Search results for "physics.ins-det"

showing 10 items of 505 documents

Measurement of radon-induced backgrounds in the NEXT double beta decay experiment

2018

The measurement of the internal $^{222}$Rn activity in the NEXT-White detector during the so-called Run-II period with $^{136}$Xe-depleted xenon is discussed in detail, together with its implications for double beta decay searches in NEXT. The activity is measured through the alpha production rate induced in the fiducial volume by $^{222}$Rn and its alpha-emitting progeny. The specific activity is measured to be $(38.1\pm 2.2~\mathrm{(stat.)}\pm 5.9~\mathrm{(syst.)})$~mBq/m$^3$. Radon-induced electrons have also been characterized from the decay of the $^{214}$Bi daughter ions plating out on the cathode of the time projection chamber. From our studies, we conclude that radon-induced backgro…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsNuclear physicsFOS: Physical scienceschemistry.chemical_elementRadonElectron01 natural sciencesAtomicMathematical SciencesHigh Energy Physics - Experimentlaw.inventionIonNuclear physicsHigh Energy Physics - Experiment (hep-ex)XenonParticle and Plasma PhysicslawDouble beta decay0103 physical sciencesDark Matter and Double Beta Decay (experiments)lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclearNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentMathematical PhysicsPhysicsQuantum PhysicsTime projection chamber010308 nuclear & particles physicsDetectorMolecularInstrumentation and Detectors (physics.ins-det)Double beta decayNuclear & Particles PhysicsCathodeDoble desintegració betachemistryPhysical Scienceslcsh:QC770-798Física nuclear
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Design and Operation of a Windowless Gas Target Internal to a Solenoidal Magnet for Use with a Megawatt Electron Beam

2019

A windowless hydrogen gas target of nominal thickness $10^{19}$ cm$^{-2}$ is an essential component of the DarkLight experiment, which is designed to utilize the megawatt electron beam at an Energy Recovery Linac (ERL). The design of such a target is challenging because the pressure drops by many orders of magnitude between the central, high-density section of the target and the surrounding beamline, resulting in laminar, transitional, and finally molecular flow regimes. The target system was assembled and operated at Jefferson Lab's Low Energy Recirculator Facility (LERF) in 2016, and subsequently underwent several revisions and calibration tests at MIT Bates in 2017. The system at dynamic…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsOrders of magnitude (temperature)Windowless gas targetNuclear engineeringDarkLightFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyCOMSOLFree molecular flow0103 physical sciencesCalibration[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsInstrumentationNuclear ExperimentPhysicsSolenoidal vector field010308 nuclear & particles physicsLaminar flowDark photonInstrumentation and Detectors (physics.ins-det)BeamlineMagnetCathode ray
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Internal alignment and position resolution of the silicon tracker of DAMPE determined with orbit data

2017

Abstract The DArk Matter Particle Explorer (DAMPE) is a space-borne particle detector designed to probe electrons and gamma-rays in the few GeV to 10 TeV energy range, as well as cosmic-ray proton and nuclei components between 10 GeV and 100 TeV. The silicon–tungsten tracker–converter is a crucial component of DAMPE. It allows the direction of incoming photons converting into electron–positron pairs to be estimated, and the trajectory and charge (Z) of cosmic-ray particles to be identified. It consists of 768 silicon micro-strip sensors assembled in 6 double layers with a total active area of 6.6 m 2 . Silicon planes are interleaved with three layers of tungsten plates, resulting in about o…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhotonSiliconProtonPhysics::Instrumentation and DetectorsAlignment; Cosmic-ray detectors; Gamma-ray telescopes; Silicon-strip detectors; Nuclear and High Energy Physics; InstrumentationGamma-ray telescopesAstrophysics::High Energy Astrophysical PhenomenaCosmic-ray detectorsFOS: Physical scienceschemistry.chemical_elementElectron01 natural sciencesSilicon-strip detectorRadiation lengthParticle detectorOptics0103 physical sciences010303 astronomy & astrophysicsInstrumentationImage resolutionNuclear and High Energy PhysicAlignmentPhysicsRange (particle radiation)010308 nuclear & particles physicsbusiness.industrySettore FIS/01 - Fisica SperimentaleInstrumentation and Detectors (physics.ins-det)Cosmic-ray detectorSilicon-strip detectorschemistryGamma-ray telescopeHigh Energy Physics::ExperimentbusinessNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Characterization of a cylindrical plastic {\beta}-detector with Monte Carlo simulations of optical photons

2017

V. Guadilla et al. -- 5 pags., 8 figs., tab.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhotonTotal absorption spectroscopyoptical photonsTotal absorption spectroscopyMonte Carlo method[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesElectromagnetic radiationMonte Carlo simulationsOptics0103 physical sciencesPlastic scintillators[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]plastic scintillators010306 general physicsAbsorption (electromagnetic radiation)Nuclear ExperimentInstrumentationPhysicsSpectrometerta114010308 nuclear & particles physicsbusiness.industryDetectortotal absorption spectroscopyComputational physicsOptical photonsDynamic Monte Carlo methodbusiness
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Coherent elastic neutrino-nucleus scattering at the European Spallation Source

2020

The European Spallation Source (ESS), presently well on its way to completion, will soon provide the most intense neutron beams for multi-disciplinary science. Fortuitously, it will also generate the largest pulsed neutrino flux suitable for the detection of Coherent Elastic Neutrino-Nucleus Scattering (CE$\nu$NS), a process recently measured for the first time at ORNL's Spallation Neutron Source. We describe innovative detector technologies maximally able to profit from the order-of-magnitude increase in neutrino flux provided by the ESS, along with their sensitivity to a rich particle physics phenomenology accessible through high-statistics, precision CE$\nu$NS measurements.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFluxFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesElectroweak interactionlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutronSpallationNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsScatteringElectroweak interactionDetectorInstrumentation and Detectors (physics.ins-det)Neutrino Detectors and Telescopes (experiments)High Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798Physics::Accelerator PhysicsNeutrinoSpallation Neutron Source
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In-flight performance of the DAMPE silicon tracker

2018

Abstract DAMPE (DArk Matter Particle Explorer) is a spaceborne high-energy cosmic ray and gamma-ray detector , successfully launched in December 2015. It is designed to probe astroparticle physics in the broad energy range from few GeV to 100 TeV. The scientific goals of DAMPE include the identification of possible signatures of Dark Matter annihilation or decay, the study of the origin and propagation mechanisms of cosmic-ray particles, and gamma-ray astronomy . DAMPE consists of four sub-detectors: a plastic scintillator strip detector, a Silicon–Tungsten tracKer–converter (STK), a BGO calorimeter and a neutron detector . The STK is composed of six double layers of single-sided silicon mi…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaGamma rayDark matterFOS: Physical sciencesCosmic rayScintillator01 natural sciences7. Clean energyOptics0103 physical sciencesDark matterNeutron detection010306 general physicsInstrumentation and Methods for Astrophysics (astro-ph.IM)Cosmic raysInstrumentationNuclear and High Energy PhysicAstroparticle physicsPhysicsCalorimeter (particle physics)010308 nuclear & particles physicsbusiness.industrySettore FIS/01 - Fisica SperimentaleDetectorGamma raysGamma rayInstrumentation and Detectors (physics.ins-det)Cosmic raySpaceborne experimentSilicon trackerHigh Energy Physics::ExperimentAstrophysics - Instrumentation and Methods for AstrophysicsbusinessCosmic rays; Dark matter; Gamma rays; Silicon tracker; Spaceborne experiment; Nuclear and High Energy Physics; Instrumentation
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Characterization and performance of the DTAS detector

2018

11 pags., 16 figs., 3 tabs.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaMonte Carlo methodspektrometritβ decayFOS: Physical sciencesNon-proportional scintillation light yield: Monte Carlo simulationsMonte Carlo simulations [Non-proportional scintillation light yield]y-ray spectrometerB decay[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesMonte Carlo simulationsOpticsDistortion0103 physical sciencesNeutron[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsAbsorption (electromagnetic radiation)Nuclear ExperimentInstrumentation[formula omitted] decayNuclear ExperimentPhysicsta114Spectrometer010308 nuclear & particles physicsbusiness.industryNaI(Tl) detectorPulse generatorTotal absorption [formula omitted]-ray spectrometerDetectornon-proportional scintillation light yieldInstrumentation and Detectors (physics.ins-det)Total absorption γ -ray spectrometerNon-proportional scintillation light yieldFísica nuclearTotal absorptionydinfysiikkabusinessDelayed neutronExotic nucleiNuclear instruments & methods inphysics research section A: Accelerators spectrometers detectors and associated equipment 910: 79-89 (2018)
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The ATLAS level-1 trigger: Status of the system and first results from cosmic-ray data

2007

The ATLAS detector at CERN's Large Hadron Collider (LHC) will be exposed to proton-proton collisions from beams crossing at 40 MHz. At the design luminosity of 10^34 cm^-2 s^-1 there are on average 23 collisions per bunch crossing. A three-level trigger system will select potentially interesting events in order to reduce the read-out rate to about 200 Hz. The first trigger level is implemented in custom-built electronics and makes an initial fast selection based on detector data of coarse granularity. It has to reduce the rate by a factor of 10^4 to less than 100 kHz. The other two consecutive trigger levels are in software and run on PC farms. We present an overview of the first-level trig…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsAtlas detectoratlas; cosmic-ray data; installation and commissioning; trigger systemFOS: Physical sciencesCosmic rayinstallation and commissioningNuclear physicsSoftwareAtlas (anatomy)medicineatlascosmic-ray dataDetectors and Experimental TechniquesInstrumentationPhysicstrigger systemLarge Hadron ColliderLuminosity (scattering theory)business.industrySettore FIS/01 - Fisica SperimentaleDetectorInstrumentation and Detectors (physics.ins-det)medicine.anatomical_structurePhysics::Accelerator PhysicsGranularitybusinessNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The MATHUSLA test stand

2020

The rate of muons from LHC $pp$ collisions reaching the surface above the ATLAS interaction point is measured and compared with expected rates from decays of $W$ and $Z$ bosons and $b$- and $c$-quark jets. In addition, data collected during periods without beams circulating in the LHC provide a measurement of the background from cosmic ray inelastic backscattering that is compared to simulation predictions. Data were recorded during 2018 in a 2.5 $\times$ 2.5 $\times$ 6.5~$\rm{m}^3$ active volume MATHUSLA test stand detector unit consisting of two scintillator planes, one at the top and one at the bottom, which defined the trigger, and six layers of RPCs between them, grouped into three $(x…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsBackscattered cosmic raysLong-lived particles; LHC; MATHUSLA; Backscattered cosmic raysFOS: Physical sciencesCosmic rayScintillator01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)0103 physical sciencesmedicineDetectors and Experimental Techniques010306 general physicsphysics.ins-detInstrumentationSettore FIS/01PhysicsLuminosity (scattering theory)MuonLarge Hadron ColliderInteraction pointhep-ex010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)Long-lived particlesMATHUSLAmedicine.anatomical_structureW′ and Z′ bosonsHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Construction of two large-size four-plane micromegas detectors

2015

We report on the construction and initial performance studies of two micromegas detector quadruplets with an area of 0.5 m$^2$. They serve as prototypes for the planned upgrade project of the ATLAS muon system. Their design is based on the resistive-strip technology and thus renders the detectors spark tolerant. Each quadruplet comprises four detection layers with 1024 readout strips and a strip pitch of 415 $\mu$m. In two out of the four layers the strips are inclined by $\pm$1.5$^{\circ}$ to allow for the measurement of a second coordinate. We present the detector concept and report on the experience gained during the detector construction. In addition an evaluation of the detector perfor…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsFOS: Physical sciencesCosmic raySTRIPS01 natural sciences030218 nuclear medicine & medical imaginglaw.inventionGaseous detector; Micromegas; Microstructure detector; Resistive couplingNuclear physics03 medical and health sciences0302 clinical medicineOpticsAtlas (anatomy)law0103 physical sciencesSpark (mathematics)medicineGaseous detectorDetectors and Experimental TechniquesInstrumentationMicrostructure detectorPhysicsResistive couplingMuon010308 nuclear & particles physicsbusiness.industryDetectorMicroMegas detectorInstrumentation and Detectors (physics.ins-det)Upgrademedicine.anatomical_structureHigh Energy Physics::ExperimentbusinessMicromegas
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