Search results for "detectors"

showing 10 items of 2229 documents

Measurement of the Atmospheric ve flux in IceCube

2012

We report the first measurement of the atmospheric electron neutrino flux in the energy range between approximately 80 GeV and 6 TeV, using data recorded during the first year of operation of IceCube's DeepCore low energy extension. Techniques to identify neutrinos interacting within the DeepCore volume and veto muons originating outside the detector are demonstrated. A sample of 1029 events is observed in 281 days of data, of which 496 $\pm$ 66(stat.) $\pm$ 88(syst.) are estimated to be cascade events, including both electron neutrino and neutral current events. The rest of the sample includes residual backgrounds due to atmospheric muons and charged current interactions of atmospheric muo…

DEEPCOREParticle physicsAMANDAPhysics::Instrumentation and DetectorsSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaGeneral Physics and Astronomyddc:500.201 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsSEARCH0103 physical sciencesddc:550010306 general physicsNeutrino oscillationDETECTORPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySolar neutrino problemCosmic neutrino backgroundNeutrino detectorPhysics and Astronomy13. Climate actionMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino astronomyNeutrinoNEUTRINO-INDUCED CASCADESAstrophysics - High Energy Astrophysical PhenomenaPhysical Review Letters
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"Table 12" of "Constraints on jet quenching in p-Pb collisions at $\mathbf{\sqrt{s_{NN}}}$ = 5.02 TeV measured by the event-activity dependence of se…

2018

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.4.

DELTARECOIL RATIOPhysics::Instrumentation and DetectorsPhysics::Atomic PhysicsNuclear ExperimentP PB -->H JET(S) X
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"Table 14" of "Constraints on jet quenching in p-Pb collisions at $\mathbf{\sqrt{s_{NN}}}$ = 5.02 TeV measured by the event-activity dependence of se…

2018

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.2.

DELTARECOIL RATIOPhysics::Instrumentation and DetectorsPhysics::Atomic PhysicsNuclear ExperimentP PB -->H JET(S) X
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"Table 13" of "Constraints on jet quenching in p-Pb collisions at $\mathbf{\sqrt{s_{NN}}}$ = 5.02 TeV measured by the event-activity dependence of se…

2018

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.2.

DELTARECOIL RATIOPhysics::Instrumentation and DetectorsPhysics::Atomic PhysicsNuclear ExperimentP PB -->H JET(S) X
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"Table 11" of "Constraints on jet quenching in p-Pb collisions at $\mathbf{\sqrt{s_{NN}}}$ = 5.02 TeV measured by the event-activity dependence of se…

2018

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.4.

DELTARECOIL RATIOPhysics::Instrumentation and DetectorsPhysics::Atomic PhysicsNuclear ExperimentP PB -->H JET(S) X
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"Table 23" of "Measurement of the production cross section for Z/gamma* in association with jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS d…

2014

Measured normalized differential cross section as a function of dijet azimuthal separation 1/sigma_DY dsigma/dDeltaPhijj (1/rad.) for the electron channel and the muon channel in the individual lepton fiducial regions and uncorrected for QED effects.

DSIG/DPHIZ ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyAstrophysics::Cosmology and Extragalactic AstrophysicsJet ProductionAzimuthal Angular DependenceInclusiveSingle Differential Cross SectionP P --> Z0 JET XP P --> GAMMA* JET XProton-Proton ScatteringHigh Energy Physics::ExperimentNuclear Experiment
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Search for Event Rate Modulation in XENON100 Electronic Recoil Data

2015

We have searched for periodic variations of the electronic recoil event rate in the (2-6) keV energy range recorded between February 2011 and March 2012 with the XENON100 detector, adding up to 224.6 live days in total. Following a detailed study to establish the stability of the detector and its background contributions during this run, we performed an un-binned profile likelihood analysis to identify any periodicity up to 500 days. We find a global significance of less than 1 sigma for all periods suggesting no statistically significant modulation in the data. While the local significance for an annual modulation is 2.8 sigma, the analysis of a multiple-scatter control sample and the phas…

Dark Matter Wimps ModulationPhysicsPhysics - Instrumentation and DetectorsCosmology and Nongalactic Astrophysics (astro-ph.CO)530 PhysicsDetectorDark matterPhase (waves)FOS: Physical sciencesGeneral Physics and AstronomySigmaInstrumentation and Detectors (physics.ins-det)AstrophysicsParticle detectorHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)RecoilModulation[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Event (particle physics)Astrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review Letters
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Design of New Resonant Haloscopes in the Search for the Dark Matter Axion: A Review of the First Steps in the RADES Collaboration

2022

This article belongs to the Special Issue Studying the Universe from Spain.

Dark matter detectorsResonant cavitiesaxionsdark matter detectorsPhysics - Instrumentation and Detectorshep-exAxionsGeneral Physics and AstronomyFOS: Physical sciencesElementary particle physicsInstrumentation and Detectors (physics.ins-det)QC793-793.5HaloscopesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)haloscopesDetectors and Experimental Techniquesphysics.ins-detParticle Physics - Experimentresonant cavities
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Dark Matter Search Results from a One Ton-Year Exposure of XENON1T

2018

We report on a search for Weakly Interacting Massive Particles (WIMPs) using 278.8 days of data collected with the XENON1T experiment at LNGS. XENON1T utilizes a liquid xenon time projection chamber with a fiducial mass of $(1.30 \pm 0.01)$ t, resulting in a 1.0 t$\times$yr exposure. The energy region of interest, [1.4, 10.6] $\mathrm{keV_{ee}}$ ([4.9, 40.9] $\mathrm{keV_{nr}}$), exhibits an ultra-low electron recoil background rate of $(82\substack{+5 \\ -3}\textrm{ (sys)}\pm3\textrm{ (stat)})$ events/$(\mathrm{t}\times\mathrm{yr}\times\mathrm{keV_{ee}})$. No significant excess over background is found and a profile likelihood analysis parameterized in spatial and energy dimensions exclude…

Dark matterGeneral Physics and Astronomychemistry.chemical_elementS030DI5WIMP: massElectronParameter spacedark matter: direct detectionGravitation and AstrophysicsS030DI101 natural sciencesS030DI3S030DI2Nuclear physicsXenonRecoilWIMPelectron: recoil0103 physical sciencesS046DM2[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsnumerical calculationsDark Matter WIMP TPC XENON Direct searchPhysicsxenon: liquidTime projection chamber010308 nuclear & particles physicsbackgrounddark matter: massGran SassoWIMP nucleonchemistryWeakly interacting massive particles[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]time projection chamber: xenon[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]
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Design, construction and cooling system performance of a prototype cryogenic stopping cell for the Super-FRS at FAIR

2015

A cryogenic stopping cell for stopping energetic radioactive ions and extracting them as a low energy beam was developed. This first ever cryogenically operated stopping cell serves as prototype device for the Low-Energy Branch of the Super-FRS at FAIR. The cell has a stopping volume that is 1 m long and 25 cm in diameter. Ions are guided by a DC field along the length of the stopping cell and by a combined RF and DC fields provided by an RE carpet at the exit-hole side. The ultra-high purity of the stopping gas required for optimum ion survival is reached by cryogenic operation. The design considerations and construction of the cryogenic stopping cell, as well as some performance character…

Dc fieldNuclear and High Energy PhysicsSPACE-CHARGEPhysics::Instrumentation and DetectorsNuclear engineering7. Clean energy01 natural sciencesIonNuclear physicsSuper-FRSENERGYCryogenic stopping cell0103 physical sciencesWater coolingddc:530FACILITYradioactive ion beams010306 general physicsInstrumentationRADIOACTIVE IONSFinal versionPhysicsCATCHERSPECTROSCOPYta114010308 nuclear & particles physicsCYCLOTRON GAS STOPPERCryocoolerSpace chargeVolume (thermodynamics)13. Climate actionIon catcherRadioactive on beamsFLIGHT MASS-SPECTROMETRYPROJECTILE FRAGMENTSBeam (structure)ION GUIDE
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