Search results for "Instrumentation"

showing 10 items of 4914 documents

The PANDA Barrel DIRC

2018

The PANDA experiment at the international accelerator Facility for Antiproton and Ion Research in Europe (FAIR) near GSI, Darmstadt, Germany will address fundamental questions of hadron physics. Excellent Particle Identification (PID) over a large range of solid angles and particle momenta will be essential to meet the objectives of the rich physics program. Charged PID for the barrel region of the PANDA target spectrometer will be provided by a DIRC (Detection of Internally Reflected Cherenkov light) detector. The Barrel DIRC will cover the polar angle range of 22$^\circ$-140$^\circ$ and cleanly separate charged pions from kaons for momenta between 0.5 GeV/c and 3.5 GeV/c with a separation…

PhysicsPhysics - Instrumentation and Detectors010308 nuclear & particles physicsbusiness.industryPhysics::Instrumentation and DetectorsBarrel (horology)FOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)01 natural sciencesOptics0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsbusinessNuclear ExperimentInstrumentationMathematical Physics
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Ultra-stable implanted 83Rb/83mKr electron sources for the energy scale monitoring in the KATRIN experiment

2012

The KATRIN experiment aims at the direct model-independent determination of the average electron neutrino mass via the measurement of the endpoint region of the tritium beta decay spectrum. The electron spectrometer of the MAC-E filter type is used, requiring very high stability of the electric filtering potential. This work proves the feasibility of implanted 83Rb/83mKr calibration electron sources which will be utilised in the additional monitor spectrometer sharing the high voltage with the main spectrometer of KATRIN. The source employs conversion electrons of 83mKr which is continuously generated by 83Rb. The K-32 conversion line (kinetic energy of 17.8 keV, natural line width of 2.7 e…

PhysicsPhysics - Instrumentation and DetectorsElectron spectrometerSpectrometerPhysics::Instrumentation and DetectorsFOS: Physical sciencesHigh voltageElectronInstrumentation and Detectors (physics.ins-det)Inelastic scatteringKinetic energyComputational physicsDetectors and Experimental TechniquesNuclear Experiment (nucl-ex)Nuclear ExperimentInstrumentationElectron neutrinoMathematical PhysicsKATRIN
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An angular-selective electron source for the KATRIN experiment

2014

The KATRIN experiment is going to search for the average mass of the electron antineutrino with a sensitivity of 0.2 eV/c2. It uses a retardation spectrometer of MAC-E filter type to accurately measure the shape of the electron spectrum at the endpoint of tritium beta decay. In order to achieve the planned sensitivity the transmission properties of the spectrometer have to be understood with high precision for all initial conditions. For this purpose an electron source has been developed that emits single electrons at adjustable total energy and adjustable emission angle. The emission is pointlike and can be moved across the full flux tube that is imaged onto the detector. Here, we demonstr…

PhysicsPhysics - Instrumentation and DetectorsFlux tubeSpectrometerPhysics::Instrumentation and Detectorsbusiness.industryDetectorFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)ElectronBeta decayHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)OpticsFilter (video)businessInstrumentationElectron neutrinoMathematical PhysicsKATRINJournal of Instrumentation
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Ultra-low material pixel layers for the Mu3e experiment

2016

The upcoming Mu3e experiment will search for the charged lepton flavour violating decay of a muon at rest into three electrons. The maximal energy of the electrons is 53 MeV, hence a low material budget is a key performance requirement for the tracking detector. In this paper we summarize our approach to meet the requirement of about 0.1 % of a radiation length per pixel detector layer. This includes the choice of thinned active monolithic pixel sensors in HV-CMOS technology, ultra-thin flexible printed circuits, and helium gas cooling.

PhysicsPhysics - Instrumentation and DetectorsMuonPixel010308 nuclear & particles physicsbusiness.industryPhysics::Instrumentation and DetectorsDetectorComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONFOS: Physical sciencesElectronInstrumentation and Detectors (physics.ins-det)Tracking (particle physics)01 natural sciencesRadiation lengthPrinted circuit boardOptics0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsbusinessInstrumentationMathematical PhysicsLepton
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nEDM experiment at PSI : data-taking strategy and sensitivity of the dataset

2018

We report on the strategy used to optimize the sensitivity of our search for a neutron electric dipole moment at the Paul Scherrer Institute. Measurements were made upon ultracold neutrons stored within a single chamber at the heart of our apparatus. A mercury cohabiting magnetometer together with an array of cesium magnetometers were used to monitor the magnetic field, which was controlled and shaped by a series of precision field coils. In addition to details of the setup itself, we describe the chosen path to realize an appropriate balance between achieving the highest statistical sensitivity alongside the necessary control on systematic effects. The resulting irreducible sensitivity is …

PhysicsPhysics - Instrumentation and DetectorsNeutron electric dipole moment010308 nuclear & particles physicsbusiness.industryMagnetometerPhysicsQC1-999Statistical sensitivityFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesMagnetic fieldlaw.inventionOpticslaw0103 physical sciencesUltracold neutrons[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsbusinessNuclear ExperimentSingle chamber
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Energy resolution studies for NEXT

2011

This work aims to present the current state of simulations of electroluminescence (EL) produced in gas-based detectors with special interest for NEXT --- Neutrino Experiment with a Xenon TPC. NEXT is a neutrinoless double beta decay experiment, thus needs outstanding energy resolution which can be achieved by using electroluminescence. The process of light production is reviewed and properties such as EL yield and associated fluctuations, excitation and electroluminescence efficiencies, and energy resolution, are calculated. An EL production region with a 5 mm width gap between two infinite parallel planes is considered, where a uniform electric field is produced. The pressure and temperatu…

PhysicsPhysics - Instrumentation and DetectorsPhotonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsFOS: Physical scienceschemistry.chemical_elementInstrumentation and Detectors (physics.ins-det)Electroluminescence7. Clean energy01 natural sciencesParticle detectorHigh Energy Physics - ExperimentComputational physicsHigh Energy Physics - Experiment (hep-ex)XenonchemistryDouble beta decay0103 physical sciencesNeutrino010306 general physicsInstrumentationMathematical PhysicsExcitationLeptonJournal of Instrumentation
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A new measurement of the neutron detection efficiency for the NaI Crystal Ball detector

2015

We report on a measurement of the neutron detection efficiency in NaI crystals in the Crystal Ball detector obtained from a study of single π0 photoproduction on deuterium using the tagged photon beam at the Mainz Microtron. The results were obtained up to a neutron energy of 400 MeV . They are compared to previous measurements made more than 15 years ago at the pion beam at the BNL AGS.

PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsDetectorNuclear TheoryFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)Neutron temperatureHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion beamDeuteriumNeutron detectionPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentPhoton beamNuclear Experiment (nucl-ex)Nuclear ExperimentInstrumentationMicrotronNuclear ExperimentMathematical PhysicsCrystal Ball
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MuPix7 - A fast monolithic HV-CMOS pixel chip for Mu3e

2016

The MuPix7 chip is a monolithic HV-CMOS pixel chip, thinned down to 50 \mu m. It provides continuous self-triggered, non-shuttered readout at rates up to 30 Mhits/chip of 3x3 mm^2 active area and a pixel size of 103x80 \mu m^2. The hit efficiency depends on the chosen working point. Settings with a power consumption of 300 mW/cm^2 allow for a hit efficiency >99.5%. A time resolution of 14.2 ns (Gaussian sigma) is achieved. Latest results from 2016 test beam campaigns are shown.

PhysicsPhysics - Instrumentation and DetectorsPixel010308 nuclear & particles physicsbusiness.industryGaussianFOS: Physical sciencesTime resolutionInstrumentation and Detectors (physics.ins-det)Semiconductor deviceChip01 natural sciencessymbols.namesakeCMOSTest beam0103 physical sciencessymbolsOptoelectronicsddc:610010306 general physicsbusinessInstrumentationGaussian processMathematical Physics
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MuPix10: First Results from the Final Design

2021

Many years of research and development of High Voltage Monolithic Active Pixel Sensors (HVMAPS) have culminated in the final design for the Mu3e pixel sensor. MuPix10 is a fully monolithic sensor with an active pixel matrix size of $20\times20\,\mathrm{mm}^2$ produced in the $180\,\mathrm{nm}$ HV-CMOS process at TSI Semiconductors. The pixel size is $80\times80\,\mathrm{\mu m}^2$. Hits are read out using a column-drain architecture and sent over up to four serial links with up to $1.6\,\left.\mathrm{Gbit}\middle/\mathrm{s}\right.$ each. By means of DC/DC converters and exclusive usage of on-chip biasing, MuPix10 is fully operable with a minimal set of electrical connections. This is an inte…

PhysicsPhysics - Instrumentation and DetectorsPixelFOS: Physical sciencesBiasingPixel matrixHigh voltageInstrumentation and Detectors (physics.ins-det)ConvertersTopologyRadiation lengthProceedings of the 29th International Workshop on Vertex Detectors (VERTEX2020)
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Classification methods for noise transients in advanced gravitational-wave detectors II: performance tests on Advanced LIGO data

2017

The data taken by the advanced LIGO and Virgo gravitational-wave detectors contains short duration noise transients that limit the significance of astrophysical detections and reduce the duty cycle of the instruments. As the advanced detectors are reaching sensitivity levels that allow for multiple detections of astrophysical gravitational-wave sources it is crucial to achieve a fast and accurate characterization of non-astrophysical transient noise shortly after it occurs in the detectors. Previously we presented three methods for the classification of transient noise sources. They are Principal Component Analysis for Transients (PCAT), Principal Component LALInference Burst (PC-LIB) and W…

PhysicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsGravitational waveReal-time computingDetectorFOS: Physical sciences01 natural sciencesLIGONoiseTransient noiseWaveletDuty cycle0103 physical sciencesSensitivity (control systems)010306 general physicsAstrophysics - Instrumentation and Methods for AstrophysicsInstrumentation and Methods for Astrophysics (astro-ph.IM)
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