Search results for "probe method"

showing 2 items of 2 documents

Light absorption and electrical transport in Si:O alloys for photovoltaics

2010

Thin films (100-500 nm) of the Si:O alloy have been systematically characterized in the optical absorption and electrical transport behavior, by varying the Si content from 43 up to 100 at. %. Magnetron sputtering or plasma enhanced chemical vapor deposition have been used for the Si:O alloy deposition, followed by annealing up to 1250 °C. Boron implantation (30 keV, 3-30× 1014 B/cm2) on selected samples was performed to vary the electrical sheet resistance measured by the four-point collinear probe method. Transmittance and reflectance spectra have been extracted and combined to estimate the absorption spectra and the optical band gap, by means of the Tauc analysis. Raman spectroscopy was …

Materials scienceAbsorption spectroscopyFour-pointAnalytical chemistryGeneral Physics and AstronomyAbsorption coefficientChemical vapor depositionBoron implantationSettore ING-INF/01 - ElettronicaSettore FIS/03 - Fisica Della Materiasymbols.namesakeElectrical resistivity and conductivityPlasma-enhanced chemical vapor depositionThin filmAbsorption (electromagnetic radiation)Electrical sheet resistanceSi contentSEMIINSULATING POLYCRYSTALLINE SILICON; SOLAR-CELLS; 3RD-GENERATION PHOTOVOLTAICS; OPTICAL-PROPERTIES; AMORPHOUS-SILICON; THIN-FILMS; CRYSTALLINEOptical absorptionProbe methodElectrical resistivityAlloy depositionSputter depositionElectrical transportsymbolsOxygen-rich siliconRaman spectroscopyOptical gapReflectance spectrumPhotovoltaic
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Superconductive and insulating inclusions for linear and non-linear conductivity equations

2015

We detect an inclusion with infinite conductivity from boundary measurements represented by the Dirichlet-to-Neumann map for the conductivity equation. We use both the enclosure method and the probe method. We use the enclosure method to prove partial results when the underlying equation is the quasilinear $p$-Laplace equation. Further, we rigorously treat the forward problem for the partial differential equation $\operatorname{div}(\sigma\lvert\nabla u\rvert^{p-2}\nabla u)=0$ where the measurable conductivity $\sigma\colon\Omega\to[0,\infty]$ is zero or infinity in large sets and $1<p<\infty$.

Pure mathematicsControl and Optimizationmedia_common.quotation_subjectMathematics::Analysis of PDEsBoundary (topology)probe methodConductivity01 natural sciencesMathematics - Analysis of PDEs35R30 35J92 (Primary) 35H99 (Secondary)FOS: MathematicsDiscrete Mathematics and CombinatoricsPharmacology (medical)Nabla symbol0101 mathematicsmedia_commonp-harmonic functionsLaplace's equationPhysicsPartial differential equationCalderón problemComputer Science::Information Retrieval010102 general mathematicsta111Zero (complex analysis)Infinity3. Good health010101 applied mathematicsNonlinear systeminclusionModeling and Simulationinverse boundary value problemAnalysisinkluusioAnalysis of PDEs (math.AP)enclosure method
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