Search results for "Instrumentation"

showing 10 items of 4914 documents

Search for new phenomena in dijet events using 37  fb−1 of pp collision data collected at s=13  TeV with the ATLAS detector

2017

Dijet events are studied in the proton-proton collision dataset recorded at root s = 13 TeV with the ATLAS detector at the Large Hadron Collider in 2015 and 2016, corresponding to integrated lumino ...

PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas detectorHigh Energy Physics::PhenomenologyCollision01 natural sciencesNuclear physicsAngular distributionmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicinePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review D
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K*(892)0 and ϕ(1020) production at midrapidity in pp collisions at s=8 TeV

2020

The production of K∗(892)0 and φ(1020) in pp collisions at s=8 TeV was measured by using Run 1 data collected by the ALICE collaboration at the CERN Large Hadron Collider (LHC). The pT-differential yields d2N/dydpT in the range 0

PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsHigh Energy Physics::Phenomenology0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment010306 general physics01 natural sciences7. Clean energyPhysical Review C
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Physics potential of beta/EC beams in regard to CP violation in neutrino oscillations

2007

The goal for future neutrino facilities is the determination of the [Ue3] mixing and CP violation in neutrino oscillations. This will require precision experiments with a very intense neutrino source. With this objective the creation of neutrino beams from the radioactive decay of boosted ions by the SPS of CERN from either beta or electron capture transitions has been propossed. We discuss the capabilities of such facilities as a function of the energy of the boost and the baseline for the detector. We conclude that the SPS upgrade to 1000 GeV is crucial to have a better sensitivity to CP violation if it is accompanied by a longer baseline. We compare the physics potential for two differen…

PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsElectron captureHigh Energy Physics::PhenomenologyFísicaNuclear physicsUpgradeBeta (plasma physics)Physics::Accelerator PhysicsCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationRadioactive decay
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Supersymmetric origin of neutrino mass

2004

Supersymmetry with breaking of R-parity provides an attractive way to generate neutrino masses and lepton mixing angles in accordance to present neutrino data. We review the main theoretical features of the bilinear R-parity breaking (BRpV) model, and stress that it is the simplest extension of the minimal supersymmetric standard model (MSSM) which includes lepton number violation. We describe how it leads to a successful phenomenological model with hierarchical neutrino masses. In contrast to seesaw models, the BRpV model can be probed at future collider experiments, like the Large Hadron Collider or the Next Linear Collider, since the decay pattern of the lightest supersymmetric particle …

PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyFísicaSupersymmetryLepton numberLightest Supersymmetric Particlelaw.inventionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawHigh Energy Physics::ExperimentNeutrinoColliderMinimal Supersymmetric Standard ModelLepton
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Upgrade of the ATLAS Level-1 trigger with an FPGA based Topological Processor

2013

The ATLAS experiment is located at the European Centre for Nuclear Research (CERN) in Switzerland. It is designed to measure decay properties of high energetic particles produced in the protons collisions at the Large Hadron Collider (LHC). The LHC has a proton collision at a frequency of 40 MHz, and thus requires a trigger system to efficiently select events down to a manageable event storage rate of about 400Hz. Event triggering is therefore one of the extraordinary challenges faced by the ATLAS detector. The Level-1 Trigger is the first rate-reducing step in the ATLAS Trigger, with an output rate of 75kHz and decision latency of less than 2.5$\mu$s. It is primarily composed of the Calori…

PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsNuclear TheoryATLAS experimentUpgrademedicine.anatomical_structureAtlas (anatomy)Optical receiversmedicinePhysics::Accelerator PhysicsSignal processing algorithmsHigh Energy Physics::ExperimentDetectors and Experimental TechniquesNuclear ExperimentField-programmable gate array
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Event plane determination with the new ALICE FIT detector

2021

During the on-going second long shutdown of LHC, the forward detectors of the ALICE experiment are implementing an extensive upgrade. In particular, a new Fast Interaction Trigger (FIT) has been designed and built. It consists of three sub-detector systems delivering a broad range of online functionalities, and an essential input for event characterization and physics analysis. For instance, FIT will deliver the precise collision time for the TOF-based particle identification, provide the centrality and the event plane information, and measure the cross section of diffractive processes. This note will discuss usage of FIT in the event plane determination during Run 3. A simulated event plan…

PhysicsParticle physicsLarge Hadron ColliderPlane (geometry)Physics::Instrumentation and DetectorstutkimuslaitteetDetectorhiukkasfysiikkahiukkaskiihdyttimetMeasure (mathematics)Particle identificationUpgradeilmaisimetNuclear Physics - ExperimentDetectors and Experimental TechniquesCentralityEvent (particle physics)Particle Physics - Experiment
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b-Hadron production in the general-mass variable-flavour-number scheme and LHC data

2018

We study inclusive b-hadron production in pp collisions at the LHC at different center-of-mass energies and compare with experimental data from the LHCb and CMS collaborations. Our predictions for cross sections differential in the transverse momentum and (pseudo-)rapidity agree with data within uncertainties due to renormalization scale variations. A small tension is found if data and theory predictions are compared for cross section ratios at different center-of-mass energies.

PhysicsParticle physicsLarge Hadron ColliderScale (ratio)010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsHadronFOS: Physical sciencesExperimental data01 natural sciencesRenormalizationVariable (computer science)Cross section (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Rapidity010306 general physics
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An upgraded ATLAS central trigger for 2015 luminosities

2013

The Central Trigger Processor (CTP) is a core unit of the first of three levels that constitute the ATLAS trigger system. Based on information from calorimeter and muon trigger processors as well as from some additional systems it produces the level-1 trigger decision and prompts the read-out of the sub-detectors. The increase in luminosity at the LHC has pushed the CTP operation to its design limits. In order to still satisfy the physics goals of the experiment after the shutdown of the LHC of 2013/2014 the CTP will be upgraded during this period. This article discusses the current Central Trigger Processor, the motivation for the upgrade, and the changes foreseen to meet the requirements …

PhysicsParticle physicsLuminosity (scattering theory)Large Hadron ColliderCalorimeter (particle physics)Physics::Instrumentation and Detectorsbusiness.industryReadout electronicsmedicine.anatomical_structureUpgradeAtlas (anatomy)Nuclear electronicsmedicinePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentbusinessComputer hardware2013 3rd International Conference on Advancements in Nuclear Instrumentation, Measurement Methods and their Applications (ANIMMA)
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Search for Magnetic Monopoles ins=7  TeVppCollisions with the ATLAS Detector

2012

This Letter presents a search for magnetic monopoles with the ATLAS detector at the CERN Large Hadron Collider using an integrated luminosity of 2.0 fb(-1) of pp collisions recorded at a center-of- ...

PhysicsParticle physicsLuminosity (scattering theory)Large Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas detectorNeutrino telescopeMagnetic monopoleGeneral Physics and AstronomyDrell–Yan process01 natural sciencesNuclear physicsMoEDAL experimentmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicinePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review Letters
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Observation of the Semileptonic D+ Decay into the K¯1(1270)0 Axial-Vector Meson

2019

By analyzing a 2.93 fb(-1) data sample of e(+)e(-) collisions, recorded at a center-of-mass energy of 3.773 GeV with the BESIII detector operated at the BEPCII collider, we report the first observa ...

PhysicsParticle physicsMesonPhysics::Instrumentation and DetectorsBranching fractionDetectorGeneral Physics and Astronomy01 natural scienceslaw.inventionlaw0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsColliderPseudovectorEnergy (signal processing)Physical Review Letters
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