Search results for "Elastic"

showing 10 items of 2162 documents

Mechanical characterisation of pentagonal gold nanowires in three different test configurations: A comparative study.

2019

Abstract Mechanical characterisation of individual nanostructures is a challenging task and can greatly benefit from the utilisation of several alternative approaches to increase the reliability of results. In the present work, we have measured and compared the elastic modulus of five-fold twinned gold nanowires (NWs) with atomic force microscopy (AFM) indentation in three different test configurations: three-point bending with fixed ends, three-point bending with free ends and cantilevered-beam bending. The free-ends condition was realized by introducing a novel approach where the NW is placed diagonally inside an inverted pyramid chemically etched in a silicon wafer. In addition, all thre…

010302 applied physicsMaterials scienceNanowireGeneral Physics and Astronomy02 engineering and technologyCell BiologyBendingEdge (geometry)021001 nanoscience & nanotechnology01 natural sciencesFinite element methodStructural BiologyIndentation0103 physical sciencesGeneral Materials ScienceWaferComposite materialDeformation (engineering)0210 nano-technologyElastic modulusMicron (Oxford, England : 1993)
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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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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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Structural phase transition in [(C2H5)4N][(CH3)4N]ZnCl4

2019

The hybrid crystal [(C2H5)4N][(CH3)4N]ZnCl4 was studied using several experimental methods. DSC studies revealed the first order phase transition to the high temperature phase at about 496 K. This phase transition was confirmed in dielectric studies. Optical observation revealed the domain structure appearance characteristic for that of the phase transition between tetragonal and orthorhombic phases. This phase transition shows a lowering of symmetry as in the case of bromide analogs. Additionally, the optical studies showed the appearance of a number of cracks in the sample and in some cases, the samples became milky after cooling from the high temperature to the room temperature phase.

010302 applied physicsPhase transitionStructural phaseMaterials scienceThermodynamics02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesCrystalPhase (matter)0103 physical sciencesGeneral Materials ScienceExperimental methods0210 nano-technologyOrganic–inorganic hybrid compounds; phase transitions; thermal and dielectric properties; ferroelastic domainsInstrumentationPhase Transitions
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Mass calibration of the energy axis in ToF- E elastic recoil detection analysis

2016

We report on procedures that we have developed to mass-calibrate the energy axis of ToF-E histograms in elastic recoil detection analysis. The obtained calibration parameters allow one to transform the ToF-E histogram into a calibrated ToF-M histogram.

010302 applied physicsPhysicsNuclear and High Energy Physicsta114Physics::Instrumentation and DetectorsPhysics::Medical PhysicsAstrophysics::Instrumentation and Methods for AstrophysicsERD02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesNuclear physicsElastic recoil detectionComputer Science::Computer Vision and Pattern RecognitionHistogramelastic recoil detection analysis0103 physical sciencesCalibrationmass calibrationToF-ENuclear Experiment0210 nano-technologyInstrumentationEnergy (signal processing)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Determination of elastoplastic properties of TiO2 thin films deposited on dual phase stainless steel using nanoindentation tests

2010

International audience; In recent years, the extraction of mechanical behaviour of thin films by nanoindentation using sharp indenter geometry has been extensively studied. This work investigates the mechanical properties of TiO2 thin film (1 µm thickness) deposited by spin coating on dual phase Duplex stainless steel and glass substrates. Experiments are carried out with different sharp triangular pyramids (a Cube corner and a Berkovich indenter) using a commercial Nano Indenter® XP apparatus. The substrate effect has been counteracted and an inverse method proposed in literature for bulk material has been adapted to assess the elastoplastic parameters of the tested thin film directly from…

010302 applied physicsSpin coatingMaterials scienceThin filmsMetallurgy02 engineering and technologySurfaces and InterfacesGeneral ChemistrySubstrate (electronics)Inverse methodNanoindentation021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesFinite element methodNanoindentationSurfaces Coatings and FilmsPhase (matter)0103 physical sciencesNano-Materials ChemistryThin film0210 nano-technologyFinite element modelingElastic modulus
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Oxy-nitrides characterization with a new ERD-TOF system

2017

Abstract A new time-of-flight (TOF) camera was installed on Elastic Recoil Detection (ERD) measurement setup on the Tandem Accelerator at Universite de Montreal. The camera consists of two timing detectors, developed and built by the Jyvaskyla group, that use a thin carbon foil and microchannel plates (MCP) to produce the start and stop signals. The position of the first detector is fixed at 18 cm from the target, while the position of the second detector can be varied between 50 and 90 cm from the first detector. This allows to increase time resolution by increasing the distance between the time-of-flight detectors or to increase solid angle by decreasing the distance. Moving the detector …

010302 applied physicsToF-ERDANuclear and High Energy PhysicsIon beam analysisMicrochannelMaterials scienceta114Physics::Instrumentation and Detectorsbusiness.industryDetectorSolid angleion beam analysis02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesSignalelastic recoil detectionElastic recoil detectionOpticsPosition (vector)0103 physical sciences0210 nano-technologybusinessInstrumentationEnergy (signal processing)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Atomic layer deposition of aluminum oxide on modified steel substrates

2016

Abstract Al 2 O 3 thin films were grown by atomic layer deposition to thicknesses ranging from 10 to 90 nm on flexible steel substrates at 300 °C using Al(CH 3 ) 3 and H 2 O as precursors. The films grown to thicknesses 9–90 nm covered the rough steel surfaces uniformly, allowing reliable evaluation of their dielectric permittivity and electrical current densities with appreciable contact yield. Mechanical behavior of the coatings was evaluated by nanoindentation. The maximum hardness values of the Al 2 O 3 films on steel reached 12 GPa and the elastic modulus exceeded 280 GPa.

010302 applied physicsYield (engineering)Materials scienceMetallurgy02 engineering and technologySurfaces and InterfacesGeneral ChemistryChemical vapor depositionNanoindentation021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesSurfaces Coatings and FilmsAtomic layer deposition0103 physical sciencesMaterials ChemistrySurface modificationThin filmComposite material0210 nano-technologyElastic modulusAluminum oxideSurface and Coatings Technology
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