Search results for "Instrumentation"

showing 10 items of 4914 documents

Use of an FPGA to identify electromagnetic clusters and isolated hadrons in the ATLAS level-1 calorimeter trigger

2003

Abstract At the full LHC design luminosity of 10 34 cm −2 s −1 , there will be approximately 109 proton–proton interactions per second. The ATLAS level-1 trigger is required to have an acceptance factor of ∼10−3. The calorimeter trigger covers the region |η|⩽5.0, and φ=0 to 2π. The distribution of transverse energy over the trigger phase space is analysed to identify candidates for electrons/photons, isolated hadrons, QCD jets and non-interacting particles. The Cluster Processor of the level-1 calorimeter trigger is designed to identify transverse energy clusters associated with the first two of these. The algorithms based on the trigger tower energies which have been designed to identify s…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonLarge Hadron ColliderLuminosity (scattering theory)Calorimeter (particle physics)Particle detectorParticle identificationNuclear physicsmedicine.anatomical_structureAtlas (anatomy)Cluster (physics)medicineDetectors and Experimental TechniquesInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Search for nonpointing photons in the diphoton andETmissfinal state ins=7  TeVproton-proton collisions using the ATLAS detector

2013

A search has been performed for photons originating in the decay of a neutral long-lived particle, exploiting the capabilities of the ATLAS electromagnetic calorimeter to make precise measurements of the flight direction of photons, as well as the calorimeter's excellent time resolution. The search has been made in the diphoton plus missing transverse energy final state, using the full data sample of 4.8 fb(-1) of 7 TeV proton-proton collisions collected in 2011 with the ATLAS detector at the LHC. No excess is observed above the background expected from Standard Model processes. The results are used to set exclusion limits in the context of gauge mediated supersymmetry breaking models, with…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas (topology)Atlas detectorHigh Energy Physics::Phenomenology01 natural sciencesSupersymmetry breakingNuclear physicsTransverse plane0103 physical sciencesNeutralinoHigh Energy Physics::ExperimentGravitino010306 general physicsPhysical Review D
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The PANDA Barrel DIRC detector

2014

Abstract The PANDA experiment at the new Facility for Antiproton and Ion Research in Europe (FAIR) at GSI, Darmstadt, will study fundamental questions of hadron physics and QCD using high-intensity cooled antiproton beams with momenta between 1.5 and 15 GeV/c. Efficient Particle Identification for a wide momentum range and the full solid angle is required for reconstructing the various physics channels of the PANDA program. Hadronic Particle Identification in the barrel region of the detector will be provided by a DIRC counter. The design is based on the successful BABAR DIRC with important improvements, such as focusing optics and fast photon timing. Several of these improvements, includin…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonLarge Hadron ColliderPhysics::Instrumentation and DetectorsHadronDetectorParticle identificationNuclear physicsConceptual designAntiprotonPhysics::Accelerator PhysicsFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Coherent pion production in neutrino nucleus collision in the 1 GeV region

1996

We calculate cross sections for coherent pion production in nuclei induced by neutrinos and antineutrinos of the electron and muon type. The analogies and differences between this process and the related ones of coherent pion production induced by photons, or the (p,n) and $(^3 He, t)$ reactions are discussed. The process is one of the several ones occurring for intermediate energy neutrinos, to be considered when detecting atmospheric neutrinos. For this purpose the results shown here can be easily extrapolated to other energies and other nuclei.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonMuonNuclear TheoryPhysics::Instrumentation and DetectorsNuclear TheoryFísicaFOS: Physical sciencesElectronCollisionNuclear physicsNuclear Theory (nucl-th)medicine.anatomical_structurePionmedicineProduction (computer science)High Energy Physics::ExperimentNeutrinoNuclear ExperimentNucleus
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Dynamically generated resonances from the vector octet-baryon decuplet interaction and their radiative decays into γ-baryon decuplet

2009

The dynamically generated resonances from vector meson-baryon decuplet are studied using Lagrangians of the hidden gauge theory for vector interactions. One shows that some of the generated states can be associated with some known baryon resonances in the PDG data, while others are predictions for new states. Furthermore, we calculate the radiative decay widths of these resonances into a photon and a baryon decuplet.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonOctetHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyRadiative decayAstronomy and AstrophysicsBaryonQuantum electrodynamicsRadiative transferGauge theoryNuclear ExperimentInstrumentationChinese Physics C
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Relic Neutrino Decoupling Including Flavour Oscillations

2005

In the early universe, neutrinos are slightly coupled when electron-positron pairs annihilate transferring their entropy to photons. This process originates non-thermal distortions on the neutrino spectra which depend on neutrino flavour, larger for nu_e than for nu_mu or nu_tau. We study the effect of three-neutrino flavour oscillations on the process of neutrino decoupling by solving the momentum-dependent kinetic equations for the neutrino spectra. We find that oscillations do not essentially modify the total change in the neutrino energy density, giving N_eff=3.046 in terms of the effective number of neutrinos, while the small effect over the production of primordial 4He is increased by…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFlavourAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaNeutrino decouplingSolar neutrino problemAstrophysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLepton
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Performance of the photon spectrometer TAPS for deep subthreshold pion detection

2005

Abstract We present in this paper the characteristics of the BaF 2 spectrometer, TAPS, which allow to detect rare electromagnetic events in a high hadronic background. The case of deep subthreshold pions produced in 36 Ar+ 197 Au collisions at 25A and 35A MeV, in which the pion signal is much weaker than the hadronic background and comparable to the cosmic ray background, is studied.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonSpectrometerSubthreshold conductionNuclear TheoryHadronCosmic raySignalNuclear physicsElectromagnetic calorimeterPionHigh Energy Physics::ExperimentNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Search for eV (pseudo)scalar penetrating particles in the SPS neutrino beam

2000

We carried out a model-independent search for light scalar or pseudoscalar particles $a$'s (an example of which is the axion) that couple to two photons by using a photon-regeneration method at high energies allowing a substantial increase in the sensitivity to $eV$ masses.\ The experimental set-up is based on elements of the CERN West Area Neutrino Facility (WANF) beam line and theNOMAD neutrino detector.\ The new particles, if they exist, could be produced through the Primakoff effect in interactions of high energy photons, generated by the 450 $GeV$ protons in the CERN SPS neutrino target, with virtual photons from the WANF horn magnetic field.\ The particles would penetrate the downstre…

PhysicsNuclear and High Energy PhysicsParticle physicsPhoton[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaVirtual particleFísicaScalar boson01 natural sciences7. Clean energyNuclear physicsPseudoscalarNeutrino detector0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentNeutrino010306 general physicsAxionPrimakoff effectParticle Physics - Experiment
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Exposing dark sector with futureZ-factories

2019

We investigate the prospects of searching dark sector models via exotic [Formula: see text]-boson decay at future [Formula: see text] colliders with Giga [Formula: see text] and Tera [Formula: see text] options. Four general categories of dark sector models: Higgs portal dark matter, vector portal dark matter, inelastic dark matter and axion-like particles, are considered. Focusing on channels motivated by the dark sector models, we carry out a model independent study of the sensitivities of [Formula: see text]-factories in probing exotic decays. The limits on branching ratios of the exotic [Formula: see text] decay are typically [Formula: see text] for the Giga [Formula: see text] and [For…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelAstrophysics::Instrumentation and Methods for AstrophysicsEffective field theoryHiggs bosonComputer Science::General LiteratureHigh Energy Physics::ExperimentComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)Astronomy and AstrophysicsTera-Atomic and Molecular Physics and OpticsInternational Journal of Modern Physics A
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Heavy neutrino mixing and single production at linear collider

1997

We study the single production of heavy neutrinos via the processes $e^-e^+ \to \nu N$ and $e^-\gamma \to W^- N$ at future linear colliders. As a base of our considerations we take a wide class of models, both with vanishing and non-vanishing left-handed Majorana neutrino mass matrix $m_L$. We perform a model independent analyses of the existing experimental data and find connections between the characteristic of heavy neutrinos (masses, mixings, CP eigenvalues) and the $m_L$ parameters. We show that with the present experimental constraints heavy neutrino masses almost up to the collision energy can be tested in the future experiments.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesMass matrix01 natural sciences7. Clean energylaw.inventionBase (group theory)High Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)law0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)Neutrino010306 general physicsColliderEigenvalues and eigenvectorsMixing (physics)Physics Letters B
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