Search results for "CERAMICS"

showing 10 items of 1599 documents

Operation of transition-edge sensors with excess thermal noise

2006

The superconducting transition-edge sensor (TES) is currently one of the most attractive choices for ultra-high resolution calorimetry in the keV x-ray band, and is being considered for future ESA and NASA missions. We have performed a study on the noise characteristics of Au/Ti bilayer TESs, at operating temperatures around ~100 mK, with the SQUID readout at 1.5 K. Experimental results indicate that without modifications the back-action noise from the SQUID chip degrades the noise characteristics significantly. We present a simple and effective solution to the problem: by installing an extra shunt resistor which absorbs the excess radiation from the SQUID input, we have reduced the excess …

PhysicsNoise powerSquidPhotonbiologybusiness.industryPhysics::Instrumentation and DetectorscalorimetersMetals and AlloysY-factorsuperconducting microwave devicesRadiationCondensed Matter PhysicsChipSQUIDNoise (electronics)biology.animalsuperconducting transistorsThermalMaterials ChemistryCeramics and Compositestransition edge sensorsOptoelectronicsElectrical and Electronic EngineeringbusinessSuperconductor Science and Technology
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Microscopic Dynamics of Hard Ellipsoids in their Liquid and Glassy Phase

2001

To investigate the influence of orientational degrees of freedom onto the dynamics of molecular systems in its supercooled and glassy regime we have solved numerically the mode-coupling equations for hard ellipsoids of revolution. For a wide range of volume fractions $\phi$ and aspect ratios $x_{0}$ we find an orientational peak in the center of mass spectra $\chi_{000}^{''}(q,\omega)$ and $\phi_{000}^{''} (q,\omega)$ about one decade below a high frequency peak. This orientational peak is the counterpart of a peak appearing in the quadrupolar spectra $\chi_{22m}^{''}(q,\omega)$ and $\phi_{22m}^{''}(q,\omega)$. The latter peak is almost insensitive on $\phi$ for $x_{0}$ close to one, i.e. f…

PhysicsRange (particle radiation)Condensed matter physicsDegrees of freedom (physics and chemistry)FOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksCondensed Matter - Soft Condensed MatterCondensed Matter PhysicsCoupling (probability)OmegaSpectral lineElectronic Optical and Magnetic MaterialsPhase (matter)Materials ChemistryCeramics and CompositesSoft Condensed Matter (cond-mat.soft)Center of massSupercooling
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The Dynamics of Supercooled Silica: Acoustic modes and Boson peak

1997

Using molecular dynamics computer simulations we investigate the dynamics of supercooled silica in the frequency range 0.5-20~THz and the wave-vector range 0.13-1.1\AA^{-1}. We find that for small wave-vectors the dispersion relations are in very good agreement with the ones found in experiments and that the frequency at which the boson-peak is observed shows a maximum at around 0.39\AA^{-1}.

PhysicsRange (particle radiation)Statistical Mechanics (cond-mat.stat-mech)Dynamics (mechanics)FOS: Physical sciencesCondensed Matter PhysicsMolecular physicsElectronic Optical and Magnetic MaterialsMolecular dynamicsDispersion relationMaterials ChemistryCeramics and CompositesBoson peakSupercoolingCondensed Matter - Statistical Mechanics
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Stochastic models for heterogeneous relaxation: Application to inhomogeneous optical lineshapes

2001

Dynamic heterogeneity has often been modeled by assuming that a single-particle observable, fluctuating at a molecular scale, is influenced by its coupling to environmental variables fluctuating on a second, perhaps slower, time scale. Starting from the most simple Gaussian Markov process we model the exchange between 'slow' and 'fast' environments by treating the fluctuating single-particle variable as a projection from a higher-dimensional Markov process. The moments of the resulting stochastic process are calculated from the corresponding Master equations or Langevin equations, depending on the model. The calculations show the importance of the way to treat exchange processes. The result…

PhysicsScale (ratio)Stochastic processStochastic modellingGaussianCondensed Matter (cond-mat)Markov processFOS: Physical sciencesCondensed MatterCondensed Matter PhysicsProjection (linear algebra)Electronic Optical and Magnetic Materialssymbols.namesakeMaster equationMaterials ChemistryCeramics and CompositessymbolsStatistical physicsRelaxation (approximation)
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An extended Ritz formulation for buckling and post-buckling analysis of cracked multilayered plates

2018

Abstract An extended Ritz formulation for the analysis of buckling and post-buckling behaviour of cracked composite multilayered plates is presented. The formulation is based on: (i) the First-order Shear Deformation Theory to model the mechanics of the multilayered plate; (ii) the von Karman’s theory to account for geometric non-linearities ; (iii) the use of an extended set of approximating functions able to model the presence of an embedded or edge crack and to capture the crack opening fields as well as the global behaviour within a single cracked domain. The numerical results of the buckling analyses and the equilibrium paths in the post-buckling regime are compared with the results fr…

PhysicsShear deformation theoryComposite numberMathematical analysisCeramics and Composite02 engineering and technologyPlate post-bucklingEdge (geometry)01 natural sciencesDomain (mathematical analysis)Finite element method010101 applied mathematics020303 mechanical engineering & transports0203 mechanical engineeringBucklingExtended Rayleigh-Ritz methodPlate bucklingCeramics and CompositesFirst-order shear deformation theory0101 mathematicsSettore ING-IND/04 - Costruzioni E Strutture AerospazialiCivil and Structural EngineeringComposite Structures
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Quantitative tests of mode-coupling theory for fragile and strong glass-formers

2001

We calculate for a binary mixture of Lennard-Jones particles the time dependence of the solution of the mode-coupling equations in which the full wave vector dependence is taken into account. In addition we also take into account the short time dynamics, which we model with a simple memory kernel. We find that the so obtained solution agrees very well with the time and wave vector dependence of the coherent and incoherent intermediate scattering functions as determined from molecular dynamics computer simulations. Furthermore we calculate the wave vector dependence of the Debye-Waller factor for a realistic model of silica and compare these results with the ones obtained from a simulation o…

PhysicsStatistical Mechanics (cond-mat.stat-mech)ScatteringBinary numberFOS: Physical sciencesFunction (mathematics)Disordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsMolecular dynamicsSimple (abstract algebra)Kernel (statistics)Mode couplingMaterials ChemistryCeramics and CompositesWave vectorStatistical physicsCondensed Matter - Statistical Mechanics
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Exploration of the double exchange in quantum cellular automata: proposal for a new class of cells

2020

In this communication we propose to considerably extend the class of systems suitable as cells for quantum cellular automata by including magnetic quantum dots and molecular mixed valence dimers exhibiting double exchange. As distinguished from the previous works we propose to use not only charges as the information carriers but also spin degrees of freedom. In this context we focus on the two key points: (1) properties of the magnetic cell as reservoir for charges carrying binary information, and (2) identification of conditions under which spin degrees of freedom can be employed.

PhysicsValence (chemistry)Magnetic PhenomenaMetals and AlloysGeneral ChemistryTopologyCatalysisSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsBinary informationQuantum dotQuantum DotsMaterials ChemistryCeramics and CompositesNanotechnologyQuantum cellular automatonChemical Communications
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Theory and modeling of polarization switching in ferroelectrics

2005

Abstract Kinetics of polarization response in ferroelectrics is reproduced within Langevin, Fokker–Planck and imaginary time Schrodinger equation techniques for energy functionals of growing complexity modeling an assembly of coarse grained particles with attractive first neighbor interaction. Symplectic integration based numerical approach captures dynamic hysteresis, polarization switching, and spatially extended stationary polarization. Solution of relevant nonstationary problem is adapted to large scale parallel computing.

Physicssymbols.namesakeClassical mechanicsMaterials ChemistryCeramics and CompositesFerroelectric hysteresissymbolsStatistical physicsSymplectic integratorPolarization (waves)FerroelectricityImaginary timeSchrödinger equationJournal of the European Ceramic Society
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Bubble motion through non-crimp fabrics during composites manufacturing

2008

Bubbles motion through interbundle channels in biaxial non-crimp fabrics is modelled. The scenario is that formed bubbles move with the resin through these channels and are trapped if the channels become too narrow. By usage of a permeability network model, existing criteria on bubble deformation and a variety of analytical and probabilistic methods it is found that the paths of the bubbles depend significantly on the position of the threads keeping the fabric together and the number of fibres crossing the interbundle channels. Another result is that the pressure difference over a trapped bubble increases with 50% in a 3D geometry possible helping the bubble to escape. A third result is tha…

Physics::Fluid DynamicsVoid (astronomy)Materials scienceTransfer moldingMechanics of MaterialsBubbleCeramics and CompositesCrimpFluid mechanicsComposite materialPorosityNetwork modelPressure differenceComposites Part A: Applied Science and Manufacturing
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Microstructural evolution and growth of crystallite size of mullite during thermal transformation of kyanite

1997

Abstract The microstructural evolution of mullite during the thermal transformation of kyanite has been studied in the temperature range 1200–1600 °C. The shape and size of the grains were analysed by means of SEM-EDS while crystallite size evolution was studied by X-ray line profile analyses. The results obtained showed that total transformation of kyanite to mullite takes place between 1350 and 1400 °C. At temperatures below 1350 °C needle-like mullite grains are always produced. At higher temperatures the mullite grains reveal rounded end platelet morphology. Evolution from needle-like to platelet shape was correlated with the X-ray data.

Platelet MorphologyMicrostructural evolutionMaterials scienceThermal transformationMineralogyMulliteAtmospheric temperature rangeKyanitevisual_artMaterials ChemistryCeramics and Compositesvisual_art.visual_art_mediumCrystalliteComposite material
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