Search results for "Scaling"

showing 10 items of 754 documents

Switching times in long-overlap Josephson junctions subject to thermal fluctuations and non-Gaussian noise sources

2014

We investigate the superconducting lifetime of long current-biased Josephson junctions, in the presence of Gaussian and non-Gaussian noise sources. In particular, we analyze the dynamics of a Josephson junction as a function of the noise signal intensity, for different values of the parameters of the system and external driving currents. We find that the mean lifetime of the superconductive state is characterized by nonmonotonic behavior as a function of noise intensity, driving frequency and junction length. We observe that these nonmonotonic behaviours are connected with the dynamics of the junction phase string during the switching towards the resistive state. An important role is played…

DYNAMICSJosephson effectKRAMERS PROBLEMPhase (waves)Thermal fluctuationsFOS: Physical sciencesNoise processes and phenomenaSettore FIS/03 - Fisica Della MateriaPi Josephson junctionSuperconductivity (cond-mat.supr-con)symbols.namesakeLEVY FLIGHTSCALING LAWSCondensed Matter::SuperconductivityMesoscale and Nanoscale Physics (cond-mat.mes-hall)Stochastic analysis methodFluctuation phenomenaANOMALOUS DIFFUSIONENHANCED STABILITYSuperconductivityPhysicsRESONANT ACTIVATIONCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsNoise (signal processing)Condensed Matter - SuperconductivityBiasingJosephson deviceCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsZERO-VOLTAGE STATEGaussian noisesymbolsZERO-VOLTAGE STATE; ALPHA-STABLE NOISE; RESONANT ACTIVATION; LEVY FLIGHT; ANOMALOUS DIFFUSION; ENHANCED STABILITY; KRAMERS PROBLEM; SCALING LAWS; DYNAMICS; BEHAVIORALPHA-STABLE NOISEBEHAVIOR
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Fast evaluation of a linear number of local exchange matrices

2002

A fast method is described for evaluating multiple exchange matrices in a Gaussian atomic orbital basis. For insulators, it is asymptotically linear scaling, and is a generalization of the linear scaling exchange (LinK) method, which was formulated for a single exchange matrix [J. Chem. Phys. 109 (1998) 1663]. It is employed to evaluate exchange-type contractions of all derivative density matrices with two-electron integrals for a series of linear alkanes, linear polyacenes, and water clusters using STO-3G, 3-21G, and 6-31G* basis sets. Significant computational savings are obtained for molecules with as few as 10 non-hydrogen atoms.

Density matrixSeries (mathematics)Basis (linear algebra)ChemistryGaussianGeneral Physics and AstronomyDerivativesymbols.namesakeComputational chemistryLinear scalesymbolsExchange matrixStatistical physicsPhysical and Theoretical ChemistryScalingChemical Physics Letters
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Sparse Image Representation by Directionlets

2010

Despite the success of the standard wavelet transform (WT) in image processing in recent years, the efficiency and sparsity of its representation are limited by the spatial symmetry and separability of its basis functions built in the horizontal and vertical directions. One-dimensional discontinuities in images (edges or contours), which are important elements in visual perception, intersect too many wavelet basis functions and lead to a non-sparse representation. To capture efficiently these elongated structures characterized by geometrical regularity along different directions (not only the horizontal and vertical), a more complex multidirectional (M-DIR) and asymmetric transform is requi…

Directional transformsbusiness.industryMultiresolution analysisWavelet transformImage codingImage processingDirectional vanishing momentsContourletImage orientation analysisWavelet transformsWaveletCurveletImage scalingImage interpolationComputer visionSeparable transformsArtificial intelligencebusinessAlgorithmMultiresolution analysisSparse representationMathematicsImage compression
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Resonance between Cantor sets

2007

Let $C_a$ be the central Cantor set obtained by removing a central interval of length $1-2a$ from the unit interval, and continuing this process inductively on each of the remaining two intervals. We prove that if $\log b/\log a$ is irrational, then \[ \dim(C_a+C_b) = \min(\dim(C_a) + \dim(C_b),1), \] where $\dim$ is Hausdorff dimension. More generally, given two self-similar sets $K,K'$ in $\RR$ and a scaling parameter $s>0$, if the dimension of the arithmetic sum $K+sK'$ is strictly smaller than $\dim(K)+\dim(K') \le 1$ (``geometric resonance''), then there exists $r<1$ such that all contraction ratios of the similitudes defining $K$ and $K'$ are powers of $r$ (``algebraic resonance…

Discrete mathematicsApplied MathematicsGeneral Mathematics010102 general mathematicsDynamical Systems (math.DS)01 natural sciences010305 fluids & plasmasIrrational rotationCantor setIterated function systemMathematics - Classical Analysis and ODEs28A80 28A78Irrational numberHausdorff dimension0103 physical sciencesArithmetic progressionClassical Analysis and ODEs (math.CA)FOS: MathematicsMathematics - Dynamical Systems0101 mathematicsAlgebraic numberScalingMathematics
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Scaling properties of topologically random channel networks

1996

Abstract The analysis deals with the scaling properties of infinite topologically random channel networks (ITRNs) fast introduced by Shreve (1967, J. Geol. , 75: 179–186) to model the branching structure of rivers as a random process. The expected configuration of ITRNs displays scaling behaviour only asymptotically, when the ruler (or ‘yardstick’) length is reduced to a very small extent. The random model can also reproduce scaling behaviour at larger ruler lengths if network magnitude and diameter are functionally related according to a reported deterministic rule. This indicates that subsets of rrRNs can be scaling and, although rrRNs are asymptotically plane-filling due to the law of la…

Discrete mathematicsDimension (vector space)YardstickLaw of large numbersStochastic processStructure (category theory)Magnitude (mathematics)Statistical physicsScalingWater Science and TechnologyMathematicsCommunication channelJournal of Hydrology
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A distributed model for continuous-wave erbium-doped fiber laser

2011

Abstract A distributed model of a continuous-wave erbium-doped fiber laser is discussed. The model is based on two contra-propagated traveling laser waves, and includes inhomogeneous pumping, excited state absorption at the pump and the laser wavelengths, amplified spontaneous emission and radial distribution of populations of erbium levels. It is shown that excited state absorption is a main limiting factor to the laser's efficiency. Moreover, consideration of radial distributions of erbium levels' populations in the model reduces laser efficiency and decreases optimal reflection of the laser output coupler. The modeling results are in excellent agreement with the experimental study on the…

Distributed feedback laserActive laser mediumMaterials sciencebusiness.industryPhysics::Opticschemistry.chemical_elementOutput couplerLaser pumpingLaserAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionErbiumOpticschemistrylawFiber laserPhysics::Atomic PhysicsLaser power scalingElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessOptics Communications
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High-efficiency Q-switched erbium fiber laser using a Bragg grating-based modulator

2002

Abstract In this work we analyze the behavior of an erbium-doped fiber laser which is based on a simple scheme. Excitation of the active medium is performed in the 980 nm pump band with a CW semiconductor laser source. Two fiber Bragg gratings acting as mirrors of the Fabry–Perot laser cavity were used. One of these gratings was mounted over a piezoelectric (PZT) element. By applying voltage pulses to the piezoelectric, the laser cavity was temporally modulated and Q-switched laser pulses up to 530 mW peak powers at 3 kHz were obtained. Typical laser emission of 2–3 μs temporal widths and 0.1 nm of optical bandwidth have been achieved when the system was operated at 18.5 kHz repetition rate…

Distributed feedback laserMaterials scienceActive laser mediumbusiness.industryLaser pumpingLaserAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsSelf-pulsationlaw.inventionOpticsFiber Bragg gratinglawFiber laserOptoelectronicsLaser power scalingElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessOptics Communications
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Dual-kind Q-switching of erbium fiber laser

2014

Two different regimes of Q-switching in the same implementation of an actively Q-switched erbium-doped fiber laser are demonstrated. Depending on the active fiber length and repetition rate of an intracavity Q-cell (acousto-optic modulator), the laser operates either in the regime of common, rather long and low-power, pulses composed of several sub-pulses or in the one of very short and powerful stimulated Brillouin scattering-induced pulses. The basic physical reason of the laser system to oscillate in one of these two regimes is the existence or absence of CW narrow-line “bad-cavity” lasing in the intervals when the Q-cell is blocked.

Distributed feedback laserMaterials sciencePhysics and Astronomy (miscellaneous)business.industryPhysics::OpticsFísicaLaser pumpingÒpticaLaserQ-switchingGain-switchinglaw.inventionOpticslawFiber laserOptoelectronicsLaser power scalingbusinessLasing threshold
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Nonlinear dynamics of a two-photon Fabry–Pérot laser

2000

Abstract The steady-state emission, stability and temporal dynamics of a single-mode two-photon laser with a Fabry–Perot cavity is investigated and compared with that of a ring-cavity laser. It is found that the Fabry–Perot cavity makes the laser less efficient than the ring cavity because of spatial hole burning, but the domain of stability is larger for the Fabry–Perot laser. The intensity and phase dynamics are numerically investigated and distinctive features are found in the phase dynamics as compared with one-photon lasers.

Distributed feedback laserMaterials sciencePhysics::Instrumentation and Detectorsbusiness.industryAstrophysics::Instrumentation and Methods for AstrophysicsPhysics::OpticsInjection seederLaserAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsIntensity (physics)law.inventionNonlinear systemOpticsTwo-photon excitation microscopylawPhysics::Atomic PhysicsLaser power scalingElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessFabry–Pérot interferometerOptics Communications
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Polarization switchable Erbium-doped all-fiber laser

2008

We report an experimental study of an erbium-doped all-fiber laser with electrically switchable output polarization. Fiber Bragg grating written in a polarization maintaining optical fiber and attached to a piezo-ceramic actuator is used to commute the polarization state of the laser emission. The laser oscillates at one of two orthogonal polarizations depending on voltage applied to the actuator.

Distributed feedback laserMaterials sciencePolarization rotatorPhysics and Astronomy (miscellaneous)business.industryPhysics::OpticsPolarization-maintaining optical fiberLaserlaw.inventionCondensed Matter::Materials ScienceOpticsFiber Bragg gratinglawFiber laserRadial polarizationPhysics::Atomic PhysicsLaser power scalingbusinessInstrumentationLaser Physics Letters
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