Search results for "Detector"

showing 10 items of 3491 documents

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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Design and development of safety and control systems in ATLAS

2021

El gran colisionador de hadrones, o LHC, es el acelerador de partículas más grande y potente del mundo. Ha sido construido por el CERN, la Organización Europea para la Investigación Nuclear, entre 1998 y 2008 en Ginebra, Suiza. Sucesivas mejoras en el LHC supondrán a partir de mediados del 2027 un incremento de la luminosidad, cuando pasará a llamarse High Luminosity LHC (HL-LHC). Esta tesis se divide en dos partes, por una parte la seguridad y operación de la infraestructura y por otra los sistemas de control y toma de datos. La primera parte de la tesis se dedica a la seguridad y operación de la infraestructura. Después de más de 10 años de funcionamiento, el riesgo de posibles fallos en …

leak detectionhadiation hardness:CIENCIAS TECNOLÓGICAS [UNESCO]CMOSexpert systemsLHCDetectors and Experimental TechniquesATLASUNESCO::CIENCIAS TECNOLÓGICASbeam telescopeSEU
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Search for pair production of first or second generation leptoquarks in proton-proton collisions at sqrt(s)=7 TeV using the ATLAS detector at the LHC

2011

This paper describes searches for the pair production of first or second generation scalar leptoquarks using 35  pb−1 of proton-proton collision data recorded by the ATLAS detector at √s=7  TeV. Leptoquarks are searched in events with two oppositely-charged muons or electrons and at least two jets, and in events with one muon or electron, missing transverse momentum and at least two jets. After event selection, the observed yields are consistent with the predicted backgrounds. Leptoquark production is excluded at the 95% CL for masses MLQ<376 (319) GeV and MLQ<422 (362) GeV for first and second generation scalar leptoquarks, respectively, when assuming the branching fraction of a leptoquark…

leptoquark: scalar ; leptoquark: branching ratio ; leptoquark: pair production ; transverse momentum: missing-energy ; ATLAS ; CERN LHC Coll ; p p: interaction ; leptoquark: search for ; final state: ((n)jet dilepton) ; final state: ((n)jet lepton) ; background ; leptoquark: mass: lower limit ; channel cross section: upper limit ; experimental results ; 7000 GeV-cmsHeraSu(15) Grand UnificationScience & Technology:Ciências Físicas [Ciências Naturais]Settore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyQuarksFísicaddc:500.2Breaking530pair production; leptoquarks;High Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareConstraintsddc:530High Energy Physics::ExperimentFísica nuclearBosonsParticle Physics - ExperimentDetectors de radiacióModel
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State of the art and prospects for halide perovskite nanocrystals

2021

Financiado para publicación en acceso aberto: Universidade de Vigo/CISUG Metal-halide perovskites have rapidly emerged as one of the most promising materials of the 21st century, with many exciting properties and great potential for a broad range of applications, from photovoltaics to optoelectronics and photocatalysis. The ease with which metal-halide perovskites can be synthesized in the form of brightly luminescent colloidal nanocrystals, as well as their tunable and intriguing optical and electronic properties, has attracted researchers from different disciplines of science and technology. In the last few years, there has been a significant progress in the shape-controlled synthesis of …

light-emitting devicesGeneral Physics and AstronomyNanotechnology02 engineering and technology010402 general chemistry01 natural sciences7. Clean energyphotocatalystsmetal-halide perovskite nanocrystalslead-free perovskite nanocrystalsPhotovoltaicsGeneral Materials ScienceNanoscience & NanotechnologyPerovskite (structure)Electronic propertiesPhysicsbusiness.industryPhysicsperovskite nanoplateletsGeneral Engineering021001 nanoscience & nanotechnology0104 chemical sciencesddc:Chemistryphotovoltaicsperovskite nanocubesmetal-halide perovskite nanocrystals; perovskite nanoplatelets; perovskite nanocubes; perovskite nanowires; lead-free perovskite nanocrystals; light-emitting devices; photovoltaics; lasers; photocatalysts; photodetectorsNanocrystalperovskite nanowiresphotodetectors2307 Química Física0210 nano-technologybusinessEngineering sciences. Technologylasers
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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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Neutrino interaction classification with a convolutional neural network in the DUNE far detector

2020

The Deep Underground Neutrino Experiment is a next-generation neutrino oscillation experiment that aims to measure CP-violation in the neutrino sector as part of a wider physics program. A deep learning approach based on a convolutional neural network has been developed to provide highly efficient and pure selections of electron neutrino and muon neutrino charged-current interactions. The electron neutrino (antineutrino) selection efficiency peaks at 90% (94%) and exceeds 85% (90%) for reconstructed neutrino energies between 2–5 GeV. The muon neutrino (antineutrino) event selection is found to have a maximum efficiency of 96% (97%) and exceeds 90% (95%) efficiency for reconstructed neutrino…

luokitus (toiminta)neutriino-oskillaatiokoneoppiminenPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyneutriinotHigh Energy Physics::Experimentneuroverkothiukkasfysiikka
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