Search results for "inho"

showing 10 items of 132 documents

Photorefractive “camera obscura”

2011

Abstract We demonstrate a novel scheme for lensless image formation which combines the properties of an amplifying dynamic hologram and a pinhole camera. The scheme is realized on the base of a SPS:Sb1% photorefractive crystal working at 633 nm.

PhysicsImage formationbusiness.industryHolographyPhotorefractive effectPhysical opticsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionOpticslawPhotorefractive crystalPinhole cameraOptoelectronicsElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessCamera obscuraOptics Communications
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A general nonexistence result for inhomogeneous semilinear wave equations with double damping and potential terms

2021

Abstract We investigate the large-time behavior of solutions for a class of inhomogeneous semilinear wave equations involving double damping and potential terms. Namely, we first establish a general criterium for the absence of global weak solutions. Next, some special cases of potential and inhomogeneous terms are studied. In particular, when the inhomogeneous term depends only on the variable space, the Fujita critical exponent and the second critical exponent in the sense of Lee and Ni are derived.

PhysicsInhomogeneous semilinear wave equationPotential termDouble damping termsFujita scaleGeneral MathematicsApplied MathematicsMathematical analysisGlobal solutionGeneral Physics and AstronomyStatistical and Nonlinear PhysicsTerm (logic)Space (mathematics)Wave equation01 natural sciencesCritical exponent010305 fluids & plasmasSettore MAT/05 - Analisi Matematica0103 physical sciences010301 acousticsCritical exponentVariable (mathematics)
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Coherent effects in the multimode dynamics of inhomogeneously broadened ring lasers

2004

We investigate under which conditions coherent effects manifest in the multimode dynamics of inhomogeneously broadened ring lasers. In particular, we demonstrate that for long enough cavities standard rate equations for class-B lasers fail in describing the multimode dynamics.

PhysicsLaser instabilities; Inhomogeneously broadened laser; Coherent effectsMulti-mode optical fiberCoherent effectsbusiness.industryDynamics (mechanics)Physics::OpticsRate equationLaserRing (chemistry)Atomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionLaser instabilitiesOpticslawInhomogeneously broadened laserFiber laserElectrical and Electronic EngineeringPhysical and Theoretical Chemistrybusiness
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Large Time Behavior for Inhomogeneous Damped Wave Equations with Nonlinear Memory

2020

We investigate the large time behavior for the inhomogeneous damped wave equation with nonlinear memory ϕtt(t,&omega

PhysicsPhysics and Astronomy (miscellaneous)General MathematicsNonlinear memoryWeak solutionlcsh:Mathematics010102 general mathematicsnonexistence resultglobal weak solutionDamped wavenonlinear memorylcsh:QA1-93901 natural sciencesinhomogeneous term010101 applied mathematicsChemistry (miscellaneous)Settore MAT/05 - Analisi MatematicaComputer Science (miscellaneous)damped wave equation0101 mathematicsMathematical physicsSymmetry
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Quantifying Artifacts in Ewald Simulations of Inhomogeneous Systems with a Net Charge

2014

Ewald summation, which has become the de facto standard for computing electrostatic interactions in biomolecular simulations, formally requires that the simulation box is neutral. For non-neutral systems the Ewald algorithm implicitly introduces a uniform background charge distribution that e ectively neutralizes the simulation box. Because a uniform distribution of counter charges typically deviates from the spatial distribution of counterions in real systems, artifacts may arise, in particular in systems with an inhomogeneous dielectric constant. Here we derive an analytical expression for the e ect of using an implicit background charge instead of explicit counterions, on the chemical po…

PhysicsUniform distribution (continuous)010304 chemical physicsCharge densityCharge (physics)02 engineering and technologyDielectricEwald simulations021001 nanoscience & nanotechnologyElectrostatics01 natural sciencesEwald summationComputer Science ApplicationsMolecular dynamicsinhomogeneous systems0103 physical sciencesStatistical physicsPhysical and Theoretical ChemistryTest particle0210 nano-technologyta116SimulationJournal of Chemical Theory and Computation
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IMAGINE: A Cold Neutron Imaging Station at the Laboratoire Léon Brillouin

2015

International audience; A second cold neutron imaging station has been open to users at the Laboratoire Léon Brillouin. The station is designed for high resolution neutron imaging and tomography. The typical field of view is 100x100 mm2 with a spatial resolution of 100 μm. Betterspatial resolutions (∼50 μm) can be achieved when reducing the field of view down to 30x30mm2. The L/D ratio can be varied from 200 to1000with pinhole sizes ranging from 20 to7 mm. Future upgrades will provide capabilities for energy resolved measurements using either a velocity selector or a double crystal monochromator. The possibility to perform polarized neutron experiments will also be provided next year.

Physicsbusiness.industryNeutron imagingField of viewRangingPhysics and Astronomy(all)7. Clean energyCold neutronlaw.inventionBrillouin zoneOpticslawNeutron imagingPinhole (optics)NeutronNeutron radiography[SDV.BBM]Life Sciences [q-bio]/Biochemistry Molecular BiologybusinessImage resolutionMonochromator
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The time-harmonic Maxwell equations

1996

In this chapter we shall see that the solution of the time-harmonic Maxwell equations with real coefficients can be transformed to time independent partial differential equations with complex coefficients. Then we introduce a finite element approximation proposed in [Křižek, Neittaanmaki, 1989]. A similar technique is analyzed in [Křižek, Neittaanmaki, 1984b], [Monk, 1992a] (for fully time dependent problems see, e.g., [Monk 1992b,c]).

Physicssymbols.namesakeJefimenko's equationsClassical mechanicsTheoretical and experimental justification for the Schrödinger equationMaxwell's equationsMaxwell's equations in curved spacetimesymbolsInhomogeneous electromagnetic wave equationMatrix representation of Maxwell's equationsMaxwell relationsElectromagnetic tensor
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Maxwell’s Equations

2012

The empirical basis of electrodynamics is defined by Faraday’s law of induction, by Gauss’ law, by the law of Biot and Savart and by the Lorentz force and the principle of universal conservation of electric charge. These laws can be tested – confirmed or falsified – in realistic experiments. The integral form of the laws deals with physical objects that are one-dimensional, two-dimensional, or three-dimensional, that is to say, objects such as linear wires, conducting loops, spatial charge distributions, etc. Thus, the integral form depends, to some extent, on the concrete experimental set-up. To unravel the relationships between seemingly different phenomena, one must switch from the integ…

Physicssymbols.namesakeJefimenko's equationsClassical mechanicsTheoretical and experimental justification for the Schrödinger equationMaxwell's equationsMaxwell's equations in curved spacetimesymbolsMatrix representation of Maxwell's equationsInhomogeneous electromagnetic wave equationLorentz forceElectromagnetic tensor
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Elasticity of Poissonian fiber networks

2000

An effective-medium model is introduced for the elasticity of two-dimensional random fiber networks. These networks are commonly used as basic models of heterogeneous fibrous structures such as paper. Using the exact Poissonian statistics to describe the microscopic geometry of the network, the tensile modulus can be expressed by a single-parameter function. This parameter depends on the network density and fiber dimensions, which relate the macroscopic modulus to the relative importance of axial and bending deformations of the fibers. The model agrees well with simulation results and experimental findings. We also discuss the possible generalizations of the model. Peer reviewed

Physicssymbols.namesakePhysicssymbolsModulusYoung's modulusStatistical physicseffective-medium modelselastic propertiesElasticity (economics)Network densityinhomogeneous materials
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Measures with predetermined regularity and inhomogeneous self-similar sets

2016

We show that if $X$ is a uniformly perfect complete metric space satisfying the finite doubling property, then there exists a fully supported measure with lower regularity dimension as close to the lower dimension of $X$ as we wish. Furthermore, we show that, under the condensation open set condition, the lower dimension of an inhomogeneous self-similar set $E_C$ coincides with the lower dimension of the condensation set $C$, while the Assouad dimension of $E_C$ is the maximum of the Assouad dimensions of the corresponding self-similar set $E$ and the condensation set $C$. If the Assouad dimension of $C$ is strictly smaller than the Assouad dimension of $E$, then the upper regularity dimens…

Pure mathematicsAssouad dimensionGeneral MathematicsOpen set01 natural sciencesMeasure (mathematics)Complete metric space54E35010305 fluids & plasmasSet (abstract data type)Dimension (vector space)0103 physical sciencesClassical Analysis and ODEs (math.CA)FOS: Mathematicsinhomogeneous self-similar setMathematics::Metric Geometry28A200101 mathematicsMathematics010102 general mathematicsta111doubling metric space54F45lower dimensionMathematics - Classical Analysis and ODEs28A75uniform perfectness
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