Search results for "ion source"

showing 10 items of 337 documents

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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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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Electron cyclotron resonance ion sources – physics, technology and future challenges

2017

This article has no abstract. peerReviewed

010302 applied physicsPhysicsECR ion sourcesta114Physics::Plasma PhysicsPhysicsQC1-9990103 physical sciences01 natural sciencesEngineering physicsElectron cyclotron resonance010305 fluids & plasmasIonEPJ Web of Conferences
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Radiofrequency and 2.45 GHz electron cyclotron resonance H−volume production ion sources

2016

The volume production of negative hydrogen ions () in plasma ion sources is based on dissociative electron attachment (DEA) to rovibrationally excited hydrogen molecules (H2), which is a two-step process requiring both, hot electrons for ionization, and vibrational excitation of the H2 and cold electrons for the formation through DEA. Traditionally ion sources relying on the volume production have been tandem-type arc discharge sources equipped with biased filament cathodes sustaining the plasma by thermionic electron emission and with a magnetic filter separating the main discharge from the formation volume. The main motivation to develop ion sources based on radiofrequency (RF) or electro…

010302 applied physicsPhysicsGeneral Physics and AstronomyPlasmaElectron01 natural sciencesElectron cyclotron resonanceIon sourceCathode010305 fluids & plasmasIonlaw.inventionElectric arclawIonization0103 physical sciencesAtomic physicsNew Journal of Physics
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Hot-cavity studies for the Resonance Ionization Laser Ion Source

2016

International audience; The Resonance Ionization Laser Ion Source (RILIS) has emerged as an important technique in many Radioactive Ion Beam (RIB) facilities for its reliability, and ability to ionize target elements efficiently and element selectively. GISELE is an off-line RILIS test bench to study the implementation of an on-line laser ion source at the GANIL separator facility. The aim of this project is to determine the best technical solution which combines high selectivity and ionization efficiency with small ion beam emittance and stable long term operation. The ion source geometry was tested in several configurations in order to find a solution with optimal ionization efficiency an…

010302 applied physicsPhysicsNuclear and High Energy PhysicsIon beamTitanium sapphire laser[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Ion gun7. Clean energy01 natural sciencesIon sourceAtmospheric-pressure laser ionizationHot cavityRadioactive Ion BeamWork function materialResonant Ionization Laser Ion SourceIon beam depositionIonization0103 physical sciencesPhysics::Accelerator PhysicsThermal emittanceAtomic physicsBeam emittance010306 general physicsInstrumentation
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H− extraction systems for CERN’s Linac4 H− ion source

2018

Abstract Linac4 is a 160 MeV linear H −  accelerator at CERN. It is an essential part of the beam luminosity upgrade of the Large Hadron Collider (LHC) and will be the primary injector into the chain of circular accelerators. It aims at increasing the beam brightness by a factor of 2, when compared to the currently used 50 MeV linear proton accelerator, Linac2. Linac4’s ion source is a cesiated RF-plasma H −  ion source. Several beam extraction systems were designed for H −  beams of 45 keV energy, 50 mA intensity and an electron to H −  ratio smaller than 5. The goal was to extract a beam with an rms-emittance of 0 . 25 π  mm mrad. One of the main challenges in designing an H −  extraction…

010302 applied physicsPhysicsNuclear and High Energy PhysicsLarge Hadron ColliderParticle acceleratorElectron01 natural sciencesIon sourceLinear particle accelerator010305 fluids & plasmasIonlaw.inventionNuclear physicslaw0103 physical sciencesPhysics::Accelerator PhysicsThermal emittanceInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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