Search results for "Lhc"

showing 10 items of 342 documents

Measurement of D-meson production at mid-rapidity in pp collisions at √s = 7 TeV

2017

The production cross sections for prompt charmed mesons D0, D+, D∗+ and D+s were measured at mid-rapidity in proton–proton collisions at a centre-of-mass energy s√=7 TeV with the ALICE detector at the Large Hadron Collider (LHC). D mesons were reconstructed from their decays D0→K−π+, D+→K−π+π+, D∗+→D0π+, D+s→ϕπ+→K−K+π+, and their charge conjugates.With respect to previous measurements in the same rapidity region, the coverage in transverse momentum (pT) is extended and the uncertainties are reduced by a factor of about two. The accuracy on the estimated total cc¯¯ production cross section is likewise improved. The measured pT-differential cross sections are compared with the results of thre…

proton–proton collisionsprotonitenergiahadronsHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimenthiukkasfysiikkaNuclear ExperimentLHC energy
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Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at √s, √sNN = 5.02 TeV

2021

Jet fragmentation transverse momentum (jT) distributions are measured in proton-proton (pp) and proton-lead (p-Pb) collisions at √sNN = 5.02 TeV with the ALICE experiment at the LHC. Jets are reconstructed with the ALICE tracking detectors and electromagnetic calorimeter using the anti-kT algorithm with resolution parameter R = 0.4 in the pseudorapidity range |η| < 0.25. The jT values are calculated for charged particles inside a fixed cone with a radius R = 0.4 around the reconstructed jet axis. The measured jT distributions are compared with a variety of parton-shower models. Herwig and Pythia 8 based models describe the data well for the higher jT region, while they underestimate the low…

related to the perturbative component of the fragmentation processthe measured trends are successfully described by all models except for Herwig. For the wide componentHerwig and PYTHIA 8 based models slightly underestimate the data for the higher jet transverse momentum region. These measurements set constraints on models of jet fragmentation and hadronisation.Nuclear and High Energy Physicswhile that of the inverse gamma function increases with increasing jet transverse momentum. For the narrow componentHeavy Ion Experimentsand with a Gaussian for lower jT values (called the “narrow component”)hiukkasfysiikkawhile they underestimate the lower jT region. The jT distributions are further characterised by fitting them with a function composed of an inverse gamma function for higher jT values (called the “wide component”)predominantly connected to the hadronisation process. The width of the Gaussian has only a weak dependence on jet transverse momentumJet fragmentation transverse momentum (jT) distributions are measured in proton-proton (pp) and proton-lead (p-Pb) collisions at √sNN = 5.02 TeV with the ALICE experiment at the LHC. Jets are reconstructed with the ALICE tracking detectors and electromagnetic calorimeter using the anti-kT algorithm with resolution parameter R = 0.4 in the pseudorapidity range |η| < 0.25. The jT values are calculated for charged particles inside a fixed cone with a radius R = 0.4 around the reconstructed jet axis. The measured jT distributions are compared with a variety of parton-shower models. Herwig and PYTHIA 8 based models describe the data well for the higher jT region
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Measurement of the Higgs boson coupling with tau leptons and search for an additional neutral MSSM Higgs boson with the ATLAS detector

2018

El Modelo Estándar de física de partículas (SM), la teoría que describe el comportamiento de las partículas subatómicas, ha sido un éxito en su precisión y exactitud. Uno de sus pilares básicos es el mecanismo de Higgs, que regula los términos de masa de las partículas fundamentales. La partícula responsable de este mecanismo es el bosón de Higgs, que fue descubierto en 2012 en los experimentos ATLAS y CMS del colisionador de partículas LHC del CERN, mediante el análisis de su acoplamiento a partículas bosónicas (fotones y bosones W y Z). Tras su descubrimiento, es necesario confirmar que el resto sus propiedades se corresponden con las predichas por el SM, como, por ejemplo, su acoplamient…

standard model:FÍSICA::Nucleónica::Detectores de partículas [UNESCO]yukawa couplingmssmhiggs bosonhiggs:FÍSICA::Nucleónica::Aceleradores de partículas [UNESCO]UNESCO::FÍSICA::Nucleónica::Aceleradores de partículassusyatlastaulhcacoplamiento de yukawabosón de higgsHigh Energy Physics::PhenomenologycernUNESCO::FÍSICA::Nucleónica::Física de partículasUNESCO::FÍSICA::Nucleónica::Detectores de partículasmodelo estándar:FÍSICA::Física de altas energías [UNESCO]:FÍSICA::Nucleónica::Física de partículas [UNESCO]supersimetríaUNESCO::FÍSICA::Física de altas energíasHigh Energy Physics::ExperimentsupersymmetryParticle Physics - Experiment
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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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Search for photonic signatures of gauge-mediated supersymmetry in 8TeV pp collisions with the ATLAS detector

2015

A search is presented for photonic signatures motivated by generalized models of gauge-mediated supersymmetry breaking. This search makes use of 20.3  fb[superscript −1] of proton-proton collision data at √s = 8  TeV recorded by the ATLAS detector at the LHC, and explores models dominated by both strong and electroweak production of supersymmetric partner states. Four experimental signatures incorporating an isolated photon and significant missing transverse momentum are explored. These signatures include events with an additional photon, lepton, b-quark jet, or jet activity not associated with any specific underlying quark flavor. No significant excess of events is observed above the Stand…

transverse momentum [photon]Большой адронный коллайдерCiencias FísicasPhysics beyond the Standard ModelPROTON-PROTON COLLISIONSFORTRAN CODEElementary particlesymmetry breaking [supersymmetry]gravitinoHigh Energy Physics - ExperimentMEASUREMENTSubatomär fysik//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)суперсимметрияSubatomic Physicsscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]HADRON COLLIDERSGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)QC8000 GeV-cmsPhysicsLarge Hadron ColliderJET ENERGYSettore FIS/01 - Fisica SperimentaleElectroweak interactionPhotonicSUPERGAUGE TRANSFORMATIONSSupersymmetryATLASbottom [jet]Supersymmetry breakingCERN LHC CollPhotonic signaturesgauge [mediation]Physical Sciencesflavor [quark]GravitinoLHCcolliding beams [p p]CIENCIAS NATURALES Y EXACTASsignatureParticle Physics - ExperimentParticle physicsNuclear and High Energy Physics530 PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesстолкновение частицpair production [neutralino]530MISSING TRANSVERSE-MOMENTUMNuclear physicsGauge-mediatedphotonic signatures; gauge-mediated supersymmetry; ATLAS detectorFysikddc:530High Energy PhysicsCiencias ExactasPROTON-PROTON COLLISIONS; MISSING TRANSVERSE-MOMENTUM; JET ENERGY; MEASUREMENT; ROOT-S=7 TEV; HADRON COLLIDERS; SUPERGAUGE TRANSFORMATIONS; FORTRAN CODE; MODEL; LHC; PERFORMANCEScience & Technologyelectroweak interactionATLAS detectorROOT-S=7 TEVHigh Energy Physics::PhenomenologyFísica//purl.org/becyt/ford/1.3 [https]PERFORMANCEAstronomíaMODELgravitationmissing-energy [transverse momentum]Proton-Proton CollisionsExperimental High Energy PhysicsHigh Energy Physics::ExperimentSupersymmetryATLAS детекторexperimental resultsLepton
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Recommendations of the LHC Dark Matter Working Group: Comparing LHC searches for dark matter mediators in visible and invisible decay channels and ca…

2019

Physics of the Dark Universe 26, 100377 (2019). doi:10.1016/j.dark.2019.100377

transverse momentum: missing-energyscale: TeVAtomic01 natural sciencesParticle and Plasma Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [p p]TeV [scale]010303 astronomy & astrophysicsPhysicsLarge Hadron ColliderCMSPhysicsaxial-vectorMonte Carlo [numerical calculations]ATLASCERN LHC Collinterpretation of experimentsrelic density [dark matter]colliding beams [p p]numerical calculations: Monte CarloAstronomical and Space SciencessignatureParticle physicsp p: scatteringDark matterlepton: couplingdark matter: production5300103 physical sciencesThermalNuclearddc:530Pseudovector010308 nuclear & particles physicsdark matter: relic densityMolecularAstronomy and Astrophysicsmediation [dark matter]dark matter: mediationproduction [dark matter]Space and Planetary Sciencemissing-energy [transverse momentum][PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]invisible decaycoupling [lepton][PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]p p: colliding beamsvectorLeptonexperimental results
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Two-particle transverse momentum correlations in pp and p-Pb collisions at energies available at the CERN Large Hadron Collider

2023

Two-particle transverse momentum differential correlators, recently measured in Pb--Pb collisions at energies available at the CERN Large Hadron Collider (LHC), provide an additional tool to gain insights into particle production mechanisms and infer transport properties, such as the ratio of shear viscosity to entropy density, of the medium created in Pb-Pb collisions. The longitudinal long-range correlations and the large azimuthal anisotropy measured at low transverse momenta in small collision systems, namely pp and p-Pb, at LHC energies resemble manifestations of collective behaviour. This suggests that locally equilibrated matter may be produced in these small collision systems, simil…

two particle correlations large hadron colliderCERN Lablongitudinallarge hadron colliderheavy ion scatteringcollectiveFOS: Physical sciencesanisotropy measuredtransverse momentum correlation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)transport theoryTeVcorrelation functionNuclear Experiment (nucl-ex)Nuclear ExperimentMonte Carloeffect viscositycorrelation long-rangetwo-particleentropy densityparticle multiplicityCERN LHC Collangular distribution anisotropybroadeningtransverse momentum lowydinfysiikkatwo particle correlations
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Measurement of dielectron production in central Pb-Pb collisions at √sNN = 2.76 TeV

2019

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. The first measurement of dielectron (e + e −) production in central (0 – 10 %) Pb – Pb collisions at √sNN=2.76TeV at the LHC is presented. The dielectron invariant-mass spectrum is compared to the expected contributions from hadron decays in the invariant-mass range 0 < mee < 3.5 GeV / c2. The ratio of data and the cocktail of hadronic contributions without vacuum ρ0 is measured in the invariant-mass range 0.15 < mee < 0.7 GeV / c2, w…

virtual [photon]:Kjerne- og elementærpartikkelfysikk: 431 [VDP]heavy ion collisionsHadrondielectron productionhiukkasfysiikkaPP01 natural sciencesS-W INTERACTIONSthermalALICEPhysics::Atomic PhysicsNuclear ExperimentBrookhaven RHIC CollPhysicsAU COLLISIONSLarge Hadron Colliderphoton: virtual ; photon: direct production ; heavy ion: scattering ; hadron: decay ; Brookhaven RHIC Coll ; transverse momentum ; CERN LHC Coll ; thermal ; ALICE ; mesonVDP::Kjerne- og elementærpartikkelfysikk: 431DIRECT PHOTON PRODUCTIONddc::Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]PRIRODNE ZNANOSTI. Fizika.:Nuclear and elementary particle physics: 431 [VDP]CERN LHC CollVDP::Nuclear and elementary particle physics: 431Transverse momentumNuclear and High Energy PhysicsRho mesondirect production [photon]MesonPAIR PRODUCTIONPhoton lepton & quark productiontransverse momentumFew-body systemsmesonNuclear physicsDIRECT PHOTON PRODUCTION; S-W INTERACTIONS; AU COLLISIONS; RHO-MESON; DIMUON PRODUCTION; PAIR PRODUCTION; PP; J/PSI; ENHANCEMENT; EMISSIONENHANCEMENTscattering [heavy ion]0103 physical sciencesRelativistic heavy-ion collisionsRHO-MESON010306 general physicsParticle & resonance productionNuclear Physicsta114010308 nuclear & particles physics:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]NATURAL SCIENCES. Physics.J/PSIPair productionDIMUON PRODUCTIONQuark–gluon plasmaHigh Energy Physics::ExperimentEMISSIONdecay [hadron]
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The ALICE experiment at the CERN LHC

2008

Journal of Instrumentation 3(08), S08002 (2008). doi:10.1088/1748-0221/3/08/S08002

visible and IR photonsLiquid detectorshigh energyPhotonPhysics::Instrumentation and DetectorsTransition radiation detectorsTiming detectors01 natural sciencesOverall mechanics designParticle identificationSoftware architecturesParticle identification methodsGaseous detectorscluster findingDetector cooling and thermo-stabilizationDetector groundingParticle tracking detectors[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Special cablesDetector alignment and calibration methodsDetectors and Experimental TechniquesNuclear ExperimentVoltage distributions.Photon detectors for UVInstrumentationMathematical PhysicsQuantum chromodynamicsPhysicsLarge Hadron ColliderSpectrometersPhysicsDetectorcalibration and fitting methodsTransition radiation detectorScintillatorsData processing methodsAnalysis and statistical methodsData reduction methodsParticle physicsCherenkov and transition radiationTime projection chambers610dE/dx detectorsNuclear physicsCalorimetersPattern recognitionGamma detectors0103 physical sciencesddc:610Solid state detectors010306 general physicsMuonInstrumentation for heavy-ion acceleratorsSpectrometerLarge detector systems for particle and astroparticle physics010308 nuclear & particles physicsCERN; LHC; ALICE; heavy ion; QGPCherenkov detectorsComputingVoltage distributionsManufacturingscintillation and light emission processesanalysis and statistical methods; calorimeters; cherenkov and transition radiation; cherenkov detectors; computing; data processing methods; data reduction methods; de/dx detectors; detector alignment and calibration methods; detector cooling and thermo-stabilization; detector design and construction technologies and materials; detector grounding; gamma detectors; gaseous detectors; instrumentation for heavy-ion accelerators; instrumentation for particle accelerators and storage rings - high energy; large detector systems for particle and astroparticle physics; liquid detectors; manufacturing; overall mechanics design; particle identification methods; particle tracking detectors; pattern recognition; cluster finding; calibration and fitting methods; photon detectors for uv; visible and ir photons; scintillators; scintillation and light emission processes; simulation methods and programs; software architectures; solid state detectors; special cables; spectrometers; time projection chambers; timing detectors; transition radiation detectors; voltage distributionsInstrumentation for particle accelerators and storage ringsInstrumentation; Mathematical PhysicsHigh Energy Physics::ExperimentSimulation methods and programsDetector design and construction technologies and materials
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Search for scalar leptoquarks in pp collisions at $\sqrt{s}$=13 TeV with the ATLAS experiment

2016

An inclusive search for a new-physics signature of lepton-jet resonances has been performed by the ATLAS experiment. Scalar leptoquarks, pair-produced in pp collisions at s √s = 13 TeV at the large hadron collider, have been considered. An integrated luminosity of 3.2 fb-1, corresponding to the full 2015 dataset was used. First (second) generation leptoquarks were sought in events with two electrons (muons) and two or more jets. The observed event yield in each channel is consistent with Standard Model background expectations. The observed (expected) lower limits on the leptoquark mass at 95% confidence level are 1100 and 1050 GeV (1160 and 1040 GeV) for first and second generation leptoqua…

Большой адронный коллайдер13000 GeV-cms((n)jet dilepton) [final state]General Physics and AstronomyElementary particleleptoquark7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentSubatomär fysikHigh Energy Physics - Experiment (hep-ex)Subatomic Physicsscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]leptoquark; ATLAS; LHC; PARTON DISTRIBUTIONS; LHCлептокваркипротон-протонные столкновенияQCPhysicsLarge Hadron Colliderleptoquark --> quark leptonATLAS experimentSettore FIS/01 - Fisica SperimentaleATLASmass dependencebranching ratio [leptoquark]CERN LHC Collleptoquark ATLAS LHCLHCcolliding beams [p p]Particle Physics - ExperimentQuarkParticle physicsleptoquark --> quark neutrino530 PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]signature [new physics]leptoquark; ATLAS; LHCFOS: Physical sciencesLHC ATLAS High Energy Physicsddc:500.2530Nuclear physicsPhysics and Astronomy (all)510 Mathematicsscalar [leptoquark]0103 physical sciencesLeptoquarkddc:530High Energy Physics010306 general physicsCiencias Exactasupper limit [mass]MuonScience & Technologyhep-ex010308 nuclear & particles physicsBranching fractionbackgroundATLAS; Leptoquark; LHC; High Energy Physics - Experiment; High Energy Physics - Experiment; Physics and Astronomy (all)High Energy Physics::PhenomenologyFísicasensitivitymass [leptoquark]PARTON DISTRIBUTIONSLeptoquarkExperimental High Energy Physicsupper limit [branching ratio]High Energy Physics::ExperimentATLAS детекторATLAS; Leptoquark; LHC; Physics and Astronomy (all)Leptonexperimental results
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