Search results for "PLASMA"

showing 10 items of 4043 documents

The power threshold of H-mode access in mixed hydrogen–tritium and pure tritium plasmas at JET with ITER-like wall

2022

The heating power to access the high confinement mode (H-mode), PLH, scales approximately inversely with the isotope mass of the main ion plasma species as found in (protonic) hydrogen, deuterium and tritium plasmas in many fusion facilities over the last decades. In first dedicated L–H transition experiments at the Joint European Torus (JET) tokamak facility with the ITER-like wall (ILW), the power threshold, PLH, was studied systematically in plasmas of pure tritium and hydrogen–tritium mixtures at a magnetic field of 1.8 T and a plasma current of 1.7 MA in order to assess whether this scaling still holds in a metallic wall device. The measured power thresholds, PLH, in Ohmically heated t…

Nuclear and High Energy Physics:Física::Física de fluids [Àrees temàtiques de la UPC]IsòtopsL–H transitionTritium plasmasPaper ; magnetic confinement fusion ; fusion plasmas ; L-H transition ; JET tokamak ; tritium plasmasTritiumCondensed Matter Physicsjet tokamakddc:magnetic confinement fusionJET tokamakPhysics::Plasma PhysicsFusion plasmastritium plasmasPhysics::Space PhysicsMagnetic confinement fusionPhysics::Accelerator Physicsfusion plasmasTokamaksl-h transitionNuclear Fusion
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Dielectron production in proton-proton and proton-lead collisions at √sNN=5.02TeV

2020

The first measurements of dielectron production at midrapidity (|ηe| < 0.8) in proton–proton and proton–lead collisions at √sNN = 5.02 TeV at the LHC are presented. The dielectron cross section is measured with the ALICE detector as a function of the invariant mass mee and the pair transverse momentum pT, ee in the ranges mee < 3.5 GeV/c2 and pT, ee < 8 GeV/c, in both collision systems. In proton–proton collisions, the charm and beauty cross sections are determined at midrapidity from a fit to the data with two different event generators. This complements the existing dielectron measurements performed at √s = 7 and 13 TeV. The slope of the √s dependence of the three measurements is…

Nuclear and High Energy Physics:Kjerne- og elementærpartikkelfysikk: 431 [VDP]ProtonHadronNuclear Theorydielectrondielectron production01 natural sciences7. Clean energyNuclear physicshadron-ion interactionshadron-hadron collisions; dielectron production;Ionic Collisionsdielectron cross sectiondielectron nuclear modification factor0103 physical sciencesInvariant massDielectronCharm (quantum number)Dielectron; hadron-hadron interactions; hadron-ion interactionsPhysics::Atomic PhysicsIonic Collisions; Relativistic Heavy-ion Collisions; Quark-Gluon Plasma010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsPhysicsVDP::Kjerne- og elementærpartikkelfysikk: 431hadron-hadron interactionNuclear matterhadron-hadron collisionsNATURAL SCIENCES. Physics.ALICE LHC proton-lead collisions proton-proton collisionsPRIRODNE ZNANOSTI. Fizika.:Nuclear and elementary particle physics: 431 [VDP]VDP::Nuclear and elementary particle physics: 431dielectron ; LHC ; dielectron cross section ; dielectron nuclear modification factorQuark–gluon plasmaQuark-Gluon PlasmaHigh Energy Physics::ExperimentLHChadron-hadron interactionsRelativistic Heavy-ion Collisions
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A study of on-line gas cell processes at IGISOL

2010

Abstract The laser ion source at the IGISOL facility, Jyvaskyla, has been used to study the effects of the passage of a primary beam through an ion guide via the dynamic time profiles of yttrium and related molecular compounds. The accessibility of a neutral fraction for laser ionization is shown to be restricted to the nozzle region in the presence of a weak plasma. The survival of this neutral fraction cannot be explained by recombination of the buffer gas alone and perhaps indicates a suppression of the transport of ions due to a plasma-generated electric field. The concept of a competition between the processes that create and destroy the ion of interest is used to explain the different…

Nuclear and High Energy PhysicsArgonBuffer gaschemistry.chemical_elementYttriumIon gunIon sourceIonIon beam depositionchemistryPhysics::Plasma PhysicsIonizationAtomic physicsInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Detailed characterization of laboratory magnetized super-critical collisionless shock and of the associated proton energization

2021

Collisionless shocks are ubiquitous in the Universe and are held responsible for the production of nonthermal particles and high-energy radiation. In the absence of particle collisions in the system, theory shows that the interaction of an expanding plasma with a pre-existing electromagnetic structure (as in our case) is able to induce energy dissipation and allow shock formation. Shock formation can alternatively take place when two plasmas interact, through microscopic instabilities inducing electromagnetic fields that are able in turn to mediate energy dissipation and shock formation. Using our platform in which we couple a rapidly expanding plasma induced by high-power lasers (JLF/Titan…

Nuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesmagnetic fieldQC770-798shock waves01 natural sciencesAtomic and Molecular Physics and OpticsPhysics - Plasma Physics010305 fluids & plasmasPlasma Physics (physics.plasm-ph)Settore FIS/05 - Astronomia E AstrofisicaNuclear Energy and Engineering[PHYS.PHYS.PHYS-PLASM-PH]Physics [physics]/Physics [physics]/Plasma Physics [physics.plasm-ph]Nuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesPhysics::Space PhysicsElectrical and Electronic Engineering010306 general physics
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Development of an MeV ion beam lithography system in Jyväskylä

2007

Abstract A lithographic facility for writing patterns with ion beams from cyclotron beams is under development for the Jyvaskyla cyclotron. Instead of focusing and deflecting the beam with electrostatic and magnetic fields a different approach is used. Here a small rectangular beam spot is defined by the shadow of a computer-controlled variable aperture in close proximity to the sample. This allows parallel exposure of rectangular pattern elements of 5–500 μm side with protons up to 6 MeV and heavy ions (20Ne, 85Kr) up to few 100 MeV. Here we present a short overview of the system under construction and development of the aperture design, which is a critical aspect for all ion beam lithogra…

Nuclear and High Energy PhysicsBeam diameterIon beamChemistrybusiness.industryIon beam lithographyFocused ion beamProton beam writingIon beam depositionOpticsPhysics::Plasma PhysicsPhysics::Accelerator PhysicsLaser beam qualityAtomic physicsNuclear ExperimentbusinessInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Broad excitations in a 2+1D overoccupied gluon plasma

2021

Motivated by the initial stages of high-energy heavy-ion collisions, we study excitations of far-from-equilibrium 2+1 dimensional gauge theories using classical-statistical lattice simulations. We evolve field perturbations over a strongly overoccupied background undergoing self-similar evolution. While in 3+1D the excitations are described by hard-thermal loop theory, their structure in 2+1D is nontrivial and nonperturbative. These nonperturbative interactions lead to broad excitation peaks in spectral and statistical correlation functions. Their width is comparable to the frequency of soft excitations, demonstrating the absence of soft quasiparticles in these theories. Our results also su…

Nuclear and High Energy PhysicsCOLLISIONSNuclear TheoryField (physics)FOS: Physical sciencesLattice QCDQC770-798hiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesPerturbative QCDfysikkField theory (psychology)Gauge theory010306 general physicsKINETIC-THEORYUNIVERSAL DYNAMICSPhysics:Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP]MASS SCALENUCLEI010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)kvarkki-gluoniplasmaPerturbative QCDLattice QCDFIELD-THEORY3. Good healthGluonHigh Energy Physics - PhenomenologyQuantum electrodynamicsQuark–gluon plasmaQuasiparticleQuark-Gluon PlasmaGAUGE-THEORIESJournal of High Energy Physics
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Ion traps and their application in spectroscopy

1996

The general behaviour of Paul- and Penning ion traps is briefly described and some emphasis is given to the storage of highly charged ions. In the second part recent examples of laser and microwave spectroscopy on stored ions are given which illustrate the high precision and high sensitivity of these devices. We point out the possible application to laser spectroscopy on highly charged ions.

Nuclear and High Energy PhysicsChemistryCondensed Matter PhysicsLaserAtomic and Molecular Physics and OpticsIonlaw.inventionPhysics::Plasma PhysicslawPhysics::Atomic PhysicsRotational spectroscopyIon trapPhysical and Theoretical ChemistryAtomic physicsSpectroscopyHyperfine Interactions
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Time profiles of ions produced in a hot-cavity resonant ionization laser ion source

2011

Abstract The time profiles of Cu, Sn, and Ni ions extracted from a hot-cavity resonant ionization laser ion source are investigated. The ions are produced in the ion source by three-photon resonant ionization with pulsed Ti:Sapphire lasers. Measurements show that the time spread of these ions generated within laser pulses of about 30 ns duration could be larger than 100 μs when the ions are extracted from the ion source. A one-dimensional ion-transport model using the Monte Carlo method is developed to simulate the time dependence of the ion pulses. The prediction of the model agrees reasonably well with the experimental data. To reproduce the observed ion time profiles, we find it necessar…

Nuclear and High Energy PhysicsChemistryIon gunCharged particleIon sourcelaw.inventionIonIon beam depositionPhysics::Plasma PhysicsReflectronlawIonizationAtomic physicsInstrumentationElectron ionizationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Exciton-created defects and their participation in energy transfer from excitons to Tl ions in KI–Tl crystal

2000

Abstract Luminescence properties (spectra, yields, kinetics) of Tl ions induced by energy transfer from different types of anion excitons were studied and compared with those observed under direct Tl ion excitation by light quanta from A and C absorption bands in KI–Tl crystal at low temperature. The mechanism of energy transfer from excitons to the impurity ions was proposed based on the exciton-created defects participating in the impurity ion excitation.

Nuclear and High Energy PhysicsCondensed Matter::OtherChemistryExcitonCondensed Matter::Mesoscopic Systems and Quantum Hall EffectSpectral lineIonCrystalCondensed Matter::Materials SciencePhysics::Plasma PhysicsImpurityAbsorption (chemistry)Atomic physicsLuminescenceInstrumentationExcitationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Preliminary Thermo-Mechanical Design of the Once Through Steam Generator and Molten Salt Intermediate Heat Exchanger for EU DEMO

2020

The European DEMOnstration power plant (DEMO) is considered to be the nearest-term fusion reactor capable of producing several hundred MWs of net electricity, operating with a closed tritium fuel-cycle (achieving the tritium self-sufficiency), and qualifing technological solutions for a fusion power plant with different breeding blanket (BB) concepts that are under investigation. The BB is a key component for the development of the DEMO plant design and, in particular, of those systems having the responsibility to remove the plasma-generated thermal power and its conversion in the electrical energy. This study deals with the preliminary thermo-mechanical design of the heat exchangers and st…

Nuclear and High Energy PhysicsDEMOnstration power plant (DEMO)Power stationbusiness.industryBoiler (power generation)Thermal power stationFusion powerBlanketCondensed Matter Physics01 natural sciences7. Clean energyGeneralLiterature_MISCELLANEOUS010305 fluids & plasmassteam generatorHeat recovery steam generator0103 physical sciencesHeat exchangerEnvironmental scienceHydraulic machineryProcess engineeringbusinessheat exchangertube sheetBalance of plant (BoP)IEEE Transactions on Plasma Science
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