Search results for "Instrumentation"

showing 10 items of 4914 documents

J/ψPolarization inppCollisions ats=7  TeV

2012

The ALICE Collaboration has studied J/psi production in pp collisions at root s = 7 TeV at the LHC through its muon pair decay. The polar and azimuthal angle distributions of the decay muons were measured, and results on the J/psi polarization parameters lambda(theta) and lambda(phi) were obtained. The study was performed in the kinematic region 2: 5 < y < 4, 2 < p(t) < 8 GeV/c, in the helicity and Collins-Soper reference frames. In both frames, the polarization parameters are compatible with zero, within uncertainties.

PhysicsParticle physicsMuonLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsGeneral Physics and AstronomyLambdaPolarization (waves)01 natural sciencesHelicityNuclear physicsAzimuthAngular distribution0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsReference framePhysical Review Letters
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Corrections to the fluxes of a Neutrino Factory

2002

In view of their physics goals, future neutrino factories from muon decay aim at an overall flux precision of ${\cal O}(1%)$ or better. We analytically study the QED radiative corrections to the neutrino differential distributions from muon decay. Kinematic uncertainties due to the divergence of the muon beam are considered as well. The resulting corrections to the neutrino flux turn out to be of order ${\cal O}(0.1%)$, safely below the required precision.

PhysicsParticle physicsMuonPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)Partícules (Física nuclear)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Flux (metallurgy)Radiative transferPhysics::Accelerator PhysicsNeutrino FactoryHigh Energy Physics::ExperimentNeutrinoEngineering (miscellaneous)Beam (structure)
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Resistive Micromegas for the Muon Spectrometer Upgrade of the ATLAS Experiment

2017

It is reported on the construction and test of large scale resistive Micromegas detectors for the ATLAS New Small Wheel upgrade. The production procedure of the 2 to 3 m2 active area is described. The validation of the construction procedure is proven with results obtained with prototype detectors showing 100 µm spatial resolution in the precision coordinate and above 98% efficiency In the context of the upgrade project of the ATLAS Muon system, we report on the construction of Micromegas detectors with an active area of 2 to 3 m$^2$ . The validation of the construction procedure is proven with results obtained with prototype detectors showing 100 $\mu $m spatial resolution in the precision…

PhysicsParticle physicsMuonPhysics::Instrumentation and DetectorsATLAS experimentDetectorContext (language use)MicroMegas detectorNuclear physicsmedicine.anatomical_structureUpgradeAtlas (anatomy)medicineHigh Energy Physics::ExperimentImage resolutionParticle Physics - Experiment
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(g−2)e,μ in an extended inverse type-III seesaw model

2021

There has been a longstanding discrepancy between the experimental measurements of the electron and muon anomalous magnetic moments and their predicted values in the Standard Model. This is particularly relevant in the case of the muon $g\ensuremath{-}2$, which has attracted a remarkable interest in the community after the long-awaited announcement of the first results by the Muon $g\ensuremath{-}2$ collaboration at Fermilab, which confirms a previous measurement by the E821 experiment at Brookhaven and enlarges the statistical significance of the discrepancy, now at $4.2\ensuremath{\sigma}$. In this paper we consider an extension of the inverse type-III seesaw with a pair of vectorlike lep…

PhysicsParticle physicsMuonSeesaw molecular geometryPhysics::Instrumentation and DetectorsInverseHigh Energy Physics::ExperimentElectroweak scaleNeutrinoType (model theory)LeptonStandard ModelPhysical Review D
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Muon-pair production by atmospheric muons in cosmoALEPH

2006

Data from a dedicated cosmic ray run of the ALEPH detector were used in a study of muon trident production, i.e., muon pairs produced by muons. Here the overburden and the calorimeters are the target materials while the ALEPH time projection chamber provides the momentum measurements. A theoretical estimate of the muon trident cross section is obtained by developing a Monte Carlo simulation for muon propagation in the overburden and the detector. Two muon trident candidates were found to match the expected theoretical pattern. The observed production rate implies that the nuclear form factor cannot be neglected for muon tridents.

PhysicsParticle physicsMuonTime projection chamberPhysics::Instrumentation and DetectorsMonte Carlo methodDetectorForm factor (quantum field theory)General Physics and AstronomyCosmic rayNuclear physicsPair productionMuon colliderPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle Physics - Experiment
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Measurement of the single π0 production rate in neutral current neutrino interactions on water

2018

The single π0 production rate in neutral current neutrino interactions on water in a neutrino beam with a peak neutrino energy of 0.6 GeV has been measured using the POD, one of the subdetectors of the T2K near detector. The production rate was measured for data taking periods when the POD contained water (2.64×1020 protons-on-target) and also periods without water (3.49×1020 protons-on-target). A measurement of the neutral current single π0 production rate on water is made using appropriate subtraction of the production rate with water in from the rate with water out of the target region. The subtraction analysis yields 106±41±69 signal events where the uncertainties are statistical (stat.…

PhysicsParticle physicsNeutral currentPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaDetectorFluxInteraction energy01 natural sciences7. Clean energyNuclear physicsCross section (physics)0103 physical sciencesMass spectrumHigh Energy Physics::ExperimentNeutrinoNuclear Experiment010306 general physicsNucleonPhysical Review D
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Mass and width of theΔ(1232)resonance using complex-mass renormalization

2016

We discuss the pole mass and the width of the $\Delta(1232)$ resonance to third order in chiral effective field theory. In our calculation we choose the complex-mass renormalization scheme (CMS) and show that the CMS provides a consistent power-counting scheme. In terms of the pion-mass dependence, we compare the convergence behavior of the CMS with the small-scale expansion (SSE).

PhysicsParticle physicsNuclear TheoryPhysics::Instrumentation and Detectors010308 nuclear & particles physicsFeynman graph01 natural sciencesResonance (particle physics)RenormalizationHigh Energy Physics - PhenomenologyThird orderHigh Energy Physics - LatticeQuantum electrodynamics0103 physical sciencesConvergence (routing)Effective field theory010306 general physicsNuclear theoryPhysical Review C
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Dynamical seesaw mechanism for Dirac neutrinos

2016

So far we have not been able to establish that, as theoretically expected, neutrinos are their own anti-particles. Here we propose a dynamical way to account for the Dirac nature of neutrinos and the smallness of their mass in terms of a new variant of the seesaw paradigm in which the energy scale of neutrino mass generation could be accessible to the current LHC experiments.

PhysicsParticle physicsNuclear and High Energy PhysicsCurrent (mathematics)Large Hadron Collider010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsDirac (video compression format)Mass generationHigh Energy Physics::PhenomenologyFOS: Physical sciencesNew variant01 natural scienceslcsh:QC1-999High Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicslcsh:PhysicsPhysics Letters B
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The Zee–Babu model revisited in the light of new data

2014

We update previous analyses of the Zee-Babu model in the light of new data, e.g., the mixing angle $\theta_{13}$, the rare decay $\mu\to e \gamma$ and the LHC results. We also analyse the possibility of accommodating the deviations in $\Gamma(H\to \gamma\gamma)$ hinted by the LHC experiments, and the stability of the scalar potential. We find that neutrino oscillation data and low energy constraints are still compatible with masses of the extra charged scalars accessible to LHC. Moreover, if any of them is discovered, the model can be falsified by combining the information on the singly and doubly charged scalar decay modes with neutrino data. Conversely, if the neutrino spectrum is found t…

PhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaScalar potential01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesCP violationNeutrino010306 general physicsNeutrino oscillationMixing (physics)Nuclear Physics B
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Energy dependence of CP-violation reach for monochromatic neutrino beam

2008

The ultimate goal for future neutrino facilities is the determination of CP violation in neutrino oscillations. Besides $| U(e3) | \ne 0$, 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 compare the physics potential for two different configurations: I) $\gamma=90$ and $\gamma=195$ (maximum achievable at present SPS) to Frejus; II) $\gamma=195$ and $\gamma=440$ (…

PhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron ColliderElectron capturePhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFísicaElementary particleMassless particleNuclear physicsHigh Energy Physics - PhenomenologyUpgradeCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationNuclear ExperimentPhysics Letters B
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