Search results for "Instrumentation"

showing 10 items of 4914 documents

Determination of the number of J/psi events with J/psi -> inclusive decays

2012

The number of J/psi events collected with the BESIII detector at the BEPC II from June 12 to July 28, 2009 is determined to be (225.3 +/- 2.8) x 10(6) using J/psi -> inclusive events, where the uncertainty is the systematic error and the statistical one is negligible.

PhysicsSystematic errorNuclear and High Energy PhysicsElectron–positron annihilationDetectorMonte Carlo methodBESIIIInclusive eventsAstronomy and AstrophysicsJ/ψ→Nuclear physicsBESIII detector; Inclusive events; J/ψ→; Number of J/ψ eventsNumber of J/ψ eventsJ/psi -> inclusive eventsnumber of J/psi eventsBESIII detectorInstrumentationChinese physics c
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Backtracing particle rays through magnetic spectrometers: avoiding systematic errors in the reconstruction of target coordinates

1993

Abstract The procedures used to model [J. Friedrich, Nucl. Instr. and Meth. A 293 (1990) 575] or to determine [N. Voegler et al., Nucl. Instr. and Meth. A 249 (1986) 337, H. Blok et al., ibid., vol. A 262 (1987) 291, and E.A.J.M. Offermann et al., ibid., vol. A 262 (1987) 298] the mapping properties of a magnetic spectrometer are based on a minimization of the variance of target coordinates . We show that backtracing with matrix elements, determined in this way, may contain systematic errors. As alternative, we propose to minimize the variance of the detector coordinates . This procedure avoids these systematic errors.

PhysicsSystematic errorNuclear and High Energy PhysicsMatrix (mathematics)OpticsSpectrometerbusiness.industryDetectorParticlebusinessInstrumentationComputational physicsNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Calibration of the NEXT-White detector using 83m Kr decays

2018

The NEXT-White (NEW) detector is currently the largest radio-pure high-pressure xenon gas time projection chamber with electroluminescent readout in the world. It has been operating at Laboratorio Subterr'aneo de Canfranc (LSC) since October 2016. This paper describes the calibrations performed using 83mKr decays during a long run taken from March to November 2017 (Run II). Krypton calibrations are used to correct for the finite drift-electron lifetime as well as for the dependence of the measured energy on the event transverse position which is caused by variations in solid angle coverage both for direct and reflected light and edge effects. After producing calibration maps to correct for …

PhysicsTime projection chamber010308 nuclear & particles physicsKryptonDetectorSolid anglechemistry.chemical_element01 natural sciencesNuclear physicsFull width at half maximumXenonchemistryDouble beta decay0103 physical sciencesCalibration010306 general physicsInstrumentationMathematical PhysicsJournal of Instrumentation
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Neutrinoless double beta decay with 82 SeF 6 and direct ion imaging

2018

We present a new neutrinoless double beta decay concept: the high pressure selenium hexafluoride gas time projection chamber. Combining techniques pioneered in high pressure xenon gas such as topological discrimination, with the high Q-value afforded by double beta decay isotope $^{82}$Se, a promising new detection technique is outlined. Lack of free electrons in SeF$_6$ mandates the use of an ion TPC. The microphysics of ion production and drift, which have many nuances, are explored. Background estimates are produced suggesting such a detector may achieve background indices of better than 1 count per ton per year in the region of interest at the 100~kg scale, and still better at the ton-s…

PhysicsTime projection chamberPhysics - Instrumentation and Detectors010308 nuclear & particles physicschemistry.chemical_elementFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)01 natural sciences7. Clean energyBeta decayParticle detectorIonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)XenonchemistryDouble beta decay0103 physical sciences010306 general physicsInstrumentationMathematical PhysicsRadioactive decayLeptonJournal of Instrumentation
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Secondary electron flight times and tracks in the carbon foil time pick-up detector

2014

Carbon foil time pick-up detectors used in the time-of-flight measurements of MeV energy ions have been studied in connection to time-of-flight-energy spectrometer used for heavy ion elastic recoil detection analysis. In experimental coincident TOF-E data characteristic halos are observed around light element isobars, and the origin of these halos were studied. The experimental data indicated that these halos originate from single electron events occurring before the electron multiplication in the microchannel plate. By means of electron trajectory simulations, this halo effect is explained to originate from single electron, emitted from the carbon foil, hitting the non-active area of the m…

PhysicsToF-ERDANuclear and High Energy Physicstiming gateta114business.industryPhysics::Instrumentation and DetectorsDetectorElectrontime-of-flightSecondary electronsElastic recoil detectionTime of flightOpticsCoincidentMicrochannel plate detectorspectrometerAtomic physicsbusinesscarbon foil time pick-up detectorInstrumentationFOIL methodNuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
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Measurement of spin correlation in ttbar production using a matrix element approach

2011

correlation, assuming that the spin of the top quark is either correlated with the spin of the anti-top quark as predicted by the standard model or is uncorrelated. For the first time we use a matrix-element-based approach to study ttbar spin correlation. We use {ttbar -> W+bW-bbar ->l+nubl-nub} final states produced in ppbar collisions at a center of mass energy sqrt(s)=1.96 TeV, where l denotes an electron or a muon. The data correspond to an integrated luminosity of 5.4 fb-1 and were collected with the dzero detector at the Fermilab Tevatron collider. The result agrees with the standard model prediction. We exclude the hypothesis that the spins of the ttbar are uncorrelated at the …

PhysicsTop quarkParticle physicsMuonLuminosity (scattering theory)010308 nuclear & particles physicsBar (music)Physics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentFermilab010306 general physicsSpin-½
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Precise measurement of the top quark mass in the dilepton channel at D0

2011

We measure the top quark mass (mt) in ppbar collisions at a center of mass energy of 1.96 TeV using dilepton ttbar->W+bW-bbar->l+nubl-nubarbbar events, where l denotes an electron, a muon, or a tau that decays leptonically. The data correspond to an integrated luminosity of 5.4 fb-1 collected with the D0 detector at the Fermilab Tevatron Collider. We obtain mt = 174.0 +- 1.8(stat) +- 2.4(syst) GeV, which is in agreement with the current world average mt = 173.3 +- 1.1 GeV. This is currently the most precise measurement of mt in the dilepton channel.

PhysicsTop quarkParticle physicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesHigh Energy Physics - ExperimentLuminosityNuclear physicsHigh Energy Physics - Experiment (hep-ex)Experimental High Energy Physics0103 physical sciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment14.65.HaCenter of mass010306 general physicsNuclear ExperimentBar (unit)
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Characterization and Error Compensation of a Rogowski Coil in the Presence of Harmonics

2011

This paper reports the results of an experimental study dealing with a commercial Rogowski coil current transducer (RCCT) in the presence of harmonic distortion. The RCCT was observed under two conditions: 1) sinusoidal excitation with frequencies from 50 to 750 Hz and 2) nonsinusoidal excitation using fundamental frequency and one harmonic, with adjustable amplitude and phase shift. The experimental results show only a weak dependence of the harmonic current ratio error and phase displacement on the amplitude and phase shift of the excitation harmonic. The phase displacement is also independent of the conductor position within the Rogowski coil window. An error compensation method, based o…

PhysicsTotal harmonic distortionFrequency responsebusiness.industryAcousticsElectrical engineeringFundamental frequencycurrent transducerRogowski coilCurrent measurement current transducer frequency response harmonic distortion power system harmonics Rogowski coil.harmonic distortionHarmonic analysisAmplitudeHarmonicsHarmonicpower system harmonicElectrical and Electronic EngineeringbusinessInstrumentationSettore ING-INF/07 - Misure Elettriche E ElettronicheRogowski coil
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A Wavelength-shifting Optical Module (WOM) for in-ice neutrino detectors

2016

7th Very Large Volume Neutrino Telescope Workshop, Rome, Italy, 14 Sep 2015 - 16 Sep 2015 ; The European physical journal / Web of Conferences 116, 01006 (2016). doi:10.1051/epjconf/201611601006

PhysicsTotal internal reflection010504 meteorology & atmospheric sciences010308 nuclear & particles physicsbusiness.industryPhysics::Instrumentation and DetectorsPhysicsQC1-999Astrophysics::High Energy Astrophysical PhenomenaDetectorWavelength shifter01 natural sciencesNoise (electronics)530WavelengthOpticsNeutrino detector0103 physical sciencesddc:530businessCherenkov radiation0105 earth and related environmental sciencesDark current
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In-trap conversion electron spectroscopy

2002

The Penning trap REXTRAP at ISOLDE was used to test the feasibility of in-trap conversion electron spectroscopy. The results of simulations, experiments with solid conversion electron sources as well as first on-line and tests with trapped radioactive ions are presented. In addition to obtaining high-resolution spectroscopic data, the detection of conversion electrons was found to be a useful tool for the diagnostics of the trap operation. The tests proved the feasibility of in-trap spectroscopy but also revealed some potential problems to be addressed in the future.

PhysicsTrap (computing)Condensed Matter::Quantum GasesNuclear and High Energy PhysicsElectronPhysics::Atomic PhysicsAtomic physicsSpectroscopyPenning trapInstrumentationElectron spectroscopyAccelerators and Storage RingsIon
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