Search results for " electron emission"

showing 10 items of 22 documents

Untersuchung der Feldelektronenemission und ihrer Temperaturabh�ngigkeit bei Stromst�rken zwischen 10?14 und 10?19 A

1964

The field emission of a tungsten point cathode at very low emission currents was investigated by means of a secondary emission multiplier. The validity of the Fowler-Nordheim equation was experimentally confirmed within the range from 10−8 to 10−19 A. The dependence of the total emission current on temperature and electrical field strength was measured in the transition region between thermionic and field emission. A comparison is drawn with the theory ofMurphy andGood.

Nuclear and High Energy PhysicsMaterials scienceAstrophysics::High Energy Astrophysical Phenomenachemistry.chemical_elementThermionic emissionAstrophysics::Cosmology and Extragalactic AstrophysicsTungstenElectrical field strengthCathodelaw.inventionField electron emissionchemistrylawLow emissionSecondary emissionPhysics::Accelerator PhysicsNuclear fusionAtomic physicsAstrophysics::Galaxy AstrophysicsZeitschrift f�r Physik
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Asymmetric tungsten oxide nanobrushes via oriented attachment and Ostwald ripening

2011

Tungsten oxide nanobrushes were synthesized using a solvothermal approach that lead to self-branching in the presence of citric acid and hexadecylamine as surfactants. Our synthetic approach yielded branched nanorods of tungsten oxide in a single synthetic step. Based on our results, we propose a phenomenological pathway for the formation, branching, and assembly of these tungsten oxide brushes. The formation of tungsten oxide brushes proceeds by thermal decomposition of ammonium tungstate in the presence of citric acid and hexadecylamine. The pale blue powder obtained after solvothermal reaction was analyzed by X-ray diffraction (XRD), transmission electron microscopy (TEM) and high-resolu…

Ostwald ripeningNanostructureMaterials scienceThermal decompositionInorganic chemistryGeneral Chemistryequipment and suppliesCondensed Matter Physicschemistry.chemical_compoundsymbols.namesakeField electron emissionTungstatechemistryTransmission electron microscopysymbolsGeneral Materials ScienceNanorodHigh-resolution transmission electron microscopy
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Synergistic effect between hydrodynamic conditions during Ti anodization and acidic treatment on the photoelectric properties of TiO2 nanotubes

2015

In the present work, the combined influence of controlled hydrodynamic conditions during Ti anodization and the acidic treatment with HClO4 on the photoelectric properties of mixed anatase/rutile TiO2 nanotubes has been studied. Anodized samples were analyzed by means of Field Emission Scanning Electronic Microscopy (FE-SEM), Confocal Raman Microscopy, electrochemical measurements (electrochemical impedance spectroscopy and Mott-Schottky analysis) and photoelectrochemical measurements. It has been observed that the use of hydrodynamic conditions increases the surface area of nanotubes, while acidic treatment enhances their conductivity. Besides, there is a clear synergistic effect between t…

PhotocurrentAnataseAnodizingChemistryHidrodinàmicaAnalytical chemistryConductivityCatalysisINGENIERIA QUIMICADielectric spectroscopyHydrodynamic conditionsElectroquímicaField electron emissionsymbols.namesakeChemical engineeringRutilesymbolsTiO2 nanotubesMott-Schottky analysisElectrochemical impedance spectroscopy (EIS)Physical and Theoretical ChemistryPhotocatalysisRaman spectroscopy
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Field Emission of Electrons Generated by the Near Field of Strongly Coupled Plasmons

2012

Field emission of electrons is generated solely by the ultrastrong near-field of strongly coupled plasmons without the help of a noticeable dc field. Strongly coupled plasmons are excited at Au nanoparticles in subnanometer distance to a Au film by femtosecond laser pulses. Field-emitted electrons from individual nanoparticles are detected by means of photoelectron emission microscopy and spectroscopy. The dependence of total electron yield and kinetic energy on the laser power proves that field emission is the underlying emission process. We derive a dynamic version of the Fowler-Nordheim equation that yields perfect agreement with the experiment.

PhysicsAstrophysics::High Energy Astrophysical PhenomenaPhysics::OpticsGeneral Physics and AstronomyElectronLaserlaw.inventionField electron emissionlawExcited stateFemtosecondLaser power scalingAtomic physicsSpectroscopyPlasmonPhysical Review Letters
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Single-component plasma of photoelectrons

2007

Abstract Ten-nanosecond pulses of photoelectrons liberated by intense UV laser pulses from a thin gold layer are captured into a single-component plasma that is ideally suited to cool antiprotons ( p ¯ ) for antihydrogen ( H ¯ ) production. Up to a billion electrons are accumulated using a series of laser pulses, more than are needed for efficient p ¯ cooling in the large traps now being used for loading p ¯ for H ¯ production. The method is demonstrated within an enclosed vacuum space that is entirely at 4 K, and is thus compatible with the exceptional cryogenic vacuum that is desirable for the long-term storage of antihydrogen. The pitfalls of other electron accumulation methods are entir…

PhysicsNuclear and High Energy PhysicsThermionic emissionPlasmaElectronPhotoelectric effectLaserlaw.inventionField electron emissionlawAntimatterPhysics::Atomic PhysicsAtomic physicsAntihydrogenPhysics Letters B
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Ferromagnetism at the summit: A perspective on: “Spin polarized field emission from Fe and co-coated W tips” by Y.R. Niu and M.S. Altman

2010

PhysicsSurface (mathematics)geographyField electron emissionSummitgeography.geographical_feature_categoryPerspective (geometry)Condensed matter physicsMaterials ChemistrySurfaces and InterfacesCondensed Matter PhysicsSpin (physics)Surfaces Coatings and FilmsSurface Science
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Valence bands of poly(methylmethacrylate) and photoion emission in vacuum ultraviolet region

1992

Photoion and photoelectron yields were measured for poly(methylmethacrylate) in the photon energy region of 8–40 eV using synchrotron radiation. Further, the valence‐band structure was investigated with ultraviolet photoelectron spectra and valence effective Hamiltonian calculations. A significant difference was observed between the photon energy dependencies of photoion and photoelectron yields. The threshold energy for photoion emission was found to be 10.5 eV, while that for photoelectron emission was 8.5 eV, indicating holes created near the valence‐band top do not contribute to the ion emission. At the higher‐energy region, the ion emission efficiency was found to be enhanced in the ph…

PmmaValence BandsAstrophysics::High Energy Astrophysical PhenomenaGeneral Physics and AstronomySynchrotron radiationPhotoelectron photoion coincidence spectroscopyAstrophysics::Cosmology and Extragalactic AstrophysicsPhoton energymedicine.disease_causeSpectral lineX-ray photoelectron spectroscopyEv Range 10−100:FÍSICA [UNESCO]medicinePmma ; Ion Emission ; Electron Emission ; Photoelectron Spectroscopy ; Ev Range 10−100 ; Valence Bands ; Band StructurePhysics::Atomic and Molecular ClustersIon EmissionPhysics::Atomic PhysicsElectron EmissionBand StructureAstrophysics::Galaxy AstrophysicsValence (chemistry)ChemistryPhotoelectron SpectroscopyUNESCO::FÍSICAThreshold energyAtomic physicsUltraviolet
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The positioning system of the ANTARES Neutrino Telescope

2012

The ANTARES neutrino telescope, located 40km off the coast of Toulon in the Mediterranean Sea at a mooring depth of about 2475m, consists of twelve detection lines equipped typically with 25 storeys. Every storey carries three optical modules that detect Cherenkov light induced by charged secondary particles (typically muons) coming from neutrino interactions. As these lines are flexible structures fixed to the sea bed and held taut by a buoy, sea currents cause the lines to move and the storeys to rotate. The knowledge of the position of the optical modules with a precision better than 10cm is essential for a good reconstruction of particle tracks. In this paper the ANTARES positioning sys…

Positioning systemDetector control systems (detector and experiment monitoring and slow-control systems architecture hardware algorithms databases)Detector modelling and simulations II (electric fieldsDetector alignment and calibration methods (lasers sources particle-beams)01 natural sciencesTiming detectorshardwareDetector alignment and calibration methods010303 astronomy & astrophysicsInstrumentationDETECTOR ALIGMENTMathematical PhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)PhysicsSOUND[SDU.ASTR]Sciences of the Universe [physics]/Astrophysics [astro-ph]Orientation (computer vision)[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]DetectorAstrophysics::Instrumentation and Methods for AstrophysicsTriangulation (computer vision)particle-beams)GeodesyDETECTOR CONTROL SYSTEMDetector modelling and simulations II (electric fields charge transport multiplication and induction pulse formation electron emission etc)Física nuclearNeutrinoAstrophysics - Instrumentation and Methods for AstrophysicsAstrophysics - High Energy Astrophysical Phenomenadatabases)sources[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]pulse formationarchitecture[PHYS.ASTR.IM]Physics [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]Astrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesddc:500.2DETECTOR MODELLING AND SIMULATIONSDetector modelling and simulations IIalgorithmsPhysics::Geophysics0103 physical sciences14. Life underwaterInstrumentation and Methods for Astrophysics (astro-ph.IM)Cherenkov radiationetc)multiplication and inductionBuoyDetector control systems010308 nuclear & particles physicsDetector control systems (detector and experiment monitoring and slow-control systemsMooringcharge transport[SDU.ASTR.IM]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]Detector alignment and calibration methods (laserselectron emissionFISICA APLICADAdetector modelling and simulations ii (electric fields; antares neutrino telescope; multiplication and induction; charge transport; pulse formation; electron emission; etc); hardware; architecture; timing detectors; detector control systems (detector and experiment monitoring and slow-control systems; algorithms; databases); sources; detector alignment; calibration.; acoustic positioning; detector alignment and calibration methods (lasers; particle-beams)
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Investigation of a Ge nanoparticle film by means of electron stimulated photon emission spectroscopy

2014

Abstract Electron stimulated photon emission spectroscopy was used for the study of the electronic structure of Ge nanoparticles. A nanoparticle film was prepared by thermal deposition on a quartz substrate. Photon emission was stimulated by electron bombardment at energies of several hundred electron volts. Electron field emission from a W-tip was used at tip voltage U t  = 100–600 eV. A spectrometer in combination with a liquid nitrogen cooled charge-coupled device (CCD) camera was used for light detection. Light emission spectra were measured in the energy range 1.18–4.2 eV. They are characterized by features at ∼1.6 and ∼3.1 eV. A comparison with light emission spectra obtained with ano…

RadiationMaterials scienceAstrophysics::Cosmology and Extragalactic AstrophysicsElectronLiquid nitrogenCondensed Matter PhysicsAtomic and Molecular Physics and OpticsSpectral lineElectronic Optical and Magnetic MaterialsField electron emissionLight emissionEmission spectrumPhysical and Theoretical ChemistryAtomic physicsSpectroscopySpectroscopyExcitationJournal of Electron Spectroscopy and Related Phenomena
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Electron Emission of Pt: Experimental Study and Comparison With Models in the Multipactor Energy Range

2016

Experimental data of secondary emission yield (SEY) and electron emission spectra of Pt under electron irradiation for normal incidence and primary energies lower than 1 keV are presented. Several relevant magnitudes, as total SEY, elastic backscattering probability, secondary emission spectrum, and backscattering coefficient, are given for different primary energies. These magnitudes are compared with theoretical or semiempirical formulas commonly used in the related literature.

Secondary electron emissionBackscatterAstrophysics::High Energy Astrophysical PhenomenaCleaningElectronSecondary emission yield (SEY01 natural sciencesElectrostatic measurements010305 fluids & plasmasBackscattering coefficientBackscatterEnergy measurementElectron emission0103 physical sciencesElectron beam effectsTEORIA DE LA SEÑAL Y COMUNICACIONESElectron beam processingEmission spectrumElectrical and Electronic EngineeringElastic backscattering probabilityElectron emission spectraMultipactor energy rangePlatinum010302 applied physicsRange (particle radiation)ChemistrySecondary emission yield (SEY)Secondary emission spectrum (SES)PtElectron irradiationCurrent measurementElectronic Optical and Magnetic MaterialsElectron backscatteringSecondary emission yieldSecondary emissionYield (chemistry)Backscattered electronsDistortion measurementAtomic physicsEnergy (signal processing)Multipactor
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