Search results for "URC"

showing 10 items of 7748 documents

Ionization efficiency studies with charge breeder and conventional electron cyclotron resonance ion source

2013

Radioactive Ion Beams play an increasingly important role in several European research facility programs such as SPES, SPIRAL1 Upgrade, and SPIRAL2, but even more for those such as EURISOL. Although remarkable advances of ECRIS charge breeders (CBs) have been achieved, further studies are needed to gain insight on the physics of the charge breeding process. The fundamental plasma processes of charge breeders are studied in the frame of the European collaboration project, EMILIE, for optimizing the charge breeding. Important information on the charge breeding can be obtained by conducting similar experiments using the gas mixing and 2-frequency heating techniques with a conventional JYFL 14 …

010302 applied physicsIonizationMaterials scienceta114[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Particle acceleratorCharge (physics)Plasma7. Clean energy01 natural sciencesIon sourceElectron cyclotron resonanceIonlaw.inventionNuclear physicsBreeder (animal)lawIonization0103 physical sciences010306 general physicsInstrumentationComputingMilieux_MISCELLANEOUS
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Experimental evidence on photo-assisted O− ion production from Al2O3 cathode in cesium sputter negative ion source

2020

The production of negative ions in cesium sputter ion sources is generally considered to be a pure surface process. It has been recently proposed that ion pair production could explain the higher-than-expected beam currents extracted from these ion sources, therefore opening the door for laser-assisted enhancement of the negative ion yield. We have tested this hypothesis by measuring the effect of various pulsed diode lasers on the O − beam current produced from Al 2O 3 cathode of a cesium sputter ion source. It is expected that the ion pair production of O − requires populating the 5d electronic states of neutral cesium, thus implying that the process should be provoked only with specific …

010302 applied physicsMaterials scienceGeneral Physics and Astronomy02 engineering and technologyPhoton energy021001 nanoscience & nanotechnologyLaser01 natural sciencesCathodeIon sourceIonlaw.inventionPhysics::Plasma PhysicslawSputtering0103 physical sciencesAtomic physics0210 nano-technologyBeam (structure)DiodeJournal of Applied Physics
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Photoelectron Emission from Metal Surfaces Induced by VUV-emission of Filament Driven Hydrogen Arc Discharge Plasma

2015

Photoelectron emission measurements have been performed using a filament-driven multi-cusp arc discharge volume production H^- ion source (LIISA). It has been found that photoelectron currents obtained with Al, Cu, Mo, Ta and stainless steel (SAE 304) are on the same order of magnitude. The photoelectron currents depend linearly on the discharge power. It is shown experimentally that photoelectron emission is significant only in the short wavelength range of hydrogen spectrum due to the energy dependence of the quantum efficiency. It is estimated from the measured data that the maximum photoelectron flux from plasma chamber walls is on the order of 1 A per kW of discharge power.

010302 applied physicsMaterials scienceHydrogenPhysics::Instrumentation and DetectorsFluxchemistry.chemical_elementFOS: Physical sciencesPlasma01 natural sciences7. Clean energyPhysics - Plasma PhysicsIon source010305 fluids & plasmasElectric arcPlasma Physics (physics.plasm-ph)chemistryPhysics::Plasma Physics0103 physical sciencesPhysics::Atomic and Molecular ClustersQuantum efficiencyPhysics::Atomic PhysicsAtomic physicsHydrogen spectral seriesOrder of magnitude
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A new 18 GHz room temperature electron cyclotron resonance ion source for highly charged ion beams

2020

An innovative 18 GHz HIISI (Heavy Ion Ion Source Injector) room temperature Electron Cyclotron Resonance (ECR) ion source (ECRIS) has been designed and constructed at the Department of Physics, University of Jyväskylä (JYFL), for the nuclear physics program of the JYFL Accelerator Laboratory. The primary objective of HIISI is to increase the intensities of medium charge states (M/Q ≅ 5) by a factor of 10 in comparison with the JYFL 14 GHz ECRIS and to increase the maximum usable xenon charge state from 35+ to 44+ to serve the space electronics irradiation testing program. HIISI is equipped with a refrigerated permanent magnet hexapole and a noncylindrical plasma chamber to achieve very stro…

010302 applied physicsMaterials scienceIon beamsyklotronittutkimuslaitteetHighly charged ionchemistry.chemical_elementhiukkaskiihdyttimet01 natural sciences7. Clean energyIon sourceElectron cyclotron resonance010305 fluids & plasmasIonXenonchemistry0103 physical sciencesIrradiationAtomic physicsInstrumentationBeam (structure)
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Optimization of a laser ion source for $^{163}$Ho isotope separation

2019

To measure the mass of the electron neutrino, the “Electron Capture in Holmium-163” (ECHo) collaboration aims at calorimetrically measuring the spectrum following electron capture in 163Ho. The success of the ECHo experiment depends critically on the radiochemical purity of the 163Ho sample, which is ion-implanted into the calorimeters. For this, a 30 kV high transmission magnetic mass separator equipped with a resonance ionization laser ion source is used. To meet the ECHo requirements, the ion source unit was optimized with respect to its thermal characteristics and material composition by means of the finite element method thermal-electric calculations and chemical equilibrium simulation…

010302 applied physicsMaterials sciencePhysics - Instrumentation and DetectorsAtomic Physics (physics.atom-ph)Electron captureFOS: Physical sciencesThermal ionizationInstrumentation and Detectors (physics.ins-det)Laser01 natural sciencesIon source010305 fluids & plasmasIsotope separationlaw.inventionPhysics - Atomic PhysicslawIonization0103 physical sciencesThermalAtomic physicsChemical equilibriumInstrumentation
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The role of seed electrons on the plasma breakdown and preglow of electron cyclotron resonance ion source

2009

The 14 GHz Electron Cyclotron Resonance Ion Source at University of Jyväskylä, Department of Physics (JYFL) has been operated in pulsed mode in order to study the plasma breakdown and preglow effect. It was observed that the plasma breakdown time and preglow characteristics are affected by seed electrons provided by a continuous low power microwave signal at secondary frequency. Sustaining low density plasma during the off-period of high power microwave pulses at the primary frequency shifts the charge state distribution of the preglow transient toward higher charge states. This could be exploited for applications requiring fast and efficient ionization of radioactive elements as proposed f…

010302 applied physicsMaterials science[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Cyclotron resonancechemistry.chemical_elementPlasmaElectron01 natural sciences7. Clean energyElectron cyclotron resonanceIon source010305 fluids & plasmasNeonchemistryIonizationBeta (plasma physics)0103 physical sciencesAtomic physicsInstrumentationComputingMilieux_MISCELLANEOUSReview of Scientific Instruments
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The effect of cavity tuning on oxygen beam currents of an A-ECR type 14 GHz electron cyclotron resonance ion source.

2016

The efficiency of the microwave-plasma coupling plays a significant role in the production of highly charged ion beams with electron cyclotron resonance ion sources (ECRISs). The coupling properties are affected by the mechanical design of the ion source plasma chamber and microwave launching system, as well as damping of the microwave electric field by the plasma. Several experiments attempting to optimize the microwave-plasma coupling characteristics by fine-tuning the frequency of the injected microwaves have been conducted with varying degrees of success. The inherent difficulty in interpretation of the frequency tuning results is that the effects of microwave coupling system and the ca…

010302 applied physicsMaterials scienceta114Highly charged ionPlasma01 natural sciencesElectron cyclotron resonanceIon sourcemicrowaves010305 fluids & plasmasIonmikroaallotPhysics::Plasma Physics0103 physical scienceselectron cyclotron resonance ion sourcesplasma chamberAtomic physicsInstrumentationBeam (structure)MicrowaveMicrowave cavityThe Review of scientific instruments
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Kinetic instabilities in pulsed operation mode of a 14 GHz electron cyclotron resonance ion source

2016

The occurrence of kinetic plasma instabilities is studied in pulsed operation mode of a 14 GHz Aelectron cyclotron resonance type electron cyclotron resonance ion source. It is shown that the temporal delay between the plasma breakdown and the appearance of the instabilities is on the order of 10- 100 ms. The most important parameters affecting the delay are magnetic field strength and neutral gas pressure. It is demonstrated that kinetic instabilities limit the high charge state ion beam production in the unstable operating regime. peerReviewed

010302 applied physicsMaterials scienceta114Ion beamCyclotron resonancePlasma01 natural sciencesplasma electronsIon sourceElectron cyclotron resonanceFourier transform ion cyclotron resonance010305 fluids & plasmasMagnetic fieldpulsed operation modePhysics::Plasma Physics0103 physical scienceselectron cyclotron resonance ion sourceskinetic instabilitiesAtomic physicsInstrumentationIon cyclotron resonanceReview of Scientific Instruments
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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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