Search results for "Radon"

showing 10 items of 116 documents

Radiogenic backgrounds in the NEXT double beta decay experiment

2019

[EN] Natural radioactivity represents one of the main backgrounds in the search for neutrinoless double beta decay. Within the NEXT physics program, the radioactivity- induced backgrounds are measured with the NEXT-White detector. Data from 37.9 days of low-background operations at the Laboratorio Subterraneo de Canfranc with xenon depleted in Xe-136 are analyzed to derive a total background rate of (0.84 +/- 0.02) mHz above 1000 keV. The comparison of data samples with and without the use of the radon abatement system demonstrates that the contribution of airborne-Rn is negligible. A radiogenic background model is built upon the extensive radiopurity screening campaign conducted by the NEX…

Nuclear and High Energy PhysicsPhysical measurementsPhysics - Instrumentation and DetectorsDark Matter and Double Beta DecayDark matterFísica -- Mesuramentschemistry.chemical_elementFOS: Physical sciencesRadon7. Clean energy01 natural sciencesAtomicMathematical SciencesHigh Energy Physics - ExperimentNuclear physicsTECNOLOGIA ELECTRONICAHigh Energy Physics - Experiment (hep-ex)XenonParticle and Plasma PhysicsDouble beta decayDark matter and double beta decay (experiments)0103 physical sciencesDark Matter and Double Beta Decay (experiments)Dark Matterlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear010306 general physicsDouble Beta DecayNatural radioactivityMathematical PhysicsPhysicsQuantum PhysicsRadiogenic nuclide010308 nuclear & particles physicsDetectorMolecularDetectorsInstrumentation and Detectors (physics.ins-det)Nuclear & Particles PhysicschemistryPhysical Scienceslcsh:QC770-798Event (particle physics)
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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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Collectivity in the light radon nuclei measured directly via Coulomb excitation

2015

Background: Shape coexistence in heavy nuclei poses a strong challenge to state-of-the-art nuclear models, where several competing shape minima are found close to the ground state. A classic region for investigating this phenomenon is in the region around Z=82 and the neutron midshell at N=104. Purpose: Evidence for shape coexistence has been inferred from α-decay measurements, laser spectroscopy, and in-beam measurements. While the latter allow the pattern of excited states and rotational band structures to be mapped out, a detailed understanding of shape coexistence can only come from measurements of electromagnetic matrix elements. Method: Secondary, radioactive ion beams of Rn202 and Rn…

Nuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]PopulationFOS: Physical sciencesCoulomb excitationshape coexistence01 natural sciences0103 physical sciencesNuclear Physics - ExperimentNeutroncollectivityNuclear Experiment (nucl-ex)010306 general physicseducationSpectroscopyNuclear ExperimentPhysicseducation.field_of_studyta114010308 nuclear & particles physicsGamma rayradonPhysique atomique et nucléaire3. Good healthRadonExcited stateQuadrupoleAtomic physicsGround state
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Measurement of the background in the NEMO 3 double beta decay experiment

2009

In the double beta decay experiment NEMO 3 a precise knowledge of the background in the signal region is of outstanding importance. This article presents the methods used in NEMO 3 to evaluate the backgrounds resulting from most if not all possible origins. It also illustrates the power of the combined tracking-calorimetry technique used in the experiment.

Nuclear and High Energy Physicscongenital hereditary and neonatal diseases and abnormalitiesSignal regionchemistry.chemical_elementFOS: Physical sciencesRadon[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsNEMODouble beta decay0103 physical sciencesNeutrino Ettore Majorana ObservatoryNuclear Experiment (nucl-ex)010306 general physicsskin and connective tissue diseasesLow radioactivityInstrumentationNuclear ExperimentPhysics010308 nuclear & particles physicsDetectorDouble beta decayPower (physics)BackgroundchemistryRadon
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X-ray production with heavy post-accelerated radioactive-ion beams in the lead region of interest for Coulomb-excitation measurements

2015

Abstract Characteristic K X-rays have been observed in Coulomb-excitation experiments with heavy radioactive-ion beams in the lead region (Z = 82), produced at the REX-ISOLDE facility, and were used to identify the decay of strongly converted transitions as well as monopole 0 2 + → 0 1 + transitions. Different targets were used, and the X-rays were detected by the Miniball γ-ray spectrometer surrounding the target position. A stable mercury isotope, as well as neutron-deficient mercury, lead, polonium, and radon isotopes were studied, and a detailed description of the analysis using the radioactive 182,184,186,188Hg isotopes is presented. Apart from strongly converted transitions originatin…

Nuclear reactionNuclear and High Energy PhysicsSpectrometerIsotopeta114Coulomb excitationchemistry.chemical_elementRadonCoulomb excitation7. Clean energychemistrygamma-ray spectroscopyExcited stateGamma spectroscopyAtomic physicsNuclear ExperimentInstrumentationPoloniumK X-ray productionNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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On the range of the radon transform and its dual

1984

OpticsRadon transformbusiness.industryGeneral MathematicsRange (statistics)businessMathematicsDual (category theory)Mathematische Annalen
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Porous measures on $\mathbb {R}^{n}$: Local structure and dimensional properties

2001

We study dimensional properties of porous measures on R n . As a corollary of a theorem describing the local structure of nearly uniformly porous measures we prove that the packing dimension of any Radon measure on R n has an upper bound depending on porosity. This upper bound tends to n - 1 as porosity tends to its maximum value.

Packing dimensionCorollaryApplied MathematicsGeneral MathematicsMathematical analysisRadon measurePorosityUpper and lower boundsLocal structurePhysics::GeophysicsMathematicsProceedings of the American Mathematical Society
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A CHARACTERIZATION OF THE WEAK RADON–NIKODÝM PROPERTY BY FINITELY ADDITIVE INTERVAL FUNCTIONS

2009

AbstractA characterization of Banach spaces possessing the weak Radon–Nikodým property is given in terms of finitely additive interval functions. Due to that characterization several Banach space valued set functions that are only finitely additive can be represented as integrals.

Pettis integralDiscrete mathematicsMathematics::Functional AnalysisPure mathematicsKurzweil-Henstock integral Pettis integral variational measure weak Radon-Nikodym property.Property (philosophy)General MathematicsBanach spacechemistry.chemical_elementRadonInterval (mathematics)Characterization (mathematics)chemistrySettore MAT/05 - Analisi MatematicaSet functionMathematicsBulletin of the Australian Mathematical Society
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Radon-Nikodym derivatives of finitely additive interval measures taking values in a Banach space with basis

2011

Let X be a Banach space with a Schauder basis {en}, and let Φ(I)= ∑n en ∫I fn(t)dt be a finitely additive interval measure on the unit interval [0, 1], where the integrals are taken in the sense of Henstock–Kurzweil. Necessary and sufficient conditions are given for Φ to be the indefinite integral of a Henstock–Kurzweil–Pettis (or Henstock, or variational Henstock) integrable function f:[0, 1] → X.

Pettis integralDiscrete mathematicsPure mathematicsHenstock–Kurzweil integralApplied MathematicsGeneral MathematicsBanach spaceMeasure (mathematics)Schauder basisRadon–Nikodym theoremSettore MAT/05 - Analisi MatematicaHenstock-Kurzweil integral Henstock-Kurzweil-Pettis integral Henstock integral variational Henstock integral Pettis integralLocally integrable functionMathematicsUnit intervalActa Mathematica Sinica, English Series
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$^{222}$Rn emanation measurements for the XENON1T experiment

2021

The selection of low-radioactive construction materials is of utmost importance for the success of low-energy rare event search experiments. Besides radioactive contaminants in the bulk, the emanation of radioactive radon atoms from material surfaces attains increasing relevance in the effort to further reduce the background of such experiments. In this work, we present the $^{222}$Rn emanation measurements performed for the XENON1T dark matter experiment. Together with the bulk impurity screening campaign, the results enabled us to select the radio-purest construction materials, targeting a $^{222}$Rn activity concentration of 10 $\mu$Bq/kg in 3.2 t of xenon. The knowledge of the distribut…

Physics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Radon emanationFOS: Physical scienceschemistry.chemical_element01 natural sciencesNOHigh Energy Physics - Experimentradon: nuclideHigh Energy Physics - Experiment (hep-ex)XENONXenon222 RnPE2_2PE2_10103 physical sciencesActivity concentration[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Dark Matter[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsEngineering (miscellaneous)background: radioactivityPhysicsradon: admixture010308 nuclear & particles physicsdetector: surfacescreeningInstrumentation and Detectors (physics.ins-det)chemistryXenon Dark matter 222 Rn radioactivityDark Matter Radon emanation XENON Direct Dark MatterDirect Dark MatterradioactivityAtomic physics
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