Search results for "Collider"

showing 10 items of 1690 documents

Upgrade of the ATLAS Level-1 Trigger with event topology information

2015

The Large Hadron Collider (LHC) in 2015 will collide proton beams with increased luminosity from \unit{10^{34}} up to \unit{3 \times 10^{34}cm^{-2}s^{-1}}. ATLAS is an LHC experiment designed to measure decay properties of high energetic particles produced in the protons collisions. The higher luminosity places stringent operational and physical requirements on the ATLAS Trigger in order to reduce the 40MHz collision rate to a manageable event storage rate of 1kHz while at the same time, selecting those events with valuable physics meaning. The Level-1 Trigger is the first rate-reducing step in the ATLAS Trigger, with an output rate of 100kHz and decision latency of less than 2.5$\mu s$. It…

PhysicsHistoryLuminosity (scattering theory)Large Hadron ColliderPhysics::Instrumentation and DetectorsEvent (computing)Processor designReal-time computingProcess (computing)Computer Science ApplicationsEducationmedicine.anatomical_structureUpgradeAtlas (anatomy)medicineAdvanced Telecommunications Computing ArchitectureParticle Physics - ExperimentJournal of Physics: Conference Series
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Associated production of weak bosons at the LHC with the ATLAS detector

2009

The study of the associated production of weak vector bosons at the LHC allows to search for New Physics through the measurement of possible deviations of the weak boson self-couplings from the expectation within the Standard Model. The sensitivity of the ATLAS experiment to Standard Model diboson (W+ W-, Wplusmn; Z0, Z0 Z0, W± γ, and Z0 γ) production in pp collisions at = 14 TeV, using final states containing electrons, muons and photons, is presented. These studies use Monte Carlo data sets with full detector simulation from the ATLAS Computer System Commissioning, which furthermore include detailed trigger information as well as effects of detector calibration and alignment corrections. …

PhysicsHistoryParticle physicsGauge bosonPhotonMuonLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsPhysics beyond the Standard ModelATLAS experimentTevatron01 natural sciencesComputer Science ApplicationsEducationNuclear physics0103 physical sciences010306 general physicsBosonJournal of Physics: Conference Series
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CP-violating MSSM Higgs at Tevatron and LHC

2010

talk presented at PASCOS 2010 (Valencia) and SUSY 10 (Bonn)

PhysicsHistoryParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciences01 natural sciencesComputer Science ApplicationsEducationStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonProduction (computer science)High Energy Physics::Experiment010306 general physicsLeptonBosonEvent generator
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Overview of searches for dark matter at the LHC

2014

Dark matter remains one of the most puzzling mysteries in Fundamental Physics of our times. Experiments at high-energy physics colliders are expected to shed light to its nature and determine its properties. This review talk focuses on recent searches for dark-matter signatures at the Large Hadron Collider, either within specific theoretical scenarios, such as supersymmetry, or in a model-independent scheme looking for mono-X events arising in WIMP-pair production.

PhysicsHistoryParticle physicsLarge Hadron ColliderDark matterFOS: Physical sciencesSupersymmetryComputer Science ApplicationsEducationHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Fundamental physicsHigh Energy Physics::ExperimentParticle Physics - Experiment
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The Capabilities of monochromatic EC neutrino beams with the SPS upgrade

2007

The goal for future neutrino facilities is the determination of the U(e3) mixing and CP violation in neutrino oscillations. This will require precision experiments with a very intense neutrino source and energy control. With this objective in mind, the creation of monochromatic neutrino beams from the electron capture decay of boosted ions by the SPS of CERN has been proposed. We discuss the capabilities of such a facility 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 reach a better sensitivity to CP violation iff it is accompanied by a longer baseline. We compare the physics potential for two different…

PhysicsHistoryParticle physicsLarge Hadron ColliderElectron capturePhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaDetectorFOS: Physical sciencesFísicaComputer Science ApplicationsEducationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)UpgradeCP violationHigh Energy Physics::ExperimentMonochromatic colorNeutrinoNeutrino oscillation
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Simultaneous analysis of neutrinoless double beta decay and LHC pp-cross sections: limits on the left-right mixing angle

2015

The extension of the Standard Model of electroweak interactions, to accommodate massive neutrinos and/or right-handed currents, is one of the fundamental questions to answer in the cross-field of particle and nuclear physics. The consequences of such extensions would reflect upon nuclear decays, like the very exotic nuclear double-beta-decay, as well as upon high-energy proton-proton reactions of the type performed at the LHC accelerator. In this talk we shall address this question by looking at the results reported by the ATLAS and CMS collaborations, where the excitation and decay of a heavy-mass boson may be mediated by a heavy-mass neutrino in proton-proton reactions leading to two jets…

PhysicsHistoryParticle physicsLarge Hadron ColliderElectroweak interactionNuclear TheoryHigh Energy Physics::PhenomenologyFísicaneutrinoless double beta decayComputer Science ApplicationsEducationStandard ModelNuclear physicsdouble-beta-decayDouble beta decayLHC acceleratorHigh Energy Physics::ExperimentLHCNeutrinoNuclear ExperimentMixing (physics)Ciencias ExactasLeptonBoson
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Long-Lived Slepton in the Coannihilation Region and Measurement of Lepton Flavour Violation at LHC

2009

When the mass difference between the lightest slepton and the lightest neutralino is smaller than the tau mass, the lifetime of the lightest slepton in the constrained Minimal Supersymmetric Standard Model (MSSM) increases in many orders of magnitude with respect to typical lifetimes of other supersymmetric particles. In a general MSSM, the lifetime of the lightest slepton is inversely proportional to the square of the intergenerational mixing in the slepton mass matrices. Such a long-lived slepton would produce a distinctive signature at LHC and a measurement of its lifetime would be relatively simple. Therefore, the long-lived slepton scenario offers an excellent opportunity to study lept…

PhysicsHistoryParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesComputer Science ApplicationsEducationHigh Energy Physics - Phenomenologymedicine.anatomical_structureHigh Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)Atlas (anatomy)NeutralinomedicineHigh Energy Physics::ExperimentMinimal Supersymmetric Standard ModelLepton
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Implications of new generations on neutrino masses

2011

We explore the possible implications that new families, that are being searched for at the LHC, would have on neutrino masses. In particular, we have explored the possibility that the smallness of the observed neutrino masses is naturally understood in a modified version of the Standard Model (SM) with complete extra generations of fermions, i.e., that have right-handed neutrinos, in which neutrino masses are generated at two loops. With one extra family it is not possible to fit the observed spectrum of masses and mixings. However, the radiative mass generated provides an important constraint in these kind of models, so the neutrino masses do not exceed their cosmological bound. Within the…

PhysicsHistoryParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaContext (language use)FermionParameter spacePartícules (Física nuclear)Computer Science ApplicationsEducationStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillation
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The polarized electron-nucleon collider project ENC at GSI/FAIR

2011

The ENC project attempts to realize an electron-nucleon collider at the upcoming Facility for Antiproton and Ion Research FAIR at GSI Darmstadt by utilizing the antiproton high-energy storage ring HESR for polarized proton and deuteron beams. The addition of a 3.3 GeV storage ring for polarized electrons will enable electron-nucleon collisions up to a center-of-mass energy of - s - 14 GeV. In such a configuration peak luminosities in the range of L = 10(32) to 10(33)cm(-')(2)s(-')(1) are feasible . Beam-beam effects in a space-charge dominated regimes in conjunction with high-energy electron cooling represents one of the main challenges for this project. In this paper beam- and spin dynamic…

PhysicsHistoryParticle physicsProtonElectronComputer Science ApplicationsEducationlaw.inventionNuclear physicslawAntiprotonFacility for Antiproton and Ion ResearchPhysics::Accelerator PhysicsHigh Energy Physics::Experimentddc:530NucleonColliderNuclear ExperimentStorage ringElectron cooling
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Performance study of the fast timing Cherenkov detector based on a microchannel plate PMT

2017

Prototype of the fast timing Cherenkov detector, applicable in high-energy collider experiments, has been developed basing on the modified Planacon XP85012 MCP-PMT and fused silica radiators. We present the reasons and description of the MCP-PMT modification, timing and amplitude characteristics of the prototype including the summary of the detector's response on particle hits at oblique angles and MCP-PMT performance at high illumination rates.

PhysicsHistoryPhotomultiplierPhysics::Instrumentation and Detectors010308 nuclear & particles physicsbusiness.industryCherenkov detectorQuantitative Biology::Tissues and OrgansDetectorAstrophysics::Instrumentation and Methods for Astrophysics01 natural sciencesParticle detectorComputer Science ApplicationsEducationlaw.inventionOpticslaw0103 physical sciencesScintillation counterMeasuring instrumentMicrochannel plate detector010306 general physicsbusinessColliderJournal of Physics: Conference Series
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