Search results for "Underground laboratory"

showing 8 items of 8 documents

First muography of Stromboli volcano

2019

AbstractMuography consists in observing the differential absorption of muons – elementary particles produced through cosmic-ray interactions in the Earth atmosphere – going through the volcano and can attain a spatial resolution of tens of meters. We present here the first experiment of nuclear emulsion muography at the Stromboli volcano. Muons have been recorded during a period of five months by a detector of 0.96 m2 area. The emulsion films were prepared at the Gran Sasso underground laboratory and were analyzed at Napoli, Salerno and Tokyo scanning laboratories. Our results highlight a significant low-density zone at the summit of the volcano with density contrast of 30–40% with respect …

0301 basic medicineDifferential absorptionmuographylcsh:MedicineVolcanologyArticle03 medical and health sciences0302 clinical medicineMuographyStromboliDensity contrastlcsh:SciencegeographyMultidisciplinarygeography.geographical_feature_categoryBedrockmuography; nuclear emulsion; Stromboli; volcanolcsh:RLandslide030104 developmental biologyAtmosphere of EarthGeophysicsvolcanoVolcanonuclear emulsionUnderground laboratorylcsh:QExperimental particle physics030217 neurology & neurosurgeryGeologySeismology
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Precise measurement of $2\nu\beta\beta$ decay of $^{100}$Mo with the CUPID-Mo detection technology

2020

We report the measurement of the two-neutrino double-beta ($2\nu\beta\beta$) decay of $^{100}$Mo to the ground state of $^{100}$Ru using lithium molybdate (\crystal) scintillating bolometers. The detectors were developed for the CUPID-Mo program and operated at the EDELWEISS-III low background facility in the Modane underground laboratory. From a total exposure of $42.235$ kg$\times$d, the half-life of $^{100}$Mo is determined to be $T_{1/2}^{2\nu}=[7.12^{+0.18}_{-0.14}\,\mathrm{(stat.)}\pm0.10\,\mathrm{(syst.)}]\times10^{18}$ years. This is the most accurate determination of the $2\nu\beta\beta$ half-life of $^{100}$Mo to date. We also confirm, with the statistical significance of $>3\sigm…

Lithium molybdatePhysics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Analytical chemistry[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex01 natural sciencesAtomicchemistry.chemical_compoundParticle and Plasma Physicstwo-neutrino double-beta decay scintillating bolometers0103 physical sciencesddc:530Beta (velocity)Nuclear[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsNuclear ExperimentEngineering (miscellaneous)physics.ins-detS076H2NPhysicsQuantum Physics010308 nuclear & particles physicsPhysicsMolecularBeta decayNuclear & Particles Physics3. Good healthchemistrydouble beta decays bolometersUnderground laboratoryGround state
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Calculation of total muon flux observed by Muon Monitor experiment

2017

An approach to calculate the flux of cosmicgenic muons detected by Muon Monitor experiment in lab LAB2400 of the Underground Laboratory in Canfranc (LSC) is described. The measuring apparatus consists of three layers of SC16 scintillation matrix detectors. The hardware function of the detector assembly was determined using computer simulation. Obtained value of the total muon ux turned out to be equal to (4.35 ± 0.2) × 10−3 m −2 s −1.

Nuclear physicsPhysicsHistoryScintillationMuonPhysics::Instrumentation and DetectorsMuon fluxDetectorUnderground laboratoryFluxHigh Energy Physics::ExperimentComputer Science ApplicationsEducationJournal of Physics: Conference Series
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Cosmic-ray muon flux at Canfranc Underground Laboratory

2019

Residual flux and angular distribution of high-energy cosmic muons have been measured in two underground locations at the Canfranc Underground Laboratory (LSC) using a dedicated Muon Monitor. The instrument consists of three layers of fast scintillation detector modules operating as 352 independent pixels. The monitor has flux-defining area of 1 m${}^{2}$, covers all azimuth angles, and zenith angles up to $80^\circ$. The measured integrated muon flux is $(5.26 \pm 0.21) \times 10^{-3}$ m${}^{-2}$s${}^{-1}$ in the Hall A of the LAB2400 and $(4.29 \pm 0.17) \times 10^{-3}$ m${}^{-2}$s${}^{-1}$ in LAB2500. The angular dependence is consistent with the known profile and rock density of the sur…

Physics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsFOS: Physical sciencesFluxlcsh:AstrophysicsCosmic rayApplied Physics (physics.app-ph)hiukkasfysiikkaScintillator01 natural sciencesNuclear physicslcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010303 astronomy & astrophysicsEngineering (miscellaneous)ZenithPhysicsMuon010308 nuclear & particles physicsCanfranc Underground LaboratoryPhysics - Applied PhysicsInstrumentation and Detectors (physics.ins-det)Azimuthilmaisimethigh-energy cosmic muonsMuon fluxlcsh:QC770-798High Energy Physics::Experimentkosminen säteily
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Results of the search for neutrinoless double-βdecay inMo100with the NEMO-3 experiment

2015

The NEMO-3 detector, which had been operating in the Modane Underground Laboratory from 2003 to 2010, was designed to search for neutrinoless double $\beta$ ($0\nu\beta\beta$) decay. We report final results of a search for $0\nu\beta\beta$ decays with $6.914$ kg of $^{100}$Mo using the entire NEMO-3 data set with a detector live time of $4.96$ yr, which corresponds to an exposure of 34.3 kg$\cdot$yr. We perform a detailed study of the expected background in the $0\nu\beta\beta$ signal region and find no evidence of $0\nu\beta\beta$ decays in the data. The level of observed background in the $0\nu\beta\beta$ signal region $[2.8-3.2]$ MeV is $0.44 \pm 0.13$ counts/yr/kg, and no events are obs…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSignal region01 natural sciencesBeta decayLower limitNuclear physicsMAJORANADouble beta decay0103 physical sciencesUnderground laboratoryBeta (velocity)Neutrino010306 general physicsPhysical Review D
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Reactor neutrino background at the proposed LAGUNA sites

2012

Abstract The electron antineutrino background from reactors is estimated in proposed LAGUNA sites using commercial fission reactors operational in 2009. Calculations are made for an input to background studies like e.g. geoneutrino measurement uncertainty estimation.

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsFissionGeoneutrinoUnderground laboratoryMeasurement uncertaintyReactor neutrinoNeutrino oscillationElectron neutrinoAtomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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Radon and material radiopurity assessment for the NEXT double beta decay experiment

2015

Artículo escrito por un elevado número de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboración, si le hubiere, y los autores pertenecientes a la UAM

Radon mitigationPhysics - Instrumentation and DetectorsNuclear engineeringchemistry.chemical_elementFOS: Physical sciencesRadon7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)XenonCambres d'ionitzacióDouble beta decayGamma detectors (HPGe)0103 physical sciencesGamma spectroscopyNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentDetectors de radiació010308 nuclear & particles physicsIonization chambersCanfranc Underground LaboratoryMaterial radiopurityFísicaTime-Projection Chamber (TPC)Instrumentation and Detectors (physics.ins-det)Double beta decaySemiconductor detectorchemistry13. Climate actionNuclear countersEnvironmental scienceNeutrino
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Solar neutrino physics with Borexino

2018

We present the most recent solar neutrino results from the Borexino experiment at the Gran Sasso underground laboratory. In particular, refined measurements of all neutrinos produced in the {\it pp} fusion chain have been made. It is the first time that the same detector measures the entire range of solar neutrinos at once. These new data weakly favor a high-metallicity Sun. Prospects for measuring CNO solar neutrinos are also discussed.

fusionPhysics - Instrumentation and Detectorsneutrino: solarPhysics::Instrumentation and DetectorsQC1-999Astrophysics::High Energy Astrophysical PhenomenaSolar neutrinoFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physics0103 physical sciencesAstrophysics::Solar and Stellar Astrophysics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)Nuclear Experiment010303 astronomy & astrophysicsBorexinoPhysicsp p: fusion010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyInstrumentation and Detectors (physics.ins-det)Gran Sasso* Automatic Keywords *Physics::Space PhysicsUnderground laboratoryBorexinoHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsNeutrinoexperimental resultsSciPost Physics Proceedings
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