Search results for "Control system"

showing 10 items of 971 documents

Influence of temperature-dependent shear viscosity on elliptic flow at backward and forward rapidities in ultrarelativistic heavy-ion collisions

2014

We explore the influence of a temperature-dependent shear viscosity over entropy density ratio $\eta/s$ on the azimuthal anisotropies v_2 and v_4 of hadrons at various rapidities. We find that in Au+Au collisions at full RHIC energy, $\sqrt{s_{NN}}=200$ GeV, the flow anisotropies are dominated by hadronic viscosity at all rapidities, whereas in Pb+Pb collisions at the LHC energy, $\sqrt{s_{NN}}=2760$ GeV, the flow coefficients are affected by the viscosity both in the plasma and hadronic phases at midrapidity, but the further away from midrapidity, the more dominant the hadronic viscosity is. We find that the centrality and rapidity dependence of the elliptic and quadrangular flows can help…

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryHadronFOS: Physical sciences01 natural sciencesNuclear physicsNuclear Theory (nucl-th)Physics::Fluid DynamicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRapiditySensitivity (control systems)Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsta114010308 nuclear & particles physicsEquation of state (cosmology)Elliptic flowHigh Energy Physics - PhenomenologyQuark–gluon plasmaHigh Energy Physics::ExperimentRelativistic Heavy Ion ColliderEnergy (signal processing)Physical review C
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The Mu3e Data Acquisition

2020

The Mu3e experiment aims to find or exclude the lepton flavour violating decay $\mu^+\to e^+e^-e^+$ with a sensitivity of one in 10$^{16}$ muon decays. The first phase of the experiment is currently under construction at the Paul Scherrer Institute (PSI, Switzerland), where beams with up to 10$^8$ muons per second are available. The detector will consist of an ultra-thin pixel tracker made from High-Voltage Monolithic Active Pixel Sensors (HV-MAPS), complemented by scintillating tiles and fibres for precise timing measurements. The experiment produces about 100 Gbit/s of zero-suppressed data which are transported to a filter farm using a network of FPGAs and fast optical links. On the filte…

Nuclear and High Energy PhysicsParticle physicsPhysics - Instrumentation and DetectorsMesonPhysics::Instrumentation and Detectorsdata acquisitionfibre: opticalFOS: Physical scienceshigh energy physics instrumentationprinted circuits7. Clean energycomputer: networkOptical fiber communicationData acquisitionsemiconductor detector: pixelOptical switchesmultiprocessor: graphicshardwareSensitivity (control systems)muon+: decay[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Electrical and Electronic EngineeringGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)scintillation counterFPGAClocksPhysicsData acquisition (DAQ)MuonPixelMesonsDetectorlepton: flavor: violationField programmable gate arraysDetectorsInstrumentation and Detectors (physics.ins-det)sensitivityNuclear Energy and EngineeringFilter (video)field programmable gate arrays (FPGAs)Data acquisition (DAQ); field programmable gate arrays (FPGAs); high energy physics instrumentation; printed circuitselectronics: readoutHigh Energy Physics::ExperimentLeptonelectronics: design
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Sensitivity of the NEXT experiment to Xe-124 double electron capture

2021

[EN] Double electron capture by proton-rich nuclei is a second-order nuclear process analogous to double beta decay. Despite their similarities, the decay signature is quite di erent, potentially providing a new channel to measure the hypothesized neutrinoless mode of these decays. The Standard-Model-allowed two-neutrino double electron capture has been predicted for a number of isotopes, but only observed in 78Kr, 130Ba and, recently, 124Xe. The sensitivity to this decay establishes a benchmark for the ultimate experimental goal, namely the potential to discover also the lepton-number-violating neutrinoless version of this process. Here we report on the current sensitivity of the NEXT-Whit…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsElectron captureDark Matter and Double Beta DecayExtrapolationFOS: Physical scienceschemistry.chemical_elementElectronsElectron01 natural sciences7. Clean energyAtomicHigh Energy Physics - ExperimentTECNOLOGIA ELECTRONICANuclear physicsHigh Energy Physics - Experiment (hep-ex)XenonParticle and Plasma PhysicsDouble beta decay0103 physical sciencesNuclear MatrixNuclearSensitivity (control systems)Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentMathematical PhysicsPhysicsQuantum PhysicsIsotope010308 nuclear & particles physicsRaigs beta -- DesintegracióDetectorFísicaMolecularDetectorsDetectorInstrumentation and Detectors (physics.ins-det)Beta DecayNuclear & Particles Physicschemistry13. Climate actionBeta rays -- Decay
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Search for two-neutrino double electron capture of $^{124}$Xe with XENON100

2017

Two-neutrino double electron capture is a rare nuclear decay where two electrons are simultaneously captured from the atomic shell. For $^{124}$Xe this process has not yet been observed and its detection would provide a new reference for nuclear matrix element calculations. We have conducted a search for two-neutrino double electron capture from the K-shell of $^{124}$Xe using 7636 kg$\cdot$d of data from the XENON100 dark matter detector. Using a Bayesian analysis we observed no significant excess above background, leading to a lower 90 % credibility limit on the half-life $T_{1/2}>6.5\times10^{20}$ yr. We also evaluated the sensitivity of the XENON1T experiment, which is currently bein…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsElectron captureenergy resolutionFOS: Physical scienceschemistry.chemical_elementelectron: captureElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBayesianX-rayneutrinoXenon0103 physical sciencesSensitivity (control systems)[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)010306 general physics[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear ExperimentPhysicsnucleus: decayTime projection chamberphotomultiplier010308 nuclear & particles physicsbackgroundInstrumentation and Detectors (physics.ins-det)dark matter: detectorAtomic shellsensitivitytime projection chamberGran SassoxenonchemistryNeutrinoAtomic physicsRadioactive decayexperimental results
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Radioactivity control strategy for the JUNO detector

2021

JUNO is a massive liquid scintillator detector with a primary scientific goal of determining the neutrino mass ordering by studying the oscillated anti-neutrino flux coming from two nuclear power plants at 53 km distance. The expected signal anti-neutrino interaction rate is only 60 counts per day, therefore a careful control of the background sources due to radioactivity is critical. In particular, natural radioactivity present in all materials and in the environment represents a serious issue that could impair the sensitivity of the experiment if appropriate countermeasures were not foreseen. In this paper we discuss the background reduction strategies undertaken by the JUNO collaboration…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsNuclear engineeringMonte Carlo methodControl (management)measurement methodsFOS: Physical sciencesQC770-798Scintillator7. Clean energy01 natural sciencesNOPE2_2Nuclear and particle physics. Atomic energy. Radioactivity0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530Sensitivity (control systems)010306 general physicsPhysicsJUNOliquid [scintillation counter]010308 nuclear & particles physicsbusiness.industryDetectorSettore FIS/01 - Fisica Sperimentaleradioactivity [background]suppression [background]Instrumentation and Detectors (physics.ins-det)Monte Carlo [numerical calculations]Nuclear powerthreshold [energy]sensitivityNeutrino Detectors and Telescopes (experiments)GEANTNeutrinobusinessEnergy (signal processing)
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High resolution detectors based on continuous crystals and SiPMs for small animal PET

2012

International audience; Sensitivity and spatial resolution are the two main factors to maximize in emission imaging. The improvement of one factor deteriorates the other with pixelated crystals. In this work we combine SiPM matrices with monolithic crystals, using an accurate γ-ray interaction position determination algorithm that provides depth of interaction. Continuous crystals provide higher sensitivity than pixelated crystals, while an accurate interaction position determination does not degrade the spatial resolution. Monte Carlo simulations and experimental data show good agreement both demonstrating sub-millimetre intrinsic spatial resolution. A system consisting in two rotating det…

Nuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsSiPMMonte Carlo methodHigh resolution01 natural sciencesCoincidence030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineOpticsSilicon photomultiplierPosition (vector)0103 physical sciencesHigh resolutionSensitivity (control systems)[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/MicroelectronicsInstrumentationImage resolutionPhysics010308 nuclear & particles physicsbusiness.industryDetectorPosition determinationPETMonolithic crystalsbusiness
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Sensitivity enhancement in pulse EPR distance measurements

2004

Established pulse EPR approaches to the measurement of small dipole-dipole couplings between electron spins rely on constant-time echo experiments to separate relaxational contributions from dipolar time evolution. This requires a compromise between sensitivity and resolution to be made prior to the measurement, so that optimum data are only obtained if the magnitude of the dipole-dipole coupling is known beforehand to a good approximation. Moreover, the whole dipolar evolution function is measured with relatively low sensitivity. These problems are overcome by a variable-time experiment that achieves suppression of the relaxation contribution by reference deconvolution. Theoretical and exp…

Nuclear and High Energy PhysicsProtein ConformationBiophysicsAnalytical chemistryBiochemistrySensitivity and Specificitylaw.inventionlawspin labelingSensitivity (control systems)protein structurepair correlation functionElectron paramagnetic resonanceCouplingSpinsChemistryPulsed EPRRelaxation (NMR)Time evolutionElectron Spin Resonance SpectroscopyPhotosystem II Protein ComplexReproducibility of ResultsSignal Processing Computer-AssistedELDORCondensed Matter PhysicsComputational physicsDeconvolutionEPRAlgorithms
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Sensitivity of a tonne-scale NEXT detector for neutrinoless double-beta decay searches

2021

The NEXT collaboration: et al.

Nuclear and High Energy Physicschemistry.chemical_elementQC770-798Parameter space01 natural sciences7. Clean energyAtomicNuclear physicsXenonParticle and Plasma PhysicsDouble beta decayNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesDark Matter and Double Beta Decay (experiments)NuclearSensitivity (control systems)010306 general physicsMathematical PhysicsPhysicsQuantum Physics010308 nuclear & particles physicsRaigs beta -- DesintegracióDetectorMolecularDetectorsNuclear & Particles PhysicschemistryBeta rays -- DecayNeutrinoTonneOrder of magnitudeJournal of High Energy Physics
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IGISOL control system modernization

2016

Abstract Since 2010, the IGISOL research facility at the Accelerator laboratory of the University of Jyvaskyla has gone through major changes. Comparing the new IGISOL4 facility to the former IGISOL3 setup, the size of the facility has more than doubled, the length of the ion transport line has grown to about 50 m with several measurement setups and extension capabilities, and the accelerated ions can be fed to the facility from two different cyclotrons. The facility has evolved to a system comprising hundreds of manual, pneumatic and electronic devices. These changes have prompted the need to modernize also the facility control system taking care of monitoring and transporting the ion beam…

Nuclear and High Energy Physicsta114ta213010308 nuclear & particles physicsComputer sciencesoftwareMaintainabilityIndustrial control systemsystem architecture01 natural scienceslaw.inventionData acquisitionlawControl system0103 physical sciencesSystems engineeringSystems architecturehardwareElectronicsEPICScontrol system010306 general physicsDistributed control systemInstrumentationRemote controlNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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High voltage conditioning of the electrostatic deflector of MARA

2016

Abstract MARA is a new recoil mass separator in the Accelerator Laboratory of University of Jyvaskyla (JYFL-ACCLAB) with a mass resolving power of 250 and an ion-optical configuration of QQQD E D M . In this paper the construction, control and conditioning of its electrostatic deflector are described. The deflector was designed for voltages up to 500 kV accross the gap, corresponding to a 3.6 MV/m field, to accomodate fusion reactions with inverse kinematics. Titanium electrodes with a beam dump opening in the anode are used. The conditioning procedure, which has been used repeatedly to take the deflector to 450 kV, is described, along with the safety systems and precautions that are in pla…

Nuclear and High Energy Physicsta114ta213business.industryChemistryehdollistaminenAnalytical chemistryhallintajärjestelmätHigh voltageAnodelaw.inventionOpticsRecoilhigh voltageconditioninglawElectroderecoil mass separatorNuclear fusionBeam dumpbusinessInstrumentationcontrol systemsSeparator (electricity)VoltageNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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