Search results for " PD"

showing 10 items of 651 documents

Synthesis and photoluminescence properties of hybrid 1D core–shell structured nanocomposites based on ZnO/polydopamine

2020

In the present work, we report on the modelling of processes at the zinc oxide and polydopamine (ZnO/ PDA) interface. The PDA layer was deposited onto ZnO nanorods (NRs) via chemical bath deposition. The defect concentrations in ZnO before and after PDA deposition were calculated and analysed. The ZnONRs/PDA core–shell nanostructures were studied by transmission electron microscopy (TEM), X-ray diffraction (XRD), Raman and Fourier-transform infrared (FTIR) spectroscopy, photoluminescence (PL) measurements, and diffuse reflectance spectroscopy. The TEM and electron energy loss spectroscopy (EELS) measurements confirmed the conformal coating of PDA, while the PL emission from ZnO and ZnONRs/P…

PhotoluminescenceMaterials scienceDiffuse reflectance infrared fourier transformGeneral Chemical EngineeringElectron energy loss spectroscopyGeneral ChemistryX-ray diffraction (XRD)symbols.namesakephotoluminescence (PL)Chemical engineeringTransmission electron microscopysymbolsNanorodzinc oxide and polydopamine (ZnO/ PDA)Fourier transform infrared spectroscopyRaman spectroscopyChemical bath deposition
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A new discretization for the polarizable continuum model within the domain decomposition paradigm

2016

International audience; We present a new algorithm to solve the polarizable continuum model equation in a framework compatible with the strategy previously developed by us for the conductor-like screening model based on Schwarz’s domain decomposition method (ddCOSMO). The new discretization is systematically improvable and is fully consistent with ddCOSMO so that it reproduces ddCOSMO results for large dielectric constants.

Physics and Astronomy (all); Physical and Theoretical Chemistry010304 chemical physicsDiscretizationChemistrySolvationGeneral Physics and AstronomyDomain decomposition methodsDielectric010402 general chemistry01 natural sciencesPolarizable continuum model0104 chemical sciencesComputational physicsPhysics and Astronomy (all)0103 physical sciences[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Statistical physicsPhysical and Theoretical ChemistrySolvent effects
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A computational method for the Helmholtz equation in unbounded domains based on the minimization of an integral functional

2012

Abstract We study a new approach to the problem of transparent boundary conditions for the Helmholtz equation in unbounded domains. Our approach is based on the minimization of an integral functional arising from a volume integral formulation of the radiation condition. The index of refraction does not need to be constant at infinity and may have some angular dependency as well as perturbations. We prove analytical results on the convergence of the approximate solution. Numerical examples for different shapes of the artificial boundary and for non-constant indexes of refraction will be presented.

Physics and Astronomy (miscellaneous)Helmholtz equationBoundary (topology)FOS: Physical sciencesElectric-field integral equationVolume integralMathematics - Analysis of PDEsSettore MAT/05 - Analisi MatematicaConvergence (routing)Refraction (sound)FOS: MathematicsBoundary value problemHelmholtz equationSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsNumerical AnalysisApplied MathematicsMathematical analysisTransparent boundary conditionMinimization of integral functionalsMathematical Physics (math-ph)Computer Science ApplicationsComputational MathematicsModeling and SimulationConstant (mathematics)Analysis of PDEs (math.AP)
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A partially reflecting random walk on spheres algorithm for electrical impedance tomography

2015

In this work, we develop a probabilistic estimator for the voltage-to-current map arising in electrical impedance tomography. This novel so-called partially reflecting random walk on spheres estimator enables Monte Carlo methods to compute the voltage-to-current map in an embarrassingly parallel manner, which is an important issue with regard to the corresponding inverse problem. Our method uses the well-known random walk on spheres algorithm inside subdomains where the diffusion coefficient is constant and employs replacement techniques motivated by finite difference discretization to deal with both mixed boundary conditions and interface transmission conditions. We analyze the global bias…

Physics and Astronomy (miscellaneous)random diffusion coefficientvariance reductionMonte Carlo method010103 numerical & computational mathematicsControl variates01 natural sciencesdiscontinuous diffusion coefficientrandom walk on spheresFOS: Mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Mathematics - Numerical Analysis0101 mathematicsElectrical impedance tomographyMathematicsNumerical AnalysisApplied MathematicsProbabilistic logicEstimatorMonte Carlo methodsreflecting Brownian motionNumerical Analysis (math.NA)Inverse problemRandom walkComputer Science Applications010101 applied mathematicsComputational MathematicsModeling and SimulationVariance reductionAlgorithmelectrical impedance tomographyJournal of Computational Physics
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Analytic solutions and Singularity formation for the Peakon b--Family equations

2012

This paper deals with the well-posedness of the b-family equation in analytic function spaces. Using the Abstract Cauchy-Kowalewski theorem we prove that the b-family equation admits, locally in time, a unique analytic solution. Moreover, if the initial data is real analytic and it belongs to H s with s>3/2, and the momentum density u 0-u 0, xx does not change sign, we prove that the solution stays analytic globally in time, for b≥1. Using pseudospectral numerical methods, we study, also, the singularity formation for the b-family equations with the singularity tracking method. This method allows us to follow the process of the singularity formation in the complex plane as the singularity a…

PhysicsAbstract Cauchy-Kowalewski theoremApplied MathematicsNumerical analysisComplex singularitiesNumerical Analysis (math.NA)Spectral analysisFourier spectrumRate of decayPeakonAnalytic solutionMomentumSingularityMathematics - Analysis of PDEsb-family equationFOS: MathematicsSpectral analysis Complex singularities b-family equation Analytic solution Abstract Cauchy-Kowalewski theoremMathematics - Numerical AnalysisComplex planeSettore MAT/07 - Fisica MatematicaMathematical physicsSign (mathematics)Analysis of PDEs (math.AP)
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Simultaneously recovering potentials and embedded obstacles for anisotropic fractional Schrödinger operators

2017

Let \begin{document}$A∈{\rm{Sym}}(n× n)$\end{document} be an elliptic 2-tensor. Consider the anisotropic fractional Schrodinger operator \begin{document}$\mathscr{L}_A^s+q$\end{document} , where \begin{document}$\mathscr{L}_A^s: = (-\nabla·(A(x)\nabla))^s$\end{document} , \begin{document}$s∈ (0, 1)$\end{document} and \begin{document}$q∈ L^∞$\end{document} . We are concerned with the simultaneous recovery of \begin{document}$q$\end{document} and possibly embedded soft or hard obstacles inside \begin{document}$q$\end{document} by the exterior Dirichlet-to-Neumann (DtN) map outside a bounded domain \begin{document}$Ω$\end{document} associated with \begin{document}$\mathscr{L}_A^s+q$\end{docume…

PhysicsControl and OptimizationApproximation property02 engineering and technology01 natural sciences010101 applied mathematicsCombinatoricssymbols.namesakeMathematics - Analysis of PDEsOperator (computer programming)Modeling and SimulationBounded functionDomain (ring theory)0202 electrical engineering electronic engineering information engineeringsymbolsDiscrete Mathematics and Combinatorics020201 artificial intelligence & image processingPharmacology (medical)Nabla symbolUniqueness0101 mathematicsAnisotropyAnalysisSchrödinger's catInverse Problems & Imaging
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Coulomb excitation of exotic nuclei at the R3B-LAND setup

2012

Exotic Ni isotopes have been measured at the R3B-LAND setup at GSI in Darmstadt, using Coulomb excitation in inverse kinematics at beam energies around 500 MeV/u. As the experimental setup allows kinematically complete measurements, the excitation energy was reconstructed using the invariant mass method. The GDR and additional low-lying strength have been observed in 68Ni, the latter exhausting 4.1(1.9)% of the E1 energy-weighted sum rule. Also, the branching ratio for the non-statistical decay of the excited 68Ni nuclei was measured and amounts to 24(4)%.

PhysicsHistoryInverse kinematicsBranching fractionFOS: Physical sciencesExotic isotopes R3B LAND GSI Coulomb excitation inverse kinematics GDR PDRCoulomb excitationComputer Science ApplicationsEducationNuclear physicsExcited stateInvariant massSum rule in quantum mechanicsNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentBeam (structure)Excitation
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Relaxation of periodic and nonstandard growth integrals by means of two-scale convergence

2019

An integral representation result is obtained for the variational limit of the family functionals $\int_{\Omega}f\left(\frac{x}{\varepsilon}, Du\right)dx$, as $\varepsilon \to 0$, when the integrand $f = f (x,v)$ is a Carath\'eodory function, periodic in $x$, convex in $v$ and with nonstandard growth.

PhysicsIntegral representationRegular polygonScale (descriptive set theory)homomgenizationFunction (mathematics)two scale convergencehomomgenization; two scale convergencehomomgenization two scale convergenceMathematics - Analysis of PDEsConvergence (routing)FOS: MathematicsRelaxation (physics)Limit (mathematics)Analysis of PDEs (math.AP)Mathematical physics
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A Remark on an Overdetermined Problem in Riemannian Geometry

2016

Let (M, g) be a Riemannian manifold with a distinguished point O and assume that the geodesic distance d from O is an isoparametric function. Let \(\varOmega \subset M\) be a bounded domain, with \(O \in \varOmega \), and consider the problem \(\varDelta _p u = -1\ \mathrm{in}\ \varOmega \) with \(u=0\ \mathrm{on}\ \partial \varOmega \), where \(\varDelta _p\) is the p-Laplacian of g. We prove that if the normal derivative \(\partial _{\nu }u\) of u along the boundary of \(\varOmega \) is a function of d satisfying suitable conditions, then \(\varOmega \) must be a geodesic ball. In particular, our result applies to open balls of \(\mathbb {R}^n\) equipped with a rotationally symmetric metr…

PhysicsIsoparametric functionComparison principleGeodesic010102 general mathematicsRotationally symmetric spacesRiemannian manifoldRiemannian geometry01 natural sciencesRotationally symmetric spaceCombinatoricsOverdetermined systemsymbols.namesakeBounded function0103 physical sciencessymbolsComparison principle; Isoparametric functions; Overdetermined PDE; Riemannian Geometry; Rotationally symmetric spaces; Mathematics (all)Isoparametric functionsMathematics (all)Overdetermined PDEMathematics::Differential Geometry010307 mathematical physics0101 mathematicsRiemannian Geometry
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Parabolic equations with natural growth approximated by nonlocal equations

2017

In this paper we study several aspects related with solutions of nonlocal problems whose prototype is $$ u_t =\displaystyle \int_{\mathbb{R}^N} J(x-y) \big( u(y,t) -u(x,t) \big) \mathcal G\big( u(y,t) -u(x,t) \big) dy \qquad \mbox{ in } \, \Omega \times (0,T)\,, $$ being $ u (x,t)=0 \mbox{ in } (\mathbb{R}^N\setminus \Omega )\times (0,T)\,$ and $ u(x,0)=u_0 (x) \mbox{ in } \Omega$. We take, as the most important instance, $\mathcal G (s) \sim 1+ \frac{\mu}{2} \frac{s}{1+\mu^2 s^2 }$ with $\mu\in \mathbb{R}$ as well as $u_0 \in L^1 (\Omega)$, $J$ is a smooth symmetric function with compact support and $\Omega$ is either a bounded smooth subset of $\mathbb{R}^N$, with nonlocal Dirichlet bound…

PhysicsKernel (set theory)Applied MathematicsGeneral Mathematics010102 general mathematicsMathematics::Analysis of PDEs01 natural sciencesParabolic partial differential equationOmega010101 applied mathematicsSymmetric functionCombinatoricssymbols.namesakeMathematics - Analysis of PDEsMathematics - Analysis of PDEs; Mathematics - Analysis of PDEsBounded functionDirichlet boundary conditionsymbolsFOS: MathematicsUniqueness0101 mathematicsAnalysis of PDEs (math.AP)
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