Search results for " detector"

showing 10 items of 2719 documents

Electroluminescence TPCs at the thermal diffusion limit

2019

Artículo escrito por un elevado número de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboración, si le hubiere, y los autores pertenecientes a la UAM

ElectroluminiscènciaNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsDark Matter and Double Beta DecayFOS: Physical scienceschemistry.chemical_elementElectronAtomic01 natural sciences7. Clean energyMathematical SciencesHigh Energy Physics - ExperimentTECNOLOGIA ELECTRONICAHigh Energy Physics - Experiment (hep-ex)Particle and Plasma PhysicsXenonIonization0103 physical sciencesDark Matter and Double Beta Decay (experiments)Nuclearlcsh:Nuclear and particle physics. Atomic energy. RadioactivityDiffusion (business)010306 general physicsMathematical PhysicsPhysicsQuantum Physics010308 nuclear & particles physicsResolution (electron density)MolecularFísicaNuclear energyInstrumentation and Detectors (physics.ins-det)Nuclear & Particles PhysicsParticle correlations and fluctuations85-05ElectroluminescencechemistryRare decayYield (chemistry)Photon productionPhysical SciencesScintillation counterEnergia nuclearlcsh:QC770-798Atomic physicsEnergy (signal processing)
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Efficient Low-Frequency Modal Analysis of Anechoic Chamber

2007

An efficient method to analyze the electromagnetic field inside rectangular anechoic and semianechoic chambers from 30 to 100 MHz is shown. A modal expansion is employed to develop the homogeneous and the inhomogeneous field. This is combined with circuital techniques to compute the effect of the layers of ferrite and dielectrics in the walls of the chamber. Several numerical results of the Free Space Transmission Loss (FSTL) of an anechoic chamber and the Normalized Site Attenuation (NSA) of a semianechoic chamber are provided.

Electromagnetic fieldEngineeringAnechoic chamberPhysics::Instrumentation and Detectorsbusiness.industryAttenuationModal analysisAcousticsTransmission lossDielectricLow frequencyPhysics::Classical PhysicsFerrite (magnet)business2007 IEEE International Symposium on Electromagnetic Compatibility
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A Geant4 simulation package for the sage spectrometer

2012

International audience; A comprehensive Geant4 simulation was built for the SAGE spectrometer. The simulation package includes the silicon and germanium detectors, the mechanical structure and the electromagnetic fields present in SAGE. This simulation can be used for making predictions through simulating experiments and for comparing simulated and experimental data to better understand the underlying physics.

Electromagnetic fieldHistorySiliconSpectrometer010308 nuclear & particles physicsComputer sciencePhysics::Instrumentation and DetectorsDetectorchemistry.chemical_elementExperimental dataGermaniumComputerApplications_COMPUTERSINOTHERSYSTEMS[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesComputer Science ApplicationsEducationComputational scienceKokeellinen ydinfysiikkachemistry0103 physical sciencesComputer Science::Mathematical Software29.40.Wk Solid-state detectors 29.30.Kv X- and gamma-ray spectroscopy 07.85.Nc X-ray and gamma-ray spectrometers 29.30.Dn Electron spectroscopyExperimental nuclear physics010306 general physics
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Beam test results of IHEP-NDL Low Gain Avalanche Detectors(LGAD)

2020

A High-Granularity Timing Detector (HGTD) is proposed based on the Low-Gain Avalanche Detector (LGAD) for the ATLAS experiment to satisfy the time resolution requirement for the up-coming High Luminosity at LHC (HL-LHC). We report on beam test results for two proto-types LGADs (BV60 and BV170) developed for the HGTD. Such modules were manufactured by the Institute of High Energy Physics (IHEP) of Chinese Academy of Sciences (CAS) collaborated with Novel Device Laboratory (NDL) of the Beijing Normal University. The beam tests were performed with 5 GeV electron beam at DESY. The timing performance of the LGADs was compared to a trigger counter consisting of a quartz bar coupled to a SiPM read…

Electron beamNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsFÍSICA DE ALTA ENERGIAPhysics::Instrumentation and DetectorsFOS: Physical sciences01 natural sciences010305 fluids & plasmassymbols.namesakeSilicon photomultiplierOpticsLGAD0103 physical sciencesGaussian functionelectron: irradiationphotomultiplier: silicon[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniques010306 general physicsInstrumentationphysics.ins-detPhysicsLarge Hadron ColliderLuminosity (scattering theory)business.industryfluctuationDetectorATLAS experimentTime resolutionDESYInstrumentation and Detectors (physics.ins-det)ATLASsymbolsHigh Energy Physics::ExperimentbusinessCFDBeam (structure)performancesemiconductor detector: design
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Lessons learned with the SAGE spectrometer

2012

The SAGE spectrometer combines a high-efficiency γ-ray detection system with an electron spectrometer. Some of the design features have been known to be problematic and surprises have come up during the early implementation of the spectrometer. Tests related to bismuth germanate Compton-suppression shields, electron detection efficiency and an improved cooling system are discussed in the paper.

Electron spectrometerMaterials scienceSpectrometerPhysics::Instrumentation and Detectors010308 nuclear & particles physicsbusiness.industryShieldsElectronCondensed Matter Physics01 natural sciencesBismuth germanateAtomic and Molecular Physics and Opticschemistry.chemical_compoundOpticschemistry0103 physical sciencesWater coolingNuclear Experiment010306 general physicsbusinessMathematical PhysicsRemote sensingPhysica Scripta
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Observation of e(+)e(-) -> gamma X(3872) at BESIII

2014

With data samples collected with the BESIII detector operating at the BEPCII storage ring at center-of-mass energies from 4.009 to 4.420 GeV, the process e(+)e(-) -> gamma X(3872) is observed for the first time with a statistical significance of 6.3 sigma. The measured mass of the X(3872) is (3871.9 +/- 0.7(stat) +/- 0.2(syst)) MeV/c(2), in agreement with previous measurements. Measurements of the product of the cross section sigma[e(+)e(-) -> gamma X(3872)] and the branching fraction B [X(3872) -> pi(+)pi(-)J/psi] at center-of-mass energies 4.009, 4.229, 4.260, and 4.360 GeV are reported. Our measurements are consistent with expectations for the radiative transition process Y(4260) -> gamm…

EnergyBESIII Detector
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Going standalone and platform-independent, an example from recent work on the ATLAS Detector Description and interactive data visualization

2019

Until recently, the direct visualization of the complete ATLAS experiment geometry and final analysis data was confined within the software framework of the experiment. To provide a detailed interactive data visualization capability to users, as well as easy access to geometry data, and to ensure platform independence and portability, great effort has been recently put into the modernization of both the core kernel of the detector description and the visualization tools. In this proceedings we will present the new tools, as well as the lessons learned while modernizing the experiment’s code for an efficient use of the detector description and for user-friendly data visualization. Until rece…

Engineering drawing010308 nuclear & particles physicsbusiness.industryAtlas detectorPhysicsQC1-999ATLAS experimentDetectorcomputer.software_genre01 natural sciencesVisualizationSoftware frameworkSoftware portabilityData visualizationKernel (image processing)0103 physical sciences010306 general physicsbusinesscomputerParticle Physics - Experiment
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The reflection coefficient of a flared microstrip line radiating in an infinite parallel-plate waveguide

1993

In this article the reflection coefficient of a tapered microstrip line radiating in an infinite parallel-plate conducting waveguide is calculated. The reflection coefficient at the feed line is evaluated by using the aperture admittance of the horn and the scattering matrix of the continuous taper. The theoretical behavior of the aperture admittance is shown and the reflection coefficient of a microstrip horn radiating in the parallel-plate region of a bootlace lens is measured in order to verify the model. © 1993 John Wiley & sons, Inc.

EngineeringAdmittancePhysics::Instrumentation and Detectorsbusiness.industryAperturePhysics::OpticsCondensed Matter PhysicsAtomic and Molecular Physics and OpticsMicrostripElectronic Optical and Magnetic Materialslaw.inventionOpticslawHorn (acoustic)Feed lineElectrical and Electronic EngineeringReflection coefficientbusinessWaveguideElectrical impedanceMicrowave and Optical Technology Letters
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Synchronization techniques for power quality instruments

2004

The measurement of voltage characteristics in power systems requires the accurate estimation of the power supply frequency and signal synchronization, even in the presence of disturbances. The authors developed and tested two innovative techniques for instrument synchronization. The first is based on signal spectral analysis techniques performed by means of the Chirp-Z transform analysis. The second is a phase-locked loop (PLL) software based on a time-domain coordinate transformation and an innovative phase-detection technique. To evaluate how synchronization techniques are adversely affected by the application of a disturbing influence, experimental tests were carried out, taking into acc…

EngineeringInstrument synchronization phase-locked loops (PLLs) power quality power system measurements spectral analysis.business.industryComputer scienceCoordinate systemControl engineeringFundamental frequencyPhase detectorSignalSynchronizationPower (physics)Phase-locked loopElectric power systemSoftwareChirpElectronic engineeringElectrical and Electronic EngineeringbusinessSettore ING-INF/07 - Misure Elettriche E ElettronicheInstrumentation
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Mechanical construction and installation of the ATLAS tile calorimeter

2013

This paper summarises the mechanical construction andinstallation of the Tile Calorimeter for the ATLASexperiment at the Large Hadron Collider in CERN, Switzerland. The TileCalorimeter is a sampling calorimeter using scintillator as the sensitivedetector and steel as the absorber and covers the central region of the ATLASexperiment up to pseudorapidities ±1.7. The mechanical construction ofthe Tile Calorimeter occurred over a periodof about 10 years beginning in 1995 with the completionof the Technical Design Report and ending in 2006 with the installationof the final module in the ATLAS cavern. Duringthis period approximately 2600 metric tons of steel were transformedinto a laminated struc…

EngineeringLarge Hadron ColliderAtlas (topology)business.industryPhysics::Instrumentation and DetectorsNuclear engineeringATLAS experimentCalorimeters; Detector design and construction technologies and materialsNuclear physicsTile calorimeterCalorimetersPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentDetectors and Experimental TechniquesMechanical constructionDetector design and construction technologies and materialsNuclear ExperimentbusinessInstrumentationMathematical Physics
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