Search results for "DETECT"

showing 10 items of 5902 documents

Formation of dislocations and hardening of LiF under high-dose irradiation with 5–21 MeV 12C ions

2017

R. Zabels, I. Manika, J. Maniks, and R.Grants acknowledge the national project IMIS2, and A. Dauletbekova, M. Baizhumanov, and M. Zdorovets the Ministry of Education and Science of the Republic of Kazakhstan for the financial support.

010302 applied physicsEnergy lossMaterials sciencePhysics::Instrumentation and DetectorsAtomic force microscopyAstrophysics::High Energy Astrophysical PhenomenaPhysics::Medical Physicsmacromolecular substances02 engineering and technologyGeneral ChemistryNanoindentation021001 nanoscience & nanotechnology01 natural sciencesMolecular physicsIsotropic etchingElastic collisionIonPhysics::Plasma Physics0103 physical sciences:NATURAL SCIENCES:Physics [Research Subject Categories]Hardening (metallurgy)General Materials ScienceIrradiationAtomic physics0210 nano-technologyApplied Physics A
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Systematic and statistical uncertainties of the hilbert-transform based high-precision FID frequency extraction method.

2021

Abstract Pulsed nuclear magnetic resonance (NMR) is widely used in high-precision magnetic field measurements. The absolute value of the magnetic field is determined from the precession frequency of nuclear magnetic moments. The Hilbert transform is one of the methods that have been used to extract the phase function from the observed free induction decay (FID) signal and then its frequency. In this paper, a detailed implementation of a Hilbert-transform based FID frequency extraction method is described, and it is briefly compared with other commonly used frequency extraction methods. How artifacts and noise level in the FID signal affect the extracted phase function are derived analytical…

010302 applied physicsLarmor precessionPhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and Detectors010308 nuclear & particles physicsNoise (signal processing)Covariance matrixMathematical analysisBiophysicsFOS: Physical sciencesAbsolute valueInstrumentation and Detectors (physics.ins-det)Condensed Matter Physics01 natural sciencesBiochemistrySignalFree induction decaysymbols.namesake0103 physical sciencessymbolsHilbert transformUncertainty analysisJournal of magnetic resonance (San Diego, Calif. : 1997)
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Photoelectron Emission from Metal Surfaces Induced by VUV-emission of Filament Driven Hydrogen Arc Discharge Plasma

2015

Photoelectron emission measurements have been performed using a filament-driven multi-cusp arc discharge volume production H^- ion source (LIISA). It has been found that photoelectron currents obtained with Al, Cu, Mo, Ta and stainless steel (SAE 304) are on the same order of magnitude. The photoelectron currents depend linearly on the discharge power. It is shown experimentally that photoelectron emission is significant only in the short wavelength range of hydrogen spectrum due to the energy dependence of the quantum efficiency. It is estimated from the measured data that the maximum photoelectron flux from plasma chamber walls is on the order of 1 A per kW of discharge power.

010302 applied physicsMaterials scienceHydrogenPhysics::Instrumentation and DetectorsFluxchemistry.chemical_elementFOS: Physical sciencesPlasma01 natural sciences7. Clean energyPhysics - Plasma PhysicsIon source010305 fluids & plasmasElectric arcPlasma Physics (physics.plasm-ph)chemistryPhysics::Plasma Physics0103 physical sciencesPhysics::Atomic and Molecular ClustersQuantum efficiencyPhysics::Atomic PhysicsAtomic physicsHydrogen spectral seriesOrder of magnitude
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Optimization of a laser ion source for $^{163}$Ho isotope separation

2019

To measure the mass of the electron neutrino, the “Electron Capture in Holmium-163” (ECHo) collaboration aims at calorimetrically measuring the spectrum following electron capture in 163Ho. The success of the ECHo experiment depends critically on the radiochemical purity of the 163Ho sample, which is ion-implanted into the calorimeters. For this, a 30 kV high transmission magnetic mass separator equipped with a resonance ionization laser ion source is used. To meet the ECHo requirements, the ion source unit was optimized with respect to its thermal characteristics and material composition by means of the finite element method thermal-electric calculations and chemical equilibrium simulation…

010302 applied physicsMaterials sciencePhysics - Instrumentation and DetectorsAtomic Physics (physics.atom-ph)Electron captureFOS: Physical sciencesThermal ionizationInstrumentation and Detectors (physics.ins-det)Laser01 natural sciencesIon source010305 fluids & plasmasIsotope separationlaw.inventionPhysics - Atomic PhysicslawIonization0103 physical sciencesThermalAtomic physicsChemical equilibriumInstrumentation
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Choice of the detectors for light impurities plasma studies at W7-X using ‘CO Monitor’ system

2019

Abstarct The ‘CO Monitor’ is a new spectrometer system dedicated for the continuous measurements of line intensities of carbon, oxygen, boron and nitrogen at the fusion plasma experiment Wendelstein 7-X (W7-X). Its main purpose is to deliver constant information about indicated elements with high time resolution (better than 1 ms), but low spatial resolution since the line shapes are not going to be investigated. The system consists of four independent channels, each equipped with dispersive element dedicated for measurement of selected line of interest. In order to perform the highest efficiency of the ‘CO Monitor’ system, it is essential to choose the proper detector type for this task. T…

010302 applied physicsMaterials scienceSpectrometerbusiness.industryMechanical EngineeringDetectorPhase (waves)PlasmaElectronXUVDetectorsWendelstein 7-XStellarator01 natural sciencesLine (electrical engineering)010305 fluids & plasmasOpticsNuclear Energy and Engineering0103 physical sciencesGeneral Materials SciencebusinessSensitivity (electronics)Image resolutionCivil and Structural EngineeringFusion Engineering and Design
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Evaluation and Comparison of Novel Precursors for Atomic Layer Deposition of Nb2O5 Thin Films

2012

Atomic layer deposition (ALD) of Nb2O5 thin films was studied using three novel precursors, namely, tBuN═Nb(NEt2)3, tBuN═Nb(NMeEt)3, and tamylN═Nb(OtBu)3. These precursors are liquid at room temperature, present good volatility, and are reactive toward both water and ozone as the oxygen sources. The deposition temperature was varied from 150 to 375 °C. ALD-type saturative growth modes were confirmed at 275 °C for tBuN═Nb(NEt2)3 and tBuN═Nb(NMeEt)3 together with both oxygen sources. Constant growth rate was observed between a temperature regions of 150 and 325 °C. By contrast, amylN═Nb(OtBu)3 exhibited limited thermal stability and thus a saturative growth mode was not achieved. All films we…

010302 applied physicsMaterials scienceta114General Chemical EngineeringAnalytical chemistrychemistry.chemical_element02 engineering and technologyGeneral Chemistry021001 nanoscience & nanotechnology01 natural sciencesOxygenAmorphous solidElastic recoil detectionAtomic layer depositionchemistry0103 physical sciencesMaterials ChemistryThermal stabilityThin film0210 nano-technologyta116Volatility (chemistry)High-κ dielectricChemistry of Materials
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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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Atomic Layer Deposition of LiF Thin Films from Lithd, Mg(thd)2, and TiF4 Precursors

2013

Lithium fluoride is an interesting material because of its low refractive index and large band gap. Previously LiF thin films have been deposited mostly by physical methods. In this study a new way of depositing thin films of LiF using atomic layer deposition (ALD) is presented. Mg(thd)2, TiF4 and Lithd were used as precursors, and they produced crystalline LiF at a temperature range of 300–350 °C. The films were studied by UV–vis spectrometry, field emission scanning electron microscopy (FESEM), X-ray diffraction (XRD), atomic force microscopy (AFM), time-of-flight elastic recoil detection analysis (ToF-ERDA), and energy dispersive X-ray spectroscopy (EDX). In addition, film adhesion was t…

010302 applied physicsMaterials scienceta214ta114Band gapGeneral Chemical EngineeringAnalytical chemistryLithium fluoride02 engineering and technologyGeneral ChemistryAtmospheric temperature range021001 nanoscience & nanotechnology01 natural sciencesElastic recoil detectionchemistry.chemical_compoundAtomic layer depositionchemistryImpurity0103 physical sciencesMaterials ChemistryThin film0210 nano-technologySpectroscopyChemistry of Materials
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Conceptual study of a heavy-ion-ERDA spectrometer for energies below 6 MeV

2017

Abstract Elastic recoil detection analysis (ERDA) is a well established technique and it offers unique capabilities in thin film analysis. Simultaneous detection and depth profiling of all elements, including hydrogen, is possible only with time-of-flight ERDA. Bragg ionization chambers or Δ E - E detectors can also be used to identify the recoiling element if sufficiently high energies are used. The chief limitations of time-of-flight ERDA are the beam induced sample damage and the requirement of a relatively large accelerator. In this paper we propose a detector setup, which could be used with 3 MeV to 6 MeV medium heavy beams from either a single ended accelerator (40Ar) or from a tandem…

010302 applied physicsNuclear and High Energy PhysicsERDASpectrometerta114Physics::Instrumentation and DetectorsChemistryDetectortime-of-flight01 natural sciencesNuclear physicsPelletronElastic recoil detectionTime of flightvetyIonizationhydrogen0103 physical sciencesIonization chamber010306 general physicsInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Analysis of thin high-k and silicide films by means of heavy ion time-of-flight forward-scattering spectrometry

2006

The use of forward scattered heavy incident ions in combination with a time-of-flight-energy telescope provides a powerful tool for the analysis of very thin (5–30 nm) films. This is because of greater stopping powers and better detector energy resolution for heavier ions than in conventional He-RBS. Because of the forward scattering angle, the sensitivity is greatly enhanced, thus reducing the ion beam induced desorption during the analysis of very thin films. The drawback of forward scattering angle is the limited mass separation for target elements. We demonstrate the performance of the technique with the analysis of 25 nm thick NiSi films and atomic layer deposited 6 nm thick HfxSiyOz f…

010302 applied physicsNuclear and High Energy PhysicsMaterials scienceIon beamSiliconbusiness.industryScatteringForward scatterchemistry.chemical_element02 engineering and technology021001 nanoscience & nanotechnology01 natural sciences7. Clean energyIonElastic recoil detectionTime of flightchemistry0103 physical sciencesOptoelectronicsAtomic physicsThin film0210 nano-technologybusinessInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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