Search results for "Particle physics"

showing 10 items of 6826 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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CP violation and the H-A lineshape

2007

In two-Higgs doublet models (and particularly in the MSSM) the CP-even (H) and CP-odd (A) neutral scalars are nearly degenerate in mass, and their s-channel production would lead to nearly overlapping resonances. CP-violating effects may connect these two Higgs bosons, giving origin to one-loop particle mixing, which, due to their mass proximity, can be resonantly enhanced, altering their lineshape significantly. We show that, in general, the effect of such a CP-violating mixing cannot be mimicked by (or be re-absorbed into) a simple redefinition of the H and A masses in the context of a CP-conserving model. Specifically, the effects of the CP-mixing are such that, either the mass-splitting…

PhysicsHistoryRange (particle radiation)Particle physicsSIMPLE (dark matter experiment)Degenerate energy levelsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaContext (language use)Computer Science ApplicationsEducationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonCP violationMixing (physics)Boson
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The backward end-cap for the PANDA electromagnetic calorimeter

2015

The PANDA experiment at the new FAIR facility will cover a broad experimental programme in hadron structure and spectroscopy. As a multipurpose detector, the PANDA spectrometer needs to ensure almost 4π coverage of the scattering solid angle, full and accurate multiple-particle event reconstruction and very good particle identification capabilities. The electromagnetic calorimeter (EMC) will be a key item for many of these aspects. Particle energies ranging from some MeVs to several GeVs have to be measured with a relative resolution of 1% ⊕ 2%/√E/GeV . It will be a homogeneous calorimeter made of PbWO4 crystals and will be operated at -25°C, in order to improve the scintillation light yiel…

PhysicsHistoryScintillationSpectrometerCalorimeter (particle physics)APDSPhysics::Instrumentation and Detectorsbusiness.industryDetectorAvalanche photodiodeParticle identificationComputer Science ApplicationsEducationlaw.inventionNuclear physicsOpticslawNuclear ExperimentbusinessEvent reconstructionJournal of Physics: Conference Series
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Neutrino masses: evidences and implications

2014

I give an overview of the evidences for neutrino masses and mixing, the associated neutrino mass generation schemes, as well as the resulting implications in particle physics experiments and cosmology.

PhysicsHistorySterile neutrinoParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaPhysics beyond the Standard ModelSolar neutrinoHigh Energy Physics::PhenomenologyMass generationSolar neutrino problemComputer Science ApplicationsEducationNuclear physicsMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationJournal of Physics: Conference Series
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