Search results for "HD"

showing 10 items of 4547 documents

A study of the optical effect of plasma sheath in a negative ion source using IBSIMU code

2020

A plasma sheath inside an ion source has a strong focusing effect on the formation of an ion beam from the plasma. Properties of the beam depend on the shape and location of the plasma sheath inside the source. The most accessible experimental data dependent on the plasma sheath are the beam phase space distribution. Variation of beam emittance is a reflection of the properties of the plasma sheath, with minimum emittance for the optimal shape of the plasma sheath. The location and shape of the plasma sheath are governed by complex physics and can be understood by simulations using plasma models in particle tracking codes like IBSimu. In the current study, a model of the D-Pace’s TRIUMF lic…

010302 applied physicsDebye sheathMaterials scienceIon beamPlasmahiukkaskiihdyttimetplasmafysiikka01 natural sciencesIon sourcenegative ion source010305 fluids & plasmassymbols.namesakeplasma sheathPhysics::Plasma Physics0103 physical sciencesPhysics::Space PhysicssymbolsPhysics::Accelerator PhysicsThermal emittanceStrong focusingBeam emittanceAtomic physicsInstrumentationBeam (structure)
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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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Mechanisms of Electron-Induced Single-Event Upsets in Medical and Experimental Linacs

2018

In this paper, we perform an in-depth analysis of the single-event effects observed during testing at medical electron linacs and an experimental high-energy electron linac. For electron irradiations, the medical linacs are most commonly used due to their availability and flexibility. Whereas previous efforts were made to characterize the cross sections at higher energies, where the nuclear interaction cross section is higher, the focus of this paper is on the complete overview of relevant electron energies. Irradiations at an electron linac were made with two different devices, with a large difference in feature size. The irradiations at an experimental linac were performed with varying en…

010302 applied physicsNuclear and High Energy PhysicsMaterials scienceta114010308 nuclear & particles physicselectronsElectron linacElectronhiukkaskiihdyttimetelektronitparticle accelerators01 natural sciencesLinear particle acceleratorNuclear physicsNuclear interactionradiation physicsCross section (physics)säteilyfysiikkaNuclear Energy and Engineering0103 physical sciencesElectrical and Electronic EngineeringEvent (particle physics)IEEE Transactions on Nuclear Science
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Measurements of the energy distribution of electrons lost from the minimum B-field -- the effect of instabilities and two-frequency heating

2020

Further progress in the development of ECR ion sources (ECRIS) requires deeper understanding of the underlying physics. One of the topics that remains obscure, though being crucial for the performance of the ECRIS, is the electron energy distribution (EED). A well-developed technique of measuring the EED of electrons escaping axially from the magnetically confined plasma of an ECRIS was used for the study of EED in unstable mode of plasma confinement, i.e. in the presence of kinetic instabilities. The experimental data were recorded for pulsed and CW discharges with a room-temperature 14 GHz ECRIS at the JYFL accelerator laboratory. The measurements were focused on observing differences bet…

010302 applied physicsPhysicsResonanceFOS: Physical sciencesPlasmaElectronhiukkaskiihdyttimetplasmafysiikka7. Clean energy01 natural sciencesPhysics - Plasma PhysicsElectron cyclotron resonanceIon source010305 fluids & plasmasMagnetic fieldIonPlasma Physics (physics.plasm-ph)Magnetic trap0103 physical sciencesAtomic physicsInstrumentation
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Lead evaporation instabilities and failure mechanisms of the micro oven at the GTS-LHC ECR ion source at CERN

2020

The GTS-LHC ECR ion source (named after the Grenoble Test Source and the Large Hadron Collider) at CERN provides heavy ion beams for the chain of accelerators from Linac3 up to the LHC for high energy collision experiments and to the Super Proton Synchrotron for fixed target experiments. During the standard operation, the oven technique is used to evaporate lead into the source plasma to produce multiple charged lead ion beams. Intensity and stability are key parameters for the beam, and the operational experience is that some of the source instabilities can be linked to the oven performance. Over long operation periods of several weeks, the evaporation is not stable which makes the tuning …

010302 applied physicsRange (particle radiation)Large Hadron ColliderMaterials scienceionitNuclear engineeringEvaporationPlasmahiukkaskiihdyttimetplasmafysiikka01 natural sciencesSuper Proton SynchrotronIon source010305 fluids & plasmasIonComputer Science::OtherPhysics::Popular Physics0103 physical scienceslyijyInstrumentationBeam (structure)
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The role of radio frequency scattering in high-energy electron losses from minimum-B ECR ion source

2021

Abstract The measurement of the axially lost electron energy distribution escaping from a minimum-B electron cyclotron resonance ion source in the range of 4–800 keV is reported. The experiments have revealed the existence of a hump at 150–300 keV energy, containing up to 15% of the lost electrons and carrying up to 30% of the measured energy losses. The mean energy of the hump is independent of the microwave power, frequency and neutral gas pressure but increases with the magnetic field strength, most importantly with the value of the minimum-B field. Experiments in pulsed operation mode have indicated the presence of the hump only when microwave power is applied, confirming that the origi…

010302 applied physics[PHYS]Physics [physics]High energyMaterials scienceScatteringAstrophysics::High Energy Astrophysical Phenomena[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]scatteringElectronhiukkaskiihdyttimetCondensed Matter Physicselektronit01 natural sciences7. Clean energyIon source010305 fluids & plasmasNuclear Energy and Engineering0103 physical sciencessirontaRadio frequencyAtomic physics
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The biased disc of an electron cyclotron resonance ion source as a probe of instability-induced electron and ion losses

2019

International audience; Electron Cyclotron Resonance Ion Source (ECRIS) plasmas are prone to kinetic instabilities resulting in loss of electron and ion confinement. It is demonstrated that the biased disk of an ECRIS can be used as a probe to quantify such instability-induced electron and ion losses occurring in less than 10 µs. The qualitative interpretation of the data is supported by the measurement of the energy spread of the extracted ion beams implying a transient plasma potential >1.5 kV during the instability. A parametric study of the electron losses combined with electron tracking simulations allows for estimating the fraction of electrons expelled in each instability event to be…

010302 applied physics[PHYS]Physics [physics]Materials sciencesyklotronit[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]ElectronPlasmahiukkaskiihdyttimetKinetic energyplasmafysiikka01 natural sciencesInstabilityElectron cyclotron resonanceIon source010305 fluids & plasmasIonPhysics::Plasma Physics0103 physical sciencesTransient (oscillation)Atomic physicsInstrumentation
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Catalytic epoxidation using dioxidomolybdenum(VI) complexes with tridentate aminoalcohol phenol ligands

2019

Reaction of the tridentate aminoalcohol phenol ligands 2,4-di-tert-butyl-6-(((2 hydroxyethyl)(methyl)amino)methyl)phenol (H2L1) and 2,4-di-tert-butyl-6-(((1-hydroxybutan-2-yl)amino)methyl)phenol (H2L2) with [MoO2(acac)2] in methanol solutions resulted in the formation of [MoO2(L1)(MeOH)] (1) and [MoO2(L2)(MeOH)] (3), respectively. In contrast, the analogous reactions in acetonitrile afforded the dinuclear complexes [Mo2O2(μ-O)2(L1)2] (2) and [Mo2O2(μ-O)2(L2)2] (4). The corresponding reactions with the potentially tetradentate ligand 3-((3,5-di-tert-butyl-2-hydroxybenzyl)(methyl)amino)propane-1,2-diol (H3L3) led to the formation of the mononuclear complex [MoO2(L3)(MeOH)] (5) in methanol whi…

010402 general chemistry01 natural sciencesMedicinal chemistryCatalysisInorganic Chemistrychemistry.chemical_compoundkatalyytitepoxidationMaterials ChemistryPhenolMoietyPhysical and Theoretical ChemistryHydrogen peroxideAcetonitrileta116010405 organic chemistryLigandmolybdenum complexSubstrate (chemistry)kompleksiyhdisteettrinuclear structure0104 chemical scienceschemistrytridentate ligandMethanolmolybdeeniInorganica Chimica Acta
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Iminium Catalysis (n → π*)

2016

010402 general chemistry01 natural sciencesMedicinal chemistrycatalystsCatalysiskatalyytitepoxidationPi interactioncatalyst turnovertyppiyhdisteetDiels-Alder reactionFriedel–Crafts reactionta116cycloadditionDiels–Alder reactioncatalysis010405 organic chemistryChemistrychiral anionsIminiumnitrogen compoundsCycloaddition0104 chemical sciencesaxially chiral catalystskatalyysicocatalyst
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Interactions of a Diplumbyne with Dinuclear Transition Metal Carbonyls to Afford Metalloplumbylenes

2020

The metathesis reactions of the diplumbyne AriPr6PbPbAriPr6 (AriPr6 = −C6H3–2,6-(C6H2–2,4,6-iPr3)2) with the dinuclear metal carbonyls Mn2(CO)10, Fe2(CO)9, and Co2(CO)8 under mild conditions afforded the complexes Mn(CO)5(PbAriPr6) (1), Fe(CO)4(PbAriPr6)2 (2), and Co4(CO)9(PbAriPr6)2 (3), respectively. Complexes 1–3 were structurally characterized by single-crystal X-ray diffraction and spectroscopically characterized by 1H, 13C{1H}, 59Co{1H}, and 207Pb{1H} NMR; UV–vis; and IR methods. They are rare examples of species formed by the direct reaction of a group 14 dimetallyne with transition metal carbonyls. Complexes 1 and 2 feature Mn–Pb or Fe–Pb single bonds, whereas in 3 a Co–Pb cluster i…

010405 organic chemistryChemistryOrganic ChemistrycarbonylsmetalsMetal carbonylkompleksiyhdisteetorganometalliyhdisteet010402 general chemistry01 natural sciencescobalttransition metals0104 chemical sciencesInorganic ChemistryTransition metalPolymer chemistrySalt metathesis reactionPhysical and Theoretical Chemistrykarbonyylitnuclear magnetic resonance spectroscopy
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