Search results for "nonlinear"

showing 10 items of 3684 documents

Optical Amplification in Hollow-Core Negative-Curvature Fibers Doped with Perovskite CsPbBr3 Nanocrystals

2019

| openaire: EC/H2020/820423/EU//S2QUIP We report a hollow-core negative-curvature fiber (HC-NCF) optical signal amplifier fabricated by the filling of the air microchannels of the fiber with all-inorganic CsPbBr3 perovskite nanocrystals (PNCs). The optimum fabrication conditions were found to enhance the optical gain, up to +3 dB in the best device. Experimental results were approximately reproduced by a gain assisted mechanism based on the nonlinear optical properties of the PNCs, indicating that signal regeneration can be achieved under low pump powers, much below the threshold of stimulated emission. The results can pave the road of new functionalities of the HC-NCF with PNCs, such as op…

FabricationMaterials scienceperovskite nanocrystalsGeneral Chemical Engineeringnonlinear optical properties02 engineering and technology01 natural scienceslcsh:Chemistry010309 opticssignal regeneration/amplification0103 physical sciencesGeneral Materials ScienceStimulated emissionFiberPerovskite (structure)business.industryDopingÒpticahollow core fibers021001 nanoscience & nanotechnologyNonlinear systemlcsh:QD1-999NanocrystalOptoelectronicsMaterials nanoestructurats0210 nano-technologybusinessSignal regenerationNanomaterials
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Implementing a Margolus Neighborhood Cellular Automata on a FPGA

2003

Margolus neighborhood is the easiest form of designing Cellular Automata Rules with features such as invertibility or particle conserving. In this paper we introduce a notation to describe completely a rule based on this neighborhood and implement it in two ways: The first corresponds to a classical RAM-based implementation, while the second, based on concurrent cells, is useful for smaller systems in which time is a critical parameter. This implementation has the feature that the evolution of all the cells in the design is performed in the same clock cycle.

Feature (computer vision)Computer scienceRule-based systemNonlinear Sciences::Cellular Automata and Lattice GasesField-programmable gate arrayAlgorithmCellular automatonReversible cellular automaton
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Feedback Classification and Optimal Control with Applications to the Controlled Lotka-Volterra Model

2023

Let M be a σ-compact C^∞ manifold of dimension n ≥ 2 and consider a single-input control system: ẋ(t) = X (x(t)) + u(t) Y (x(t)), where X , Y are C^∞ vector fields on M. We prove that there exist an open set of pairs (X , Y ) for the C^∞ –Whitney topology such that they admit singular abnormal rays so that the spectrum of the projective singular Hamiltonian dynamics is feedback invariant. It is applied to controlled Lotka–Volterra dynamics where such rays are related to shifted equilibria of the free dynamics.

Feedback classificationLotka-Volterra modelFeedback classification Nonlinear systems Lotka-Volterra model Optimal control Direct numerical methodsDirect numerical methodsNonlinear systems[MATH.MATH-OC] Mathematics [math]/Optimization and Control [math.OC][MATH.MATH-OC]Mathematics [math]/Optimization and Control [math.OC]Optimal control
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Avoiding strange attractors in efficient parametric families of iterative methods for solving nonlinear problems

2019

[EN] Searching zeros of nonlinear functions often employs iterative procedures. In this paper, we construct several families of iterative methods with memory from one without memory, that is, we have increased the order of convergence without adding new functional evaluations. The main aim of this manuscript yields in the advantage that the use of real multidimensional dynamics gives us to decide among the different classes designed and, afterwards, to select its most stable members. Moreover, we have found some elements of the family whose behavior includes strange attractors of different kinds that must be avoided in practice. In this sense, Feigenbaum diagrams have resulted an extremely …

Feigenbaum diagramsNumerical AnalysisMathematical optimizationRelation (database)Iterative methodApplied MathematicsNonlinear problems010103 numerical & computational mathematicsConstruct (python library)01 natural sciencesComputational efficiency010101 applied mathematicsComputational MathematicsNonlinear systemRate of convergenceAttractorIterative methods with and without memoryNumerical tests0101 mathematicsMATEMATICA APLICADAQualitative analysisMathematicsParametric statisticsApplied Numerical Mathematics
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Coherent control in single plasmonic nanostructures

2015

Coherent control in plasmonic nanostructures is a door to space-time confinement of optical excitation and femtosecond super-resolution spectroscopy. Towards this goal, here we demonstrate femtosecond pulse-shaping of single gold nanostructure and local phase compensation.

Femtosecond pulse shapingMaterials scienceNanostructurebusiness.industryOptical physicsPhysics::OpticsNonlinear opticsOptical polarizationCondensed Matter::Materials ScienceCoherent controlFemtosecondPhysics::Atomic and Molecular ClustersOptoelectronicsbusinessPlasmon
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All-fiber processing of terahertz-bandwidth signals based on cascaded tapered fibers

2013

Tapered single-mode fibers are employed to perform dynamic pulse shaping in a bandwidth of several terahertz. The transfer function of cascaded biconical tapers is controlled by introducing a phase shift into one of them through mechanical stretching. It is a simple and low-cost technique with potential to process signals with bandwidths as large as those allocated by standard optical fiber while introducing little degradation. Femtosecond pulses are shaped to prove the concept. (C) 2013 Optical Society of America

Femtosecond pulse shapingMaterials scienceOptical fiberbusiness.industryTerahertz radiationBandwidth (signal processing)Physics::OpticsNonlinear opticsFiber measurementsTransfer functionPulse shapingAtomic and Molecular Physics and Opticslaw.inventionOpticslawTEORIA DE LA SEÑAL Y COMUNICACIONESFemtosecondFiber design and fabricationDispersion.businessOptics Letters
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Towards CEP stable, single-cycle pulse compression with bulk material

2010

We demonstrate both experimentally and numerically that self-steepening during propagation in a hollow-fiber followed by linear propagation through glass in the anomalous dispersion enables pulse compression down to 1.6 cycles at 1.8 µm wavelength.

Femtosecond pulse shapingMaterials sciencebusiness.industryPhysics::OpticsNonlinear opticsSecond-harmonic generationWavelengthOpticsPulse compressionHigh harmonic generationHigh Energy Physics::ExperimentbusinessSelf-phase modulationUltrashort pulseInternational Conference on Ultrafast Phenomena
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All-fibered high-quality low duty-cycle 20-GHz and 40-GHz picosecond pulse sources

2007

International audience; In this work, we demonstrate all-fibered 20-GHz and 40-GHz picosecond pulse sources with duty cycles as low as 1/14. The pulse train is achieved via the high-quality compression of an initial sinusoidal beating through four segments of optical fibers. General design rules are proposed and experimental results are in agreement with numerical predictions.

Femtosecond pulse shapingOptical fiberMaterials science02 engineering and technology01 natural scienceslaw.invention010309 optics020210 optoelectronics & photonicsQuality (physics)OpticsFiber Bragg gratinglaw0103 physical sciences0202 electrical engineering electronic engineering information engineeringPulse waveElectrical and Electronic EngineeringOptical amplifier[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryNonlinear opticsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsPicosecond pulsePulse compressionDuty cycleOptoelectronicsbusinessUltrashort pulsePhase modulation
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320GHz, 640GHz and 1THz femtosecond pulse sources based on multiple four wave mixing in highly non linear optical fibers

2006

Ultra-high repetition rate, transform-limited femtosecond pulse trains have been generated around 1555 nm at 320 GHz, 640 GHz and 1 THz through the compression of a dual frequency beat-signal in a highly nonlinear optical fiber.

Femtosecond pulse shapingOptical fiberMaterials scienceFemtosecond pulsebusiness.industryTerahertz radiationPhysics::OpticsNonlinear optics02 engineering and technology021001 nanoscience & nanotechnology01 natural scienceslaw.invention010309 opticsNonlinear systemFour-wave mixingOpticslawPulse compression0103 physical sciencesOptoelectronics0210 nano-technologybusinessComputingMilieux_MISCELLANEOUS
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Impact of initial pulse shape on the nonlinear spectral compression in optical fibre

2018

International audience; We theoretically study the effects of the temporal intensity profile of the initial pulse on the nonlinear spectral compression process arising from nonlinear propagation in an optical fibre. Various linearly chirped input pulse profiles are considered, and their dynamics is explained with the aid of time-frequency representations. While initially parabolic-shaped pulses show enhanced spectral compression compared to Gaussian pulses, no significant spectral narrowing occurs when initially super-Gaussian pulses are used. Triangular pulses lead to a spectral interference phenomenon similar to the Fresnel bi-prism experiment.

Femtosecond pulse shapingOptical fiberMaterials scienceGaussianNonlinear spectral compression02 engineering and technologynonlinear fiber optics01 natural scienceslaw.invention010309 opticssymbols.namesake020210 optoelectronics & photonicsOpticslaw0103 physical sciences0202 electrical engineering electronic engineering information engineeringElectrical and Electronic Engineering[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryPulse shapingAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsPulse (physics)Nonlinear systemsymbolsbusinessUltrashort pulseBandwidth-limited pulsepulse shaping
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