Search results for "Nuclear Instrumentation"

showing 8 items of 8 documents

Excess electronic recoil events in XENON1T

2020

We report results from searches for new physics with low-energy electronic recoil data recorded with the XENON1T detector. With an exposure of 0.65 t-y and an unprecedentedly low background rate of $76\pm2$ events/(t y keV) between 1 and 30 keV, the data enables sensitive searches for solar axions, an enhanced neutrino magnetic moment, and bosonic dark matter. An excess over known backgrounds is observed at low energies and most prominent between 2 and 3 keV. The solar axion model has a 3.4$\sigma$ significance, and a 3D 90% confidence surface is reported for axion couplings to electrons, photons, and nucleons. This surface is inscribed in the cuboid defined by $g_{ae}<3.8 \times 10^{-12}$,…

xenon: targetaxionssolar axionmagnetic momentdimension: 3neutrino: solarPhysics beyond the Standard ModelSolar neutrinodark matter: direct detection01 natural sciences7. Clean energyHigh Energy Physics - ExperimentDark matter direct detection axionHigh Energy Physics - Experiment (hep-ex)neutrinoXENONHigh Energy Physics - Phenomenology (hep-ph)background: lowRecoilelectron: recoil[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]beta-raysParticle Physics Experimentscoupling: (axion 2electron)multi-purpose particle detectornuclear instrumentationComputingMilieux_MISCELLANEOUSinstrumentationPhysicsxenon: liquidboson: dark matteraxion 2nucleontritiumnew physics: search forsemileptonic decayboson: vectortensionneutrino: magnetic momentHigh Energy Physics - Phenomenologyaxion 2photonlow backgroundbosonNeutrinoionizing radiationNucleonAstrophysics - Cosmology and Nongalactic AstrophysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)dark matter detectorelectronic recoilElectron captureXENON1T detectorDark matterlow-energy electronic recoil dataFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]dark matterNONuclear physicsPE2_2PE2_1tritium: semileptonic decay0103 physical sciencessolar axion modelsurface[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]axion: couplingPE2_4010306 general physicspseudoscalarAxiondark matter: vectordark matter XENON1T detector electronic recoilsolar neutrinodetectorDark Matter Axions Beta Decay Liquid Xenon TPC010308 nuclear & particles physicsaxion 2electroncoupling: (axion 2nucleon)dark matter: detectormodel: axionGran Sassometrology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]axionstellar constraintscoupling: (axion 2photon)High Energy Physics::Experimentparticle dark matterdirect detectionbeta decayaxion: solar[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]experimental results
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Contributions to Phase Two of AGATA electronics

2020

En el campo de la física nuclear, la espectroscopia de rayos gamma de alta resolución es un método preciso para estudiar la estructura del núcleo, extrayendo la energía y la distribución angular de los fotones gamma emitidos en las transiciones entre estados nucleares. Para obtener núcleos en un estado excitado y por tanto emitan rayos gamma, hemos de hacer chocar la materia, produciendo reacciones nucleares (espectroscopia de haz) o recurrir a desintegraciones radiactivas (espectroscopia de desintegración). Los detectores de semiconductor de germanio de alta pureza (HPGe) han demostrado tener una buena respuesta interaccionando con rayos gamma. Al igual que otros detectores de basados en s…

:CIENCIAS TECNOLÓGICAS [UNESCO]Gamma Ray SpectroscopyJESD204 protocolTime Domain MultiplexingUNESCO::CIENCIAS TECNOLÓGICASAGATAApplied Electronics & Instrumentation EngineeringHigh Speed Digital DesignFPGANuclear Instrumentation
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Vers une architecture électronique unifiée et zéro temps mort pour l'instrumentation nucléaire

2014

International audience; Dans l'instrumentation nucléaire, et d'autres domaines tels que les applications de la physique des particules, l'analyse de signaux médicaux (Tomographie par Émission de Positons (TEP), Électro-EncéphaloGraphie (EEG)) ou la détection de signaux radar, le signal mesuré est composé d'impulsions dont la date d'arrivée est aléatoire, et dont l'amplitude et la durée sont non déterministes. La grande variété d'applications nécessite de disposer d'une architecture flexible pouvant être aisément reprogrammée. De plus, l'exigence de mesures en temps réel impose de disposer d'une grande capacité de calcul et de bande passante pour la mise en forme et l'extraction des caractér…

instrumentation[INFO.INFO-AR]Computer Science [cs]/Hardware Architecture [cs.AR][INFO.INFO-AR] Computer Science [cs]/Hardware Architecture [cs.AR]detectorElectronic architectureimpulse processingspectrum analysis[PHYS.PHYS.PHYS-INS-DET] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]sensor[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][ INFO.INFO-AR ] Computer Science [cs]/Hardware Architecture [cs.AR]real time processingsignal processingnuclear instrumentation
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The next generation nuclear instruments: AGATA and NEDA, and nuclear structure studies near N=Z line

2017

The first part of this thesis is devoted to the development of a large array of neutron detectors NEDA (NEutron Detector Array) and their conceptual design using Monte-Carlo simulations. Prior to the development of NEDA, the neutron detection with liquid scintillators is discussed in Chapter 2. In Chapter 3, the design criteria and simulations of NEDA are discussed. NEDA aims to build a neutron detector array with high efficiency, based on liquid scintillators. NEDA will be coupled to the high-purity γ-ray detector arrays, like AGATA, EXOGAM, to be used as a trigger or complementary detector in the contemporary nuclear physics experiments, which aim to investigate the structure of the exoti…

PhysicsNeutron DetectionDetectorsNEDANuclear Structure220806 - DETECTORES DE PARTICULASExperimental Nuclear PhysicsLiquid Scintillator Detectors220719 - ESTRUCTURA NUCLEAR220717 - REACCION NUCLEAR Y DISPERSIONNuclear ExperimentAGATAGe Semiconductor DetectorsNuclear InstrumentationNuclear Physics
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Auto-Adaptive Trigger and Pulse Extraction for Digital Processing in Nuclear Instrumentation

2015

International audience; This paper presents a novel auto-adaptive method for pulse triggering and extraction. Pulse triggering uses a threshold that must be placed as close as possible to the noise level. We do this by means of an adaptive threshold level based on real-time noise level estimation. A dynamic estimation of the pulse length is also used for pulse selection. The proposed approach is largely insensitive to noise and enables autonomous extraction of pulses regardless of their shape, height or length. The proposed approach can be used with numerous types of detectors from an analog-to-digital converter, and can be used in conjunction with various pulse processing techniques such a…

Nuclear and High Energy PhysicsEngineeringNoise (signal processing)business.industryDetectorPulse durationData acquisitionPulse processingtriggerPulse (physics)NOISEdigital pulse processing (DPP)Nuclear Energy and Engineering[INFO.INFO-TS]Computer Science [cs]/Signal and Image ProcessingElectronic engineeringDETECTORSExtraction (military)Instrumentation (computer programming)[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Electrical and Electronic EngineeringNoise levelbusinessdigital signal processing (DSP)nuclear instrumentation
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VERS UNE ARCHITECTURE UNIFIÉE ET ZÉRO TEMPS MORT POUR L'INSTRUMENTATION NUCLÉAIRE

2014

National audience; Dans l’instrumentation nucléaire, et d’autres domaines tels que les applications de la physique des particules, l’analyse de signaux médicaux (Tomographie par Emission de Positons (TEP), Electro-EncephaloGraphie (EEG)) ou la détection de signaux radar, le signal mesuré est composé d’impulsions dont la date d’arrivée est aléatoire, et dont l’amplitude et la durée sont non-d´eterministes. La grande variété d’applications nécessite de disposer d’une architecture flexible pouvant être aisément reprogrammée. De plus, l’exigence de mesures en temps réel impose de disposer d’une grande capacité de calcul et de bande passante pour la mise en forme et l’extraction des caractéristi…

instrumentation[INFO.INFO-AR]Computer Science [cs]/Hardware Architecture [cs.AR][INFO.INFO-AR] Computer Science [cs]/Hardware Architecture [cs.AR][ INFO.INFO-TS ] Computer Science [cs]/Signal and Image Processing[INFO.INFO-TS] Computer Science [cs]/Signal and Image ProcessingDigital Pulse Processing[SPI.TRON] Engineering Sciences [physics]/Electronicselectronic architecture[ SPI.TRON ] Engineering Sciences [physics]/Electronics[SPI.TRON]Engineering Sciences [physics]/Electronicsreal time measurementimpulse separation[INFO.INFO-TS]Computer Science [cs]/Signal and Image ProcessingDigital Signal Processing[ INFO.INFO-AR ] Computer Science [cs]/Hardware Architecture [cs.AR]Digital Architecturesignal processingnuclear instrumentation
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Improved calculations of beta decay backgrounds to new physics in liquid xenon detectors

2020

We present high-precision theoretical predictions for the electron energy spectra for the ground-state to ground-state $\beta$ decays of $^{214}$Pb, $^{212}$Pb, and $^{85}$Kr most relevant to the background of liquid xenon dark matter detectors. The effects of nuclear structure on the spectral shapes are taken into account using large-scale shell model calculations. Final spectra also include atomic screening and exchange effects. The impact of nuclear structure effects on the $^{214}$Pb and $^{212}$Pb spectra below $\approx100$ keV, pertinent for several searches for new physics, are found to be comparatively larger than those from the atomic effects alone. We find that the full calculatio…

electronElectron01 natural sciencesSpectral lineHigh Energy Physics - ExperimentspectrumHigh Energy Physics - Experiment (hep-ex)Xenon[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]beta-raysground stateNuclear Experiment (nucl-ex)Nuclear Experimentnuclear instrumentationPhysicsinstrumentationxenon: liquidnew physics: search forNuclear structureaxial-vectorsemileptonic decayCoupling (probability)simulation3. Good healthradioactivityGround stateionizing radiationSemileptonic decay[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]energy spectrumFOS: Physical scienceschemistry.chemical_elementspectrum analysis[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear physics0103 physical sciencesstructure[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsnumerical calculationssignal processingPseudovectorkryptonnucleus: semileptonic decayleaddetector010308 nuclear & particles physicsbackgroundscreeningDecay data measurementshell modelnuclear matter: effectdark matter: detector[INFO.INFO-MO]Computer Science [cs]/Modeling and Simulationcoupling: axial-vectorxenonmetrologychemistry13. Climate actionspectralelectron: energy spectrum
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Une architecture programmable de traitement des impulsions zéro-temps mort pour l'instrumentation nucléaire

2015

In the field of nuclear instrumentation, digital signal processing architectures have to deal with the poissonian characteristic of the signal, composed of random arrival pulses which requires current architectures to work in dataflow. Thus, the real-time needs implies losing pulses when the pulse rate is too high. Current architectures paralyze the acquisition of the signal during the pulse processing inducing a time during no signal can be processed, this is called the dead time. These issue have led current architectures to use dedicated solutions based on reconfigurable components such as FPGAs. The requirement of end users to implement a wide range of applications on a large number of …

[INFO.INFO-AR]Computer Science [cs]/Hardware Architecture [cs.AR]Architecture électroniqueInstrumentation nucléaireRadioactivité[ INFO.INFO-TS ] Computer Science [cs]/Signal and Image Processing[INFO.INFO-TS] Computer Science [cs]/Signal and Image ProcessingDigital Signal Processing (DSP)traitement du signalNuclear instrumentation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Distributed computing[INFO.INFO-TS]Computer Science [cs]/Signal and Image ProcessingTraitement numérique du signal (TNS)Électronique numériqueMesureArchitecture électronique distribuée[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Digital Pulse Processing (DPP)signal processingTraitement numérique des impulsions (DPP)
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