Search results for "Computer Science Application"

showing 10 items of 3998 documents

WIMPy baryogenesis with sterile neutrinos

2015

In this talk we propose a mechanism for baryogenesis from particle decays or annihilations that can work at the TeV scale. Some heavy particles annihilate or decay into a heavy sterile neutrino N (with M 1 TeV) and a "light" one ν (with m 100 GeV), generating an asymmetry among the two helicity degrees of freedom of v. This asymmetry is partially transferred to Standard Model leptons via fast Yukawa interactions and reprocessed into a baryon asymmetry by the electroweak sphalerons. We illustrate this mechanism in a WIMPy baryogenesis model where the helicity asymmetry is generated in the annihilation of dark matter. This model connects the baryon asymmetry, dark matter, and neutrino masses.

PhysicsHistoryParticle physicsSterile neutrinoAstrophysics::High Energy Astrophysical Phenomenamedia_common.quotation_subjectHigh Energy Physics::PhenomenologyDark matterElectroweak interactionAsymmetryComputer Science ApplicationsEducationBaryogenesisNuclear physicsBaryon asymmetryHigh Energy Physics::ExperimentNeutrinoLeptonmedia_commonJournal of Physics: Conference Series
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Physics of nuclear processes triggered by the interplay of strong and weak interactions

2012

Neutrinoless double beta (0νββ) decay of nuclei is a process that requires the neutrino to be a massive Majorana particle and thus cannot proceed in the standard model of electro-weak interactions. Recent results of the neutrino-oscillation experiments have produced accurate information on the mixing of neutrinos and their squared mass differences. The 0νββ decay takes place in atomic nuclei where it can be observed, at least in principle, by underground neutrino experiments. The information about the weak-interaction observables, like the neutrino mass, has to be filtered from the data through the nuclear matrix elements (NMEs). In this article recent work of the Jyv¨askyl¨a group on the N…

PhysicsHistoryParticle physicsSterile neutrinoHigh Energy Physics::PhenomenologyBeta decayBeta-decay stable isobarsComputer Science ApplicationsEducationNuclear physicsMAJORANATheoretical nuclear physicsDouble beta decayAtomic nucleusteoreettinen ydinfysiikkaHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationNuclear Experiment
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Search for sterile neutrinos at radioactive ion beam facilities

2013

We propose applications of Radioactive Ion Beam facilities to investigate physics beyond the Standard Model. In particular, we focus upon the search for sterile neutrinos by means of a low energy beta-beam with a Lorentz boost factor of 1. In the considered setup, collected 8Li radioactive ions are sent inside a 4? detector filled with a liquid scintillator, with inverse-beta decay as neutrino detection channel. We provide exclusion curves for the sterile neutrino mixing parameters, based upon the 3+1 formalism, depending upon the achievable ion intensity. The proposed experiment represents a possible alternative to clarify the current anomalies observed in neutrino experiments.

PhysicsHistoryParticle physicsSterile neutrinoIon beamPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyScintillatorComputer Science ApplicationsEducationIonNuclear physicsNeutrino detectorMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoJournal of Physics: Conference Series
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The NEXT double beta decay experiment

2016

NEXT (Neutrino Experiment with a Xenon TPC) is a neutrinoless double-beta (ββ0v) decay experiment at Laboratorio Subterraneo de Canfranc (LSC). It is an electroluminescent Time Projection Chamber filled with high pressure 136Xe gas with separated function capabilities for calorimetry and tracking. Energy resolution and background suppression are the two key features of any neutrinoless double beta decay experiment. NEXT has both good energy resolution (< 1% FWHM) and an extra handle for background identification provided by track reconstruction. We expect a background rate of 4 × 10-4 counts keV-1 kg-1 yr-1, and a sensitivity to the Majorana neutrino mass of between 80-160 meV (depending on…

PhysicsHistoryParticle physicsTime projection chamberScale (ratio)010308 nuclear & particles physicsDetectorchemistry.chemical_elementTracking (particle physics)01 natural sciencesComputer Science ApplicationsEducationNuclear physicsMAJORANAXenonchemistryDouble beta decay0103 physical sciencesNeutrino010306 general physicsJournal of Physics: Conference Series
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Precision mass measurements for nuclear astro- and neutrino physics

2012

Nuclear masses are indispensable ingredients in numerous physics applications ranging from nuclear structure physics, where, e.g., the shell closures and nucleon correlation energies can be studied by accurate mass measurements, via the nuclear astrophysics, where the masses of nuclei far from the valley of β-stability determine the pathways of, e.g., rp-and r-processes of nucleosynthesis in stars, to tests of the standard model and fundamental interactions, where, e.g., the very-accurate masses of parent and superallowed β-decay daughter nuclei serve as one of inputs for the checking of the unitarity of the CKM quark-mixing matrix. In this review we focus on recent direct mass measurements…

PhysicsHistoryParticle physicsUnitarityNuclear TheoryNuclear structurePenning trapComputer Science ApplicationsEducationStandard ModelNuclear physicsNucleosynthesisNuclear astrophysicsNeutrinoNuclear ExperimentNucleonJournal of Physics: Conference Series
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Future axion searches with the International Axion Observatory (IAXO)

2013

Çetin, Serkant Ali (Dogus Author) -- Conference full title: 6th Symposium on Large TPCs for Low Energy Rare Event Detection; Paris; France; 17 December 2012 through 19 December 2012. The International Axion Observatory (IAXO) is a new generation axion helioscope aiming at a sensitivity to the axion-photon coupling of gaγ ∼ few × 10-12 GeV-1, i.e. 1-1.5 orders of magnitude beyond the one achieved by CAST, currently the most sensitive axion helioscope. The main elements of IAXO are an increased magnetic field volume together with extensive use of x-ray focusing optics and low background detectors, innovations already successfully tested in CAST. Additional physics cases of IAXO could include …

PhysicsHistoryParticle physicssolar axionOrders of Magnitude010308 nuclear & particles physicsRare event detectionSingle photon detectorsLow Background Detectors01 natural sciencesdark matterWhite DwarfsComputer Science ApplicationsEducationLow energyObservatory0103 physical sciencessolar axions; dark matter; Single photon detectorssolar axionsddc:530X-ray Focusing Optics010306 general physicsAxion
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Calorimetry triggering in ATLAS

2009

The ATLAS experiment is preparing for data taking at 14 TeV collision energy. A rich discovery physics program is being prepared in addition to the detailed study of Standard Model processes which will be produced in abundance. The ATLAS multi-level trigger system is designed to accept one event in 2 105 to enable the selection of rare and unusual physics events. The ATLAS calorimeter system is a precise instrument, which includes liquid Argon electro-magnetic and hadronic components as well as a scintillator-tile hadronic calorimeter. All these components are used in the various levels of the trigger system. A wide physics coverage is ensured by inclusively selecting events with candidate …

PhysicsHistoryParticle physicstrigger systemPhotonAtlas (topology)Physics::Instrumentation and DetectorsATLAS experimentMonte Carlo methodFísicaATLAS experimentCosmic rayComputer Science ApplicationsEducationCalorimeterNuclear physicsData acquisitionMeasuring instrument[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]calorimeter systemHigh Energy Physics::ExperimentCiencias Exactas
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Differences between photoluminescence spectra of type-I and type-II quantum dots

2008

Semiconductor quantum dots which trap simultaneously electrons and holes are called quantum dots of type-I. Contrary to these structures, empty dots of type-II attract only one type of charged carriers and repel the other. Particularities of confining potential are unaccessible by any direct measurements, thus recognition of quantum dot type by indirect method is highly desired. Our proposal is to distinguish between the two types of quantum dots via a comparison of photoluminescence spectra of these structures, which differ in both cases qualitatively.

PhysicsHistoryPhotoluminescenceCondensed matter physicsQuantum point contactElectronFermionCondensed Matter::Mesoscopic Systems and Quantum Hall EffectComputer Science ApplicationsEducationQuantum dot laserQuantum dotCharge carrierEmission spectrumJournal of Physics: Conference Series
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Study of the Planacon XP85012 photomultiplier characteristics for its use in a Cherenkov detector

2016

Main properties of the multi-anode microchannel plate photomultiplier to be used in a Cherenkov detector are discussed. The laboratory test results obtained using irradiation of the MCP-PMT photocathode by picosecond optical laser pulses with different intensities (from single photon regime to the PMT saturation conditions) are presented. peerReviewed

PhysicsHistoryPhotomultiplierPhotonPhysics::Instrumentation and DetectorsCherenkov detectorbusiness.industryPhysics::Medical PhysicsAstrophysics::Instrumentation and Methods for AstrophysicsPhysics::OpticsLaserPhotocathodeComputer Science ApplicationsEducationlaw.inventionOpticslawPicosecondMicrochannel plate detectorIrradiationbusinessCherenkov detectorJournal of Physics: Conference Series
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Performance study of the fast timing Cherenkov detector based on a microchannel plate PMT

2017

Prototype of the fast timing Cherenkov detector, applicable in high-energy collider experiments, has been developed basing on the modified Planacon XP85012 MCP-PMT and fused silica radiators. We present the reasons and description of the MCP-PMT modification, timing and amplitude characteristics of the prototype including the summary of the detector's response on particle hits at oblique angles and MCP-PMT performance at high illumination rates.

PhysicsHistoryPhotomultiplierPhysics::Instrumentation and Detectors010308 nuclear & particles physicsbusiness.industryCherenkov detectorQuantitative Biology::Tissues and OrgansDetectorAstrophysics::Instrumentation and Methods for Astrophysics01 natural sciencesParticle detectorComputer Science ApplicationsEducationlaw.inventionOpticslaw0103 physical sciencesScintillation counterMeasuring instrumentMicrochannel plate detector010306 general physicsbusinessColliderJournal of Physics: Conference Series
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