Search results for "Natural science"

showing 10 items of 34579 documents

Recent improvements of the LPSC charge breeder

2017

International audience; PSC has developed the PHOENIX electron cyclotron resonance Charge Breeder since 2000. The performances have been improved over time acting on the 1+ and N+ beam optics, the base vacuum and the 1+ beam injection. A new objective is to update the booster design to enhance high charge state production and 1+ N+ efficiencies, reduce the co-extracted background beam and improve the ion source tunability. The first step, consisting in increasing the peak magnetic field at injection from 1.2 T to 1.6 T was implemented and significant improvement in 1+N+ efficiencies are reported: 12.9% of 23Na8+, 24.2% of 40Ar8+, 13.3% of 132Xe26+ and 13% of 133Cs26+. The next steps of the …

010302 applied physicsMaterials scienceta114Nuclear engineering[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]syklotronitCharge (physics)plasmatekniikka01 natural sciences7. Clean energy010305 fluids & plasmaselectron cyclotron resonanceBreeder (animal)0103 physical sciencesplasma
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Photoelectron Emission from Metal Surfaces Induced by Radiation Emitted by a 14 GHz Electron Cyclotron Resonance Ion Source

2015

Photoelectron emission measurements have been performed using a room-temperature 14 GHz ECR ion source. It is shown that the photoelectron emission from Al, Cu, and stainless steel (SAE 304) surfaces, which are common plasma chamber materials, is predominantly caused by radiation emitted from plasma with energies between 8 eV and 1 keV. Characteristic X-ray emission and bremsstrahlung from plasma have a negligible contribution to the photoelectron emission. It is estimated from the measured data that the maximum conceivable photoelectron flux from plasma chamber walls is on the order of 10% of the estimated total electron losses from the plasma. peerReviewed

010302 applied physicsMaterials scienceta114Physics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaCyclotron resonanceBremsstrahlungFOS: Physical sciencesPlasmaElectronphotoelectron emissionRadiation01 natural sciences7. Clean energyElectron cyclotron resonanceIon sourcePhysics - Plasma Physics010305 fluids & plasmasPlasma Physics (physics.plasm-ph)Physics::Plasma Physics0103 physical scienceselectron cyclotron resonance ion sourcesPlasma diagnosticsAtomic physicsInstrumentation
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Deviation of H− beam extraction simulation model

2018

Negative hydrogen ion source extraction system development is dependent on accurate and fast simulation methods for modelling the behaviour of ion and electron beams. Traditionally this type of work has been done using ray-tracing extraction codes, such as IBSimu. The plasma extraction model in IBSimu has been observed to under-estimate the charge density near the plasma sheath, leading to incorrect prediction of the current at which the system produces the optimum emittance. It is suspected that this deviation results from the approximations made by the model, neglecting the magnetic field and collisional effects near the sheath region. Results and comparisons to simulations are presented …

010302 applied physicsMaterials scienceta114business.industryExtraction (chemistry)tietokonegrafiikkaplasmafysiikka01 natural sciencesOpticsion sourcesPhysics::Plasma Physicscomputer graphics0103 physical sciencessimulointi010306 general physicsbusinessBeam (structure)plasma sheaths
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Power efficiency improvements with the radio frequency H− ion source

2016

CW 13.56 MHz radio frequency-driven H(-) ion source is under development at the University of Jyväskylä for replacing an existing filament-driven ion source at the MCC30/15 cyclotron. Previously, production of 1 mA H(-) beam, which is the target intensity of the ion source, has been reported at 3 kW of RF power. The original ion source front plate with an adjustable electromagnet based filter field has been replaced with a new front plate with permanent magnet filter field. The new structure is more open and enables a higher flux of ro-vibrationally excited molecules towards the plasma electrode and provides a better control of the potential near the extraction due to a stronger separation …

010302 applied physicsMaterials scienceta114ta213Electromagnetbusiness.industryRF power amplifierCyclotronPlasma01 natural sciencesIon sourcelaw.inventionion sourceslawMagnet0103 physical sciencesOptoelectronicsRadio frequencypower efficiency010306 general physicsbusinessInstrumentationElectrical efficiencyReview of Scientific Instruments
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New progress of high current gasdynamic ion source (invited).

2016

The experimental and theoretical research carried out at the Institute of Applied Physics resulted in development of a new type of electron cyclotron resonance ion sources (ECRISs)—the gasdynamic ECRIS. The gasdynamic ECRIS features a confinement mechanism in a magnetic trap that is different from Geller’s ECRIS confinement, i.e., the quasi-gasdynamic one similar to that in fusion mirror traps. Experimental studies of gasdynamic ECRIS were performed at Simple Mirror Ion Source (SMIS) 37 facility. The plasma was created by 37.5 and 75 GHz gyrotron radiation with power up to 100 kW. High frequency microwaves allowed to create and sustain plasma with significant density (up to 8 × 1013 cm−3 ) …

010302 applied physicsMaterials scienceta114ta213ion beamsPlasma01 natural sciencesIon sourceElectron cyclotron resonance010305 fluids & plasmaslaw.inventionIonlawGyrotronIonizationgasdynamic ECRIS0103 physical scienceselectron cyclotron resonance ion sourcesThermal emittanceAtomic physicsInstrumentationMicrowaveThe Review of scientific instruments
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Atomic Layer Deposition of LiF Thin Films from Lithd, Mg(thd)2, and TiF4 Precursors

2013

Lithium fluoride is an interesting material because of its low refractive index and large band gap. Previously LiF thin films have been deposited mostly by physical methods. In this study a new way of depositing thin films of LiF using atomic layer deposition (ALD) is presented. Mg(thd)2, TiF4 and Lithd were used as precursors, and they produced crystalline LiF at a temperature range of 300–350 °C. The films were studied by UV–vis spectrometry, field emission scanning electron microscopy (FESEM), X-ray diffraction (XRD), atomic force microscopy (AFM), time-of-flight elastic recoil detection analysis (ToF-ERDA), and energy dispersive X-ray spectroscopy (EDX). In addition, film adhesion was t…

010302 applied physicsMaterials scienceta214ta114Band gapGeneral Chemical EngineeringAnalytical chemistryLithium fluoride02 engineering and technologyGeneral ChemistryAtmospheric temperature range021001 nanoscience & nanotechnology01 natural sciencesElastic recoil detectionchemistry.chemical_compoundAtomic layer depositionchemistryImpurity0103 physical sciencesMaterials ChemistryThin film0210 nano-technologySpectroscopyChemistry of Materials
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Quasi-static behaviour and damage assessment of flax/epoxy composites

2015

Experimental investigations were conducted on flax and E-glass fibres reinforced epoxy matrix composites subjected to quasi-static loadings. Flax/epoxy samples having [0]12, [90]12, [0/90]3S and [±45]3S stacking sequences, with a fibre volume fraction of 43% have been tested under tension, compression and in-plane shear loadings. Overall, the compression strength of glass/epoxy was 76% greater than for the flax/epoxy composite. The damage evolution of flax/epoxy of [0/90]3S and [±45]3S samples has been evaluated in terms of transverse crack densities with respect to the load increment. The crack density exhibited a classical “S” shaped pattern for [0/90]3S and linearly for [±45]3S specimens…

010302 applied physicsMatériaux [Sciences de l'ingénieur]Materials sciencePolymer-matrix compositesComposite numberMechanical properties02 engineering and technologyEpoxy matrixEpoxy021001 nanoscience & nanotechnologyE-glass fibres01 natural sciences[SPI]Engineering Sciences [physics]Compressive strengthDamage mechanicsDamage mechanicsvisual_art0103 physical sciencesVolume fractionvisual_art.visual_art_mediumFlax fibresMécanique: Mécanique des matériaux [Sciences de l'ingénieur]Composite material0210 nano-technologyQuasistatic process
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Measuring rain energy with the employment of “Arduino”

2016

This paper presents the performances of rainfall energy harvesting through the use of a piezoelectric transducer and an Arduino-based measuring system. Diverse studies agree on the possibility of generating electricity from rainfall, but to date, a study that can measure the quantity of energy produced during rainfall is still missing. The present study begins with results obtained from laboratory researchers using piezoelectric transducers and oscilloscopes — to measure the energy produced from a single raindrop — and concludes with an ad hoc Arduino-based measuring system, aimed at measuring the actual amount of electrical energy produced by a piezoelectric transducer that is exposed to r…

010302 applied physicsMeasure (data warehouse)EngineeringEnergy harvestingbusiness.industryElectric potential energyElectrical engineering02 engineering and technologySettore ING-IND/32 - Convertitori Macchine E Azionamenti Elettrici021001 nanoscience & nanotechnologySettore ING-INF/01 - Elettronica01 natural sciencesSettore ING-IND/31 - ElettrotecnicaElectricity generationTransducerArduino0103 physical sciencesOscilloscope0210 nano-technologybusinessEnergy harvestingPiezoelectric sensorEnergy (signal processing)2016 IEEE International Conference on Renewable Energy Research and Applications (ICRERA)
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State-space formulation of scalar Preisach hysteresis model for rapid computation in time domain

2015

A state-space formulation of classical scalar Preisach model (CSPM) of hysteresis is proposed. The introduced state dynamics and memory interface allow to use the state equation, which is rapid in calculation, instead of the original Preisach equation. The main benefit of the proposed modeling approach is the reduced computational effort which requires only a single integration over the instantaneous line segment in the Preisach plane. Numerical evaluations of the computation time and model accuracy are provided in comparison to the CSPM which is taken as a reference model.

010302 applied physicsMemory interfacePreisach model of hysteresis0209 industrial biotechnologyApplied MathematicsComputationScalar (mathematics)02 engineering and technologySystems and Control (eess.SY)01 natural sciences020901 industrial engineering & automationLine segmentControl theoryModeling and Simulation0103 physical sciencesFOS: Electrical engineering electronic engineering information engineeringApplied mathematicsComputer Science - Systems and ControlTime domainReference modelMathematics
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Integral imaging with Fourier-plane recording

2017

Integral Imaging is well known for its capability of recording both the spatial and the angular information of threedimensional (3D) scenes. Based on such an idea, the plenoptic concept has been developed in the past two decades, and therefore a new camera has been designed with the capacity of capturing the spatial-angular information with a single sensor and after a single shot. However, the classical plenoptic design presents two drawbacks, one is the oblique recording made by external microlenses. Other is loss of information due to diffraction effects. In this contribution report a change in the paradigm and propose the combination of telecentric architecture and Fourier-plane recordin…

010302 applied physicsMicrolensDiffractionIntegral imagingPlane (geometry)Computer sciencebusiness.industryComputationComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONOblique case01 natural sciencesÒptica Aparells i instruments010309 opticssymbols.namesakeFourier transformOptics0103 physical sciencessymbolsComputer visionDepth of fieldArtificial intelligenceFourier Anàlisi debusinessThree-Dimensional Imaging, Visualization, and Display 2017
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