Search results for "PROTON-PROTON COLLISIONS"

showing 10 items of 128 documents

Measurement of W ± Z production in proton-proton collisions at √s =7 TeV with the ATLAS detector

2012

A study of W±Z production in proton-proton collisions at √s=7 TeV is presented using data corresponding to an integrated luminosity of 4.6 fb−1 collected with the ATLAS detector at the Large Hadron Collider in 2011. In total, 317 candidates, with a background expectation of 68±10 events, are observed in double-leptonic decay final states with electrons, muons and missing transverse momentum. The total cross-section is determined to be σtotWZ=19.0+1.4−1.3(stat.)±0.9(syst.)±0.4(lumi.) pb, consistent with the Standard Model expectation of 17.6+1.1−1.0 pb. Limits on anomalous triple gauge boson couplings are derived using the transverse momentum spectrum of Z bosons in the selected events. The …

Physics and Astronomy (miscellaneous)Proton7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Naturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massNuclear ExperimentQCDetectors de radiacióBosonPhysicsddc:539Large Hadron ColliderSettore FIS/01 - Fisica Sperimentalez bosonATLASmedicine.anatomical_structureComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCNatural SciencesParticle Physics - ExperimentParticle physicsATLAS; detectorCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciences530Partícules (Física nuclear)Standard ModelNuclear physicsAtlas (anatomy)0103 physical sciencesmedicineddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias ExactasGauge bosonMuonScience & TechnologyATLAS detector010308 nuclear & particles physicsFísicaCol·lisions (Física nuclear)Experimental High Energy Physicsproton-proton collisionsHigh Energy Physics::ExperimentEuropean Physical Journal C
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Charm-quark fragmentation fractions and production cross section at midrapidity in pp collisions at the LHC

2022

Physical review / D 105(1), L011103 (2022). doi:10.1103/PhysRevD.105.L011103

Physics and Astronomy (miscellaneous)electron p: interactionPROTON-PROTON COLLISIONSMESON PRODUCTIONROOT-S=5.02 TEVmeasured [cross section]hiukkasfysiikka2760 GeV-cms/nucleon01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)ALICEscattering [p p]ground state [charm]Charm; p-p collisions[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experimentcharm: ground statep-p collisionsMeson productioninteraction [electron p]CERN LHC Coll7000 GeV-cms/nucleonParticle Physics - Experimentperturbation theory [quantum chromodynamics]p p: scatteringCharmcharm: fragmentation ; p p: scattering ; electron p: interaction ; charm: ground state ; quantum chromodynamics: perturbation theory ; cross section: measured ; hadron hadron: interaction ; CERN LHC Coll ; rapidity ; ALICE ; experimental results ; 2760 GeV-cms/nucleon ; 5020 GeV-cms/nucleon ; 7000 GeV-cms/nucleoneducationFOS: Physical sciencesfragmentation [charm][PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530114 Physical sciencesProton-proton collisions0103 physical sciencescharm fragmentation fractions nuclear physicsddc:5305020 GeV-cms/nucleonNuclear Physics - Experimentcharm: fragmentationD-0quantum chromodynamics: perturbation theory010306 general physicshadron hadron: interactionPROTON-PROTON COLLISIONS; MESON PRODUCTION; ROOT-S=5.02 TEV; QCD; D-0interaction [hadron hadron]010308 nuclear & particles physicsHigh Energy Physics::Phenomenologycross section: measuredRoot-s=5.02 tevQCDQcdrapidityHigh Energy Physics::Experimentkvanttiväridynamiikkaexperimental results
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Production of π0 and η mesons up to high transverse momentum in pp collisions at 2.76 TeV

2017

The invariant differential cross sections for inclusive π0 and η mesons at midrapidity were measured in pp collisions at √s = 2.76 TeV for transverse momenta 0.4 < pT < 40 GeV/c and 0.6 < pT < 20 GeV/c, respectively, using the ALICE detector. This large range in pT was achieved by combining various analysis techniques and different triggers involving the electromagnetic calorimeter (EMCal). In particular, a new single-cluster, shower-shape based method was developed for the identification of highpT neutral pions, which exploits that the showers originating from their decay photons overlap in the EMCal. Above 4 GeV/c, the measured cross sections are found to exhibit a similar power-law behav…

Physics and Astronomy (miscellaneous)eta mesonsHigh Energy Physics::Experimentproton-proton collisionspionshiukkasfysiikkaNuclear ExperimentEngineering (miscellaneous)particel physics
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Single hadron response measurement and calorimeter jet energy scale uncertainty with the ATLAS detector at the LHC

2013

The uncertainty on the calorimeter energy response to jets of particles is derived for the ATLAS experiment at the Large Hadron Collider (LHC). First, the calorimeter response to single isolated charged hadrons is measured and compared to the Monte Carlo simulation using proton-proton collisions at centre-of-mass energies of √s = 900 GeV and 7 TeV collected during 2009 and 2010. Then, using the decay of Ks and Λ particles, the calorimeter response to specific types of particles (positively and negatively charged pions, protons, and anti-protons) is measured and compared to the Monte Carlo predictions. Finally, the jet energy scale uncertainty is determined by propagating the response uncert…

Physics and Astronomy (miscellaneous)large hadron colliderPhysics::Instrumentation and DetectorsHadronMonte Carlo methodNuclear Theory01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Naturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentPhysicsJet (fluid)End-Cap CalorimeterLarge Hadron ColliderATLAS experimentSettore FIS/01 - Fisica Sperimentalemedicine.anatomical_structurePhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHC ATLAS High Energy PhysicsNatural SciencesParticle Physics - ExperimentParticle physics530 PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicsPionAtlas (anatomy)0103 physical sciencesBeam TestsmedicineFysikddc:530010306 general physicsEngineering (miscellaneous)Ciencias ExactasScience & TechnologyHadron-Hadron ScatteringATLAS detectorCalorimeter (particle physics)010308 nuclear & particles physicsFísicaBarrel Calorimeterjet energyExperimental High Energy Physicsproton-proton collisionsHigh Energy Physics::Experiment
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SU(5)-inspired double beta decay

2015

The short-range part of the neutrinoless double beta amplitude is generated via the exchange of exotic particles, such as charged scalars, leptoquarks and/or diquarks. In order to give a sizable contribution to the total decay rate, the masses of these exotics should be of the order of (at most) a few TeV. Here, we argue that these exotics could be the “light” (i.e., weak-scale) remnants of some B – L violating variants of SU(5). We show that unification of the standard model gauge couplings, consistent with proton decay limits, can be achieved in such a setup without the need to introduce supersymmetry. Since these nonminimal SU(5)-inspired models violate B – L, they generate Majorana neut…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaBeta decayProton-proton collisionsNuclear physicsDiquarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayGrand unified theoriesLeptoquarkHigh Energy Physics::ExperimentNeutrino oscillation
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"Table 41" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum integrated yield vs multiplicity - V0M multiplicity classes, average of particle and antiparticle

Physics::General PhysicsP P --&gt; Kstar+XKstar13000.0Proton-Proton CollisionsSIGyieldResonanceV0M Multiplicity
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"Table 2" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class II, average of particle and antiparticle

Physics::General PhysicsP P --&gt; Kstar+XKstar13000.0YieldsProton-Proton CollisionsComputer Science::Computational GeometrySIGResonanceV0M Multiplicity
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"Table 1" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class I, average of particle and antiparticle

Physics::General PhysicsP P --&gt; Kstar+XKstar13000.0YieldsProton-Proton CollisionsHigh Energy Physics::ExperimentNuclear ExperimentSIGResonanceV0M Multiplicity
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"Table 4" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class IV+V, average of particle and antiparticle

Physics::General PhysicsP P --&gt; Kstar+XKstar13000.0YieldsProton-Proton CollisionsSIGResonancePhysics::GeophysicsV0M Multiplicity
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"Table 6" of "Multiplicity dependence of K*(892)$^{0}$ and $\phi$(1020) production in pp collisions at $\sqrt{s}$ = 13 TeV"

2020

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class VII, average of particle and antiparticle

Physics::General PhysicsP P --&gt; Kstar+XKstar13000.0YieldsProton-Proton CollisionsSIGResonanceV0M Multiplicity
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