Search results for " DETECTOR."

showing 10 items of 2685 documents

Measurement of the Fluctuations in the Number of Muons in Extensive Air Showers with the Pierre Auger Observatory

2021

The successful installation, commissioning, and operation of the Pierre Auger Observatory would not have been possible without the strong commitment and effort from the technical and administrative staff in Malargue. We are very grateful to the following agencies and organizations for financial support: Argentina-Comision Nacional de Energia Atomica, Agencia Nacional de Promocion Cientifica y Tecnologica (ANPCyT), Consejo Nacional de Investigaciones Cientificas y Tecnicas (CONICET), Gobierno de la Provincia de Mendoza, Municipalidad de Malargue, NDM Holdings and Valle Las Lenas; in gratitude for their continuing cooperation over land access; Australia-the Australian Research Council; Brazil…

interaction: modelPhysics::Instrumentation and DetectorsAstronomyHadronGeneral Physics and AstronomyUltra-high energy cosmic rays muons properties hadronic models01 natural sciencescosmic ray; particle interaction; astroparticle detectorsAugerHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)ironsurface [detector]Observatory[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]cosmic rayPhysics4. EducationPhysicsSettore FIS/01 - Fisica Sperimentalemeasured [fluctuation]model [interaction]Astrophysics::Instrumentation and Methods for Astrophysicsmodel: hadronicfluctuation: measured3. Good healthAugerobservatoryparticle interactionSciences exactes et naturellesatmosphere [showers]model [particle]airCherenkov counter: waterAstrophysics::High Energy Astrophysical PhenomenaUHE [cosmic radiation]FOS: Physical sciencesCosmic raydetector: fluorescenceNuclear physicsastroparticle detectorscosmic raysmuon0103 physical sciencescalorimeterddc:53014. Life underwatercosmic radiation: UHEHigh Energy Physicsdistribution functionelectromagnetic component010306 general physicsAstrophysiquePierre Auger Observatoryfluorescence [detector]Muonshowers: atmospherehep-exdetector: surfacewater [Cherenkov counter]particle: modelSmall deviationsFísicaASTROFÍSICAAir showerExperimental High Energy PhysicsElementary Particles and Fieldshadronic [model]High Energy Physics::Experiment
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Exploration of jet substructure using iterative declustering in pp and Pb–Pb collisions at LHC energies

2020

The ALICE collaboration at the CERN LHC reports novel measurements of jet substructure in pp collisions at $\sqrt{s}$= 7 TeV and central Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. Jet substructure of track-based jets is explored via iterative declustering and grooming techniques. We present the measurement of the momentum sharing of two-prong substructure exposed via grooming, the $z_{\rm{g}}$, and its dependence on the opening angle, in both pp and Pb-Pb collisions. We also present the first measurement of the distribution of the number of branches obtained in the iterative declustering of the jet, which is interpreted as the number of its hard splittings. In Pb-Pb collisions, we…

jet substructure pp and Pb-Pb collisionsheavy ion: scattering:Kjerne- og elementærpartikkelfysikk: 431 [VDP]Physics::Instrumentation and DetectorsMonte Carlo methodPb-Pbjet quenchin; jet substructure; heavy-ion collisionshiukkasfysiikkapp and Pb-Pb collisionsnucl-expp01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)ALICEjetscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]color: coherenceNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentMonte Carlojet ; declustering ; pp ; Pb-PbPhysicsLarge Hadron ColliderPhysicsVDP::Kjerne- og elementærpartikkelfysikk: 431suppressionlcsh:QC1-999PRIRODNE ZNANOSTI. Fizika.CERN LHC Coll:Nuclear and elementary particle physics: 431 [VDP]VDP::Nuclear and elementary particle physics: 431PYTHIAdeclusteringLHCpp collisionsParticle Physics - ExperimentCoherence (physics)Nuclear and High Energy Physicsp p: scatteringAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencesNuclear physicsheavy-ion; pp collisions; jet substructure; ALICEscattering [heavy ion]0103 physical sciencesddc:530jet substructureNuclear Physics - Experiment010306 general physicsenhancementjet quenchin010308 nuclear & particles physicshep-exheavy-ion collisionsNATURAL SCIENCES. Physics.7000 GeV-cms/nucleon 2760 GeV-cms/nucleonHeavy ion interactionQGPQuark–gluon plasmaheavy-ioncoherence [color]SubstructureHigh Energy Physics::ExperimentLHC jet QGPLHC High-Energy Physicslcsh:Physicsexperimental results
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Laser assisted decay spectroscopy at the CRIS beam line at ISOLDE

2012

A new collinear resonant ionization spectroscopy (Cris)beam line has recently been installed at Isolde, Cern utilising lasers to combine collinear laser spectroscopy and resonant ionization spectroscopy. The combined technique offers the ability to purify an ion beam that is heavily contaminated with radioactive isobars, including the ground state of an isotope from its isomer, allowing sensitive secondary experiments to be performed. A new programme aiming to use the Cris technique for the separation of nuclear isomeric states for decay spectroscopy will commence in 2011. A decay spectroscopy station, consisting of a rotating wheel implantation system for alpha decay spectroscopy, and thre…

laser assisted decay spectroscopyHistoryIon beamCRIS beam line[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyParticle detector010305 fluids & plasmasEducationlaw.inventionlawIonization0103 physical sciencesNuclear Experiment010306 general physicsSpectroscopyComputingMilieux_MISCELLANEOUSChemistryLaserComputer Science ApplicationsSemiconductor detectorcollinear resonant ionization spectroscopyPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentAlpha decayAtomic physicsRadioactive decay
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Invited Article: Ultra-broadband terahertz coherent detection via a silicon nitride-based deep sub-wavelength metallic slit

2018

We present a novel class of CMOS-compatible devices aimed to perform the solid-state-biased coherent detection of ultrashort terahertz pulses, i.e., featuring a gap-free bandwidth at least two decades-wide. Such a structure relies on a 1-µm-wide slit aperture located between two parallel aluminum pads, embedded in a 1-µm-thick layer of silicon nitride, and deposited on a quartz substrate. We show that this device can detect ultra-broadband terahertz pulses by employing unprecedented low optical probe energies of only a few tens of nanojoules. This is due to the more than one order of magnitude higher nonlinear coefficient of silicon nitride with respect to silica, the nonlinear material emp…

lcsh:Applied optics. PhotonicsMaterials scienceComputer Networks and CommunicationsTerahertz radiationTerahertz radiationPhysics::Optics02 engineering and technology7. Clean energy01 natural scienceslaw.invention010309 opticschemistry.chemical_compoundlawSolid-state devicesElectric field0103 physical sciencesBroadbandDynamic rangebusiness.industrylcsh:TA1501-1820021001 nanoscience & nanotechnologyLaserAtomic and Molecular Physics and OpticsTerahertz detectorSilicon nitridechemistryOptoelectronics0210 nano-technologybusinessOrder of magnitudeVoltageAPL Photonics
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Electro-optical characterization of new classes of Silicon Carbide UV photodetectors

2014

In this paper, we present the fabrication process steps and the characterization of 4H-SiC vertical Schottky UV detectors, where interdigitated strips, acting as top metal contacts, have been realized in $\hbox{Ni}_{2}\hbox{Si}$ . These devices exploit the pinch-off surface effect. $I$ – $V$ and $C$ – $V$ characteristics, as functions of temperature, were measured in dark conditions. In addition, we have carried out responsivity measurements, for wavelengths ranging from 200 to 400 nm, at varying package temperature and applied reverse bias. A comparison among devices having different strip pitch sizes has been performed, thus finding out that the 10- $\mu\hbox{m}$ pitch class demonstrates …

lcsh:Applied optics. PhotonicsMaterials scienceFabricationbusiness.industrysic uv photodetector detector silicon carbide responsivitySchottky diodePhotodetectorlcsh:TA1501-1820Settore ING-INF/02 - Campi ElettromagneticiSTRIPSTemperature measurementSettore ING-INF/01 - ElettronicaAtomic and Molecular Physics and OpticsPhotodiodelaw.inventionResponsivitychemistry.chemical_compoundchemistrylawSilicon carbideOptoelectronicslcsh:QC350-467Electrical and Electronic Engineeringbusinesslcsh:Optics. Light
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Employing Microwave Graphene Field Effect Transistors for Infrared Radiation Detection

2018

In this work, we investigate the possibility of employing graphene field effect transistors, specifically designed for microwave applications, as infrared detectors for telecom applications. Our devices have been fabricated on a sapphire substrate employing CVD-grown transferred graphene. The roles of both the gate dielectric and the DC bias conditions have been evaluated in order to maximize the infrared generated signal through an experimental investigation of the signal-to-noise ratio dependence on the transistor operating point.

lcsh:Applied optics. PhotonicsTechnologyMaterials scienceAtomic and Molecular Physics and OpticInfraredGate dielectricPhysics::Optics02 engineering and technologyDielectricgraphene field effect transistor01 natural sciencesSettore ING-INF/01 - Elettronicalaw.inventionCondensed Matter::Materials Scienceinfrared detectorslaw0103 physical sciencesmicrowave transistorlcsh:QC350-467Electrical and Electronic Engineering010306 general physicsGraphene; graphene field effect transistors; infrared detectors; microwave transistors; Atomic and Molecular Physics and Optics; Electrical and Electronic Engineeringbusiness.industryGraphenePhotoconductivityTransistormicrowave transistorslcsh:TA1501-1820021001 nanoscience & nanotechnologyAtomic and Molecular Physics and Opticsinfrared detector2018-020-021849 ALDOptoelectronicsGraphene0210 nano-technologybusinessddc:600Microwavegraphene field effect transistorslcsh:Optics. LightDC biasIEEE Photonics Journal
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LBNO-DEMO (WA105): a large demonstrator of the Liquid Argon double phase TPC

2016

LBNO-DEMO (WA105) is a large demonstrator of the double phase liquid argon TPC intended to develop and test the main elements of the GLACIER-based design for the purpose of scaling it up to the 10–50 kton size needed for Long Baseline Neutrino Oscillation studies. The crucial components of the design are: ultra-high argon purity in non-evacuable tank, long drifts, very high drift voltages, large area Micro Pattern Gas Detectors, and cold preamplifiers. The active volume of the demonstrator is 6×6×6 m3 (approximately 300t). WA105 is under construction at CERN and will be exposed to charged particle beams (0.5-20 GeV/c) in the North Area in 2018. The data will provide the necessary calibratio…

liguid argonPhysics::Instrumentation and DetectorsHigh Energy Physics::Experimentlong baseline neutrinostime projection chamber
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Seasonal Modulation of the $^7$Be Solar Neutrino Rate in Borexino

2017

We detected the seasonal modulation of the $^7$Be neutrino interaction rate with the Borexino detector at the Laboratori Nazionali del Gran Sasso in Italy. The period, amplitude, and phase of the observed time evolution of the signal are consistent with its solar origin, and the absence of an annual modulation is rejected at 99.99\% C.L. The data are analyzed using three methods: the sinusoidal fit, the Lomb-Scargle and the Empirical Mode Decomposition techniques, which all yield results in excellent agreement.

liquid scintillators detectorsPhysics - Instrumentation and Detectorsexperimental methodsneutrino: solarPhysics::Instrumentation and DetectorsSolar neutrinolow background detectorsSolar neutrinos01 natural sciencesflux: time dependenceneutrino: fluxHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Liquid scintillators detectors; Low background detectors; Neutrino oscillations; Solar neutrinos; Astronomy and Astrophysics[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Borexinoneutrino: interactionMSW effectPhysicsNeutrino oscillationsDetectorAstrophysics::Instrumentation and Methods for AstrophysicsInstrumentation and Detectors (physics.ins-det)neutrino electron: elastic scatteringmodulationAmplitudeModulationsolar neutrinosBorexinoNeutrinoLiquid scintillators detectorFLUXLow background detectordata analysis methodNeutrino oscillationFOS: Physical sciencesSolar neutrinoNuclear physicsTIME-SERIES ANALYSIS[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]Low background detectorsLiquid scintillators detectorsSEARCH0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]SPACED DATA010306 general physicsNeutrino oscillationbackground: radioactivityneutrino oscillations010308 nuclear & particles physicsAstronomy and AstrophysicsEMPIRICAL MODE DECOMPOSITIONberylliumGran SassoHigh Energy Physics::Experimentneutrino: oscillationEvent (particle physics)experimental results
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Separation of atomic and molecular ions by ion mobility with an RF carpet

2021

Gas-filled stopping cells are used at accelerator laboratories for the thermalization of high-energy radioactive ion beams. Common challenges of many stopping cells are a high molecular background of extracted ions and limitations of extraction efficiency due to space-charge effects. At the FRS Ion Catcher at GSI, a new technique for removal of ionized molecules prior to their extraction out of the stopping cell has been developed. This technique utilizes the RF carpet for the separation of atomic ions from molecular contaminant ions through their difference in ion mobility. Results from the successful implementation and test during an experiment with a 600~MeV/u $^{124}$Xe primary beam are…

low-energy RIBPhysics - Instrumentation and DetectorsOrders of magnitude (temperature)beam purificationFOS: Physical sciences010402 general chemistrynucl-ex01 natural sciences530Ionmenetelmätion mobilityIonizationMoleculeddc:530Physical and Theoretical ChemistryfysiikkaNuclear Experiment (nucl-ex)Nuclear ExperimentInstrumentationphysics.ins-detSpectroscopyIon transporterRange (particle radiation)ionitChemistry010401 analytical chemistryExtraction (chemistry)gas cellpuhdistusInstrumentation and Detectors (physics.ins-det)Condensed Matter Physics0104 chemical sciencesmolecular contaminationBeamlinespace chargeAtomic physicserottaminen (tekniikka)epäpuhtaudet
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Towards 14C-free liquid scintillator

2017

A series of measurements has been started where the 14C concentration is determined from several liquid scintillator samples. A dedicated setup has been designed and constructed with the aim of measuring concentrations smaller than 10−18. Measurements take place in two underground laboratories: in the Baksan Neutrino Observatory, Russia, and in the new Callio Lab in the Pyhäsalmi mine, Finland. Low-energy neutrino detection with a liquid scintillator requires that the intrinsic 14C concentration in the liquid is extremely low. In the Borexino CTF detector the concentration of 2 × 10−18 has been achieved being the lowest value ever measured. In principle, the older the oil or gas source that…

low-energy neutrino detectionPhysics::Instrumentation and Detectorsilmaisimethiilineutriinotliquid scintillatorsisotope ratio
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