0000000000208861

AUTHOR

A.b. Redwine

showing 7 related works from this author

Mitigation of backgrounds from cosmogenic 137 Xe in xenon gas experiments using 3 He neutron capture

2020

[EN] Xe-136 is used as the target medium for many experiments searching for 0 nu beta beta. Despite underground operation, cosmic muons that reach the laboratory can produce spallation neutrons causing activation of detector materials. A potential background that is difficult to veto using muon tagging comes in the form of Xe-137 created by the capture of neutrons on Xe-136. This isotope decays via beta decay with a half-life of 3.8 min and a Q(beta) of similar to 4.16 MeV. This work proposes and explores the concept of adding a small percentage of He-3 to xenon as a means to capture thermal neutrons and reduce the number of activations in the detector volume. When using this technique we f…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsScintillation and light emission processesGas and liquid scintillatorsFOS: Physical scienceschemistry.chemical_element01 natural sciences7. Clean energyHigh Energy Physics - ExperimentTECNOLOGIA ELECTRONICANuclear physicsGaseous detectorsSolidHigh Energy Physics - Experiment (hep-ex)XenonDouble beta decay0103 physical sciencesIsotopes of xenonSpallationNeutron010306 general physicsPhysics010308 nuclear & particles physicsFísicaInstrumentation and Detectors (physics.ins-det)Beta DecayNeutron temperatureNeutron capturechemistryScintillatorsRadioactive decayJournal of Physics G: Nuclear and Particle Physics
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Boosting background suppression in the NEXT experiment through Richardson-Lucy deconvolution

2021

The NEXT collaboration: et al.

Nuclear and High Energy PhysicsIonizationPhysics - Instrumentation and DetectorsIonitzacióFOS: Physical sciencesdouble beta decayRichardson–Lucy deconvolutionBragg peakElectronQC770-79801 natural sciencesSignalHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)IonizationDouble beta decayNuclear and particle physics. Atomic energy. Radioactivitygas0103 physical sciences010306 general physicsPhysics010308 nuclear & particles physicsRaigs beta -- DesintegracióInstrumentation and Detectors (physics.ins-det)Computational physicsdark matter and double beta decay (experiments)Beta rays -- DecayDeconvolutionEnergy (signal processing)
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Dependence of polytetrafluoroethylene reflectance on thickness at visible and ultraviolet wavelengths in air

2020

[EN] Polytetrafluoroethylene (PTFE) is an excellent diffuse reflector widely used in light collection systems for particle physics experiments. However, the reflectance of PTFE is a function of its thickness. In this work, we investigate this dependence in air for light of wavelengths 260 nm and 450 nm using two complementary methods. We find that PTFE reflectance for thicknesses from 5 mm to 10 mm ranges from 92.5% to 94.5% at 450 nm, and from 90.0% to 92.0% at 260 nm We also see that the reflectance of PIFE of a given thickness can vary by as much as 2.7% within the same piece of material. Finally, we show that placing a specular reflector behind the PTFE can recover the loss of reflectan…

Physics - Instrumentation and DetectorsFOS: Physical sciencesLibrary science7. Clean energy01 natural sciences030218 nuclear medicine & medical imagingSynthetic materialsTECNOLOGIA ELECTRONICA03 medical and health sciences0302 clinical medicinePolitical science0103 physical sciencesmedia_common.cataloged_instanceEuropean unionInstrumentationUltraviolet radiationMathematical Physicsmedia_common010308 nuclear & particles physicsEuropean researchTime projection Chambers (TPC)Instrumentation and Detectors (physics.ins-det)Visible radiationDouble-beta decay detectorsReflectivityDetector design and construction technologies and materialsNational laboratory
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Demonstration of background rejection using deep convolutional neural networks in the NEXT experiment

2021

[EN] Convolutional neural networks (CNNs) are widely used state-of-the-art computer vision tools that are becoming increasingly popular in high-energy physics. In this paper, we attempt to understand the potential of CNNs for event classification in the NEXT experiment, which will search for neutrinoless double-beta decay in Xe-136. To do so, we demonstrate the usage of CNNs for the identification of electron-positron pair production events, which exhibit a topology similar to that of a neutrinoless double-beta decay event. These events were produced in the NEXT-White high-pressure xenon TPC using 2.6 MeV gamma rays from a Th-228 calibration source. We train a network on Monte Carlo-simulat…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsCalibration (statistics)Computer Science::Neural and Evolutionary ComputationNuclear physicsFOS: Physical sciencesTopology (electrical circuits)01 natural sciencesConvolutional neural networkAtomicPartícules (Física nuclear)High Energy Physics - ExperimentInteraccions electró-positróTECNOLOGIA ELECTRONICAHigh Energy Physics - Experiment (hep-ex)Particle and Plasma PhysicsDouble beta decay0103 physical sciencesDark Matter and Double Beta Decay (experiments)NuclearNuclear Matrixlcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsElectron-positron interactionsMathematical PhysicsParticles (Nuclear physics)PhysicsQuantum Physics010308 nuclear & particles physicsbusiness.industryEvent (computing)Network onSIGNAL (programming language)MolecularFísicaPattern recognitionDetectorInstrumentation and Detectors (physics.ins-det)Beta DecayDouble beta decayNuclear & Particles PhysicsDoble desintegració betaIdentification (information)lcsh:QC770-798Física nuclearArtificial intelligencebusinessJournal of High Energy Physics
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The dynamics of ions on phased radio-frequency carpets in high pressure gases and application for barium tagging in xenon gas time projection chambers

2022

NEXT Collaboration: et al.

Nuclear and High Energy PhysicsInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Sensitivity of the NEXT experiment to Xe-124 double electron capture

2021

[EN] Double electron capture by proton-rich nuclei is a second-order nuclear process analogous to double beta decay. Despite their similarities, the decay signature is quite di erent, potentially providing a new channel to measure the hypothesized neutrinoless mode of these decays. The Standard-Model-allowed two-neutrino double electron capture has been predicted for a number of isotopes, but only observed in 78Kr, 130Ba and, recently, 124Xe. The sensitivity to this decay establishes a benchmark for the ultimate experimental goal, namely the potential to discover also the lepton-number-violating neutrinoless version of this process. Here we report on the current sensitivity of the NEXT-Whit…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsElectron captureDark Matter and Double Beta DecayExtrapolationFOS: Physical scienceschemistry.chemical_elementElectronsElectron01 natural sciences7. Clean energyAtomicHigh Energy Physics - ExperimentTECNOLOGIA ELECTRONICANuclear physicsHigh Energy Physics - Experiment (hep-ex)XenonParticle and Plasma PhysicsDouble beta decay0103 physical sciencesNuclear MatrixNuclearSensitivity (control systems)Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentMathematical PhysicsPhysicsQuantum PhysicsIsotope010308 nuclear & particles physicsRaigs beta -- DesintegracióDetectorFísicaMolecularDetectorsDetectorInstrumentation and Detectors (physics.ins-det)Beta DecayNuclear & Particles Physicschemistry13. Climate actionBeta rays -- Decay
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Mitigation of backgrounds from cosmogenic 137Xe in xenon gas experiments using 3He neutron capture

2021

136Xe is used as the target medium for many experiments searching for 0¿ßß. Despite underground operation, cosmic muons that reach the laboratory can produce spallation neutrons causing activation of detector materials. A potential background that is difficult to veto using muon tagging comes in the form of 137Xe created by the capture of neutrons on 136Xe. This isotope decays via beta decay with a half-life of 3.8 min and a Q ß of ~4.16 MeV. This work proposes and explores the concept of adding a small percentage of 3He to xenon as a means to capture thermal neutrons and reduce the number of activations in the detector volume. When using this technique we find the contamination from 137Xe …

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