Search results for "physics.ins-det"

showing 10 items of 505 documents

Suppression of Penning discharges between the KATRIN spectrometers

2020

The KArlsruhe TRItium Neutrino experiment (KATRIN) aims to determine the effective electron (anti)neutrino mass with a sensitivity of $0.2\textrm{ eV/c}^2$ (90$\%$ C.L.) by precisely measuring the endpoint region of the tritium $\beta$-decay spectrum. It uses a tandem of electrostatic spectrometers working as MAC-E (magnetic adiabatic collimation combined with an electrostatic) filters. In the space between the pre-spectrometer and the main spectrometer, an unavoidable Penning trap is created when the superconducting magnet between the two spectrometers, biased at their respective nominal potentials, is energized. The electrons accumulated in this trap can lead to discharges, which create a…

Speichertechnik - Abteilung BlaumPhysics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsPenning trapFOS: Physical scienceslcsh:AstrophysicsSuperconducting magnetElectronTritiumKATRIN01 natural sciencesNuclear physics0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. RadioactivityElectron Captureddc:530[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsNuclear ExperimentEngineering (miscellaneous)PhysicsSpectrometer010308 nuclear & particles physicsPhysicsInstrumentation and Detectors (physics.ins-det)Químicamagnet: superconductivityspectrometer: electrostaticPenning trapBeamlineBeta (plasma physics)electron: backgroundlcsh:QC770-798NeutrinoNeutrino MassKATRIN
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Gamma-induced background in the KATRIN main spectrometer

2019

The KATRIN experiment aims to measure the effective electron antineutrino mass $$m_{\overline{\nu }_e}$$ mν¯e with a sensitivity of $${0.2}\,{\hbox {eV}/\hbox {c}^2}$$ 0.2eV/c2 using a gaseous tritium source combined with the MAC-E filter technique. A low background rate is crucial to achieving the proposed sensitivity, and dedicated measurements have been performed to study possible sources of background electrons. In this work, we test the hypothesis that gamma radiation from external radioactive sources significantly increases the rate of background events created in the main spectrometer (MS) and observed in the focal-plane detector. Using detailed simulations of the gamma flux in the e…

Speichertechnik - Abteilung BlaumPhysics - Instrumentation and Detectorsgamma ray: backgroundshieldingshielding: magneticPhysicsFOS: Physical scienceslcsh:AstrophysicsInstrumentation and Detectors (physics.ins-det)electron: secondarysensitivityKATRINbackground: lowlcsh:QB460-466electron: backgroundlcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530gamma ray: flux[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Electromagnetismonumerical calculationselectrostatic
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Recent Borexino results and prospects for the near future

2015

The Borexino experiment, located in the Gran Sasso National Laboratory, is an organic liquid scintillator detector conceived for the real time spectroscopy of low energy solar neutrinos. The data taking campaign phase I (2007 - 2010) has allowed the first independent measurements of 7Be, 8B and pep fluxes as well as the first measurement of anti-neutrinos from the earth. After a purification of the scintillator, Borexino is now in phase II since 2011. We review here the recent results achieved during 2013, concerning the seasonal modulation in the 7Be signal, the study of cosmogenic backgrounds and the updated measurement of geo-neutrinos. We also review the upcoming measurements from phase…

Sterile neutrinoPhysics - Instrumentation and Detectorsneutrino: solarPhysics::Instrumentation and DetectorsSolar neutrinoQC1-999Astrophysics::High Energy Astrophysical Phenomenascintillation counter: liquidFOS: Physical sciencesScintillator53001 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all)Low energy[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physics[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]BorexinoPhysics010308 nuclear & particles physicsneutrino: energy: lowgeophysicsbackgroundPhysicsDetectorneutrino: flux: measuredHigh Energy Physics::PhenomenologyInstrumentation and Detectors (physics.ins-det)neutrino: particle sourceneutrino: sterileantineutrinoGran SassoNEUTRINOS13. Climate actionBorexinoHigh Energy Physics::ExperimentNeutrinoNational laboratory
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Method for finding the critical temperature of the island in a SET structure

2008

We present a method to measure the critical temperature of the island of a superconducting single electron transistor. The method is based on a sharp change in the slope of the zero-bias conductance as a function of temperature. We have used this method to determine the superconducting phase transition temperature of the Nb island of an superconducting single electron transistor with Al leads. We obtain $T_\mathrm{c}^\mathrm{Nb}$ as high as 8.5 K and gap energies up to $\Delta_\mathrm{Nb}\simeq 1.45$ meV. By looking at the zero bias conductance as a function of magnetic field instead of temperature, also the critical field of the island can be determined. Using the orthodox theory, we have …

SuperconductivityHistoryPhysics - Instrumentation and DetectorsMaterials scienceCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsBand gapTransition temperatureFOS: Physical sciencesCoulomb blockadeInstrumentation and Detectors (physics.ins-det)ElectronAtmospheric temperature rangeComputer Science ApplicationsEducationMagnetic fieldMesoscale and Nanoscale Physics (cond-mat.mes-hall)Critical fieldJournal of Physics: Conference Series
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Highly sensitive superconducting circuits at ∼700 kHz with tunable quality factors for image-current detection of single trapped antiprotons

2016

We developed highly-sensitive image-current detection systems based on superconducting toroidal coils and ultra-low noise amplifiers for non-destructive measurements of the axial frequencies (550$\sim$800$\,$kHz) of single antiprotons stored in a cryogenic multi-Penning-trap system. The unloaded superconducting tuned circuits show quality factors of up to 500$\,$000, which corresponds to a factor of 10 improvement compared to our previously used solenoidal designs. Connected to ultra-low noise amplifiers and the trap system, signal-to-noise-ratios of 30$\,$dB at quality factors of > 20$\,$000 are achieved. In addition, we have developed a superconducting switch which allows continuous tu…

SuperconductivityPhysicsSpeichertechnik - Abteilung BlaumPhysics - Instrumentation and DetectorsSolenoidal vector fieldbusiness.industryAmplifierDetectorFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)01 natural sciencesNoise (electronics)010305 fluids & plasmasQuality (physics)Antiproton0103 physical sciencesOptoelectronicsDetectors and Experimental Techniques010306 general physicsbusinessphysics.ins-detInstrumentationElectronic circuit
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Commissioning of the ATLAS Muon Spectrometer with cosmic rays

2010

The ATLAS detector at the Large Hadron Collider has collected several hundred million cosmic ray events during 2008 and 2009. These data were used to commission the Muon Spectrometer and to study the performance of the trigger and tracking chambers, their alignment, the detector control system, the data acquisition and the analysis programs. We present the performance in the relevant parameters that determine the quality of the muon measurement. We discuss the single element efficiency, resolution and noise rates, the calibration method of the detector response and of the alignment system, the track reconstruction efficiency and the momentum measurement. The results show that the detector i…

SystemAstrofísicaDriftPhysics - Instrumentation and DetectorsMuon SpectrometerPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsTracking (particle physics)01 natural sciences7. Clean energyHigh Energy Physics - ExperimentDrift TubeMDTHigh Energy Physics - Experiment (hep-ex)Data acquisitionATLAS muon spectrometer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesNuclear ExperimentPhysicsLarge Hadron Collidercosmic ray eventsDetectorSettore FIS/01 - Fisica SperimentaleBeamInstrumentation and Detectors (physics.ins-det)ATLASmedicine.anatomical_structureTrack ReconstructionPhysical SciencesFísica nuclearLHCmuon measurementFOS: Physical sciencesCosmic rayddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesCalibrationmedicineFysikddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsEngineering (miscellaneous)Ciencias ExactasMuonChambersMuon TrackCosmologiaATLAS detector010308 nuclear & particles physicsFísicaTrack SegmentPhysics::Accelerator Physicsproton-proton collisionsHigh Energy Physics::Experiment
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Readiness of the ATLAS Tile Calorimeter for LHC collisions

2010

67 páginas.-- El PDF es la versión pre-print (arXiv:1007.5423v2).-- The ATLAS Collaboration.-- et al.

SystemPhysics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsPerformance7. Clean energy01 natural sciences030218 nuclear medicine & medical imagingSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)0302 clinical medicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesDetectors de radiaciócosmic rayPhysicsLarge Hadron ColliderDetectorSettore FIS/01 - Fisica SperimentaleAstrophysics::Instrumentation and Methods for AstrophysicsInstrumentation and Detectors (physics.ins-det)ATLASmedicine.anatomical_structureScintillatorsPhysical Sciencesmagnetic-fields; scintillators; electronics; performance; systemLHCCol·lisionadors d'hadronsPhotomultiplierFOS: Physical sciencesCosmic rayddc:500.2Noise (electronics)530LHC collisions; AtlasNuclear physics03 medical and health sciencesAtlas (anatomy)0103 physical sciencesCalibrationmedicinetile hadronic calorimeterFysikddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsEngineering (miscellaneous)Ciencias ExactasCalorimeter (particle physics)010308 nuclear & particles physicsFísicaMagnetic-FieldsHigh Energy Physics::ExperimentElectronics
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Open data from the first and second observing runs of advanced LIGO and advanced Virgo

2021

Abbot, Rich, et al. (Virgo and MAGIC Collaboration)

TechnologyGravitational Waves Open Data O1 O2 LIGO VirgoAstronomyStrain measurementGravitational Waveopen dataData representation and management; Gravitational Waves; GWOSC; Scientific databasesgravitational waves; open data01 natural sciencesGeneral Relativity and Quantum CosmologySoftwareDocumentationDESIGNOpen DataComputer softwareData productsLIGOQC12-AXIS VIBRATION ISOLATIONmedia_commonSettore FIS/010303 health sciencesData representation and management/dk/atira/pure/sustainabledevelopmentgoals/partnershipsGravitational effectsBINARY MERGERSComputer Science ApplicationsOpen data[PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc]Open scienceAstrophysics - Instrumentation and Methods for Astrophysicsdata analysis methodData productsgr-qcmedia_common.quotation_subjectReal-time computingScientific databasesFOS: Physical sciencesO2PUBLIC ADVANCED LIGOGeneral Relativity and Quantum Cosmology (gr-qc)Gravity wavesprogrammingO103 medical and health sciencesQA76.75-76.765Dewey Decimal Classification::000 | Allgemeines Wissenschaft::000 | Informatik Wissen Systeme::004 | InformatikSDG 17 - Partnerships for the GoalsGWOSC Scientific databases Data representation and management Gravitational Waves0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsGRAVITATIONAL-WAVE CATALOGInstrumentation and Methods for Astrophysics (astro-ph.IM)STFCAstrophysique030304 developmental biologyGravitational WavesScience & Technologybusiness.industryGravitational waveVirgogravitational radiationRCUKGWOSC; Scientific databases; Data representation and management; Gravitational WavesStrain dataData-quality informationComputer Science Software EngineeringLIGOgravitational radiation detectordetector: sensitivityScientific databasemonitoringVIRGOSkygravitational radiation: emissionComputer ScienceGWOSCddc:004businessSoftwareastro-ph.IM
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First results on ProtoDUNE-SP liquid argon time projection chamber performance from a beam test at the CERN Neutrino Platform

2020

The ProtoDUNE-SP detector was constructed and operated on the CERN Neutrino Platform. We thank the CERN management for providing the infrastructure for this experiment and gratefully acknowledge the support of the CERN EP, BE, TE, EN, IT and IPT Departments for NP04/ProtoDUNE-SP. This documentwas prepared by theDUNEcollaboration using the resources of the Fermi National Accelerator Laboratory (Fermilab), a U.S. Department of Energy, Office of Science, HEP User Facility. Fermilab is managed by Fermi Research Alliance, LLC (FRA), acting under Contract No. DE-AC02-07CH11359. This work was supported by CNPq, FAPERJ, FAPEG and FAPESP, Brazil; CFI, IPP and NSERC, Canada; CERN; MSMT, Czech Republi…

TechnologyHIGH-ENERGYPhysics - Instrumentation and DetectorsPhysics::Instrumentation and Detectorsfar detectorbeam transportNoble liquid detectors (scintillation ionization double-phase)Cms Experıment01 natural sciences7. Clean energy09 EngineeringParticle identificationHigh Energy Physics - Experiment030218 nuclear medicine & medical imagingHigh Energy Physics - Experiment (hep-ex)0302 clinical medicineNoble liquid detectors (scintillationDetectors and Experimental TechniquesInstrumentationInstruments & Instrumentationphysics.ins-dettime resolutionMathematical PhysicsPhysics02 Physical SciencesTime projection chamberLarge Hadron ColliderDetectorInstrumentation and Detectors (physics.ins-det)double-phase)Nuclear & Particles PhysicsLIGHTNeutrinoParticle Physics - ExperimentperformanceNoble liquid detectors(scintillation ionization double-phase)noiseCERN LabLarge detector systems for particle and astroparticle physics Noble liquid detectors (scintillation ionization double-phase) Time projection Chambers (TPC)530 Physicsenergy lossTime projection chambersFOS: Physical sciencesParticle detectorNuclear physics03 medical and health sciencesneutrino: deep underground detector0103 physical sciencesionizationDeep Underground Neutrino ExperimentHigh Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]signal processingactivity reportScience & Technology010308 nuclear & particles physicshep-exLarge detector systems for particle and astroparticle physicsTime projection Chambers (TPC)530 Physiksensitivitycalibrationtime projection chamber: liquid argonExperimental High Energy PhysicsLarge detector systems for particle and astroparticle physicsingle-phase)Large detector systems for particle and astroparticle physics; Noble liquid detectors (scintillation ionization double-phase); Time projection Chambers (TPC)High Energy Physics::Experimentphoton: detectorparticle identificationcharged particle: irradiationBeam (structure)
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Microwave-free magnetometry with nitrogen-vacancy centers in diamond

2016

We use magnetic-field-dependent features in the photoluminescence of negatively charged nitrogen-vacancy centers to measure magnetic fields without the use of microwaves. In particular, we present a magnetometer based on the level anti-crossing in the triplet ground state at 102.4 mT with a demonstrated noise floor of 6 nT/$\sqrt{\text{Hz}}$, limited by the intensity noise of the laser and the performance of the background-field power supply. The technique presented here can be useful in applications where the sensor is placed closed to conductive materials, e.g. magnetic induction tomography or magnetic field mapping, and in remote-sensing applications since principally no electrical acces…

TechnologyPhysics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)MagnetometerFOS: Physical sciences02 engineering and technologyengineering.material01 natural scienceslaw.inventionEngineeringlaw0103 physical sciencescond-mat.mes-hallMesoscale and Nanoscale Physics (cond-mat.mes-hall)010306 general physicsphysics.ins-detApplied PhysicsPhysicsCondensed Matter - Mesoscale and Nanoscale Physicsbusiness.industryDiamondInstrumentation and Detectors (physics.ins-det)021001 nanoscience & nanotechnologyNoise floorMagnetic fieldPhysical SciencesengineeringOptoelectronicsMagnetic induction tomographyphysics.optics0210 nano-technologybusinessGround stateNoise (radio)MicrowavePhysics - OpticsOptics (physics.optics)
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