Search results for "plasma physics"

showing 10 items of 393 documents

Measurement of the W boson mass

1996

The W boson mass is measured using proton-proton collision data at root s = 13 TeV corresponding to an integrated luminosity of 1.7fb(-1) recorded during 2016 by the LHCb experiment. With a simultaneous fit of the muon q/p(T) distribution of a sample of W ->mu y decays and the phi* distribution of a sample of Z -> mu mu decays the W boson mass is determined to be

13000 GeV-cmsTevatronparton: distribution functionQC770-798W: leptonic decay7. Clean energy01 natural sciencesLuminosityPhysics Particles & FieldsSubatomär fysikHadron-Hadron scattering (experiments)scattering [p p]Electroweak interactionNuclear Experimentparticle identification [muon]Settore FIS/01PhilosophyPhysicsCoupling (probability)CERN LHC CollHadron colliderPhysical SciencesTransverse masscolliding beams [p p]distribution function [parton]Collider Detector at FermilabParticles and fieldCOLLISIONSp p: scatteringCERN PBARP COLLIDERAstrophysics::High Energy Astrophysical PhenomenaW: mass: measuredStandard ModelNuclear physicsddc:530010306 general physics0206 Quantum PhysicsMuonScience & Technology010308 nuclear & particles physicsWeinberg angleHEPFERMILAB TEVATRONElectroweak interaction Hadron-Hadron scattering (experiments) QCD For- ward physicsCDFp p: colliding beamsPhysics::Instrumentation and DetectorsElectron–positron annihilation= 1.8 TEVGeneral Physics and Astronomy= 1.8 TEV; PBARP COLLISIONS; DECAYVector bosonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Computer Science::Systems and ControlSubatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PhysicFermilabBosonPhysics0105 Mathematical PhysicsStatistics::ApplicationsSettore FIS/01 - Fisica Sperimentalestatistical [error]Nuclear & Particles PhysicsCENTRAL TRACKING CHAMBERerror: statisticalCENTRAL ELECTROMAGNETIC CALORIMETERTransverse momentum0202 Atomic Molecular Nuclear Particle and Plasma PhysicsLHCmass: measured [W]Particle Physics - ExperimentStatistics::TheoryParticle physicsNuclear and High Energy Physicselectroweak interaction: precision measurementRegular Article - Experimental PhysicsTRANSVERSE ENERGYFOS: Physical sciencesmuon: particle identification530Particle decayPBARP COLLISIONSNuclear and particle physics. Atomic energy. Radioactivityprecision measurement [electroweak interaction]0103 physical sciencesForward physicVECTOR BOSONElectroweak interaction Hadron-Hadron scattering (experiments) QCD Forward physicsCERN PBARP COLLIDER; CENTRAL ELECTROMAGNETIC CALORIMETER; CENTRAL TRACKING CHAMBER; = 1.8 TEV; PARTON DISTRIBUTIONS; FERMILAB TEVATRON; VECTOR BOSON; TRANSVERSE ENERGY; CDF; COLLISIONShep-exHigh Energy Physics::PhenomenologyLHC-BQCDleptonic decay [W]LHCbPARTON DISTRIBUTIONSMass spectrumForward physicsPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentDECAYHumanitiesexperimental results
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Large numbers of cold positronium atoms created in laser-selected Rydberg states using resonant charge exchange

2016

Lasers are used to control the production of highly excited positronium atoms (Ps*). The laser light excites Cs atoms to Rydberg states that have a large cross section for resonant charge-exchange collisions with cold trapped positrons. For each trial with 30 million trapped positrons, more than 700 000 of the created Ps* have trajectories near the axis of the apparatus, and are detected using Stark ionization. This number of Ps* is 500 times higher than realized in an earlier proof-of-principle demonstration (2004 Phys. Lett. B 597 257). A second charge exchange of these near-axis Ps* with trapped antiprotons could be used to produce cold antihydrogen, and this antihydrogen production is e…

ANTIHYDROGENGeneral PhysicsAntiparticlepositronium0205 Optical Physics0307 Theoretical And Computational ChemistryPLASMASCONFINEMENTPhysics Atomic Molecular & Chemical01 natural sciences010305 fluids & plasmasPositroniumsymbols.namesake0202 Atomic Molecular Nuclear Particle And Plasma PhysicsIonization0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic Physics010306 general physicsAntihydrogenpositronsPhysicsCondensed Matter::Quantum GasesScience & TechnologyPhysicsOpticsRydberg statesCondensed Matter PhysicsAtomic and Molecular Physics and Opticscharge-exchangeExcited stateAntimatterPhysical SciencesRydberg formulasymbolsAtomic physicsLepton
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Design of a 10 GHz minimum-B quadrupole permanent magnet electron cyclotron resonance ion source

2020

This paper presents a simulation study of a permanent magnet electron cyclotron resonance ion source (ECRIS) with a minimum-B quadrupole magnetic field topology. The magnetic field is made to conform to conventional ECRIS with $B_\textrm{min}/B_\textrm{ECR}$ of 0.67 and a last closed magnetic isosurface of 1.86$B_\textrm{ECR}$ at 10 GHz. The distribution of magnetic field gradients parallel to the field, affecting the electron heating efficiency, cover a range from 0 to 13 T/m, being similar to conventional ECRIS. Therefore it is expected that the novel ion source produces warm electrons and high charge state ions in significant number. Single electron tracking simulations are used to estim…

Accelerator Physics (physics.acc-ph)PhysicsIon beam analysis010308 nuclear & particles physicsFOS: Physical sciencesElectron01 natural sciences7. Clean energyIon sourceElectron cyclotron resonance030218 nuclear medicine & medical imagingIon03 medical and health sciences0302 clinical medicineBeamlinePhysics::Plasma PhysicsMagnet0103 physical sciencesQuadrupolePhysics::Accelerator PhysicsPhysics - Accelerator PhysicsAtomic physicsInstrumentationMathematical PhysicsJournal of Instrumentation
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The modelling of the cathode sheath of an electrical arc in vacuum

2003

This paper presents a simple model of the fragment in the cathode electrical arc root taking into account the physical phenomena occuring on the cathode surface and the sheath. The goal is the obtainment of characteristics values of the heat flux, the electrons, and atoms density in the sheath. Computation is carried out on a one-dimensional model with a coupling between the equation obtained in the sheath and an enthalpy model of the cathode to describe the temperature evolution. In the modelling, we introduce a friction zone above the sheath edge to characterize the heavy particle interactions. Numerical simulation shows that the ionic friction phenomenon deriving from ion–atom collision …

Acoustics and UltrasonicsvacuumIonic bondingarc rootheat fluxElectroncathode sheatharc01 natural sciences010305 fluids & plasmaslaw.inventionElectric arcCross section (physics)lawPhysics::Plasma Physics[PHYS.PHYS.PHYS-PLASM-PH]Physics [physics]/Physics [physics]/Plasma Physics [physics.plasm-ph]0103 physical sciences010306 general physicsCouplingComputer simulationChemistryMechanics[ PHYS.PHYS.PHYS-PLASM-PH ] Physics [physics]/Physics [physics]/Plasma Physics [physics.plasm-ph]Condensed Matter PhysicsCathodeSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsHeat flux
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Gain lifetime measurement of a Ni-like Ag soft X-ray laser

2012

International audience; Experimental results of a two-stage Ni-like Ag soft X-ray laser operated in a seed-amplifier configuration are presented. Both targets were pumped applying the double-pulse grazing incidence technique with intrinsic travelling wave excitation. The injection of the seed X-ray laser into the amplifier target was realized by a spherical mirror. The results show amplification of the seed X-ray laser and allow for a direct measurement of the gain lifetime. The experimental configuration is suitable for providing valuable input for computational simulations. (C) 2012 Optical Society of America

Amplified spontaneous emissionCODEPhysics::OpticsCurved mirrorBEAM01 natural scienceslaw.inventionCOHERENT010309 opticsLaser linewidthOptics[PHYS.PHYS.PHYS-PLASM-PH]Physics [physics]/Physics [physics]/Plasma Physics [physics.plasm-ph]law0103 physical sciencesSpontaneous emission010306 general physicsPhysics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryAmplifierLaserAtomic and Molecular Physics and OpticsTemporal resolutionOptoelectronicsbusinessExcitationOptics Express
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Electrochemical pH Control at Gold Nanowires

2018

In this work, interdigitated arrays of nanowire electrodes are used with one array acting as the working electrode while the other is used to generate the required protons. Finite element simulations of the pH control electrodes were performed to provide insight on the generation and subsequent diffusion of protons. This informed the inter-tine spacing of the electrodes used.. This electrochemical pH control method was then used to enable the detection of analytes of interest.

AnalyteWorking electrodeMaterials sciencePhysics::Instrumentation and Detectorsbusiness.industry020209 energy010401 analytical chemistryPh controlNanowire02 engineering and technologypH control gold nanowire heavy metal in situ simulationElectrochemistry01 natural sciencesFinite element method0104 chemical sciencesSettore ING-IND/23 - Chimica Fisica ApplicataPhysics::Plasma PhysicsElectrode0202 electrical engineering electronic engineering information engineeringOptoelectronicsDiffusion (business)business2018 IEEE 18th International Conference on Nanotechnology (IEEE-NANO)
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Diagnostics of Helium-Argon Arc Discharge Plasma Based on Spectral Line Shape Measurements

1999

Electron densities and ion (gas) temperatures on the axis of an arc discharge plasma, produced at atmospheric pressure in a gas mixture of 95% helium and 5% argon, are determined at two arc currents. The evaluation of both main plasma parameters is based on line shape measurements, the ion temperature on the Doppler broadening of selected ArII lines, while the electron density on the Stark broadening of the hydrogen Hp line which appear in the spectrum due to hydrogen traces in the applied gases. The significance of reliable plasma diagnostics for determination of atomic structure data is discussed.

ArgonMaterials sciencePlasma parametersGeneral Physics and Astronomychemistry.chemical_elementPlasmaSpectral line shapeElectric arcchemistryPhysics::Plasma PhysicsPlasma diagnosticsPhysics::Atomic PhysicsAtomic physicsHeliumDoppler broadeningActa Physica Polonica A
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Access to Gamma-ray Spectroscopy of Neutron-Rich sdfp Shell Nuclei

2000

γ-rays in neutron-rich sdfp shell nuclei, produced in deep-inelastic processes during collisions of 37Cl and 40Ar ions on 208Pb and of 48Ca ions on 48Ca, have been studied using large Ge multidetector arrays. Candidates for new yrast states in heavy argon and sulfur isotopes have been identified.

ArgonMaterials scienceYrastNuclear TheoryShell (structure)chemistry.chemical_elementCoulomb excitationIsotopes of sulfurIonchemistryPhysics::Plasma PhysicsNeutronGamma spectroscopyAtomic physicsNuclear Experiment
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Superficial defects induced by argon and oxygen bombardments on (110) TiO2 surfaces

1998

Abstract Compositional and chemical changes of titanium dioxide monocrystalline surfaces induced by bombardment with 4 keV argon and oxygen ions have been studied by AES, XPS and AFM. Argon ion bombardment induced strong changes in the composition and chemical state of the surface: loss of oxygen due to preferential sputtering occurred, and, related to this, Ti4+ species were reduced to Ti3+ and Ti2+. During oxygen bombardment, competition between preferential sputtering of oxygen ions of the oxide surface and oxygen implantation was observed. This phenomenon was found to be strongly dependent upon the incidence angle of the oxygen ions. Moreover, an oxygen bombardment with normal incidence…

ArgonOxidechemistry.chemical_elementSurfaces and InterfacesCondensed Matter PhysicsPhotochemistryOxygenSurfaces Coatings and FilmsMonocrystalline siliconCondensed Matter::Materials ScienceChemical statechemistry.chemical_compoundchemistryX-ray photoelectron spectroscopyPhysics::Plasma PhysicsSputteringTitanium dioxideMaterials Chemistrysense organsPhysics::Chemical PhysicsNuclear chemistrySurface Science
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Modeling And Measurements Of The Arc Plasma In A Mixture Of Gases

2006

Radial distributions of Ar mass fractions and temperatures in plasmas produced in a wall-stabilized arc have been calculated. Modeling have been performed for many different mixtures of Ar+N2 and three different arc currents. The obtained results show that the radial distributions of Ar mass fractions strongly depend on the chemical composition of the plasma. In plasmas containing large amount of Ar the distributions have local minima at the arc axis (in high temperature plasma regions), whereas in plasmas consisting mainly of nitrogen the distributions reveal maxima on the discharge axis. Those features seem to be connected with the dissociation of the nitrogen.

ArgonPlasma cleaningchemistry.chemical_elementPlasmaDissociation (chemistry)chemistryPhysics::Plasma PhysicsPhysics::Space PhysicsAstrophysics::Solar and Stellar AstrophysicsPlasma diagnosticsElectric currentAtomic physicsChemical compositionMass fractionAIP Conference Proceedings
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