Search results for " function"

showing 10 items of 9395 documents

Isolated roundings and flattenings of submanifolds in Euclidean spaces

2005

We introduce the concepts of rounding and flattening of a smooth map $g$ of an $m$-dimensional manifold $M$ to the euclidean space $\R^n$ with $m<n$, as those points in $M$ such that the image $g(M)$ has contact of type $\Sigma^{m,\dots,m}$ with a hypersphere or a hyperplane of $\R^n$, respectively. This includes several known special points such as vertices or flattenings of a curve in $\R^n$, umbilics of a surface in $\R^3$, or inflections of a surface in $\R^4$.

Surface (mathematics)Euclidean spaceGeneral MathematicsImage (category theory)Mathematical analysisEuclidean distance matrixHypersphereType (model theory)53A05Manifoldheight function53A07CombinatoricsDistance from a point to a plane58K05Distance squared functionMathematicsTohoku Mathematical Journal
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New construction of algebro-geometric solutions to the Camassa-Holm equation and their numerical evaluation

2011

An independent derivation of solutions to the Camassa-Holm equation in terms of multi-dimensional theta functions is presented using an approach based on Fay's identities. Reality and smoothness conditions are studied for these solutions from the point of view of the topology of the underlying real hyperelliptic surface. The solutions are studied numerically for concrete examples, also in the limit where the surface degenerates to the Riemann sphere, and where solitons and cuspons appear.

Surface (mathematics)General MathematicsFOS: Physical sciencesGeneral Physics and AstronomyRiemann sphereTheta function01 natural sciences010305 fluids & plasmassymbols.namesake[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]0103 physical sciencesLimit (mathematics)0101 mathematics[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Shallow water equationsNonlinear Sciences::Pattern Formation and SolitonsMathematical PhysicsMathematicsSmoothnessCamassa–Holm equationNonlinear Sciences - Exactly Solvable and Integrable Systems010102 general mathematicsMathematical analysisGeneral Engineering[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Mathematical Physics (math-ph)Nonlinear Sciences::Exactly Solvable and Integrable SystemssymbolsExactly Solvable and Integrable Systems (nlin.SI)Hyperelliptic surfaceProc. R. Soc. Lond. Ser. A Math. Phys. Eng. Sci. 468 (2012), no. 2141, 1371–1390
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INITIAL PARAMETRIC REPRESENTATION OF BLOBS

2009

Blobs, developed by J.F. Blinn in 1982, are the implicit surfaces obtained by composition of a real numerical function and a distance function. Since, many authors (C. Murakami, H. Nishimura, G. Wyvill…) defined their own function of density, from these implicit surfaces are interesting from several points of view. In particular, their fusion makes it possible to easily obtain an implicit equation of resulting surface. However, these surfaces do not admit a parametric equation yet. In this article, we will establish the parametric equation of two blobs in fusion, defined by the function of density of C. Murakami, by using an algebraic method. Then, we will develop another method, based on …

Surface (mathematics)Implicit functionDifferential equationApplied MathematicsMathematical analysisFunction (mathematics)Composition (combinatorics)Theoretical Computer ScienceComputational MathematicsComputational Theory and MathematicsGeometry and TopologyParametric equationRepresentation (mathematics)Parametric statisticsMathematicsInternational Journal of Computational Geometry &amp; Applications
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Polarity Effects on ZnO Films Grown along the Nonpolar[112¯0]Direction

2005

The surface electrical properties of ZnO thin films grown along the nonpolar $[11\overline{2}0]$ direction have been investigated by Kelvin probe microscopy on a nanometer scale. Two different charge domains, with a 75 meV work function difference, coexist within the ZnO surface, which is covered by rhombohedral pyramids whose sidewalls are shown to be ${10\overline{1}1}$-type planes. The presence and relative orientation of the two kinds of charge domains are explained in terms of the atomic arrangement at the ${10\overline{1}1}$ polar surfaces.

Surface (mathematics)Kelvin probe force microscopeMaterials scienceCondensed matter physicsbusiness.industryPolarity (physics)General Physics and AstronomyCharge (physics)Orientation (vector space)OpticsPolarWork functionThin filmbusinessPhysical Review Letters
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Roughening of the Cu(110) surface

1993

The structure of the Cu(110) surface is studied at high temperatures using a combination of lattice-gas Monte Carlo and molecular dynamics methods with identical many-atom interactions derived from the effective medium theory. The anisotropic six-vertex model is used in the interpretation of the lattice-gas results. We find a clear roughening transition around T_R=1000K and T_R/T_M=0.81. Molecular dynamics reveals the clustering of surface defects as the atomistic mechanism of the transition and allows us to estimate characteristic time scales. For the system of size 50x50, the time scale of the local roughening at 1150 K of an initially smooth surface is of the order of 100 ps.

Surface (mathematics)Materials scienceCondensed Matter (cond-mat)Monte Carlo methodFOS: Physical sciencesGeneral Physics and Astronomychemistry.chemical_elementCondensed Matter02 engineering and technology01 natural sciencesInterpretation (model theory)Molecular dynamicsTransition metalPhase (matter)Vacancy defect0103 physical sciencesAnisotropy010306 general physicsPhysicsCondensed matter physicsOrder (ring theory)021001 nanoscience & nanotechnologyCopperSmooth surfaceCorrelation function (statistical mechanics)chemistry0210 nano-technologyPhysical Review Letters
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Bundlet Model for Single-Wall Carbon Nanotubes, Nanocones and Nanohorns

2012

This paper discusses the existence of single-wall carbon nanocones (SWNCs), especially nanohorns (SWNHs), in organic solvents in the form of clusters. A theory is developed based on a bundlet model describing their distribution function by size. Phenomena have a unified explanation in bundlet model in which free energy of an SWNC, involved in a cluster, is combined from two components: a volume one, proportional to number of molecules n in a cluster, and a surface one proportional to n1/2. Bundlet model enables describing distribution function of SWNC clusters by size. From purely geometrical differences, bundlet (SWNCs) and droplet (fullerene) models predict different behaviours. The SWNCs…

Surface (mathematics)Materials scienceFullereneDistribution functionlawChemical physicsCluster (physics)MoleculeNanotechnologyLigand cone angleCarbon nanotubeCarbon nanoconelaw.inventionInternational Journal of Chemoinformatics and Chemical Engineering
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Calculations of atomic and electronic structure for (100) surfaces of SrTiO3 perovskite

2002

AbstractWe present and discuss main results of the calculations for the surface relaxation and rumpling of SrTiO3 surfaces with TiO2 and SrO terminations using a wide variety of methods of modern computational physics and chemistry, including the shell model (SM) and ab initio methods based on Hartree-Fock (HF) and Density Functional Theory (DFT). The HF and DFT formalisms with different exchange-correlation functionals are implemented into Crystal-98 computer code using a Gaussian-type basis set. We demonstrate that a hybrid B3PW formalism gives the best results for the bulk SrTiO3 properties. Results are compared with previous ab initio plane-wave LDA calculations and LEED experiments. Ou…

Surface (mathematics)Materials scienceSHELL modelRelaxation (NMR)Ab initioDensity functional theoryElectronic structureMolecular physicsBasis setPerovskite (structure)
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Single-shot ultrafast laser processing of high-aspect-ratio nanochannels using elliptical Bessel beams

2017

Ultrafast lasers have revolutionized material processing, opening a wealth of new applications in many areas of science. A recent technology that allows the cleaving of transparent materials via non-ablative processes is based on focusing and translating a high-intensity laser beam within a material to induce a well-defined internal stress plane. This then enables material separation without debris generation. Here, we use a non-diffracting beam engineered to have a transverse elliptical spatial profile to generate high aspect ratio elliptical channels in glass of dimension 350 nm x 710 nm, and subsequent cleaved surface uniformity at the sub-micron level.

Surface (mathematics)Materials scienceScanning electron microscopeFOS: Physical sciencesApplied Physics (physics.app-ph)02 engineering and technology01 natural scienceslaw.invention010309 opticssymbols.namesakeOpticslaw0103 physical sciences[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]Plane (geometry)business.industryPhysics - Applied Physics021001 nanoscience & nanotechnologyLaserAtomic and Molecular Physics and OpticsTransverse planesymbols0210 nano-technologybusinessUltrashort pulseBessel functionBeam (structure)Physics - OpticsOptics (physics.optics)Optics Letters
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Monotony Based Imaging in EIT

2010

We consider the problem of determining conductivity anomalies inside a body from voltage‐current measurements on its surface. By combining the monotonicity method of Tamburrino and Rubinacci with the concept of localized potentials, we derive a new imaging method that is capable of reconstructing the exact (outer) shape of the anomalies. We furthermore show that the method can be implemented without solving any non‐homogeneous forward problems and show a first numerical result.

Surface (mathematics)Partial differential equationMathematical analysisMonotonic functionBoundary value problemOperator theoryConductivityElectrical impedance tomographyMathematicsMathematical OperatorsAIP Conference Proceedings
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Does Young's equation hold on the nanoscale? A Monte Carlo test for the binary Lennard-Jones fluid

2010

When a phase-separated binary ($A+B$) mixture is exposed to a wall, that preferentially attracts one of the components, interfaces between A-rich and B-rich domains in general meet the wall making a contact angle $\theta$. Young's equation describes this angle in terms of a balance between the $A-B$ interfacial tension $\gamma_{AB}$ and the surface tensions $\gamma_{wA}$, $\gamma_{wB}$ between, respectively, the $A$- and $B$-rich phases and the wall, $\gamma _{AB} \cos \theta =\gamma_{wA}-\gamma_{wB}$. By Monte Carlo simulations of bridges, formed by one of the components in a binary Lennard-Jones liquid, connecting the two walls of a nanoscopic slit pore, $\theta$ is estimated from the inc…

Surface (mathematics)PhysicsCondensed matter physicsStatistical Mechanics (cond-mat.stat-mech)Monte Carlo methodGeneral Physics and AstronomyThermodynamic integrationFOS: Physical sciencesComputational Physics (physics.comp-ph)Contact angleSurface tensionPhysics::Fluid DynamicsDistribution functionWetting transitionPhysics - Computational PhysicsScalingCondensed Matter - Statistical Mechanics
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