flavors and gluons. Additionally, a new technique, the SystemN method, for determining the misidentification rate directly from data is presented.

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryTevatronFOS: Physical sciencesJet (particle physics)01 natural sciencesBottom quarkHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderInstrumentationPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyD0 experimentGluonExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::Experiment
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Measurement of the combined rapidity and pT dependence of dijet azimuthal decorrelations in pp¯ collisions at s=1.96 TeV

2013

We present the first combined measurement of the rapidity and transverse momentum dependence of dijet azimuthal decorrelations, using the recently proposed quantity R-Delta phi. The variable R-Delta phi measures the fraction of the inclusive dijet events in which the azimuthal separation of the two jets with the highest transverse momenta is less than a specified value of the parameter Delta phi(max). The quantity R-Delta phi is measured in p (p) over bar collisions at root s = 1.96 TeV, as a function of the dijet rapidity interval, the total scalar transverse momentum, and Delta phi(max). The measurement uses an event sample corresponding to an integrated luminosity of 0.7 fb(-1) collected…

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)Large Hadron Collider010308 nuclear & particles physicsScalar (mathematics)TevatronPerturbative QCD7. Clean energy01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentRapidityFermilab010306 general physicsColliderPhysics Letters B
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Observation and studies of double J/psi production at the Tevatron

2014

We present the observation of doubly-produced $J/\psi$ mesons with the D0 detector at Fermilab in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV. The production cross section for both singly and doubly-produced $J/\psi$ mesons is measured using a sample with an integrated luminosity of 8.1fb$^{-1}$. For the first time, the double $J/\psi$ production cross section is separated into contributions due to single and double parton scatterings. Using these measurements, we determine the effective cross section $\sigma_{eff}$, a parameter characterizing an effective spatial area of the parton-parton interactions and related to the parton spatial density inside the nucleon.

Nuclear and High Energy PhysicsParticle physicsMesonDOUBLE-PARTON SCATTERINGP(P)OVER-BAR COLLISIONSTevatronFOS: Physical sciencesPartonPSI-PSI-PRODUCTIONAstronomy & Astrophysics7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentPhysics Particles & FieldsNuclear physicsHigh Energy Physics - Experiment (hep-ex)Cross section (physics)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsNuclear ExperimentRUN-IIPhysicsLuminosity (scattering theory)Science & TechnologyPP COLLISIONS010308 nuclear & particles physicshep-exPhysicsHigh Energy Physics::PhenomenologyExperimental High Energy PhysicsPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGProduction (computer science)High Energy Physics::ExperimentNucleon
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Measurement of the semileptonic charge asymmetry in B-0 meson mixing with the D0 detector

2012

We present a measurement of the semileptonic mixing asymmetry for B0 mesons, a^d_{sl}, using two independent decay channels: B0 -&gt; mu+D-X, with D- -&gt; K+pi-pi-; and B0 -&gt; mu+D*-X, with D*- -&gt; antiD0 pi-, antiD0 -&gt; K+pi- (and charge conjugate processes). We use a data sample corresponding to 10.4 fb^{-1} of ppbar collisions at sqrt(s) = 1.96 TeV, collected with the D0 experiment at the Fermilab Tevatron collider. We extract the charge asymmetries in these two channels as a function of the visible proper decay length (VPDL) of the B0 meson, correct for detector-related asymmetries using data-driven methods, and account for dilution from charge-symmetric processes using Monte Car…

Nuclear and High Energy PhysicsParticle physicsMesonmedia_common.quotation_subjectMonte Carlo methodTevatronFOS: Physical sciences01 natural sciencesAsymmetryHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsCollidermedia_commonPhysics010308 nuclear & particles physicsCharge (physics)B-factoryExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentPACS numbers: 11.30.Er 12.15.Ff 14.40.Nd
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Measurement of the electric charge of the top quark intt¯events

2014

We present a measurement of the electric charge of top quarks using t (t) over bar events produced in p (p) over bar collisions at the Tevatron. The analysis is based on fully reconstructed t (t) over bar pairs in lepton + jets final states. Using data corresponding to 5.3 fb(-1) of integrated luminosity, we exclude the hypothesis that the top quark has a charge of Q = -4/3e at a significance greater than 5 standard deviations. We also place an upper limit of 0.46 on the fraction of such quarks that can be present in an admixture with the standard model top quarks (Q = +2/3e) at a 95% confidence level.

QuarkPhysicsNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronOmega baryon01 natural sciencesElectric chargeSigma baryonStandard ModelNuclear physics0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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Search for third generation scalar leptoquarks in pp collisions at √s = 7 TeV with the ATLAS detector

2013

A search for pair-produced third generation scalar leptoquarks is presented, using proton-proton collisions at √s = 7 TeV at the LHC. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 4.7 fb[superscript −1]. Each leptoquark is assumed to decay to a tau lepton and a b-quark with a branching fraction equal to 100%. No statistically significant excess above the Standard Model expectation is observed. Third generation leptoquarks are therefore excluded at 95% confidence level for masses less than 534 GeV.

Physics::Instrumentation and Detectors01 natural sciences7. Clean energyHigh Energy Physics - ExperimentScatteringHigh Energy Physics - Experiment (hep-ex)Naturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQCPhysicsLuminosity (scattering theory)Large Hadron ColliderSettore FIS/01 - Fisica SperimentaleATLAShadron-hadronmedicine.anatomical_structureComputingMethodologies_DOCUMENTANDTEXTPROCESSINGhadron-hadron; scatteringFísica nuclearLHCNatural SciencesParticle Physics - ExperimentHadron-HadronParticle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências Físicas530 PhysicsScalar (mathematics):Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2leptoquarksHadron-hadron scattering530Standard ModelNuclear physicsAtlas (anatomy)0103 physical sciencesmedicineLeptoquarkHigh Energy Physics010306 general physicsCiencias ExactasScience & TechnologyHadron-Hadron ScatteringATLAS detector010308 nuclear & particles physicsBranching fractionscatteringHigh Energy Physics::PhenomenologyFísicaHADRON-HADRON COLLISIONSExperimental High Energy Physicsproton-proton collisionsHigh Energy Physics::ExperimentLEPTOQUARKSLeptonThe Journal of High Energy Physics
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Precision Measurement of the Top Quark Mass in &lt;span class="aps-inline-formula"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="in…

2014

We measure the mass of the top quark in lepton$+$jets final states using the full sample of $$p\bar{p}$$ collision data collected by the D0 experiment in Run II of the Fermilab Tevatron Collider at $$\sqrt s=1.96 $$TeV, corresponding to $$9.7 {\rm fb}^{-1}$$ of integrated luminosity. We use a matrix element technique that calculates the probabilities for each event to result from $$t\bar t$$ production or background. The overall jet energy scale is constrained in situ by the mass of the $W$ boson. We measure $$m_t=174.98\pm0.76$$ GeV. In conclusion, this constitutes the most precise single measurement of the top-quark mass.

PhysicsTop quarkParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyD0 experiment7. Clean energylaw.inventionNuclear physicslawHigh Energy Physics::ExperimentProduction (computer science)FermilabColliderBosonLeptonPhysical Review Letters
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Search for Higgs boson production in oppositely charged dilepton and missing energy final states in9.7  fb−1ofpp¯collisions ats=1.96  TeV

2013

We present a search for Higgs boson in final states with two oppositely charged leptons and large missing transverse energy as expected in H -> WW -> lvlv decays. The events are selected from the full Run II data sample of 9.7 fb-1 of ppbar collisions collected with the D0 detector at the Fermilab Tevatron Collider at sqrt s = 1.96 TeV. To validate our search methodology, we measure the non-resonant W W production cross section and find sigma_WW = 11.6 +/- 0.7 pb, in agreement with the standard model prediction. In the Higgs boson search, no significant excess above the background expectation is observed. Upper limits at the 95% confidence level on the Higgs boson production cross section a…

PhysicsNuclear and High Energy PhysicsParticle physicsMissing energyLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatron7. Clean energy01 natural scienceslaw.inventionStandard ModelNuclear physicslaw0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentFermilab010306 general physicsColliderLeptonPhysical Review D
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Search for lepton flavour violation in the e mu continuum with the ATLAS detector in root s=7 TeV pp collisions at the LHC

2012

This paper presents a search for the t-channel exchange of an R-parity violating scalar top quark ([~ over t] ) in the e[superscript ±]μ[superscript ∓] continuum using 2.1 fb[superscript −1] of data collected by the ATLAS detector in s√=7 TeV pp collisions at the Large Hadron Collider. Data are found to be consistent with the expectation from the Standard Model backgrounds. Limits on R-parity-violating couplings at 95 % C.L. are calculated as a function of the scalar top mass ( m[subscript bar over t]). The upper limits on the production cross section for pp→eμX, through the t-channel exchange of a scalar top quark, ranges from 170 fb for m[subscript ~ over t]=95 GeV to 30 fb for m[subscrip…

Top quarkPhysics and Astronomy (miscellaneous)Hadron01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentSUPERSYMMETRYPair ProductionPhysicsddc:539eμ continuumLarge Hadron ColliderSettore FIS/01 - Fisica SperimentaleScalar LeptoquarksSupersymmetryHERAATLASComputer Science::Computers and SocietyPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCParticle Physics - ExperimentParticle physics[PHYS.ASTR.IM]Physics [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]leptonsCiências Naturais::Ciências FísicasScalar (mathematics):Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physicsViolació CP (Física nuclear)0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)lepton flavour violation; eμ continuum; ATLAS detector; LHCCiencias ExactasHeraScience & TechnologyATLAS detector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísica[SDU.ASTR.IM]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]Pair productionHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Experimental High Energy PhysicsHigh Energy Physics::ExperimentLeptonEuropean Physical Journal C
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Inclusive Production of theX(4140)State inpp¯Collisions at D0

2015

We present a study of the inclusive production of the $X(4140)$ with the decay to the $J/\psi \phi$ final state in hadronic collisions. Based on $10.4~\rm{fb^{-1}}$ of $p \overline p $ collision data collected by the D0 experiment at the Fermilab Tevatron collider, we report the first evidence for the prompt production of $X(4140)$ and find the fraction of $X(4140)$ events originating from $b$ hadrons to be $f_b=0.39\pm 0.07 {\rm \thinspace (stat)} \pm 0.10 {\rm \thinspace (syst)} $. The ratio of the non-prompt $X(4140)$ production rate to the $B_s^0$ yield in the same channel is $R=0.19 \pm 0.05 {\rm \thinspace (stat)} \pm 0.07 {\rm \thinspace (syst)}$. The values of the mass $M=4152.5 \pm…

PhysicsParticle physicsDirect production010308 nuclear & particles physics0103 physical sciencesHadronTevatronGeneral Physics and AstronomyProduction (computer science)State (functional analysis)010306 general physics01 natural sciencesProduction ratePhysical Review Letters
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Measurement of differentialtt¯production cross sections inpp¯collisions

2014

The production of top quark-antiquark pair events in pp collisions at root s= 1.96 TeV is studied as a function of the transverse momentum and absolute value of the rapidity of the top quarks as well as of the invariant mass of the tt pair. We select events containing an isolated lepton, a large imbalance in transverse momentum, and four or more jets with at least one jet identified as originating from a b quark. The data sample corresponds to 9.7 fb(-1) of integrated luminosity recorded with the D0 detector during Run II of the Fermilab Tevatron Collider. Observed differential cross sections are consistent with standard model predictions.

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatron01 natural sciences7. Clean energyBottom quarkStandard ModelNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentInvariant massRapidityFermilab010306 general physicsLeptonPhysical Review D
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Search for a Fourth Generationt′Quark inpp¯Collisions ats=1.96  TeV

2011

We present a search for pair production of a fourth generation t' quark and its antiparticle, followed by their decays to a W boson and a jet, based on an integrated luminosity of 5.3/fb of proton-antiproton collisions at sqrt{s}=1.96 TeV collected by the D0 Collaboration at the Fermilab Tevatron Collider. We set upper limits on the t't'bar production cross section that exclude at the 95% C.L. a t' quark that decays exclusively to W+jet with a mass below 285 GeV. We observe a small excess in the muon+jets channel which reduces the mass range excluded compared to the expected limit of 320 GeV in the absence of a signal.

QuarkPhysicsAntiparticleParticle physicsTop quarkMuon010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyJet (particle physics)01 natural sciences7. Clean energyNuclear physicsPair production0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilabNuclear Experiment010306 general physicsPhysical Review Letters
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Combination of the top-quark mass measurements from the Tevatron collider

2012

Aaltonen, T. et al.

FERMILAB TEVATRON COLLIDERNuclear and High Energy PhysicsPAIR PRODUCTIONNuclear TheoryFOS: Physical sciencesLibrary science01 natural sciences7. Clean energyWorld classHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsTEVATRONNuclear Experimentproton antiproton collisions; FERMILAB TEVATRON COLLIDER; Top quark; Top quark properties; JET ENERGY SCALE; PARTON DISTRIBUTIONS; PAIR PRODUCTIONPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTop quark propertiesTop quarkResearch councilPARTON DISTRIBUTIONSExperimental High Energy Physicsproton antiproton collisionsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGCDFHigh Energy Physics::ExperimentJET ENERGY SCALE
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Combination of D0 measurements of the top quark mass

2017

We present a combination of measurements of the top quark mass by the D0 experiment in the lepton+jets and dilepton channels. We use all the data collected in Run I (1992--1996) at $\sqrt s=1.8$ TeV and Run II (2001--2011) at $\sqrt s=1.96$ TeV of the Tevatron $p \bar{p}$ collider, corresponding to integrated luminosities of 0.1 fb$^{-1}$ and 9.7 fb$^{-1}$, respectively. The combined result is: $m_t = 174.95 \pm0.40\,{\rm(stat)} \pm 0.64\,{\rm(syst)}\,{\rm{GeV}}=174.95 \pm 0.75 \, {\rm{GeV}}$.

Top quarkQ007TPtop: mass: measured((n)jet dilepton) [final state]Tevatronpair production [top]01 natural scienceslaw.inventionPhysics Particles & FieldsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)lawDZERO[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Batavia TEVATRON CollNuclear ExperimentPhysicsscattering [anti-p p]PhysicsGLOBAL QCD ANALYSISDetectorROOT-S=7ATLASPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGmass: measured [top]top: pair production((n)jet lepton) [final state]Particle physics1800 GeV-cms1960 GeV-cmsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesfinal state: ((n)jet lepton)Astronomy & Astrophysicsanti-p p: colliding beamsNuclear physicsEVENTS[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciencesanti-p p: scatteringddc:530Combined resultHigh Energy Physics010306 general physicsColliderDETECTORScience & TechnologyPP COLLISIONS1960 GeV-cms010308 nuclear & particles physicsfinal state: ((n)jet dilepton)hep-exHigh Energy Physics::PhenomenologyD0 experimentDIFFERENCEPARTON DISTRIBUTIONSExperimental High Energy PhysicsPhysics::Accelerator PhysicsTEVHigh Energy Physics::Experiment1800 GeV-cmscolliding beams [anti-p p]Leptonexperimental results
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WγProduction and Limits on AnomalousWWγCouplings inpp¯Collisions ats=1.96  TeV

2011

We measure the cross section and the difference in rapidities between photons and charged leptons for inclusive W -> lnu+gamma production in egamma and mugamma final states. Using data corresponding to an integrated luminosity of 4.2 fb-1 collected with the D0 detector at the Fermilab Tevatron Collider, the cross section multiplied by the branching fraction for the process ppbar -> Wgamma+X -> lnugamma+X, measured to be 15.8 +/- 0.8 (stat.) +/- 1.2 (syst.) pb, and the distribution of the charge-signed photon-lepton rapidity difference are found to be in agreement with the standard model. These results provide the most stringent limits on anomalous WWgamma couplings for data from hadron coll…

PhysicsParticle physics010308 nuclear & particles physicsBranching fractionHadronTevatronGeneral Physics and Astronomy01 natural sciences7. Clean energylaw.inventionStandard ModelTheoretical physicslaw0103 physical sciencesHigh Energy Physics::ExperimentRapidityFermilab010306 general physicsColliderLeptonPhysical Review Letters
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Readiness of the ATLAS Tile Calorimeter for LHC collisions

2010

67 páginas.-- El PDF es la versión pre-print (arXiv:1007.5423v2).-- The ATLAS Collaboration.-- et al.

SystemPhysics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsPerformance7. Clean energy01 natural sciences030218 nuclear medicine & medical imagingSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)0302 clinical medicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesDetectors de radiaciócosmic rayPhysicsLarge Hadron ColliderDetectorSettore FIS/01 - Fisica SperimentaleAstrophysics::Instrumentation and Methods for AstrophysicsInstrumentation and Detectors (physics.ins-det)ATLASmedicine.anatomical_structureScintillatorsPhysical Sciencesmagnetic-fields; scintillators; electronics; performance; systemLHCCol·lisionadors d'hadronsPhotomultiplierFOS: Physical sciencesCosmic rayddc:500.2Noise (electronics)530LHC collisions; AtlasNuclear physics03 medical and health sciencesAtlas (anatomy)0103 physical sciencesCalibrationmedicinetile hadronic calorimeterFysikddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsEngineering (miscellaneous)Ciencias ExactasCalorimeter (particle physics)010308 nuclear & particles physicsFísicaMagnetic-FieldsHigh Energy Physics::ExperimentElectronics
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Studies ofWboson plus jets production inpp¯collisions ats=1.96  TeV

2013

We present a comprehensive analysis of inclusive W(-> ev) + n-jet (n >= 1, 2, 3, 4) production in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV at the Tevatron collider using a 3.7 fb(-1) data set collected by the D0 detector. Differential cross sections are presented as a function of the jet rapidities (y), lepton transverse momentum (P-T) and pseudorapidity (eta), the scalar sum of the transverse energies of the W boson and all jets (H-T), leading dijet P-T and invariant mass, dijet rapidity separations for a variety of jet pairings for P-T-ordered and angular-ordered jets, dijet opening angle, dijet azimuthal angular separations for P-T-ordered and angular-ordered j…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronPerturbative QCD7. Clean energy01 natural sciencesNuclear physicsPseudorapidity0103 physical sciencesHigh Energy Physics::ExperimentInvariant massRapidityResummation010306 general physicsParton showerLeptonPhysical Review D
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Evidence for Spin correlation in tt̄ production

2012

Made available in DSpace on 2022-04-29T03:09:47Z (GMT). No. of bitstreams: 0 Previous issue date: 2012-01-19 We present a measurement of the ratio of events with correlated t and t̄ spins to the total number of tt̄ events. This ratio f is evaluated using a matrix-element-based approach in 729 tt̄ candidate events with a single lepton (electron or muon) and at least four jets. The analyzed pp̄ collisions data correspond to an integrated luminosity of 5.3fb -1 and were collected with the D0 detector at the Fermilab Tevatron collider operating at a center-of-mass energy √s=1.96TeV. Combining this result with a recent measurement of f in dileptonic final states, we find f in agreement with the …

PhysicsParticle physicsMuonLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronGeneral Physics and Astronomy7. Clean energy01 natural scienceslaw.inventionStandard ModelNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentFermilabCenter of mass010306 general physicsColliderLepton
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Search for flavor changing neutral currents in decays of top quarks

2011

We present a search for flavor changing neutral currents in decays of top quarks. The analysis is based on a search for ttbar -&gt; l'null + jets (l, l' = e, mu) final states using 4.1 fb^-1 of integrated luminosity of ppbar collisions at sqrt(s) = 1.96 TeV. We extract limits on the branching ratio B(t -&gt; Zq) (q = u, c quarks), assuming anomalous tuZ or tcZ couplings. We do not observe any sign of such anomalous coupling and set a limit of B &lt; 3.2% at 95% C.L.

CouplingPhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsBranching fractionFlavor-changing neutral currentHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsSign (mathematics)
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Measurement of theBs0Lifetime in the Flavor-Specific Decay ChannelBs0→Ds−μ+νX

2015

We present an updated measurement of the B-s(0) lifetime using the semileptonic decays B-s(0) -> D-s(-)mu(+)nu X, with D-s(-) -> phi pi(-) and phi -> K+K- (and the charge conjugate process). This measurement uses the full Tevatron Run II sample of proton-antiproton collisions at root s = 1.96 TeV, comprising an integrated luminosity of 10.4 fb(-1). We find a flavor-specific lifetime tau(fs)(B-s(0)) = 1.479 +/- 0.010(stat) +/- 0.021(syst) ps. This technique is also used to determine the B-0 lifetime using the analogous B-0 -> D- mu(+)nu X decay with D- -> phi pi(-) and phi -> K+K-, yielding tau(B-0) = 1.534 +/- 0.019(stat) +/- 0.021(syst) ps. Both measurements are consistent with the current…

Nuclear physicsPhysicsParticle physics13. Climate actionTevatronGeneral Physics and AstronomyHigh Energy Physics::ExperimentNuclear Experiment7. Clean energyLuminosityPhysical Review Letters
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Measurement of spin correlation in tt¯ production using dilepton final states

2011

We measure the correlation between the spin of the top quark and the spin of the anti-top quark in (ttbar -> W+ W- b bbar -> l+ nu b l- nubar bbar) final states produced in ppbar collisions at a center of mass energy sqrt(s)=1.96 TeV, where l is an electron or muon. The data correspond to an integrated luminosity of 5.4 fb-1 and were collected with the D0 detector at the Fermilab Tevatron collider. The correlation is extracted from the angles of the two leptons in the t and tbar rest frames, yielding a correlation strength C= 0.10^{+0.45}_{-0.45}, in agreement with the NLO QCD prediction within two standard deviations, but also in agreement with the no correlation hypothesis.

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physicsTop quarkMuonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatron01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentFermilabCenter of mass010306 general physicsLeptonPhysics Letters B
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Measurement of the inclusive jet cross-section in pp collisions at $\sqrt{s}=2.76\ \mbox{TeV}$ and comparison to the inclusive jet cross-section at $…

2013

The inclusive jet cross-section has been measured in proton-proton collisions at sqrt(s)=2.76 TeV in a dataset corresponding to an integrated luminosity of 0.20pb-1 collected with the ATLAS detector at the Large Hadron Collider in 2011. Jets are identified using the anti-kt algorithm with two radius parameters of 0.4 and 0.6. The inclusive jet double-differential cross-section is presented as a function of the jet transverse momentum pT and jet rapidity y, covering a range of 20 &lt;= pT &lt; 430 GeV and |y| &lt; 4.4. The ratio of the cross-section to the inclusive jet cross-section measurement at sqrt(s)=7 TeV, published by the ATLAS Collaboration, is calculated as a function of both trans…

Physics and Astronomy (miscellaneous)Cern Pbarp ColliderCiencias FísicasMonte Carlo methodParton01 natural sciences7. Clean energyHigh Energy Physics - ExperimentEp Scattering//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)PhysicsLarge Hadron ColliderSettore FIS/01 - Fisica SperimentalePerturbative QCDATLASPerturbation-TheoryINCLUSIVE JET CROSS SECTIONPhysical SciencesLHCCIENCIAS NATURALES Y EXACTASParticle Physics - ExperimentParticle physicsShowersCiências Naturais::Ciências Físicas530 PhysicsAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesFísica de Partículas y CamposNuclear physicsDeep-Inelastic ScatteringFragmentation0103 physical sciencesFysikRapidityddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Science & Technology010308 nuclear & particles physicsParton DistributionsFísica//purl.org/becyt/ford/1.3 [https]Deep inelastic scatteringDistribution function(P)over-Bar-P CollisionsHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentDimensionless quantityModelThe European Physical Journal C
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Search for top and bottom squarks from gluino pair production in final states with missing transverse energy and at least three b-jets with the ATLAS…

2012

This letter reports the results of a search for top and bottom squarks from gluino pair production in 4.7 fb[superscript −1] of pp collisions at s√=7 TeV using the ATLAS detector at the LHC. The search is performed in events with large missing transverse momentum and at least three jets identified as originating from a b-quark. Exclusion limits are presented for a variety of gluino-mediated models with gluino masses up to 1 TeV excluded.

Physics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsHigh Energy Physics::LatticeQuarks01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Dynamical Symmetry-BreakingPionsNaturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]WeakGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Detectors de radiacióQCPhysicsddc:539GluinoLarge Hadron ColliderSettore FIS/01 - Fisica SperimentaleSupersymmetryATLASTransverse planeFísica nuclearLHCNatural SciencesParticle Physics - ExperimentQuarkParticle physicssquarks; gluino pair production; ATLAS detector; b -jetsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]Supergauge TransformationsFOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physicsPionCurrents0103 physical sciencesddc:530Symmetry breakingHigh Energy Physics010306 general physicsEngineering (miscellaneous); Physics and Astronomy (miscellaneous)Engineering (miscellaneous)Ciencias ExactasScience & TechnologyATLAS detector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaPair productionCol·lisions (Física nuclear)HADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentSupersymmetrySQUARKModel
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Search for universal extra dimensions in ppbar collisions

2012

We present a search for Kaluza-Klein (KK) particles predicted by models with universal extra dimensions (UED) using a data set corresponding to an integrated luminosity of 7.3 fb$^{-1}$, collected by the D0 detector at a $p\bar p$ center of mass energy of 1.96 TeV. The decay chain of KK particles can lead to a final state with two muons of the same charge. This signature is used to set a lower limit on the compactification scale of $R^{-1}&gt;260$ GeV in a minimal UED model.

PhysicsParticle physicsMuonCompactification (physics)010308 nuclear & particles physicsDetectorGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesLower limitHigh Energy Physics - ExperimentNuclear physicsUniversal extra dimensionHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentDecay chain010306 general physicsTellurium compounds
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Zγproduction and limits on anomalousZZγandZγγcouplings inpp¯collisions ats=1.96  TeV

2012

We present a measurement of ppbar->Zgamma->ll+gamma (l = e, mu) production with a data sample corresponding to an integrated luminosity of 6.2 fb^{-1} collected by the D0 detector at the Fermilab Tevatron ppbar Collider. The results of the electron and muon channels are combined, and we measure the total production cross section and the differential cross section dsigma/dp_T^gamma, where p_T^gamma is the momentum of the photon in the plane transverse to the beamline. The results obtained are consistent with the standard model predictions from next-to-leading order calculations. We use the transverse momentum spectrum of the photon to place limits on anomalous ZZgamma and Zgammagamma couplin…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonMuonLuminosity (scattering theory)010308 nuclear & particles physicsTevatron01 natural sciencesStandard Modellaw.inventionlaw0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilab010306 general physicsColliderLeptonPhysical Review D
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Measurement of Associated Production ofZBosons with Charm Quark Jets inpp¯Collisions ats=1.96  TeV

2014

We present the first measurements of the ratios of cross sections sigma(p (p) over bar -> Z + c jet)/sigma(p (p) over bar -> Z + jet) and sigma(p (p) over bar -> Z + jet)/sigma(p (p) over bar -> Z + b jet) for the associated production of a Z boson with at least one charm or bottom quark jet. Jets have transverse momentum p(T)(jet) > 20 GeV and pseudorapidity vertical bar eta(jet)vertical bar collisions collected with the D0 detector at the Fermilab Tevatron Collider at root s = 1.96 TeV. The measurements show significant deviations from perturbative QCD calculations and predictions from various event generators.

PhysicsJet (fluid)Particle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyPerturbative QCD7. Clean energyBottom quarkCharm quarkNuclear physicsPseudorapidityHigh Energy Physics::ExperimentNuclear ExperimentBar (unit)BosonPhysical Review Letters
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Tevatron Combination of Single-Top-Quark Cross Sections and Determination of the Magnitude of the Cabibbo-Kobayashi-Maskawa Matrix Element Vtb

2015

et al.

QuarkTop quarkParticle physicsP(P)OVER-BAR COLLISIONS; JET IDENTIFICATION; ROOT-S=7 TEV; HIGGS-BOSON; CHANNEL; DETECTOR; ATLASJET IDENTIFICATIONmeasured [channel cross section]P(P)OVER-BAR COLLISIONSTevatronGeneral Physics and AstronomyFOS: Physical sciencesmeasured [cross section]Astrophysics::Cosmology and Extragalactic Astrophysicssingle production [top]7. Clean energyHigh Energy Physics - ExperimentMeasurements of cross sections for single-top-quark productionNuclear physicsproton-antiproton collisionsHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all)CHANNELDZEROddc:550[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Batavia TEVATRON Collcross section measurementDETECTORPhysicsscattering [anti-p p]1960 GeV-cmsROOT-S=7 TEVCabibbo–Kobayashi–Maskawa matrixSigmaATLASMeasurements of cross sections for single-top-quark production; proton-antiproton collisions; cross section measurement2 [dimension]missing-energy [transverse energy]CKM matrixExperimental High Energy PhysicsHiggs bosonComputingMethodologies_DOCUMENTANDTEXTPROCESSINGCDFHigh Energy Physics::ExperimentPhysics and Astronomy (all) Nuclear and high energy physicscolliding beams [anti-p p]coupling [quark]HIGGS-BOSON
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Measurement of the pp¯→W+b+X production cross section at s=1.96 TeV

2013

We present a measurement of the cross section for $W$ boson production in association with at least one {$b$-quark} jet in proton-antiproton collisions. The measurement is made using data corresponding to an integrated luminosity of 6.1\ifb recorded with the D0 detector at the Fermilab Tevatron \ppbar Collider at $\sqrt{s}=1.96$ TeV. We measure an inclusive cross section of {$\sigma(W \sim(\to\mu\nu) + b + X) = 1.04 \pm 0.05\thinspace$(stat.) $\pm 0.12 \thinspace$(syst.) pb} and $\sigma(W (\to e\nu) + b + X) = 1.00$ \pm 0.04 \thinspace$(stat.) $\pm 0.12 \thinspace$(syst.) pb in the phase space defined by $p_T^\nu > 25$ GeV, $p_T^{\text{$b$-jet}}>20$ GeV, $|\eta^{\text{$b$-jet}}| 20$ GeV and…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsTevatronOrder (ring theory)01 natural sciences7. Clean energyLuminosityNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)Combined resultNuclear Experiment010306 general physicsLeptonBosonPhysics Letters B
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Evidence for Simultaneous Production ofJ/ψandϒMesons

2016

We report evidence for the simultaneous production of $J/\psi$ and $\Upsilon$ mesons in 8.1 fb$^{-1}$ of data collected at $\sqrt{s}=$1.96 TeV by the D0 experiment at the Fermilab $p \bar p$ Tevatron Collider. Events with these characteristics are expected to be produced predominantly by gluon-gluon interactions. In this analysis, we extract the effective cross section characterizing the initial parton spatial distribution, $\sigma_{eff}=2.2\pm 0.7\mbox{(stat)} \pm 0.9 \mbox{(syst)} ~\mbox{mb}$.

PhysicsParticle physicsMeson010308 nuclear & particles physicsNuclear TheoryHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyPartonD0 experiment01 natural scienceslaw.inventionNuclear physicsPair productionlaw0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)FermilabNuclear Experiment010306 general physicsColliderPhysical Review Letters
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Measurement of the Effective Weak Mixing Angle in pp¯→Z/γ*→ℓ+ℓ− Events

2018

We present a measurement of the effective weak mixing angle parameter sin(2)theta(l)(eff) in p (p) over bar -> Z/gamma* -> mu(+)mu(-) events at a center-of-mass energy of 1.96 TeV, collected by the D0 detector at the Fermilab Tevatron Collider and corresponding to 8.6 fb(-1) of integrated luminosity. The measured value of sin(2)theta(l)(eff)[mu mu] = 0.23016 +/- 0.00064 is further combined with the result from the D0 measurement in p (p) over bar -> Z/gamma* -> e(+)e(-) events, resulting in sin(2)theta(l)(eff)[comb] = 0.23095 +/- 0.00040. This combined result is the most precise measurement from a single experiment at a hadron collider and is the most precise determination using the couplin…

QuarkPhysicsLuminosity (scattering theory)Large Hadron Collider010308 nuclear & particles physicsTevatronGeneral Physics and Astronomy01 natural sciences7. Clean energylaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderMixing (physics)Bar (unit)Physical Review Letters
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Search for same-sign top-quark production and fourth-generation down-type quarks in pp collisions at √s = 7 TeV with the ATLAS detector

2012

A search is presented for same-sign top-quark production and down-type heavy quarks of charge −1/3 in events with two isolated leptons (e or μ) that have the same electric charge, at least two jets and large missing transverse momentum. The data are selected from pp collisions at √s=7TeV recorded by the ATLAS detector and correspond to an integrated luminosity of 1.04 fb−1. The observed data are consistent with expectations from Standard Model processes. Upper limits are set at 95 % confidence level on the cross section of new sources of same-sign top-quark pair production of 1.4-2.0 pb depending on the assumed mediator mass. Upper limits are also set on the pair-production cross-section fo…

Top quarkFOURTH GENERATIONHardron-Hadron Scattering01 natural sciences7. Clean energySettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:539PhysicsSettore FIS/01 - Fisica SperimentaleATLASmedicine.anatomical_structureComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCpp collisionsParticle Physics - ExperimentQuarkNuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2Hadron-hadron scatteringTOP QUARKElectric charge530Standard ModelquarksNuclear physicsAtlas (anatomy)0103 physical sciencesmedicineddc:530High Energy Physics010306 general physicsScience & Technology010308 nuclear & particles physicsATLAS DetectorHigh Energy Physics::PhenomenologyFísicaCharge (physics)PERFORMANCEPair productionHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentLepton
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Forward-backward correlations and charged-particle azimuthal distributions in $pp$ interactions using the ATLAS detector

2012

Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a r…

Particle physicsNuclear and High Energy PhysicsAtlas detectorCiências Naturais::Ciências FísicasMonte Carlo method:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesForward backwardKinematicsddc:500.2Hadron-hadron scattering01 natural sciences530High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ddc:539PhysicsLarge Hadron ColliderScience & TechnologyATLAS detector010308 nuclear & particles physicsScatteringAcceleradors de partículesSettore FIS/01 - Fisica SperimentaleFísicaATLASCharged particleAzimuthPARTON DISTRIBUTIONSHADRON-HADRON COLLISIONSExperimental High Energy PhysicsFísica nuclearHigh Energy Physics::ExperimentLHCFRAGMENTATIONParticle Physics - Experiment
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Measurement of Leptonic Asymmetries and Top Quark Polarization in ttbar Production

2013

We present measurements of lepton (l) angular distributions in ttbar -&gt; W+ b W- b -&gt; l+ nu b l- nubar bbar decays produced in ppbar collisions at a center-of-mass energy of sqrt(s)=1.96TeV, where l is an electron or muon. Using data corresponding to an integrated luminosity of 5.4fb^-1, collected with the D0 detector at the Fermilab Collider, we find that the angular distributions of l- relative to anti-protons and l+ relative to protons are in agreement with each other. Combining the two distributions and correcting for detector acceptance we obtain the forward-backward asymmetry A^l_FB = (5.8 +- 5.1(stat) +- 1.3(syst))%, compared to the standard model prediction of A^l_FB (predicted…

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMuon010308 nuclear & particles physicsmedia_common.quotation_subjectDetectorFOS: Physical sciencesElectronPolarization (waves)01 natural sciences7. Clean energyAsymmetryHigh 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::ExperimentFermilab010306 general physicsLeptonmedia_common
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Forward-backward asymmetry in top quark-antiquark production

2011

Made available in DSpace on 2022-04-29T02:17:17Z (GMT). No. of bitstreams: 0 Previous issue date: 2011-12-12 We present a measurement of forward-backward asymmetry in top quark-antiquark production in proton-antiproton collisions in the final state containing a lepton and at least four jets. Using a data set corresponding to an integrated luminosity of 5.4fb -1, collected by the D0 experiment at the Fermilab Tevatron Collider, we measure the tt̄ forward-backward asymmetry to be (9.2±3.7)% at the reconstruction level. When corrected for detector acceptance and resolution, the asymmetry is found to be (19.6±6.5)%. We also measure a corrected asymmetry based on the lepton from a top quark deca…

Nuclear and High Energy PhysicsTop quarkParticle physicsmedia_common.quotation_subjectTevatronFOS: Physical sciences01 natural sciences7. Clean energyAsymmetryHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear Experimentmedia_commonQuantum chromodynamicsPhysics010308 nuclear & particles physicsGenerator (category theory)High Energy Physics::PhenomenologyGluonProduction (computer science)High Energy Physics::ExperimentLepton
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Precision Measurement of the RatioB(t→Wb)/B(t→Wq)and Extraction ofVtb

2011

We present a measurement of the ratio of top quark branching fractions R = B(t -> Wb)/B(t -> Wq), where q can be a d, s or b quark, in the lepton+jets and dilepton ttbar final states. The measurement uses data from 5.4 fb-1 of ppbar collisions collected with the D0 detector at the Fermilab Tevatron Collider. We measure R = 0.90 +/- 0.04, and we extract the CKM matrix element |Vtb| as |Vtb| = 0.95 +/- 0.02, assuming unitarity of the 3x3 CKM matrix.

QuarkPhysicsTop quarkParticle physicsUnitarity010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixBranching fractionHigh Energy Physics::PhenomenologyTevatronGeneral Physics and Astronomy7. Clean energy01 natural sciencesBottom quarkNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsPhysical Review Letters
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Measurement of the forward-backward asymmetry ofΛandΛ¯production inpp¯collisions

2016

We study $\Lambda$ and $\bar{\Lambda}$ production asymmetries in $p \bar{p} \rightarrow \Lambda (\bar{\Lambda}) X$, $p \bar{p} \rightarrow J/\psi \Lambda (\bar{\Lambda}) X$, and $p \bar{p} \rightarrow \mu^\pm \Lambda (\bar{\Lambda}) X$ events recorded by the D0 detector at the Fermilab Tevatron collider at $\sqrt{s} = 1.96$ TeV. We find an excess of $\Lambda$'s ($\bar{\Lambda}$'s) produced in the proton (antiproton) direction. This forward-backward asymmetry is measured as a function of rapidity. We confirm that the $\bar{\Lambda}/\Lambda$ production ratio, measured by several experiments with various targets and a wide range of energies, is a universal function of "rapidity loss", i.e., th…

PhysicsParticle physics010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyUniversal functionTevatronForward backwardLambda01 natural sciencesAsymmetryNuclear physicsAntiproton0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentRapidityFermilab010306 general physicsmedia_commonPhysical Review D
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Search for Higgs boson production in oppositely charged dilepton and missing energy events inpp¯collisions ats=1.96  TeV

2012

We present a search for the standard model Higgs boson using events with two oppositely charged leptons and large missing transverse energy as expected in $H\rightarrow WW$ decays. The events are selected from data corresponding to 8.6 \ifb\ of integrated luminosity in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV collected with the D0 detector at the Fermilab Tevatron Collider. No significant excess above the standard model background expectation in the Higgs boson mass range this search is sensitive to is observed, and upper limits on the Higgs boson production cross section are derived.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMissing energyLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatron01 natural scienceslaw.inventionStandard ModelNuclear physicslaw0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsColliderLeptonPhysical Review D
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Search for first generation leptoquark pair production in the electron + missing energy + jets final state

2011

We present a search for the pair production of first generation scalar leptoquarks (LQ) in data corresponding to an integrated luminosity of 5.4 fb$^{-1}$ collected with the D0 detector at the Fermilab Tevatron Collider in ppbar collisions at $\sqrt{s}=1.96$ TeV. In the channel $LQ \bar{LQ} \rightarrow e\nu_e qq'$, where q, q' are u or d quarks, no significant excess of data over background is observed, and we set a 95% C.L. lower limit of 326 GeV on the leptoquark mass, assuming equal probabilities of leptoquark decays to eq and $\nu_e q'$.

PhysicsNuclear and High Energy PhysicsParticle physicsMissing energy010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesElementary particle7. Clean energy01 natural scienceslaw.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decayPair productionlaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]LeptoquarkHigh Energy Physics::Experiment010306 general physicsColliderLepton
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Measurement of t ¯ t production with a veto on additional central jet activity in pp collisions at √ s = 7 TeV using the ATLAS detector

2012

A measurement of the jet activity in t[bar over t] events produced in proton–proton collisions at a centre-of-mass energy of 7 TeV is presented, using 2.05 fb[superscript −1] of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. The t[bar over t] events are selected in the dilepton decay channel with two identified b-jets from the top quark decays. Events are vetoed if they contain an additional jet with transverse momentum above a threshold in a central rapidity interval. The fraction of events surviving the jet veto is presented as a function of this threshold for four different central rapidity interval definitions. An alternate measurement is also perfor…

Top quarkPhysics and Astronomy (miscellaneous)Hadron7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentQuark Pair ProductionHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors de radiacióPhysicsddc:539Jet (fluid)Large Hadron ColliderLuminosity (scattering theory)central jet activity; pp collisions; ATLAS detectorSettore FIS/01 - Fisica SperimentaleProduction Cross-SectionATLASmedicine.anatomical_structurePhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCParticle Physics - ExperimentParticle physicsjet activityCiências Naturais::Ciências FísicasRegular Article - Experimental PhysicsScalar (mathematics):Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physicsAtlas (anatomy)0103 physical sciencesmedicineFysikRapidityddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)QUARK PAIR PRODUCTIONCiencias ExactasScience & TechnologyATLAS detector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Experimental High Energy PhysicsHigh Energy Physics::Experimentproton-proton collisions
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Search for the Standard Model Higgs Boson in AssociatedWHProduction in9.7  fb−1ofpp¯Collisions with the D0 Detector

2012

We present a search for the standard model Higgs boson in final states with a charged lepton (electron or muon), missing transverse energy, and two or three jets, at least one of which is identified as a b-quark jet. The search is primarily sensitive to WH→lνbb production and uses data corresponding to 9.7 fb(-1) of integrated luminosity collected with the D0 detector at the Fermilab Tevatron pp Collider at √s = 1.96 TeV. We observe agreement between the data and the expected background. For a Higgs boson mass of 125 GeV, we set a 95% C.L. upper limit on the production of a standard model Higgs boson of 5.2 × σ(SM), where σ(SM) is the standard model Higgs boson production cross section, whi…

PhysicsParticle physicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronGeneral Physics and Astronomy01 natural sciences7. Clean energylaw.inventionStandard ModelNuclear physicslaw0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentFermilab010306 general physicsColliderLeptonBosonPhysical Review Letters
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Tevatron constraints on models of the Higgs boson with exotic spin and parity using decays to bottom-antibottom quark pairs.

2015

et al.

QuarkParticle physicsHiggs bosonSTANDARD MODELTevatronFOS: Physical sciencesGeneral Physics and AstronomyATLAS DETECTORD0 EXPERIMENT01 natural sciences7. Clean energy530CDF collaborationHigh Energy Physics - ExperimentVector bosonNuclear physicsproton-antiproton collisionsHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all)SEARCH0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fysik010306 general physicsPhysics and Astronomy (all). B-JET IDENTIFICATIONCDF collaboration; Higgs boson; proton-antiproton collisionsDETECTORBosonPhysicsB-JET IDENTIFICATIONLarge Hadron Collider010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyATLASD0 experimentPARTON DISTRIBUTIONSExperimental High Energy PhysicsPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonATLAS; Higgs; Hadron-Hadron ScatteringHigh Energy Physics::ExperimentLHCB-JET IDENTIFICATION; STANDARD MODEL; PARTON DISTRIBUTIONS; ATLAS; DETECTOR; D0 EXPERIMENT; LHC; SEARCH
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Jet energy scale determination in the D0 experiment

2013

The calibration of jet energy measured in the \DZero detector is presented, based on ppbar collisions at a center-of-mass energy of 1.96 TeV at the Fermilab Tevatron collider. Jet energies are measured using a sampling calorimeter composed of uranium and liquid argon as the passive and active media, respectively. This paper describes the energy calibration of jets performed with photon+jet, Z+jet and dijet{} events, with jet transverse momentum pT &gt; 6 GeV and pseudorapidity range |eta| &lt; 3.6. The corrections are measured separately for data and simulation, achieving a precision of 1.4%-1.8% for jets in the central part of the calorimeter and up to 3.5% for the jets with pseudorapidity…

Nuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaTevatronFOS: Physical sciencesParton7. Clean energy01 natural scienceslaw.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderNuclear ExperimentInstrumentationPhysicsJet (fluid)Calorimeter (particle physics)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGluonPseudorapidityExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::Experiment
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Charged-particle multiplicities in pp interactions at s=900 GeV measured with the ATLAS detector at the LHC

2010

The first measurements from proton-proton collisions recorded with the ATLAS detector at the LHC are presented. Data were collected in December 2009 using a minimum-bias trigger during collisions at a centre-of-mass energy of 900 GeV. The charged-particle multiplicity, its dependence on transverse momentum and pseudorapidity, and the relationship between mean transverse momentum and charged-particle multiplicity are measured for events with at least one charged particle in the kinematic range vertical bar eta vertical bar 500 MeV. The measurements are compared to Monte Carlo models of proton-proton collisions and to results from other experiments at the same centre-of-mass energy. The charg…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsAtlas detectorMonte Carlo methodMultiplicity (mathematics)01 natural sciences7. Clean energyCharged particleNuclear physicsMinimum biasPseudorapidity0103 physical sciencesTransverse momentumHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysics Letters B
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Search for Higgs bosons of the minimal supersymmetric standard model in pp¯ collisions at s=1.96 TeV

2012

We report results from searches for neutral Higgs bosons produced in p-pbar collisions recorded by the Dzero experiment at the Fermilab Tevatron Collider. We study the production of inclusive neutral Higgs boson in the tautau final state and in association with a b quark in the btautau and bbb final states. These results are combined to improve the sensitivity to the production of neutral Higgs bosons in the context of the minimal supersymmetric standard model (MSSM). The data are found to be consistent with expectation from background processes. Upper limits on MSSM Higgs boson production are set for Higgs boson masses ranging from 90 to 300 GeV. We exclude tanBeta>20-30 for Higgs boson ma…

Condensed Matter::Quantum GasesPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyElementary particleTechnicolor01 natural sciences7. Clean energyBottom quarkStandard ModelNuclear physicssymbols.namesake0103 physical sciencessymbolsHiggs bosonHigh Energy Physics::Experiment010306 general physicsHiggs mechanismMinimal Supersymmetric Standard ModelBosonPhysics Letters B
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Study of double parton interactions indiphoton+dijetevents inpp¯collisions ats=1.96  TeV

2016

We use a sample of diphoton+dijet events to measure the effective cross section of double parton interactions, which characterizes the area containing the interacting partons in proton-antiproton collisions, and find it to be σeff=19.3±1.4(stat)±7.8(syst) mb. The sample was collected by the D0 detector at the Fermilab Tevatron collider in $$p\bar{p}$$ collisions at $$\sqrt{s} = 1.96$$ TeV and corresponds to an integrated luminosity of 8.7 fb-1.

PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronParton7. Clean energy01 natural sciencesMeasure (mathematics)law.inventionNuclear physicslaw0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilabNuclear Experiment010306 general physicsColliderPhysical Review D
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Measurement of theWBoson Production Charge Asymmetry inpp¯→W+X→eν+XEvents ats=1.96  TeV

2014

We present a measurement of the W boson production charge asymmetry in p (p) over bar -> W + X -> ev + X events at a center of mass energy of 1.96 TeV, using 9.7 fb(-1) of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider. The neutrino longitudinal momentum is determined by using a neutrino weighting method, and the asymmetry is measured as a function of the W boson rapidity. The measurement extends over wider electron pseudorapidity region than previous results and is the most precise to date, allowing for precise determination of proton parton distribution functions in global fits.

PhysicsParticle physicsLuminosity (scattering theory)media_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyAsymmetrylaw.inventionNuclear physicslawPseudorapidityPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentRapidityFermilabNeutrinoCollidermedia_commonPhysical Review Letters
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Search for strong gravity signatures in same-sign dimuon final states using the ATLAS detector at the LHC

2012

A search for microscopic black holes has been performed in a same-sign dimuon final state using 1.3 fb[superscript −1] of proton–proton collision data collected with the ATLAS detector at a centre of mass energy of 7 TeV at the CERN Large Hadron Collider. The data are found to be consistent with the expectation from the Standard Model and the results are used to derive exclusion contours in the context of a low scale gravity model.

Atlas detectorPhysics::Instrumentation and DetectorsHadron01 natural sciencesHigh Energy Physics - ExperimentMicro black holeHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentDetectors de radiacióPhysicsINTERAÇÕES NUCLEARESLarge Hadron ColliderBLACK HOLEAtlas (topology)Strong gravityAcceleradors de partículesExtra DimensionsSettore FIS/01 - Fisica SperimentaleMicroscopic black holesATLASExtra dimensionsLarge Hadron ColliderComputingMethodologies_DOCUMENTANDTEXTPROCESSINGExtra dimensionsAtlasLHCParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsDIMENSIONSCOLLISIONSSame-sign dimuonsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2GRAVITY ON BRANE WORLDS530Partícules (Física nuclear)Nuclear physics0103 physical sciencesddc:530High Energy Physics010306 general physicsBLACK-HOLESMILLIMETERCiencias ExactasScience & TechnologyROOT-S=7 TEVATLAS detector010308 nuclear & particles physicssame-sign dimuons; microscopic black holes; extra dimensions; lhc; atlasFísicaCollisionLHC; ATLAS; Microscopic black holes; Extra dimensions; Same-sign dimuonsHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Experimental High Energy PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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Measurement of angular correlations of jets at s=1.96 TeV and determination of the strong coupling at high momentum transfers

2012

We present a measurement of the average value of a new observable at hadron colliders that is sensitive to QCD dynamics and to the strong coupling constant, while being only weakly sensitive to parton distribution functions. The observable measures the angular correlations of jets and is defined as the number of neighboring jets above a given transverse momentum threshold which accompany a given jet within a given distance Delta-R in the plane of rapidity and azimuthal angle. The ensemble average over all jets in an inclusive jet sample is measured and the results are presented as a function of transverse momentum of the inclusive jets, in different regions of Delta-R and for different tran…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsTevatronPerturbative QCDObservablePartonJet (particle physics)01 natural sciencesNuclear physicsMomentum0103 physical sciencesHigh Energy Physics::ExperimentRapidity010306 general physicsPhysics Letters B
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Measurement of the anomalous like-sign dimuon charge asymmetry with9  fb−1ofpp¯collisions

2011

We present an updated measurement of the anomalous like-sign dimuon charge asymmetry A(sl)(b) for semileptonic b-hadron decays in 9.0 fb(-1) of p (p) over bar collisions recorded with the D0 detector at a center-of-mass energy of root s = 1.96 TeV at the Fermilab Tevatron collider. We obtain A(sl)(b) = (-0.787 +/- 0.172(stat) +/- 0.093(syst)%. This result differs by 3.9 standard deviations from the prediction of the standard model and provides evidence for anomalously large CP violation in semileptonic neutral B decay. The dependence of the asymmetry on the muon impact parameter is consistent with the hypothesis that it originates from semileptonic b-hadron decays.

PhysicsNuclear and High Energy PhysicsParticle physicsMuon010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatron01 natural sciencesAsymmetrylaw.inventionStandard ModelNuclear physicslaw0103 physical sciencesCP violationHigh Energy Physics::ExperimentFermilabImpact parameterNuclear Experiment010306 general physicsCollidermedia_commonPhysical Review D
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Search for the Standard Model Higgs Boson inZH→ℓ+ℓ−bb¯Production with the D0 Detector in9.7  fb−1ofpp¯Collisions ats=1.96  TeV

2012

We acknowledge support from the DOE and NSF (USA); CEA and CNRS/IN2P3 (France); FASI, Rosatom, and RFBR (Russia); CNPq, FAPERJ, FAPESP, and FUNDUNESP (Brazil); DAE and DST (India); Colciencias (Colombia); CONACyT (Mexico); KRF and KOSEF (Korea); CONICET and UBACyT (Argentina); FOM (Netherlands); STFC and the Royal Society (United Kingdom); MSMT and GACR (Czech Republic); CRC Program and NSERC (Canada); BMBF and DFG (Germany); SFI (Ireland); The Swedish Research Council (Sweden); and CAS and CNSF (China).

PhysicsParticle physics010308 nuclear & particles physicsResearch council0103 physical sciencesGeneral Physics and Astronomy010306 general physics01 natural sciences7. Clean energyTellurium compoundsHumanitiesPhysical Review Letters
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Search for pair production of the scalar top quark in muon+tau final states

2012

We present a search for the pair production of scalar top quarks ($\tilde{t}_{1}$), the lightest supersymmetric partners of the top quarks, in $p\bar{p}$ collisions at a center-of-mass energy of 1.96 TeV, using data corresponding to an integrated luminosity of {7.3 $fb^{-1}$} collected with the \dzero experiment at the Fermilab Tevatron Collider. Each scalar top quark is assumed to decay into a $b$ quark, a charged lepton, and a scalar neutrino ($\tilde{\nu}$). We investigate final states arising from $\tilde{t}_{1} \bar{\tilde{t}_{1}} \rightarrow b\bar{b}\mu\tau \tilde{\nu} \tilde{\nu}$ and $\tilde{t}_{1} \bar{\tilde{t}_{1}} \rightarrow b\bar{b}\tau\tau \tilde{\nu} \tilde{\nu}$. With no si…

QuarkPhysicsNuclear and High Energy PhysicsTop quarkParticle physicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciences7. Clean energyStandard ModelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Pair production0103 physical sciencesExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Production (computer science)High Energy Physics::Experiment010306 general physicsComputer Science::Data Structures and AlgorithmsEnergy (signal processing)Lepton
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Search for a Higgs boson in diphoton final states with the D0 detector in9.6  fb−1ofpp¯collisions ats=1.96  TeV

2013

We present a search for a Higgs boson decaying into a pair of photons based on 9.6 fb-1 of p-pbar collisions at sqrt(s)=1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. The search employs multivariate techniques to discriminate signal from the non-resonant background and is separately optimized for a standard model and a fermiophobic Higgs boson. No significant excess of data above the background prediction is observed and upper limits on the product of the cross section and branching fraction are derived at the 95% confidence level as a function of Higgs boson mass. For a standard model Higgs boson with mass of 125 GeV, the observed (expected) upper limits are a f…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonLarge Hadron Collider010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyTevatron01 natural sciencesStandard Modellaw.inventionNuclear physicslaw0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysical Review D
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Muon reconstruction and identification with the Run II D0 detector

2013

We present an overview of the muon reconstruction and identification methods employed by the D0 Collaboration to analyze the Run II (2001-2011) ppbar data of the Fermilab Tevatron collider at sqrt s = 1.96 TeV. We discuss the performance of these methods, how it is measured using D0 data, and how it is properly modeled by the D0 simulation program. In its pseudorapidity acceptance, eta&lt; 2, the muon system identifies high-pT muons (pT&gt;10 GeV) with efficiencies ranging from 72% to 89%. Muons tracks are reconstructed in the D0 central tracking system with efficiencies ranging from 85% to 92% and with a typical relative momentum resolution of 10% for pT = 40 GeV. Isolation criteria reject…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonBar (music)DetectorTevatronFOS: Physical sciencesRangingHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)lawPseudorapidityExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Physics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilabColliderInstrumentation
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Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

2013

Measurements of the production of jets of particles in association with a Z boson in pp collisions at s√ = 7 TeV are presented, using data corresponding to an integrated luminosity of 4.6 fb[superscript −1] collected by the ATLAS experiment at the Large Hadron Collider. Inclusive and differential jet cross sections in Z events, with Z decaying into electron or muon pairs, are measured for jets with transverse momentum p [subscript T] > 30 GeV and rapidity |y| < 4.4. The results are compared to next-to-leading-order perturbative QCD calculations, and to predictions from different Monte Carlo generators based on leading-order and next-to-leading-order matrix elements supplemented by parton sh…

Physics::Instrumentation and Detectorslarge hadron colliderPartonJet (particle physics)01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)QChadron-hadron scatteringPhysicsLarge Hadron ColliderLuminosity (scattering theory)Settore FIS/01 - Fisica SperimentaleATLAS experimentPerturbative QCDz bosonATLASLHCParticle Physics - ExperimentParticle physicsNuclear and High Energy Physics530 PhysicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesATLAS experimentddc:500.2Hadron-hadron scattering530Nuclear physics0103 physical sciencesddc:530RapidityHigh Energy Physics010306 general physicsCiencias ExactasScience & TechnologyMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaQCDHADRON-HADRON COLLISIONSExperimental High Energy Physicsproton-proton collisionsHigh Energy Physics::Experiment
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ATLAS measurements of the properties of jets for boosted particle searches

2012

Measurements are presented of the properties of high transverse momentum jets, produced in proton-proton collisions at a center-of-mass energy of √s=7  TeV. The data correspond to an integrated luminosity of 35  pb−1 and were collected with the ATLAS detector in 2010. Jet mass, width, eccentricity, planar flow and angularity are measured for jets reconstructed using the anti-kt algorithm with distance parameters R=0.6 and 1.0, with transverse momentum pT>300  GeV and pseudorapidity |η|<2. The measurements are compared to the expectations of Monte Carlo generators that match leading-logarithmic parton showers to leading-order, or next-to-leading-order, matrix elements. The generators describ…

Atlas detectorMonte Carlo methodParton7. Clean energy01 natural sciencesNucleonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentNUCLEONATLAS; jets; boostedQCDetectors de radiacióQuantum chromodynamicsPhysicsLarge Hadron ColliderAcceleradors de partículesSettore FIS/01 - Fisica SperimentaleATLASINCLUSIVE JET CROSS SECTIONLarge Hadron ColliderPseudorapidityTransverse momentumComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCFRAGMENTATIONNucleonParticle Physics - ExperimentjetsNuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências Físicas530 PhysicsAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Proton-proton collisionsNuclear physics0103 physical sciencesddc:530High Energy Physics010306 general physicsCiencias ExactasScience & TechnologyATLAS detector010308 nuclear & particles physicsFísicaMODELHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)PARTON DISTRIBUTIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentModel
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Search for a heavy neutral particle decaying into an electron and a muon using 1 fb−1 of ATLAS data

2011

A search is presented for a high mass neutral particle that decays directly to the e±μ∓ final state. The data sample was recorded by the ATLAS detector in s√=7~TeVpp collisions at the LHC from March to June 2011 and corresponds to an integrated luminosity of 1.07 fb−1. The data are found to be consistent with the Standard Model background. The high e±μ∓ mass region is used to set 95% confidence level upper limits on the production of two possible new physics processes: tau sneutrinos in an R-parity violating supersymmetric model and Z′-like vector bosons in a lepton flavor violating model.

Particle physicsHIGH MASS RESONANCEPhysics and Astronomy (miscellaneous)Ciências Naturais::Ciências FísicasPhysics beyond the Standard Model:Ciências Físicas [Ciências Naturais]FOS: Physical scienceshigh mass neutral particleElementary particleddc:500.253001 natural sciences7. Clean energyPartícules (Física nuclear)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fysikheavy neutral particle decaying; electron; muon; ATLASddc:530High Energy Physics010306 general physicsNeutral particleEngineering (miscellaneous)PhysicsLarge Hadron ColliderMuonScience & TechnologyATLAS detector010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaSupersymmetryFermionATLASQCDHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Physical SciencesHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentLepton
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Search forZH→ℓ+ℓ−bb¯production in9.7  fb−1ofpp¯collisions with the D0 detector

2013

We present a search for the standard model (SM) Higgs boson produced in association with a Z boson in 9.7 fb-1 of ppbar collisions collected with the D0 detector at the Fermilab Tevatron Collider at sqrt{s} = 1.96 TeV. Selected events contain one reconstructed Z -> e+e- or Z -> mu+mu- candidate and at least two jets, including at least one jet likely to contain a b quark. To validate the search procedure, we also measure the cross section for ZZ production, and find that it is consistent with the SM expectation. We set upper limits at the 95% C.L. on the product of the ZH production cross section and branching ratio B(H -> bbbar) for Higgs boson masses 90

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyTevatronJet (particle physics)01 natural sciences7. Clean energyBottom quarklaw.inventionStandard Modellaw0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysical Review D
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Measurement of the top quark charge in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector

2013

A measurement of the top quark electric charge is carried out in the ATLAS experiment at the Large Hadron Collider using 2.05 fb[superscript −1] of data at a centre-of-mass energy of 7 TeV. In units of the elementary electric charge, the top quark charge is determined to be 0.64 ± 0.02 (stat.) ± 0.08 (syst.) from the charges of the top quark decay products in single lepton t[¯ over t] candidate events. This excludes models that propose a heavy quark of electric charge −4/3, instead of the Standard Model top quark, with a significance of more than 8σ.

top physics; hadron-hadron scatteringNuclear and High Energy PhysicsTop quarkParticle physics530 PhysicsAtlas detectorCiências Naturais::Ciências Físicastop physicsHigh Energy Physics::Lattice:Ciências Físicas [Ciências Naturais]FOS: Physical sciences7. Clean energy01 natural sciences530High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Naturvetenskap0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics010306 general physicsQCCiencias Exactashadron-hadron scatteringtop quarkPhysicsLarge Hadron ColliderHadron-Hadron ScatteringScience & TechnologyATLAS detector010308 nuclear & particles physicsAtlas (topology)Settore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaATLASTop physicsHADRON-HADRON COLLISIONSproton-proton collisionsHigh Energy Physics::ExperimentLHCHadron-Hadron Scattering; Top physicsNatural SciencesParticle Physics - ExperimentLepton
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Measurement of the forward-backward asymmetries in the production ofΞandΩbaryons inpp¯collisions

2016

We measure the forward-backward asymmetries $A_{\rm FB}$ of charged $\Xi$ and $\Omega$ baryons produced in $p \bar{p}$ collisions recorded by the D0 detector at the Fermilab Tevatron collider at $\sqrt{s} = 1.96$ TeV as a function of the baryon rapidity $y$. We find that the asymmetries $A_{\rm FB}$ for charged $\Xi$ and $\Omega$ baryons are consistent with zero within statistical uncertainties.

PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronZero (complex analysis)01 natural sciencesMeasure (mathematics)law.inventionBaryonNuclear physicslaw0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentRapidityProduction (computer science)FermilabNuclear Experiment010306 general physicsColliderPhysical Review D
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Search for the standard model Higgs boson in tau lepton final states

2012

We present a search for the standard model Higgs boson in final states with an electron or muon and a hadronically decaying tau lepton in association with zero, one, or two or more jets using data corresponding to an integrated luminosity of up to 7.3 fb^{-1} collected with the D0 detector at the Fermilab Tevatron collider. The analysis is sensitive to Higgs boson production via gluon gluon fusion, associated vector boson production, and vector boson fusion, and to Higgs boson decays to tau lepton pairs or W boson pairs. Observed (expected) limits are set on the ratio of 95% C.L. upper limits on the cross section times branching ratio, relative to those predicted by the Standard Model, of 1…

Nuclear and High Energy PhysicsParticle physicsTevatronFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentVector bosonStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsBosonCondensed Matter::Quantum GasesPhysicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyScalar bosonExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonHigh Energy Physics::ExperimentLeptonPhysics Letters B
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Hunt for new phenomena using large jet multiplicities and missing transverse momentum with ATLAS in 4.7 fb[superscript −1] of √s = 7 TeV proton-proto…

2012

Results are presented of a search for new particles decaying to large numbers of jets in association with missing transverse momentum, using 4.7 fb[superscript −1] of pp collision data at √s = 7 TeV collected by the ATLAS experiment at the Large Hadron Collider in 2011. The event selection requires missing transverse momentum, no isolated electrons or muons, and from ≥6 to ≥9 jets. No evidence is found for physics beyond the Standard Model. The results are interpreted in the context of a MSUGRA/CMSSM supersymmetric model, where, for large universal scalar mass m [subscript 0], gluino masses smaller than 840 GeV are excluded at the 95% confidence level, extending previously published limits.…

Particle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências FísicasPhysics beyond the Standard Model:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.201 natural sciences7. Clean energy530High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsNuclear ExperimentCiencias ExactasPhysicsddc:539GluinoLarge Hadron ColliderHadron-Hadron ScatteringScience & Technology010308 nuclear & particles physicsProton-proton collisionATLAS experimentSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaSupersymmetryATLASHadron-Hadron scatteringLarge Hadron ColliderHADRON-HADRON COLLISIONSNeutralinoHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentMinimal Supersymmetric Standard ModelLepton
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Measurement of the forward-backward asymmetry in top quark-antiquark production inpp¯collisions using thelepton+jetschannel

2014

We present a measurement of the forward-backward asymmetry in top quark-antiquark production using the full Tevatron Run II data set collected by the D0 experiment at Fermilab. The measurement is performed in lepton + jets final states using a new kinematic fitting algorithm for events with four or more jets and a new partial reconstruction algorithm for events with only three jets. Corrected for detector acceptance and resolution effects, the asymmetry is evaluated to be A(FB) = (10.6 +/- 3.0)%. Results are consistent with the standard model predictions which range from 5.0% to 8.8%. We also present the dependence of the asymmetry on the invariant mass of the top quark-antiquark system and…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsHigh Energy Physics::Latticemedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronD0 experimentAsymmetryStandard ModelNuclear physicsHigh Energy Physics::ExperimentInvariant massFermilabmedia_commonLeptonPhysical Review D
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Measurement of inclusive jet and dijet cross sections in proton-proton collisions at 7 TeV centre-of-mass energy with the ATLAS detector

2011

Jet cross sections have been measured for the first time in proton-proton collisions at a centre-of-mass energy of 7 TeV using the ATLAS detector. The measurement uses an integrated luminosity of 17 nb−1 recorded at the Large Hadron Collider. The anti-k t algorithm is used to identify jets, with two jet resolution parameters, R=0.4 and 0.6. The dominant uncertainty comes from the jet energy scale, which is determined to within 7% for central jets above 60 GeV transverse momentum. Inclusive single-jet differential cross sections are presented as functions of jet transverse momentum and rapidity. Dijet cross sections are presented as functions of dijet mass and the angular variable χ. The res…

:Mathematics and natural science: 400::Physics: 430 [VDP]Physics and Astronomy (miscellaneous)4-Jet Observables:Mathematics and natural science: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]01 natural sciencesHigh Energy Physics - Experimentlaw.inventionHigh Energy Physics - Experiment (hep-ex)law[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Angular-DistributionsMediciónQuantum chromodynamicsPhysicsJet (fluid)MultiplicitiesLarge Hadron ColliderLuminosity (scattering theory)Settore FIS/01 - Fisica SperimentaleHERAATLASINCLUSIVE JET CROSS SECTIONmedicine.anatomical_structurePhotoproductionPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCParticle Physics - ExperimentjetsParticle physicsCiências Naturais::Ciências FísicasStrong-Coupling Alpha(S)Astrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesmedicineFysikRapidityddc:530High Energy Physics010306 general physicsColliderEngineering (miscellaneous)Ciencias ExactasHeraCalorimeterATLAS detector010308 nuclear & particles physicsParton DistributionsFísicaATLAS detector; proton-proton collisionsExperimental High Energy PhysicsHigh Energy Physics::ExperimentResolutionCollider
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Limits on anomalous trilinear gauge boson couplings from WW, WZ and Wγ production in pp¯ collisions at s=1.96 TeV

2012

We present searches for the anomalous γWW and ZWW trilinear gauge boson couplings from WW and WZ production using lepton plus dijet final states and a combination with results from Wγ, WW, and WZ production with leptonic final states. The analyzed data correspond to up to 8.6fb -1 of integrated luminosity collected by the D0 detector in pp- collisions at s=1.96TeV. We set the most stringent limits at a hadron collider to date assuming two different relations between the anomalous coupling parameters δκ γ, λ, and δg1Z for a cutoff energy scale Λ=2TeV. The combined 68% C.L. limits are -0.057lδκ γl0.154, -0.015lλl0.028, and -0.008lδg1Zl0.054 for the LEP parameterization, and -0.007lδκl0.081 an…

CouplingPhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonLuminosity (scattering theory)Large Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenology01 natural sciences7. Clean energyNuclear physics0103 physical sciencesQuadrupoleCutoffHigh Energy Physics::Experiment010306 general physicsMagnetic dipoleLeptonPhysics Letters B
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Search for anomalous Wtb couplings in single top quark production in pp¯ collisions at s=1.96 TeV

2012

We present new direct constraints on a general $Wtb$ interaction using data corresponding to an integrated luminosity of 5.4 fb$^{-1}$ collected by the D0 detector at the Tevatron $p\bar{p}$ collider. The standard model provides a purely left-handed vector coupling at the $Wtb$ vertex, while the most general, lowest dimension Lagrangian allows right-handed vector and left- or right-handed tensor couplings as well. We obtain precise limits on these anomalous couplings by comparing the data to the expectations from different assumptions on the $Wtb$ coupling.

QuarkCouplingPhysicsNuclear and High Energy PhysicsParticle physicsTop quark010308 nuclear & particles physicsTevatronElementary particle01 natural sciencesNuclear physics0103 physical sciencesGrand Unified TheoryHigh Energy Physics::ExperimentTensorQuantum field theory010306 general physicsPhysics Letters B
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Measurement of the Forward-Backward Asymmetry in the Production ofB±Mesons inpp¯Collisions ats=1.96  TeV

2015

We present a measurement of the forward-backward asymmetry in the production of B-+/- mesons, A(FB)(B-+/-) using B-+/- -> J/ Psi K-+/- decays in 10.4 fb(-1) of p (p) over bar collisions at root s = 1.96 TeV collected by the D0 experiment during Run II of the Tevatron collider. A nonzero asymmetry would indicate a preference for a particular flavor, i.e., b quark or (b) over bar antiquark, to be produced in the direction of the proton beam. We extract A(FB) (B-+/-) from a maximum likelihood fit to the difference between the numbers of forward-and backward-produced B-+/- mesons. We measure an asymmetry consistent with zero: A(FB) (B-+/-) = [-0.24 +/- 0.41 (stat) +/- 0.19 (syst)] %.

QuarkPhysicsParticle physicsProtonMeson010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronGeneral Physics and Astronomy01 natural sciencesBottom quarkAsymmetryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentB mesonRapidity010306 general physicsmedia_commonPhysical Review Letters
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Bs0lifetime measurement in theCP-odd decay channelBs0→J/ψ f0(980)

2016

The lifetime of the $B^{0}_{s}$ meson is measured in the decay channel $B^{0}_{s} \to J/\psi\mbox{ }\pi^+ \pi^-$ with $880 \leq M_{\pi^+\pi^-} \leq 1080$ MeV/$c^2$, which is mainly a CP-odd state and dominated by the $f_{0}(980)$ resonance. In 10.4 fb$^{-1}$ of data collected with the D0 detector in Run II of the Tevatron, the lifetime of the $B^{0}_{s}$ meson is measured to be $\tau(B^{0}_{s}) = 1.70\pm 0.14 \mbox{ (stat)} \pm 0.05 \mbox{ (syst) ps}$. Neglecting CP violation in $B_s^0/\bar{B}_s^0$ mixing, the measurement can be translated into the width of the heavy mass eigenstate of the $B^0_s$, $\Gamma_H = 0.59 \pm 0.05 \mbox{ (stat)} \pm 0.02 \mbox{ (syst)} \mbox{ ps$^{-1}$}$.

PhysicsParticle physicsMeson010308 nuclear & particles physics0103 physical sciencesTevatronCP violationResonanceStatistical physics010306 general physics01 natural sciencesPhysical Review D
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Search for the standard model Higgs boson inℓν+jetsfinal states in9.7  fb−1ofpp¯collisions with the D0 detector

2013

Searches for the Higgs boson have started as soon as the underlying model for particle mass generation has been proposed, and the search went on for several decades at LEP, Tevatron and LHC. Last year the ATLAS and CMS Collaborations at the Large Hadron Collider (LHC) have reported the observation of a new boson [1, 2]. At the same time the CDF and D0 Collaborations reported combined evidence for a particle, with a mass consistent with that of the new boson observed at LHC [3]. This thesis presents the search by the D0 collaboration for the SM Higgs boson using events containing one isolated charged lepton (l = e or μ), a significant imbalance in transverse energy (6ET ), and two or more je…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatron01 natural sciencesb-taggingStandard ModelNuclear physics0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLeptonBosonMinimal Supersymmetric Standard ModelPhysical Review D
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Search for anomalous production of prompt like-sign muon pairs and constraints on physics beyond the Standard Model with the ATLAS detector

2012

An inclusive search for anomalous production of two prompt, isolated muons with the same electric charge is presented. The search is performed in a data sample corresponding to 1.6  fb−1 of integrated luminosity collected in 2011 at √s=7  TeV with the ATLAS detector at the LHC. Muon pairs are selected by requiring two isolated muons of the same electric charge with pT>20  GeV and |η|<2.5. Minimal requirements are placed on the rest of the event activity. The distribution of the invariant mass of the muon pair m(μμ) is found to agree well with the background expectation. Upper limits on the cross section for anomalous production of two muons with the same electric charge are placed as a func…

Physics beyond the Standard Model01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Subatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QCDetectors de radiacióPhysicsLarge Hadron ColliderAcceleradors de partículesSettore FIS/01 - Fisica SperimentaleATLASIsolated muonsInclusive searchComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCParticle Physics - ExperimentStandard modelNUMBER-VIOLATING PROCESSESNuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências Físicas530 PhysicsLEPTON-NUMBERAtlas detector:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2Electric charge530Partícules (Física nuclear)Nuclear physicsanomalous production; muon pairs0103 physical sciencesddc:530High Energy Physics010306 general physicsLEFT-RIGHT SYMMETRYScience & TechnologyMuon010308 nuclear & particles physicsBranching fractionFísicaNEW PHYSICSFermionLepton numberPair productionHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHadronic collidersHigh Energy Physics::ExperimentCHARGED HIGGS BOSONS
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Precise measurement of the top quark mass in the dilepton channel at D0

2011

We measure the top quark mass (mt) in ppbar collisions at a center of mass energy of 1.96 TeV using dilepton ttbar-&gt;W+bW-bbar-&gt;l+nubl-nubarbbar events, where l denotes an electron, a muon, or a tau that decays leptonically. The data correspond to an integrated luminosity of 5.4 fb-1 collected with the D0 detector at the Fermilab Tevatron Collider. We obtain mt = 174.0 +- 1.8(stat) +- 2.4(syst) GeV, which is in agreement with the current world average mt = 173.3 +- 1.1 GeV. This is currently the most precise measurement of mt in the dilepton channel.

PhysicsTop quarkParticle physicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesHigh Energy Physics - ExperimentLuminosityNuclear physicsHigh Energy Physics - Experiment (hep-ex)Experimental High Energy Physics0103 physical sciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment14.65.HaCenter of mass010306 general physicsNuclear ExperimentBar (unit)
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Model independent search for new phenomena inpp¯collisions ats=1.96  TeV

2012

We describe a model independent search for physics beyond the standard model in lepton final states. We examine 117 final states using 1.1 fb$^{-1}$ of $p \bar{p}$ collisions data at $\sqrt{s} = 1.96$ TeV collected with the D0 detector. We conclude that all observed discrepancies between data and model can be attributed to uncertainties in the standard model background modeling, and hence we do not see any evidence for physics beyond the standard model.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBar (music)Physics beyond the Standard ModelDetector01 natural sciencesStandard ModelNuclear physics0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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Odderon Exchange from Elastic Scattering Differences between pp and pp¯ Data at 1.96 TeV and from pp Forward Scattering Measurements

2021

We describe an analysis comparing the p p ¯ elastic cross section as measured by the D0 Collaboration at a center-of-mass energy of 1.96 TeV to that in p p collisions as measured by the TOTEM Collaboration at 2.76, 7, 8, and 13 TeV using a model-independent approach. The TOTEM cross sections, extrapolated to a center-of-mass energy of s = 1.96 TeV , are compared with the D0 measurement in the region of the diffractive minimum and the second maximum of the p p cross section. The two data sets disagree at the 3.4 σ level and thus provide evidence for the t -channel exchange of a colorless, C -odd gluonic compound, also known as the odderon. We combine these results with a TOTEM analysis of th…

Quantum chromodynamicsPhysicsElastic scatteringParticle physics010308 nuclear & particles physicsForward scatterScatteringStrong interactionGeneral Physics and Astronomy01 natural sciencesScattering amplitudeCross section (physics)0103 physical sciences010306 general physicsBar (unit)Physical Review Letters
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Search for violation of Lorentz invariance in top quark pair production and decay

2012

Using data collected with the D0 detector at the Fermilab Tevatron Collider, corresponding to 5.3 fb$^{-1}$ of integrated luminosity, we search for violation of Lorentz invariance by examining the \ttbar production cross section in lepton+jets final states. We quantify this violation using the standard-model extension framework, which predicts a dependence of the \ttbar production cross section on sidereal time as the orientation of the detector changes with the rotation of the Earth. Within this framework, we measure components of the matrices $(c_Q)_{\mu\nu 33}$ and $(c_U)_{\mu\nu 33}$ containing coefficients used to parametrize violation of Lorentz invariance in the top quark sector. Wit…

PhysicsTop quarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesGeneral Physics and AstronomyLorentz covariance01 natural sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pair productionStandard-Model ExtensionExperimental High Energy Physics0103 physical sciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Production (computer science)High Energy Physics::Experiment010306 general physicsLepton
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Precise measurement of the top quark mass in dilepton decays using optimized neutrino weighting

2016

We measure the top quark mass in dilepton final states of top-antitop events in proton-antiproton collisions at sqrt(s) = 1.96 TeV, using data corresponding to an integrated luminosity of 9.7 fb^-1 at the Fermilab Tevatron Collider. The analysis features a comprehensive optimization of the neutrino weighting method to minimize the statistical uncertainties. We also improve the calibration of jet energies using the calibration determined in top-antitop to lepton+jets events, which reduces the otherwise limiting systematic uncertainty from the jet energy scale. The measured top quark mass is mt = 173.32 +/- 1.36(stat) +/- 0.85(syst) GeV.

Top quarkdependence [flavor]TevatronATLAS DETECTORJet (particle physics)pair production [top]7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentPhysics Particles & FieldsSubatomär fysikHigh Energy Physics - Experiment (hep-ex)DZEROSubatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]HADRON COLLIDERSBatavia TEVATRON CollFermilabNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Physicsscattering [anti-p p]Luminosity (scattering theory)PhysicsNuclear & Particles Physicslcsh:QC1-999Physics NuclearPhysical SciencesPOLEflavor [quark]mass: measured [top]Neutrinotop quark mass; dilepton decays; neutrino weightingdata analysis methodParticle physicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaSTANDARD MODELFOS: Physical sciencesAstronomy & AstrophysicsAccelerator Physics and Instrumentation530Standard ModelNuclear physics0202 Atomic Molecular Nuclear Particle And Plasma Physicsfinal state [dilepton]0103 physical sciencesMODEL HIGGS-BOSONddc:530High Energy Physics010306 general physics1960 GeV-cmsScience & TechnologyPP COLLISIONSIDENTIFICATION010308 nuclear & particles physicsDATA processing & computer scienceHigh Energy Physics::PhenomenologyAcceleratorfysik och instrumenteringenergy [jet]PRODUCTION CROSS-SECTION(MS)OVER-BAR MASSEScalibration [jet]Experimental High Energy PhysicsPhysics::Accelerator PhysicsTEVHigh Energy Physics::Experimentddc:004statisticalcolliding beams [anti-p p]lcsh:Physicsexperimental resultsLepton
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Measurement of the differential cross sections for isolated direct photon pair production in pp¯ collisions at s=1.96 TeV

2013

We present measurements of direct photon pair production cross sections using 8.5 fb(-1) of data collected with the D0 detector at the Fermilab Tevatron p (p) over bar collider. The results are presented as differential distributions of the photon pair invariant mass d sigma/dM(gamma gamma), pair transverse momentum d sigma/dp(T)(gamma gamma) azimuthal angle between the photons d sigma/d Delta(phi)(gamma gamma), and polar scattering angle in the Collins-Soper frame d sigma/d vertical bar cos theta*vertical bar. Measurements are performed for isolated photons with transverse momenta p(T)(gamma) > 18 (17) GeV for the leading (next-to-leading) photon in P-T, pseudorapidities vertical bar eta(g…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsPhoton010308 nuclear & particles physicsBar (music)Astrophysics::High Energy Astrophysical PhenomenaTevatron7. Clean energy01 natural sciencesNuclear physicsPair production0103 physical sciencesHigh Energy Physics::ExperimentInvariant massRapidity010306 general physicsParton showerPhysics Letters B
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The ATLAS Inner Detector commissioning and calibration

2010

The ATLAS Inner Detector is a composite tracking system consisting of silicon pixels, silicon strips and straw tubes in a 2 T magnetic field. Its installation was completed in August 2008 and the detector took part in data-taking with single LHC beams and cosmic rays. The initial detector operation, hardware commissioning and insitu calibrations are described. Tracking performance has been measured with 7.6 million cosmic-ray events, collected using a tracking trigger and reconstructed with modular pattern-recognition and fitting software. The intrinsic hit efficiency and tracking trigger efficiencies are close to 100%. Lorentz angle measurements for both electrons and holes, specific energ…

Physics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsAstronomyTracking (particle physics)Modules7. Clean energy01 natural sciencesATLAS; calibrationHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Heavy IonsDetectors and Experimental TechniquesDetectors de radiacióPhysicsLarge Hadron ColliderDetectorSettore FIS/01 - Fisica SperimentaleInstrumentation and Detectors (physics.ins-det)ATLASAstrophysics and CosmologyTransition radiation detectormedicine.anatomical_structureIonization EnergyComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCElementary ParticlesQuantum Field TheoryParticle physicsFOS: Physical sciencesCosmic rayddc:500.2HadronsSilicon Pixel Sensors530OpticsQuantum Field TheoriesAtlas (anatomy)0103 physical sciencesCalibrationmedicineddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Measurement Science and InstrumentationOptoelectronics010306 general physicsString TheoryEngineering (miscellaneous)ReadoutNuclear PhysicsATLAS detectorbusiness.industry010308 nuclear & particles physicsFísicaSemiconductor TrackerTransition radiationExperimental High Energy Physicsbusiness
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Search for Violation ofCPTand Lorentz Invariance inBs0Meson Oscillations

2015

We present the first search for CPT-violating effects in the mixing of B-s(0) mesons using the full Run II data set with an integrated luminosity of 10.4 fb(-1) of proton-antiproton collisions coll ...

PhysicsParticle physicsLuminosity (scattering theory)Meson010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyLorentz covariance01 natural sciencesAsymmetryTheoretical physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsMixing (physics)media_commonPhysical Review Letters
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Model-independent measurement of t-channel single top quark production in pp¯ collisions at s=1.96 TeV

2011

We present a model-independent measurement of $t$-channel electroweak production of single top quarks in $\ppbar$ collisions at $\sqrt{s}=1.96\;\rm TeV$. Using $5.4\;\rm fb^{-1}$ of integrated luminosity collected by the D0 detector at the Fermilab Tevatron Collider, and selecting events containing an isolated electron or muon, missing transverse energy and one or two jets originating from the fragmentation of $b$ quarks, we measure a cross section $\sigma({\ppbar}{\rargap}tqb+X) = 2.90 \pm 0.59\;\rm (stat+syst)\; pb$ for a top quark mass of $172.5\;\rm GeV$. The probability of the background to fluctuate and produce a signal as large as the one observed is $1.6\times10^{-8}$, corresponding…

QuarkPhysicsNuclear and High Energy PhysicsTop quarkParticle physicsMuon010308 nuclear & particles physicsElectroweak interactionTevatronParticle acceleratorElectron7. Clean energy01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentFermilabNuclear Experiment010306 general physicsPhysics Letters B
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Search for massive long-lived highly ionising particles with the ATLAS detector at the LHC

2011

A search is made for massive highly ionising particles with lifetimes in excess of 100 ns, with the ATLAS experiment at the Large Hadron Collider, using 3.1 pb-1 of pp collision data taken at √s = 7TeV. The signature of energy loss in the ATLAS inner detector and electromagnetic calorimeter is used. No such particles are found and limits on the production cross section for electric charges 6e ≤ |q| ≤ 17e and masses 200 GeV ≤ m ≤ 1000 GeV are set in the range 1–12 pb for different hypotheses on the production mechanism.

Nuclear and High Energy PhysicsParticle physicsNew PhysicsCiências Naturais::Ciências FísicasPhysics::Instrumentation and DetectorsPhysics beyond the Standard Model:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesHigh-energy collider experiment; Long-lived particle; Highly ionising; New physicsHigh-energy collider experimentddc:500.253001 natural sciencesHigh Energy Physics - ExperimentNuclear physicslong-lived particle; high-energy collider experiment; new physics; highly ionisingHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)0103 physical sciencesMASSIVE CHARGED PARTICLESmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy PhysicsHighly ionisingNew physics010306 general physicsNuclear ExperimentPhysicsRange (particle radiation)Large Hadron ColliderScience & Technology010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleDetectorATLAS experimentDrell–Yan processFísicaATLASLong-lived particleTransition radiation detectormedicine.anatomical_structureExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Search for charged massive long-lived particles

2012

We report on a search for charged massive long-lived particles (CMLLPs), based on 5.2 fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron $p\bar{p}$ collider. We search for events in which one or more particles are reconstructed as muons but have speed and ionization energy loss $(dE/dx)$ inconsistent with muons produced in beam collisions. CMLLPs are predicted in several theories of physics beyond the standard model. We exclude pair-produced long-lived gaugino-like charginos below 267 GeV and higgsino-like charginos below 217 GeV at 95% C.L., as well as long-lived scalar top quarks with mass below 285 GeV.

Particle physicsPhysics beyond the Standard ModelTevatronFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesHigh Energy Physics - ExperimentStandard Modellaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderPhysicsMuonLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyParticle acceleratorExperimental High Energy PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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Search for Down-Type Fourth Generation Quarks with the ATLAS Detector in Events with One Lepton and Hadronically Decaying W Bosons

2012

This Letter presents a search for pair production of heavy down-type quarks decaying via b′→Wt in the lepton+jets channel, as b′¯b′→W−tW+¯t→b¯bW+W−W+W−→l±νb¯bq¯qq¯qq¯q. In addition to requiring exactly one lepton, large missing transverse momentum, and at least six jets, the invariant mass of nearby jet pairs is used to identify high transverse momentum W bosons. In data corresponding to an integrated luminosity of 1.04  fb−1 from pp collisions at √s=7  TeV recorded with the ATLAS detector, a heavy down-type quark with mass less than 480 GeV can be excluded at the 95% confidence level.

QuarkTop quarkParticle physicsFOURTH GENERATIONCiências Naturais::Ciências FísicasAtlas detectorAtlas detectorAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesGeneral Physics and Astronomyddc:500.253001 natural sciencesHigh Energy Physics - ExperimentquarksNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesddc:550Fourth generationInvariant mass010306 general physicsNuclear ExperimentDetectors de radiacióBosonPhysicsScience & Technology010308 nuclear & particles physicsATLAS DetectorSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaTop quarkPair productionHADRON-HADRON COLLISIONSExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHadronic collidersFísica nuclearHigh Energy Physics::Experimentheavy down-type quarks; quarkParticle Physics - ExperimentLepton
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Tevatron Run II combination of the effective leptonic electroweak mixing angle

2018

The Ministry of Science and Innovation and the Consolider-Ingenio 2010 Program and the European Union community Marie Curie Fellowship Contract No. 302103.

Drell-Yan processsemianalytical programsPhysics and Astronomy (miscellaneous)FERMION PAIR PRODUCTIONUPGRADETevatronhadron-colliders01 natural sciencesHigh Energy Physics - ExperimentPhysics Particles & Fieldselectron: pair productionHigh Energy Physics - Experiment (hep-ex)MONTE-CARLOUNIVERSAL MONTE-CARLOELECTROMAGNETIC CALORIMETERDZERO[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]HADRON COLLIDERSangular distributionBatavia TEVATRON CollMonte CarloPhysicsscattering [anti-p p]gauge bosonPhysicsElectroweak interactionDrell–Yan processWeinberg anglespontaneous symmetry breaking [electroweak interaction]muon: pair productionPhysical Sciencesmixing angle [electroweak interaction]bosonPHOTOSmass: measured [W]asymmetryParticle physicsFOS: Physical sciencesSEMIANALYTICAL PROGRAMddc:500.2Astronomy & Astrophysicselectroweak interaction: spontaneous symmetry breaking114 Physical sciences530programmingW: mass: measuredStandard Modelanti-p p: colliding beams[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]hadroproduction [Z0]0103 physical sciencesanti-p p: scatteringddc:530High Energy Physicspair production [electron]pair production [muon]CALORIMETER010306 general physicsQED RADIATIVE-CORRECTIONSQed radiative-corrections; fermion pair production; universal; Monte Carlo; parton distributions; hadron-colliders; electromagnetic; calorimeter;semianalytical programs; E(+)E(-) annihilation; boson; production; D0 detectorGauge bosonBOSON PRODUCTIONMuonScience & Technologyelectroweak interaction: mixing angleAnti-p p: scattering | anti-p p: colliding beams | Z0: hadroproduction | Z0: leptonic decay | electroweak interaction: spontaneous symmetry breaking | electroweak interaction: mixing angle | muon: pair production | W: mass: measured | Weinberg angle | Batavia TEVATRON Coll | angular distribution | electron: pair production | Drell-Yan process | gauge boson | programming | asymmetry | CDF | DZERO | experimental resultsIDENTIFICATION010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyuniversalWeinberg angleZ0: hadroproductionQED RADIATIVE-CORRECTIONS; FERMION PAIR PRODUCTION; UNIVERSAL; MONTE-CARLO; PARTON DISTRIBUTIONS; HADRON COLLIDERS; ELECTROMAGNETIC; CALORIMETER; SEMIANALYTICAL PROGRAM; E(+)E(-) ANNIHILATION; BOSON; PRODUCTION; D0 DETECTORleptonic decay [Z0]E(+)E(-) ANNIHILATIONelectromagneticPARTON DISTRIBUTIONSExperimental High Energy PhysicsZ0: leptonic decayD0 DETECTORCDFHigh Energy Physics::Experimentproductioncolliding beams [anti-p p]Leptonexperimental results
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Determination of the pole and MS¯ masses of the top quark from the tt¯ cross section

2011

We use higher-order quantum chromodynamics calculations to extract the mass of the top quark from the ttbar cross section measured in the lepton+jets channel in ppbar collisions at sqrt(s)=1.96 TeV using 5.3 fb-1 of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider. The extracted top quark pole mass and MSbar mass are compared to the current Tevatron average top quark mass obtained from direct measurements.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyTevatronD0 experiment7. Clean energy01 natural sciencesBottom quarkNuclear physics0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentB mesonFermilab010306 general physicsPhysics Letters B
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Search for a narrowtt¯resonance inpp¯collisions ats=1.96  TeV

2012

We report a search for a narrow ttbar resonance that decays into a lepton+jets final state based on an integrated luminosity of 5.3/fb of proton-antiproton collisions at sqrt{s}=1.96 TeV collected by the D0 Collaboration at the Fermilab Tevatron Collider. We set upper limits on the production cross section of such a resonance multiplied by its branching fraction to ttbar which we compare to predictions for a leptophobic topcolor Z' boson. We exclude such a resonance at the 95% confidence level for masses below 835 GeV.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyTevatronTopcolor01 natural sciencesResonance (particle physics)law.inventionNuclear physicslaw0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilabNuclear Experiment010306 general physicsColliderBosonLeptonPhysical Review D
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Search for decays of stopped, long-lived particles from 7 TeV pp collisions with the ATLAS detector

2012

New metastable massive particles with electric and colour charge are features of many theories beyond the Standard Model. A search is performed for long-lived gluino-based R-hadrons with the ATLAS detector at the LHC using a data sample corresponding to an integrated luminosity of 31 pb[superscript −1]. We search for evidence of particles that have come to rest in the ATLAS detector and decay at some later time during the periods in the LHC bunch structure without proton–proton collisions. No significant deviations from the expected backgrounds are observed, and a cross-section limit is set. It can be interpreted as excluding gluino-based R-hadrons with masses less than 341 GeV at the 95 % …

Physics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsPhysics beyond the Standard ModelCiencias Físicas01 natural sciencesLong lived particlesLuminosityHigh Energy Physics - Experiment//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)R-hadronspp collisions; ATLAS detector[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentDetectors de radiacióPhysicsGluinoLarge Hadron ColliderSplit supersymmetrySettore FIS/01 - Fisica SperimentaleATLASmedicine.anatomical_structurePhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASParticle physicsFOS: Physical sciencesddc:500.2530Partícules (Física nuclear)Nuclear physicsAtlas (anatomy)0103 physical sciencesCollidersmedicineFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Split Supersymmetry010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNEW PHYSICS//purl.org/becyt/ford/1.3 [https]AstronomíaR-hadronHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Experimental High Energy PhysicsNeutralinoHigh Energy Physics::Experiment
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Combined search for the Higgs boson with the D0 experiment

2013

We perform a combination of searches for standard model Higgs boson production in $p\bar{p}$ collisions recorded by the D0 detector at the Fermilab Tevatron Collider at a center of mass energy of $\sqrt{s}=1.96$ TeV. The different production and decay channels have been analyzed separately, with integrated luminosities of up to 9.7 fb$^{-1}$ and for Higgs boson masses $90\leq M_H \leq 200$ GeV. We combine these final states to achieve optimal sensitivity to the production of the Higgs boson. We also interpret the combination in terms of models with a fourth generation of fermions, and models with suppressed Higgs boson couplings to fermions. The result excludes a standard model Higgs boson …

Nuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::LatticeTevatronFOS: Physical sciences01 natural sciencesStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsNuclear ExperimentPhysicsCondensed Matter::Quantum GasesLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFermionD0 experimentSearch for the Higgs bosonExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonHigh Energy Physics::Experiment
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Search for events with large missing transverse momentum, jets, and at least two tau leptons in 7 TeV proton–proton collision data with the ATLAS det…

2012

A search for events with large missing transverse momentum, jets, and at least two tau leptons has been performed using 2 fb[superscript −1] of proton–proton collision data at √s = 7 TeV recorded with the ATLAS detector at the Large Hadron Collider. No excess above the Standard Model background expectation is observed and a 95% CL upper limit on the visible cross section for new phenomena is set, where the visible cross section is defined by the product of cross section, branching fraction, detector acceptance and event selection efficiency. A 95% CL lower limit of 32 TeV is set on the gauge-mediated supersymmetry breaking (GMSB) scale Λ independent of tan β. These limits provide the most s…

Nuclear and High Energy PhysicsParticle physicsAtlas detectortau leptonsAstrophysics::High Energy Astrophysical PhenomenaPhysics beyond the Standard ModelMonte Carlo methodFOS: Physical sciencesddc:500.27. Clean energy01 natural sciences530Partícules (Física nuclear)Settore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)tau leptons; jets; ATLAS detector0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physicstransverse momentum: missing-energy; new physics; Monte Carlo; supersymmetry: symmetry breaking; 70000 GeV-cms; jet: multiple production; mediation: gauge; supersymmetry: parameter space; tau: semileptonic decay; CERN LHC Coll; ATLAS; p p --> (n)jet 2tau anything; experimental results; cross section: upper limit; p p: scattering010306 general physicsNuclear ExperimentCiencias ExactasDetectors de radiacióPhysics010308 nuclear & particles physicsAcceleradors de partículesSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaATLASCollisionDYNAMICAL SUPERSYMMETRY BREAKINGHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Experimental High Energy PhysicsTransverse momentumComputingMethodologies_DOCUMENTANDTEXTPROCESSINGPhysics::Accelerator Physicsproton-proton collisionsHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentLepton
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Observation of a narrow mass state decaying intoΥ(1S)+γinpp¯collisions ats=1.96  TeV

2012

Using data corresponding to an integrated luminosity of 1.3 fb(-1), we observe a narrow mass state decaying into Gamma(1S) + gamma, where the Gamma(1S) meson is detected by its decay into a pair of oppositely charged muons, and the photon is identified through its conversion into an electron-positron pair. The significance of this observation is 5.6 standard deviations. The mass of the state is centered at 10.551 +/- 0.014(stat) +/- 0.017(syst) GeV/c(2), which is consistent with that of the state recently observed by the ATLAS Collaboration.

PhysicsNuclear and High Energy PhysicsPhotonMuonMeson010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaState (functional analysis)01 natural sciencesLuminosityNuclear physicsmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review D
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Measurement of spin correlation between top and antitop quarks produced in pp¯ collisions at s=1.96 TeV

2016

Department of Energy (United States of America); National Science Foundation (United States of America); Alternative Energies and Atomic Energy Commission (France); National Center for Scientific Research/ National Institute of Nuclear and Particle Physics (France); Ministry of Education and Science of the Russian Federation (Russia); National Research Center "Kurchatov Institute" of the Russian Federation (Russia); Russian Foundation for Basic Research (Russia); National Council for the Development of Science and Technology (Brazil); Carlos Chagas Filho Foundation for the Support of Research in the State of Rio de Janeiro (Brazil); Department of Atomic Energy (India); Department of Science…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsmedia_common.quotation_subjectAtomic energyLibrary science7. Clean energy01 natural scienceslanguage.human_languageBildungGermanNuclear physicsState (polity)Basic research0103 physical scienceslanguageChristian ministry010306 general physicsChinaResearch centermedia_commonPhysics Letters B
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Measurement of the production fraction times branching fractionf(b→Λb)·B(Λb→J/ψΛ)

2011

The \Lambda_b(udb) baryon is observed in the decay \Lambda_b --> J/\psi \Lambda using 6.1 fb^{-1} of p\bar{p} collisions collected with the D0 detector at \sqrt{s}=1.96 TeV. The production fraction multiplied by the branching fraction for this decay relative to that for the decay B^0 --> J/\psi K^0_s is measured to be 0.345 \pm 0.034 (stat.) \pm 0.033 (syst.) \pm 0.003 (PDG). Using the world average value of f(b --> B^0)B(B^0 --> J/\psi K^0_s) = (1.74 \pm 0.08) \times 10^{-5}, we obtain f(b --> \Lambda_b)B(\Lambda_{b} --> J/\psi \Lambda) = (6.01 \pm 0.60 (stat.) \pm 0.58 (syst.) \pm 0.28 (PDG)) \times 10^{-5}. This measurement represents an improvement in precision by about a factor of thre…

BaryonPhysicsNuclear and High Energy PhysicsTheoretical physics010308 nuclear & particles physicsBranching fraction0103 physical sciencesAnalytical chemistryProduction (computer science)010306 general physicsLambda01 natural sciencesPhysical Review D
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Evidence for s-channel single top quark production in pp¯ collisions at s=1.96 TeV

2013

We present measurements of the cross sections for the two main production modes of single top quarks in p (p) over bar collisions at root s = 1.96 TeV in the Run II data collected with the DO detector at the Fermilab Tevatron Collider, corresponding to an integrated luminosity of 9.7 fb(-1). The s-channel cross section is measured to be sigma(p (p) over bar -> tb + X) = 1.10(-0.31)(+0.33) pb with no assumptions on the value of the t-channel cross section. Similarly, the t-channel cross section is measured to be sigma(p (p) over bar -> tqb + X) = 3.07(-0.49)(+0.54) pb. We also measure the s + t combined cross section as sigma(p (p) over bar -> tb + X, tqb + X) = 4.11(-0.55)(+0.60) ph and set…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixTevatron01 natural sciences7. Clean energylaw.inventionNuclear physicsCross section (physics)law0103 physical sciencesFermilab010306 general physicsColliderBar (unit)Physics Letters B
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Measurement of the distributions of event-by-event flow harmonics in lead-lead collisions at = 2.76 TeV with the ATLAS detector at the LHC

2013

We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; ISF, MINERVA, GIF, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW, Poland; GRICES and FCT, Portu…

Atlas detectorUnfolding01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Heavy-ion collisionNaturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)RELATIVISTIC HEAVY-ION COLLISIONSNuclear ExperimentNuclear ExperimentQCunfoldingPhysicsLarge Hadron ColliderAtlas (topology)4. EducationSettore FIS/01 - Fisica SperimentaleEvent-By-Event FluctuationElliptic flowHeavy-Ion CollisionsHarmonic FlowCharged particlehadron-hadron scattering; harmonic flow; event-by-event fluctuation; unfolding; heavy-ion collisionHarmonicsImpact parameterNatural Sciencesharmonic flowParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências Físicas530 Physics:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesComputer Science::Digital Libraries530Nuclear physics0103 physical sciencesHeavy ion collisionsddc:530Rapidity010306 general physicsevent-by-event fluctuationCiencias ExactasScience & TechnologyHadron-Hadron Scattering010308 nuclear & particles physicsFísicaheavy ion collisionHeavy-ion collision; harmonic flow; event-by-event fluctuation; unfolding; Hadron-Hadron Scattering
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Measurement of Wγ and Zγ production in proton-proton collisions at √s =7 TeV with the ATLAS detector

2011

Artículo escrito por un elevado número de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboración, si le hubiere, y los autores pertenecientes a la UAM

Particle physics:Mathematics and natural science: 400::Physics: 430 [VDP]Nuclear and High Energy PhysicsProtonAtlas detectorFOS: Physical sciencesddc:500.2:Mathematics and natural science: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]Hadron-hadron scattering01 natural sciences7. Clean energy530High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)0103 physical sciencesmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsPhysicsW BOSONHadron-Hadron Scattering010308 nuclear & particles physicsATLAS experimentHigh Energy Physics::PhenomenologyFísicaATLASHigh energy photonmedicine.anatomical_structureZ BOSONW and Z bosonsHADRON-HADRON COLLISIONSFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Search for the Higgs boson in lepton, tau and jets final states

2013

We present a search for the standard model Higgs boson in final states with an electron or muon and a hadronically decaying tau lepton in association with two or more jets using 9.7 fb^{-1} of Run II Fermilab Tevatron Collider data collected with the D0 detector. The analysis is sensitive to Higgs boson production via gluon fusion, associated vector boson production, and vector boson fusion, followed by the Higgs boson decay to tau lepton pairs or to W boson pairs. The ratios of 95% C.L. upper limits on the cross section times branching ratio to those predicted by the standard model are obtained for orthogonal subsamples that are enriched in either H -&gt; tau tau decays or H -&gt; WW decay…

PhysicsNuclear and High Energy PhysicsParticle physicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciences01 natural sciences7. Clean energySearch for the Higgs bosonVector bosonStandard ModelGluonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesExperimental High Energy PhysicsHiggs boson[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsLepton
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Measurement of the tt¯ production cross section using dilepton events in pp¯ collisions

2011

We present a measurement of the a production cross section sigma((u) over bar) in p (p) over bar collisions at root s = 1.96 TeV using 5.4 fb(-1) of integrated luminosity collected with the D0 detector. We consider final states with at least two jets and two leptons (ee, e mu, mu mu), and events with one jet for the e mu final state as well. The measured cross section is sigma((u) over bar) = 7.36(-0.79)(+0.90)(stat + syst) pb. This result combined with the cross section measurement in the lepton + jets final state yields sigma((u) over bar) = 7.56(-0.56)(+0.63)(stat + syst) pb, which agrees with the standard model expectation. The relative precision of 8% of this measurement is comparable …

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsSigmaJet (particle physics)7. Clean energy01 natural sciencesStandard ModelNuclear physicsCross section (physics)0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)010306 general physicsBar (unit)LeptonPhysics Letters B
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Evidence for the spin-0 nature of the Higgs boson using ATLAS data

2013

We acknowledge the support of ANPCyT, Argentina; YerPhl, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; ISF, MINERVA, GIF, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW, Poland; GRICES and FCT, Portu…

Physics::Instrumentation and DetectorsCiencias FísicasHiggs boson; Parity; Spinspin01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHiggs boson; Spin; Parity//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)Naturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QCPhysicsLarge Hadron ColliderAtlas (topology)4. EducationATLAS experimentSettore FIS/01 - Fisica SperimentaleATLASQuantum numberParityparityHiggs bosonComputingMethodologies_DOCUMENTANDTEXTPROCESSINGCondensed Matter::Strongly Correlated ElectronsFísica nuclearLHCNatural SciencesParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASParticle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências Físicas530 PhysicsHiggs boson:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicsSpin0103 physical sciencesddc:530HiggsbosonHigh Energy Physics010306 general physicsCiencias ExactasCoupling constantparity; spin; higgs bosonspin-0 natureScience & Technology010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaParity (physics)//purl.org/becyt/ford/1.3 [https]Higgs boson; Parity; Spin; Nuclear and High Energy PhysicsATLAS dataAstronomíaHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentLepton
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Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector

2011

A measurement of jet activity in the rapidity interval bounded by a dijet system is presented. Events are vetoed if a jet with transverse momentum greater than 20 GeV is found between the two boundary jets. The fraction of dijet events that survive the jet veto is presented for boundary jets that are separated by up to six units of rapidity and with mean transverse momentum 50 < p¯T < 500 GeV. The mean multiplicity of jets above the veto scale in the rapidity interval bounded by the dijet system is also presented as an alternative method for quantifying perturbative QCD emission. The data are compared to a next-to-leading order plus parton shower prediction from the powheg-box, an all-order…

DIJETSParticle physicsNuclear and High Energy Physics:Mathematics and natural science: 400::Physics: 430 [VDP]Ciências Naturais::Ciências FísicasAtlas detectorAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]Monte Carlo methodFOS: Physical sciencesddc:500.2:Mathematics and natural science: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]01 natural sciences530High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Rapidityddc:530High Energy PhysicsResummation010306 general physicsParton showerNuclear ExperimentPhysicsScience & TechnologyHadron-Hadron Scattering010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyPerturbative QCDATLASBounded functionHADRON-HADRON COLLISIONSTransverse momentumFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Commissioning of the ATLAS Muon Spectrometer with cosmic rays

2010

The ATLAS detector at the Large Hadron Collider has collected several hundred million cosmic ray events during 2008 and 2009. These data were used to commission the Muon Spectrometer and to study the performance of the trigger and tracking chambers, their alignment, the detector control system, the data acquisition and the analysis programs. We present the performance in the relevant parameters that determine the quality of the muon measurement. We discuss the single element efficiency, resolution and noise rates, the calibration method of the detector response and of the alignment system, the track reconstruction efficiency and the momentum measurement. The results show that the detector i…

SystemAstrofísicaDriftPhysics - Instrumentation and DetectorsMuon SpectrometerPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsTracking (particle physics)01 natural sciences7. Clean energyHigh Energy Physics - ExperimentDrift TubeMDTHigh Energy Physics - Experiment (hep-ex)Data acquisitionATLAS muon spectrometer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesNuclear ExperimentPhysicsLarge Hadron Collidercosmic ray eventsDetectorSettore FIS/01 - Fisica SperimentaleBeamInstrumentation and Detectors (physics.ins-det)ATLASmedicine.anatomical_structureTrack ReconstructionPhysical SciencesFísica nuclearLHCmuon measurementFOS: Physical sciencesCosmic rayddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesCalibrationmedicineFysikddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsEngineering (miscellaneous)Ciencias ExactasMuonChambersMuon TrackCosmologiaATLAS detector010308 nuclear & particles physicsFísicaTrack SegmentPhysics::Accelerator Physicsproton-proton collisionsHigh Energy Physics::Experiment
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Readiness of the ATLAS liquid argon calorimeter for LHC collisions

2010

The ATLAS liquid argon calorimeter has been operating continuously since August 2006. At this time, only part of the calorimeter was readout, but since the beginning of 2008, all calorimeter cells have been connected to the ATLAS readout system in preparation for LHC collisions. This paper gives an overview of the liquid argon calorimeter performance measured in situ with random triggers, calibration data, cosmic muons, and LHC beam splash events. Results on the detector operation, timing perfor-mance, electronics noise, and gain stability are presented. High energy deposits from radiative cosmic muons and beam splash events allow to check the intrinsic constant term of the energy resolutio…

Physics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)large hadron colliderPhysics::Instrumentation and DetectorsMonte Carlo method7. Clean energy01 natural sciences010305 fluids & plasmasHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Radiative transfer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesDetectors de radiacióPhysicsLarge Hadron ColliderAcceleradors de partículesDetectorSettore FIS/01 - Fisica SperimentaleInstrumentation and Detectors (physics.ins-det)ATLASLHC Collisionsmedicine.anatomical_structurePhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCNoise (radio)chemistry.chemical_elementFOS: Physical sciencesComputer Science::Digital Libraries530Partícules (Física nuclear)Nuclear physicsAtlas (anatomy)0103 physical sciencesmedicineATLAS; liquid argon; calorimeter; LHC; collisionsFysikddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsEngineering (miscellaneous)Ciencias ExactasArgónArgonCalorimeter (particle physics)010308 nuclear & particles physicsFísicachemistryExperimental High Energy PhysicsHigh Energy Physics::Experimentelectromagnetic shower
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Search for second generation scalar leptoquarks in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

2012

The results of a search for the production of second generation scalar leptoquarks are presented for final states consisting of either two muons and at least two jets or a muon plus missing transverse momentum and at least two jets. A total of 1.03 fb−1 integrated luminosity of proton-proton collision data produced by the Large Hadron Collider at \(\sqrt{s}=7~\mbox{TeV}\) and recorded by the ATLAS detector is used for the search. The event yields in the signal regions are found to be consistent with the Standard Model background expectations. The production of second generation leptoquarks is excluded for a leptoquark mass mLQ<594 (685) GeV at 95 % confidence level, for a branching ratio of…

Physics and Astronomy (miscellaneous)Atlas detectorPhysics::Instrumentation and DetectorsCiencias Físicas7. Clean energy01 natural sciencesHigh Energy Physics - Experiment//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)Naturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentDetectors de radiacióddc:539PhysicsLarge Hadron ColliderSettore FIS/01 - Fisica SperimentaleScalar LeptoquarksATLASComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCNatural SciencesParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASQuarkPair productionCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2leptoquarks530Partícules (Física nuclear)Nuclear physicsLeptoquarks0103 physical sciencesLeptoquarkddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias ExactasHadron-Hadron ScatteringMuonScience & TechnologyATLAS detector010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyScalar (physics)Física//purl.org/becyt/ford/1.3 [https]AstronomíaPair productionHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Experimental High Energy PhysicsPhysics::Accelerator Physicsproton-proton collisionsHigh Energy Physics::Experiment
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Study of the X±(5568) state with semileptonic decays of the Bs0 meson

2018

We present a study of the X±(5568) using semileptonic decays of the Bs0 meson using the full run II integrated luminosity of 10.4  fb-1 in proton-antiproton collisions at a center of mass energy of 1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. We report evidence for a narrow structure, X±(5568), in the decay sequence X±(5568)→Bs0π± where Bs0→μ∓Ds±X, Ds±→ϕπ± which is consistent with the previous measurement by the D0 Collaboration in the hadronic decay mode, X±(5568)→Bs0π± where Bs0→J/ψϕ. The mass and width of this state are measured using a combined fit of the hadronic and semileptonic data, yielding m=5566.9-3.1+3.2(stat)-1.2+0.6(syst)  MeV/c2, Γ=18.6-6.1+7.9(s…

PhysicsParticle physicsLuminosity (scattering theory)Meson010308 nuclear & particles physicsHadronTevatronState (functional analysis)01 natural sciences7. Clean energylaw.inventionlaw0103 physical sciencesHigh Energy Physics::ExperimentCenter of massFermilabNuclear Experiment010306 general physicsColliderPhysical Review D
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Search for anomalous quarticWWγγcouplings in dielectron and missing energy final states inpp¯collisions ats=1.96  TeV

2013

We present a search for anomalous components of the quartic gauge boson coupling WW gamma gamma in events with an electron, a positron and missing transverse energy. The analyzed data correspond to 9.7 fb(-1) of integrated luminosity collected by the D0 detector in p (p) over bar collisions at root s 1.96 TeV. The presence of anomalous quartic gauge couplings would manifest itself as an excess of boosted WW events. No such excess is found in the data, and we set the most stringent limits to date on the anomalous coupling parameters a(0)(W) and a(C)(W). When a form factor with Lambda(cutoff) = 0.5 TeV is used, the observed upper limits at 95% C. L. are vertical bar a(0)(W)/Lambda(2)vertical …

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonMissing energyLuminosity (scattering theory)010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Gauge (firearms)Lambda01 natural sciencesQuartic function0103 physical sciencesHigh Energy Physics::ExperimentStatistical physics010306 general physicsBar (unit)Physical Review D
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Double parton interactions inγ+3jet andγ+b/cjet+2jet events inpp¯collisions ats=1.96 TeV

2014

We determine the fraction of events with double parton (DP) Scattering in a single p (p) over bar collisions at root s = 1.96 TeV in gamma + 3 jet and gamma + b/c jet + 2 jet events collected with the D0 detector and corresponding to an integrated luminosity of about 8.7 fb(-1). The DP fractions and effective cross sections (sigma(eff)) are measured for both event samples using the same kinematic selections. The measured DP fractions range from 0.21 to 0.17, with effective cross sections in the gamma + 3 jet and gamma + b/cjet + 2 jet samples of sigma(incl)(eff) = 12.7 +/- 0.2(stat) +/- 1.3(syst) mb and sigma(HF)(eff) = 14.6 +/- 0.6(stat) +/- 3.2(syst) mb, respectively.

PhysicsNuclear and High Energy PhysicsParticle physicsJet (fluid)Luminosity (scattering theory)PhotonScatteringAstrophysics::High Energy Astrophysical PhenomenaSigmaPartonNuclear physicsHigh Energy Physics::ExperimentNuclear ExperimentBar (unit)Physical Review D
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Measurement of top quark polarization in tt¯ lepton+jets final states

2017

Department of Energy (USA); National Science Foundation (USA); Alternative Energies and Atomic Energy Commission and National Center for Scientific Research/National Institute of Nuclear and Particle Physics (France); Ministry of Education and Science of the Russian Federation (Russia); National Research Center "Kurchatov Institute" of the Russian Federation (Russia); Russian Foundation for Basic Research (Russia); Carlos Chagas Filho Foundation for the Support of Research in the State of Rio de Janeiro (Brazil); Department of Science and Technology (India); Administrative Department of Science, Technology and Innovation (Colombia); National Council of Science and Technology (Mexico); Natio…

Physics010308 nuclear & particles physicsAtomic energyLibrary science7. Clean energy01 natural scienceslanguage.human_languageBildungGermanBasic research0103 physical scienceslanguageRussian federationChristian ministry010306 general physicsChinaResearch centerPhysical Review D
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Measurement of the forward-backward asymmetry inΛb0andΛ¯b0baryon production inpp¯collisions ats=1.96TeV

2015

We measure the forward-backward asymmetry in the production of Lambda(0)(b) and (Lambda) over bar (0)(b) baryons as a function of rapidity in p (p) over bar collisions at root s = 1.96 TeV using 10.4 fb(-1) of data collected with the D0 detector at the Fermilab Tevatron collider. The asymmetry is determined by the preference of Lambda(0)(b) or (Lambda) over bar (0)(b) particles to be produced in the direction of the beam protons or antiprotons, respectively. The measured asymmetry integrated over rapidity y in the range 0.1 < vertical bar y vertical bar < 2.0 is A = 0.04 +/- 0.07(stat) +/- 0.02(syst).

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronLambdaAsymmetrylaw.inventionBaryonNuclear physicslawAntiprotonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentRapidityNuclear ExperimentCollidermedia_commonBar (unit)Physical Review D
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Simultaneous measurement of forward-backward asymmetry and top polarization in dilepton final states fromtt¯production at the Tevatron

2015

We present a simultaneous measurement of the forward-backward asymmetry and the top-quark polarization in t (t) over bar production in dilepton final states using 9.7 fb(-1) of proton-antiproton collisions at root s = 1.96 TeV with the D0 detector. To reconstruct the distributions of kinematic observables we employ a matrix element technique that calculates the likelihood of the possible t (t) over bar kinematic configurations. After accounting for the presence of background events and for calibration effects, we obtain a forward-backward asymmetry of A(t (t) over bar) = (15.0 +/- 6.4(stat) +/- 4.9(syst)) % and a top-quark polarization times spin analyzing power in the beam basis of kappa P…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsmedia_common.quotation_subjectTevatronObservableForward backwardPolarization (waves)01 natural sciencesAsymmetryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentMatrix elementNuclear Experiment010306 general physicsLeptonmedia_commonPhysical Review D
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Combined Forward-Backward Asymmetry Measurements in Top-Antitop Quark Production at the Tevatron

2018

The CDF and D0 experiments at the Fermilab Tevatron have measured the asymmetry between yields of forward- and backward-produced top and antitop quarks based on their rapidity difference and the asymmetry between their decay leptons. These measurements use the full data sets collected in proton-antiproton collisions at a center-of-mass energy of √s=1.96  TeV. We report the results of combinations of the inclusive asymmetries and their differential dependencies on relevant kinematic quantities. The combined inclusive asymmetry is At¯tFB=0.128±0.025. The combined inclusive and differential asymmetries are consistent with recent standard model predictions.

Top quarkTevatronGeneral Physics and Astronomypair production [top]01 natural sciences7. Clean energyHigh Energy Physics - ExperimentSubatomär fysikHigh Energy Physics - Experiment (hep-ex)DZEROSubatomic Physicsddc:550[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Quantum ChromodynamicsBatavia TEVATRON CollGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)media_commonPhysicsscattering [anti-p p]Particle properties02 Physical Sciencesrapidity: differenceCDF; Tevatron; top-quarkPhysicsdifference [rapidity]asymmetry [angular distribution]kinematicsPhysical Sciencestop: pair productionQuarkParticle physicsGeneral Physicsangular distribution: asymmetryTevatron Collidermedia_common.quotation_subjectPhysics MultidisciplinaryFOS: Physical sciencesForward backwardddc:500.2Hadron-hadron interactionsAsymmetryComputer Science::Digital Libraries114 Physical sciencesMarie curieCDF Collaborationanti-p p: colliding beamsPhysics and Astronomy (all)[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciencesanti-p p: scatteringmedia_common.cataloged_instanceddc:530High Energy PhysicsEuropean union010306 general physicsScience & Technology1960 GeV-cms010308 nuclear & particles physicshep-exHigh Energy Physics::PhenomenologyTop quarkQ007TFBResearch councilExperimental High Energy PhysicsCDFHigh Energy Physics::Experimentcolliding beams [anti-p p]High Energy Physics Top quark Hadron-hadron interactions Quantum Chromodynamics Particle properties Tevatron ColliderD0 Collaborationexperimental resultsPhysical Review Letters
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Measurement of the ratio of three-jet to two-jet cross sections in pp¯ collisions at s=1.96 TeV

2013

We present a measurement of the ratio of multijet cross sections in pp-bar collisions at sqrt(s) = 1.96 TeV at the Fermilab Tevatron Collider. The measurement is based on a data set corresponding to an integrated luminosity of 0.7 fb-1 collected with the D0 detector. The ratio of the inclusive three-jet to two-jet cross sections, R3/2, has been measured as a function of the jet transverse momenta. The data are compared to QCD predictions in different approximations. Popular tunes of the PYTHIA event generator do not agree with the data, while SHERPA provides a reasonable description of the data. A perturbative QCD prediction in next-to-leading order in the strong coupling constant, correcte…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsTevatronPerturbative QCDJet (particle physics)01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderEvent generatorPhysics Letters B
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Bounds on an Anomalous Dijet Resonance inW+jetsProduction inpp¯Collisions ats=1.96  TeV

2011

We present a study of the dijet invariant mass spectrum in events with two jets produced in association with a $W$ boson in data corresponding to an integrated luminosity of 4.3 fb$^{-1}$ collected with the D0 detector at $\sqrt{s} =1.96$ TeV. We find no evidence for anomalous resonant dijet production and derive upper limits on the production cross section of an anomalous dijet resonance recently reported by the CDF Collaboration, investigating the range of dijet invariant mass from 110 to 170 GeV/$c^2$. The probability of the D0 data being consistent with the presence of a dijet resonance with 4 pb production cross section at 145 GeV/$c^2$ is $8\times 10^{-6}$.

PhysicsParticle physicsLuminosity (scattering theory)Mass distribution010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyElementary particle01 natural sciencesResonance (particle physics)Spectral lineNuclear physics0103 physical sciencesMass spectrumHigh Energy Physics::ExperimentInvariant mass010306 general physicsBosonPhysical Review Letters
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Search for excited electrons and muons in root s=8 TeV proton-proton collisions with the ATLAS detector

2013

The ATLAS detector at the Large Hadron Collider is used to search for excited electrons and excited muons in the channel pp → ℓℓ* → ℓℓγ, assuming that excited leptons are produced via contact interactions. The analysis is based on 13 fb[superscript −1] of pp collisions at a centre-of-mass energy of 8 TeV. No evidence for excited leptons is found, and a limit is set at the 95% credibility level on the cross section times branching ratio as a function of the excited-lepton mass m[subscript ℓ*]. For m[subscript ℓ*] ≥ 0.8 TeV, the respective upper limits on σB(ℓ* → ℓγ) are 0.75 and 0.90 fb for the e* and μ* searches. Limits on σB are converted into lower bounds on the compositeness scale Λ. In …

Atlas detectorPhysics::Instrumentation and DetectorsCiencias FísicasGeneral Physics and Astronomy01 natural sciences7. Clean energyHigh Energy Physics - Experiment//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QCPhysicsddc:539Excited leptonsLarge Hadron ColliderLepton ProductionSettore FIS/01 - Fisica SperimentaleBranching ratioHERAATLASLarge Hadron ColliderExcited statePhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGQuarkLHCContact interactionExcited electronsParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASQuarkParticle physicsCiências Naturais::Ciências Físicas530 PhysicsParticle physics and field theory:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2excited electrons; muons; proton–proton collisions; ATLAS detector530Nuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsCentre-of-mass energiesCiencias ExactasHeraScience & TechnologyMuonATLAS detectorProton proton collisions010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyATLAS detectorsFísica//purl.org/becyt/ford/1.3 [https]AstronomíaHADRON-HADRON COLLISIONSExperimental High Energy PhysicsEp CollisionsHigh Energy Physics::Experimentproton-proton collisionsLepton
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Measurement of the top quark-pair production cross section with ATLAS in pp collisions at $\sqrt{s}=7$  TeV

2011

A measurement of the production cross-section for top quark pairs($\ttbar$) in $pp$ collisions at $\sqrt{s}=7 \TeV$ is presented using data recorded with the ATLAS detector at the Large Hadron Collider. Events are selected in two different topologies: single lepton (electron $e$ or muon $\mu$) with large missing transverse energy and at least four jets, and dilepton ($ee$, $\mu\mu$ or $e\mu$) with large missing transverse energy and at least two jets. In a data sample of 2.9 pb-1, 37 candidate events are observed in the single-lepton topology and 9 events in the dilepton topology. The corresponding expected backgrounds from non-$\ttbar$ Standard Model processes are estimated using data-driv…

QuarkTop quarkParticle physicsleptonsleptonPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsAtlas detector:Ciências Físicas [Ciências Naturais]Hadronddc:500.2TOP QUARK01 natural sciences7. Clean energydileptonHigh Energy Physics - ExperimentquarksNuclear physicspp collisionNaturvetenskap0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy PhysicsNuclear Experiment010306 general physicsEngineering (miscellaneous)Ciencias ExactasPhysicsScience & TechnologyLarge Hadron ColliderATLAS detectorATLAS detector; LHC; pp collisions; leptons; quarks010308 nuclear & particles physicsAtlas (topology)Settore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaATLASPair productionHadronic Collisionsproton-proton collisionsFísica nuclearHigh Energy Physics::ExperimentLHCNatural Sciencespp collisionsParticle Physics - ExperimentLeptonThe European Physical Journal C
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Measurement of multi-jet cross sections in proton-proton collisions at a 7 TeV center-of-mass energy

2011

Inclusive multi-jet production is studied in proton–proton collisions at a center-of-mass energy of 7 TeV, using the ATLAS detector. The data sample corresponds to an integrated luminosity of 2.4 pb−1. Results on multi-jet cross sections are presented and compared to both leading-order plus parton-shower Monte Carlo predictions and to next-to-leading-order QCD calculations.

ProtonPhysics and Astronomy (miscellaneous)EventsMonte Carlo methodJet (particle physics)01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQuantum chromodynamicsPhysicsLuminosity (scattering theory)PhysicsSettore FIS/01 - Fisica SperimentaleHERAATLASINCLUSIVE JET CROSS SECTIONPhotoproductionmedicine.anatomical_structurePhysical SciencesFísica nuclearLHCParticle Physics - ExperimentSimulationParticle physicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesproton–proton collisions; center-of-mass energymedicineFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)HeraScience & Technology010308 nuclear & particles physicsAntiproton ColliderHADRON-HADRON COLLISIONSHigh Energy Physics::ExperimentCenter of mass
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A search for t[bar over t] resonances in lepton+jets events with highly boosted top quarks collected in pp collisions at √s = 7 TeV with the ATLAS de…

2012

A search for resonant production of high-mass top-quark pairs is performed on 2.05 fb[superscript −1] of proton-proton collisions at √s = 7 TeV collected in 2011 with the ATLAS experiment at the Large Hadron Collider. This analysis of the lepton+jets final state is specifically designed for the particular topology that arises from the decay of highly boosted top quarks. The observed t[bar over t] invariant mass spectrum is found to be compatible with the Standard Model prediction and 95% credibility level upper limits are derived on the t[bar over t] production rate through new massive states. An upper limit of 0.7 pb is set on the production cross section times branching fraction of a narr…

Top quark01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massPartículas ElementalesQCDetectors de radiacióddc:539PhysicsLarge Hadron ColliderSettore FIS/01 - Fisica SperimentaleATLAS experimentATLASComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCParticle Physics - ExperimentQuarkNuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530TOP QUARKPartícules (Física nuclear)Nuclear physics0103 physical sciencesddc:530High Energy Physics010306 general physicstop quarkCiencias ExactasScience & TechnologyHadron-Hadron Scattering010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyFísicaNEW PHYSICSGluonHADRON-HADRON COLLISIONSCol·lisions (Física nuclear)Experimental High Energy PhysicsHigh Energy Physics::ExperimentLepton
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Measurement of the Semileptonic Charge Asymmetry usingBs0→DsμXDecays

2013

We present a measurement of the time-integrated flavor-specific semileptonic charge asymmetry in the decays of B{sub s}{sup 0} mesons that have undergone flavor mixing, a{sub sl}{sup s}, using B{sub s}{sup 0} ({bar B}{sub s}{sup 0}) {yields} D{sub s}{sup {-+}} {mu}{sup {+-}} X decays, with D{sub s}{sup {-+}} {yields} {phi}{pi}{sup {-+}} and {phi} {yields} K{sup +}K{sup -}, using 10.4 fb{sup -1} of proton-antiproton collisions collected by the D0 detector during Run II at the Fermilab Tevatron Collider. A fit to the difference between the time-integrated D{sub s}{sup -} and D{sub s}{sup +} mass distributions of the B{sub s}{sup 0} and {bar B}{sub s}{sup 0} candidates yields the flavor-specif…

PhysicsParticle physicsMeson010308 nuclear & particles physicsmedia_common.quotation_subjectGeneral Physics and AstronomyCharge (physics)01 natural sciencesAsymmetryStandard ModelCrystallographyTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesMass spectrumHigh Energy Physics::Experiment010306 general physicsmedia_commonPhysical Review Letters
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Search for microscopic black holes in a like-sign dimuon final state using large track multiplicity with the ATLAS detector

2013

A search is presented for microscopic black holes in a like-sign dimuon final state in proton-proton collisions at √s= 8 TeV. The data were collected with the ATLAS detector at the Large Hadron Collider in 2012 and correspond to an integrated luminosity of 20.3 fb-1. Using a high track multiplicity requirement, 0.6±0.2 background events from Standard Model processes are predicted and none observed. This result is interpreted in the context of low-scale gravity models and 95% CL lower limits on microscopic black hole masses are set for different model assumptions.

Atlas detectorCiencias FísicasNuclear TheoryHadronDimensions01 natural sciencesHigh Energy Physics - Experiment//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)Micro black hole[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QANuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)QCPhysicsLarge Hadron ColliderLARGE EXTRA DIMENSIONSSettore FIS/01 - Fisica Sperimentaleblack holes; ATLAS detector; microscopicATLASPhysical SciencesLHCParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASNuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências Físicas530 PhysicsAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physics0103 physical sciencesFysikddc:530High Energy PhysicsMultiplicity (chemistry)010306 general physicsCiencias ExactasScience & TechnologyATLAS detector010308 nuclear & particles physicsMillimeterFísica//purl.org/becyt/ford/1.3 [https]black holesAstronomíaBlack holeHADRON-HADRON COLLISIONSExperimental High Energy PhysicsTevPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentGravity SignaturesPHYSICAL REVIEW D
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Measurement of the differential cross sectiondσ/dtin elasticpp¯scattering ats=1.96  TeV

2012

We present a measurement of the elastic differential cross section $d\sigma(p\bar{p}\rightarrow p\bar{p})/dt$ as a function of the four-momentum-transfer squared t. The data sample corresponds to an integrated luminosity of $\approx 31 nb^{-1}$ collected with the D0 detector using dedicated Tevatron $p\bar{p} $ Collider operating conditions at sqrt(s) = 1.96 TeV and covers the range $0.26 <|t|< 1.2 GeV^2$. For $|t|<0.6 GeV^2$, d\sigma/dt is described by an exponential function of the form $Ae^{-b|t|}$ with a slope parameter $ b = 16.86 \pm 0.10(stat) \pm 0.20(syst) GeV^{-2}$. A change in slope is observed at $|t| \approx 0.6 GeV^2$, followed by a more gradual |t| dependence with increasing …

PhysicsElastic scatteringNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsScatteringTevatronSigma01 natural sciencesExponential functionlaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsColliderBar (unit)Physical Review D
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Search for new phenomena in final states with large jet multiplicities and missing transverse momentum at s√=8 TeV proton-proton collisions using the…

2013

A search is presented for new particles decaying to large numbers (7 or more) of jets, with missing transverse momentum and no isolated electrons or muons. This analysis uses 20.3 fb[superscript −1] of pp collision data at s√ = 8 TeV collected by the ATLAS experiment at the Large Hadron Collider. The sensitivity of the search is enhanced by considering the number of b-tagged jets and the scalar sum of masses of large-radius jets in an event. No evidence is found for physics beyond the Standard Model. The results are interpreted in the context of various simplified supersymmetry-inspired models where gluinos are pair produced, as well as an mSUGRA/CMSSM model.

ExoticsPhysics::Instrumentation and DetectorsCiencias FísicasPhysics beyond the Standard ModelElectron01 natural sciences7. Clean energyHigh Energy Physics - Experiment//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)Jets[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QChadron-hadron scatteringPhysicsGluinoLarge Hadron ColliderSettore FIS/01 - Fisica SperimentaleATLAS experimentSupersymmetryATLASJet physicsPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASNuclear and High Energy PhysicsParticle physicsHadron-Hadron Scattering; Jet physics; Supersymmetry ExoticsCiências Naturais::Ciências Físicas530 Physics:Ciências Físicas [Ciências Naturais]Scalar (mathematics)FOS: Physical sciencesHadron-hadron scattering530Nuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsScience & TechnologyMuon010308 nuclear & particles physicssupersymmetry; hadron-hadron scattering; jet physics; exoticsHigh Energy Physics::PhenomenologyexoticsFísica//purl.org/becyt/ford/1.3 [https]Hadron scatteringAstronomíaHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentSupersymmetrysupersymmetry
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Measurement ofsin2θeffℓandZ-light quark couplings using the forward-backward charge asymmetry inpp¯→Z/γ*→e+e−events withL=5.0  fb−1ats=1.96  TeV

2011

We measure the mass dependence of the forward-backward charge asymmetry in 157,553 $p\bar{p} \rightarrow Z/\gamma^{*} \rightarrow e^+e^-$ interactions, corresponding to 5.0 fb$^{-1}$ of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider at $\sqrt{s}=1.96$ TeV. The effective weak mixing angle ($\sin^2\theta_{eff}^{lept}$) from this process involving predominantly the first generation of quarks is extracted as $\sin^2\theta_{eff}^{lept} = 0.2309 \pm 0.0008 ({stat.}) \pm 0.0006 ({syst.})$. We also present the most precise direct measurement of the vector and axial-vector couplings of $u$ and $d$ quarks to the $Z$ boson.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronDrell–Yan processCharge (physics)Weinberg angle7. Clean energy01 natural sciencesAsymmetryNuclear physics0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsmedia_commonBosonPhysical Review D
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Search for charged massive long-lived particles ats=1.96  TeV

2013

We present a search for charged massive long-lived particles (CMLLPs) that are pair produced in p-pbar collisions at sqrt(s)= 1.96 TeV collected by the D0 experiment at the Fermilab Tevatron collider. Our result is a combination of two searches where either one or both CMLLPs are reconstructed in the detector. We select events with muon-like particles that have both speed and ionization energy loss dE/dx different from muons produced in p-pbar collisions. In the absence of evidence for CMLLPs corresponding to 6.3 fb-1 of integrated luminosity, we set limits on the CMLLP masses in several supersymmetric models, excluding masses below 278 GeV for long-lived gaugino-like charginos, and masses …

PhysicsNuclear and High Energy PhysicsParticle physicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronSupersymmetry01 natural sciences7. Clean energylaw.inventionNuclear physicsPair productionCharginolaw0103 physical sciencesHigh Energy Physics::ExperimentFermilabNuclear Experiment010306 general physicsColliderLeptonPhysical Review D
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Evidence for aBs0π±State

2016

Made available in DSpace on 2022-04-28T19:03:57Z (GMT). No. of bitstreams: 0 Previous issue date: 2016-07-07 We report evidence for a narrow structure, X(5568), in the decay sequence X(5568)→Bs0π±, Bs0→J/ψφ, J/ψ→μ+μ-, φ→K+K-. This is evidence for the first instance of a hadronic state with valence quarks of four different flavors. The mass and natural width of this state are measured to be m=5567.8±2.9(stat)-1.9+0.9(syst) MeV/c2 and Γ=21.9±6.4(stat)-2.5+5.0(syst) MeV/c2. If the decay is X(5568)→Bs∗π±→Bs0γπ± with an unseen γ, m(X(5568)) will be shifted up by m(Bs∗)-m(Bs0)∼49 MeV/c2. This measurement is based on 10.4 fb-1 of pp collision data at s=1.96 TeV collected by the D0 experiment at th…

PhysicsHadronic decay010308 nuclear & particles physicsHadronTevatronAnalytical chemistryGeneral Physics and Astronomy7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesPiHigh Energy Physics::ExperimentTetraquarkNuclear Experiment010306 general physicsPhysical Review Letters
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The large TNO 2002 TC302

2020

VizieR online Data Catalogue associated with article published in journal Astronomy &amp; Astrophysics with title 'The large Trans-Neptunian object 2002 TC302 from combined stellar occultation photometry and astrometry data.' (bibcode: 2020A&amp;A...639A.134O)

PhotometryEphemeridesCCD photometryAstrometryAsteroidsOccultationSolar system
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