Search results for " Collider"

showing 10 items of 1415 documents

The PANDA Barrel DIRC

2016

The PANDA detector at the international accelerator Facility for Antiproton and Ion Research in Europe (FAIR) addresses fundamental questions of hadron physics. Experiments concerning charmonium spectroscopy, the search for hybrids and glueballs and the interaction of hidden and open charm particles with nucleons and nuclei will be performed with antiproton beams impinging on hydrogen or nuclear targets. Cooled beams allow the precision scan of resonances in formation experiments. The momentum range of the antiproton beam between 1.5 GeV/c and 15 GeV/c tests predictions by perturbation theory and will reveal deviations originating from strong QCD . An excellent hadronic particle identificat…

PhysicsPhotonLarge Hadron Collider010308 nuclear & particles physicsHadron01 natural sciences7. Clean energyParticle identificationNuclear physicsDetection of internally reflected Cherenkov lightAntiproton0103 physical sciencesPhysics::Accelerator PhysicsFacility for Antiproton and Ion ResearchHigh Energy Physics::Experimentddc:610Nuclear Experiment010306 general physicsInstrumentationMathematical PhysicsCherenkov radiation
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Search for new phenomena in the WW→lνl′ν′ final state in pp collisions at s=7TeV with the ATLAS detector

2013

This Letter reports a search for a heavy particle that decays to WW using events produced in pp collisions at root s = 7 TeV. The data were recorded in 2011 by the ATLAS detector and correspond to an integrated luminosity of 4.7 fb(-1). WW -> lvl'v' (l,l' = e or mu) final states are considered and the distribution of the transverse mass of the W W candidates is found to be consistent with Standard Model expectations. Upper limits on the production cross section times branching ratio into W boson pairs are set for Randall-Sundrum and bulk Randall-Sundrum gravitons, which result in observed 95% CL lower limits on the masses of the two particles of 1.23 TeV and 0.84 TeV, respectively.

PhysicsPhysics::General PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderLuminosity (scattering theory)010308 nuclear & particles physicsBranching fractionTechnicolor01 natural sciencesEngineering physicsStandard Modelmedicine.anatomical_structureAtlas (anatomy)Randall–Sundrum model0103 physical sciencesmedicineTransverse massHigh Energy Physics::Experiment010306 general physicsPhysics Letters B
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Search for Dilepton Resonances inppCollisions ats=7  TeVwith the ATLAS Detector

2011

This Letter reports on a search for narrow high-mass resonances decaying into dilepton final states. The data were recorded by the ATLAS experiment in pp collisions at root s = 7 TeV at the Large Hadron Collider and correspond to a total integrated luminosity of 1.08 (1.21) fb(-1) in the e(+)e(-) (mu(+)mu(-)) channel. No statistically significant excess above the standard model expectation is observed and upper limits are set at the 95% C. L. on the cross section times branching fraction of Z' resonances and Randall-Sundrum gravitons decaying into dileptons as a function of the resonance mass. A lower mass limit of 1.83 TeV on the sequential standard model Z' boson is set. A Randall-Sundrum…

PhysicsPhysics::General PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyHadronATLAS experimentGeneral Physics and AstronomyElementary particle01 natural sciencesNuclear physicsRandall–Sundrum model0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsLeptonBosonPhysical Review Letters
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Overview of HVCMOS pixel sensors

2015

High voltage CMOS (HVCMOS) sensors are presently considered for the use in Mu3e experiment, ATLAS and CLIC. These sensors can be implemented in commercial HVCMOS processes. HVCMOS sensors feature fast charge collection by drift and high radiation tolerance. The sensor element is an n-well/p-type diode. This proceeding-paper gives an overview of HVCMOS projects and the recent results.

PhysicsPixelCompact Linear Colliderbusiness.industryAtlas detectorElectrical engineeringHigh radiationHigh voltageParticle detectorCMOSComputerSystemsOrganization_SPECIAL-PURPOSEANDAPPLICATION-BASEDSYSTEMSbusinessInstrumentationMathematical PhysicsDiodeJournal of Instrumentation
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Top quark tensor couplings

2011

We compute the real and imaginary parts of the one-loop electroweak contributions to the left and right tensorial anomalous couplings of the $tbW$ vertex in the Standard Model (SM). For both tensorial couplings we find that the real part of the electroweak SM correction is close to 10$%$ of the leading contribution given by the QCD gluon exchange. We also find that the electroweak real and imaginary parts for the anomalous right coupling are almost of the same order of magnitude. The one loop SM prediction for the real part of the left coupling is close to the 3$\sigma$ discovery limit derived from $b\rightarrow s \gamma$. Besides, taking into account that the predictions of new physics int…

PhysicsQuantum chromodynamicsCouplingNuclear and High Energy PhysicsParticle physicsTop quarkLarge Hadron ColliderPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyElectroweak interactionFOS: Physical sciencesGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Física nuclearHigh Energy Physics::ExperimentOrder of magnitudeJournal of High Energy Physics
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Observation of a NewχbState in Radiative Transitions toΥ(1S)andΥ(2S)at ATLAS

2012

The χb(nP) quarkonium states are produced in proton-proton collisions at the Large Hadron Collider at √s=7  TeV and recorded by the ATLAS detector. Using a data sample corresponding to an integrated luminosity of 4.4  fb-1, these states are reconstructed through their radiative decays to Υ(1S,2S) with Υ→μ+μ-. In addition to the mass peaks corresponding to the decay modes χb(1P,2P)→Υ(1S)γ, a new structure centered at a mass of 10.530±0.005(stat)±0.009(syst)  GeV is also observed, in both the Υ(1S)γ and Υ(2S)γ decay modes. This structure is interpreted as the χb(3P) system.

PhysicsQuantum chromodynamicsLarge Hadron Collider010308 nuclear & particles physicsAtlas (topology)Atlas detectorHadronGeneral Physics and AstronomyQuarkonium01 natural sciencesNuclear physics0103 physical sciencesBound stateRadiative transferHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review Letters
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Soft-virtual corrections to Higgs production atN3LO

2015

The authors compute certain (soft-virtual) corrections to the Higgs boson production in the gluon-gluon fusion at next-to-next-to-next-to-leading order in QCD. Such higher loop calculations are essential for comparing the theoretical predictions with the experimental results of the Higgs boson production at LHC.

PhysicsQuantum chromodynamicsLoop (topology)Nuclear and High Energy PhysicsHiggs fieldParticle physicsLarge Hadron ColliderHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHiggs bosonDrell–Yan processHigh Energy Physics::ExperimentProduction (computer science)Physical Review D
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Constraints on jet quenching in p–Pb collisions at sNN=5.02 TeV measured by the event-activity dependence of semi-inclusive hadron-jet distributions

2018

The ALICE Collaboration reports the measurement of semi-inclusive distributions of charged-particle jets recoiling from a high-transverse momentum trigger hadron in p–Pb collisions at √sNN = 5.02 TeV. Jets are reconstructed from charged-particle tracks using the anti-kT algorithm with resolution parameter R = 0.2 and 0.4. A data-driven statistical approach is used to correct the uncorrelated background jet yield. Recoil jet distributions are reported for jet transverse momentum 15 < pch T,jet < 50 GeV/c and are compared in various intervals of p–Pb event activity, based on charged-particle multiplicity and zero-degree neutral energy in the forward (Pb-going) direction. The semi-inclusive ob…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHadronObservable01 natural sciencesNuclear physicsRecoil0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsJet quenchingOrder of magnitudePhysics Letters B
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Multiplicity dependence of inclusive J/ψ production at midrapidity in pp collisions at s=13 TeV

2020

Measurements of the inclusive J/ψ yield as a function of charged-particle pseudorapidity density dNch/dη in pp collisions at √s = 13 TeV with ALICE at the LHC are reported. The J/ψ meson yield is measured at midrapidity (|y| < 0.9) in the dielectron channel, for events selected based on the charged-particle multiplicity at midrapidity (|η| < 1) and at forward rapidity (−3.7 < η < −1.7 and 2.8 < η < 5.1); both observables are normalized to their corresponding averages in minimum bias events. The increase of the normalized J/ψ yield with normalized dNch/dη is significantly stronger than linear and dependent on the transverse momentum. The data are compared to theoretical predictions, which de…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsLarge Hadron ColliderMeson010308 nuclear & particles physicsMultiplicity (mathematics)Quarkonium01 natural sciencesNuclear physicsPseudorapidityYield (chemistry)0103 physical sciencesRapidity010306 general physicsPhysics Letters B
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Global baryon number conservation encoded in net-proton fluctuations measured in Pb–Pb collisions at sNN=2.76 TeV

2020

Experimental results are presented on event-by-event net-proton fluctuation measurements in Pb–Pb collisions at sNN=2.76 TeV, recorded by the ALICE detector at the CERN LHC. These measurements have as their ultimate goal an experimental test of Lattice QCD (LQCD) predictions on second and higher order cumulants of net-baryon distributions to search for critical behavior near the QCD phase boundary. Before confronting them with LQCD predictions, account has to be taken of correlations stemming from baryon number conservation as well as fluctuations of participating nucleons. Both effects influence the experimental measurements and are usually not considered in theoretical calculations. For t…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsLarge Hadron ColliderProton010308 nuclear & particles physicsCritical phenomenaHigh Energy Physics::PhenomenologyLattice field theoryLattice QCD01 natural sciencesNuclear physics0103 physical sciencesBaryon numberNuclear Experiment010306 general physicsNucleonPhysics Letters B
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