Search results for "Second-harmonic generation"

showing 10 items of 116 documents

Ultraviolet quasi-phase-matched second harmonic generation in surface periodically poled lithium niobate optical waveguides

2007

The compatibility of low concentration (alpha-phase) proton exchange channel waveguides with electric field surface periodic poling of congruent lithium niobate (SPPLN) crystals has been experimentally demonstrated. With such waveguides, we obtained ultraviolet second harmonic generation (SHG) by first order quasi-phase-matching (QPM), a result made possible by the fabrication, on Z-cut LN crystals, of periodic structures with a pitch down to 750 nm. Nonlinear copropagating QPM-SHG measurements have been carried out on such structures. The pump source was a Ti:sapphire laser with a tunability range of 700-980 nm and a 40 GHz linewidth. We have measured UV continuous wave light at 390 nm by …

Quasi-phase-matchingMaterials sciencebusiness.industryLithium niobateSecond-harmonic generationNonlinear opticsCondensed Matter PhysicsLaserIndustrial and Manufacturing EngineeringAtomic and Molecular Physics and Opticslaw.inventionQPM SHG PPLN Optical Waveguides Nonlinear Opticschemistry.chemical_compoundLaser linewidthOpticschemistryPeriodic polinglawContinuous wavebusinessInstrumentationLaser Physics
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GENERAZIONE DI SECONDA ARMONICA IN GUIDA D’ONDA IN TANTALATO DI LITIO CONGRUENTE CON POLING PERIODICO E CONVERSIONE DI LUNGHEZZA D’ONDA IN BANDA C + L

2010

Here we show the results obtained by the characterization of a lithium-tantalate based device for second-harmonic-generation and all-optical wavelength conversion. The waveguides have been obtained by proton-exchange in a periodically-poled congruent lithium tantalate substrate.

Second-harmonic generation Lithium tantalate Wavelength shifter
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Sensitivity of SHG-FROG for the characterization of ultrahigh-repetition-rate telecommunication laser sources

2004

International audience; We analyze experimentally the sensitivity of second-harmonic generation frequency-resolved optical gating (SHG-FROG) for the complete intensity and phase characterization of both a sinusoidal beat signal and a train of 1.3 ps pulses at a repetition rate of 160 GHz at 1550 nm. Using a commercially-available optical spectrum analyzer in the SHG-FROG set-up, incident pulses with energies of only 125 and 190 fJ, which correspond to the beat signal and the 1.3 ps pulse train, respectively, have been accurately characterized.

Second-harmonic generationIntensityMaterials scienceOptical fiber1.55 MU-MOptical communicationBeat (acoustics)Optical spectrum analyzer02 engineering and technologyGating01 natural scienceslaw.invention010309 optics020210 optoelectronics & photonicsOpticslaw0103 physical sciences0202 electrical engineering electronic engineering information engineeringPulse waveOptical fibersOptical communicationElectrical and Electronic EngineeringInstrumentationFROGHigh bit rate[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]Pulse characterization[ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industry160 GHzSecond-harmonic generationLaserAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsControl and Systems EngineeringTelecommunicationsbusinessOptical Fiber Technology
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Efficient energy conversion for cubic third-harmonic generation that is phase matched in KTiOPO(4).

2000

We demonstrate, for the first time to our knowledge, that efficient third-harmonic generation can be achieved with a cubic contribution much larger than the quadratic processes. An energy-conversion efficiency of 2.4% is achieved for cubic third-harmonic generation that is phase matched along the x axis of a KTiOPO(4) crystal by use of a picosecond fundamental laser emitting at 1618 nm. The associated cascading processes are only 10% of the pure cubic interaction, which is very suitable for study of the specific quantum optical correlations. Calculations of the third-harmonic generation conversion efficiency with respect to group-velocity dispersion and to the longitudinal Gaussian beam pro…

Sum-frequency generationMaterials sciencebusiness.industryEnergy conversion efficiencyPhase (waves)Second-harmonic generationLaserAtomic and Molecular Physics and Opticslaw.inventionOpticslawPicosecondDispersion (optics)businessGaussian beamOptics letters
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A set-up for simultaneous measurement of second harmonic generation and streaming potential and some test applications.

2018

We present a measurement cell that allows simultaneous measurement of second harmonic generation (SHG) and streaming potential (SP) at mineral-water interfaces with flat specimen that are suitable for non-linear optical (NLO) studies. The set-up directly yields SHG data for the interface of interest and can also be used to obtain information concerning the influence of flow on NLO signals from that interface. The streaming potential is at present measured against a reference substrate (PTFE). The properties of this inert reference can be independently determined for the same conditions. With the new cell, for the first time the SHG signal and the SP for flat surfaces have been simultaneousl…

Sum-frequency generationSecond-harmonic generation02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnology01 natural sciencesSignalMolecular physicsStreaming current0104 chemical sciencesSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsBiomaterialsElectrokinetic phenomenaColloid and Surface ChemistryFlow velocityPoint of zero charge0210 nano-technologyPolarization (electrochemistry)Journal of colloid and interface science
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Time evolution of the microwave second-order response of YBaCuO powder

2003

Transient effects in the microwave second-order response of YBaCuO powder are investigated. The time evolution of the second harmonic signal has been measured for about 300 s after the sample had been exposed to variations of the DC magnetic field. We show that in different time scales the transient response has different origin. In the time scale of milliseconds the transient response of samples in the critical state is ascribable to processes of flux redistribution induced by the switching on/off of the microwave field. At longer times, the time evolution of the second harmonic signal can be ascribed to motion of fluxons induced by the variation of the DC magnetic field. In particular, di…

SuperconductivityMillisecondMaterials scienceCondensed matter physicsFluxonCondensed Matter - SuperconductivityTime evolutionEnergy Engineering and Power TechnologySecond-harmonic generationFOS: Physical sciencesCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsMagnetic fieldSuperconductivity (cond-mat.supr-con)Fluxon dynamics Magnetic relaxation Non-linear microwave responseTransient responseElectrical and Electronic EngineeringMicrowave
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Time evolution of the microwave second-harmonic response of MgB2 superconductor

2003

We report on transient effects in the microwave second-order response of two ceramic MgB2 samples. The time evolution of the second-harmonic signal is investigated for about 500 s after the sample has been exposed to a variation of the dc magnetic field. We suggest that during the first seconds the response is determined by diffusive motion of fluxons, while in the time scale of minutes it is ruled by magnetic relaxation over the surface barrier.

SuperconductivityPhysicsCondensed matter physicsFluxonCondensed Matter - SuperconductivityTime evolutionFOS: Physical sciencesEnergy Engineering and Power TechnologySecond-harmonic generationCondensed Matter PhysicsSignalElectronic Optical and Magnetic MaterialsMagnetic fieldSuperconductivity (cond-mat.supr-con)Condensed Matter::SuperconductivityTransient (oscillation)Electrical and Electronic EngineeringMicrowavePhysica C: Superconductivity
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Microwave second-harmonic response of ceramic MgB2 samples

2005

Nonlinear microwave response of different ceramic MgB2 samples has been investigated by the technique of second-harmonic emission. The second-harmonic signal has been investigated as a function of temperature, DC magnetic field and input microwave power. The attention has mainly been devoted to the response at low magnetic fields, where nonlinear processes arising from motion of Abrikosov fluxons are ineffective. The results show that different mechanisms are responsible for the nonlinear response in the different ranges of temperature. At low temperatures, the nonlinear response is due to processes involving weak links. At temperatures close to Tc, a further contribution to the harmonic em…

SuperconductivityPhysicscircuit modelCondensed matter physicsField (physics)Condensed Matter - SuperconductivityVortex flowEnergy Engineering and Power TechnologySecond-harmonic generationFOS: Physical sciencesCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsMagnetic fieldSuperconductivity (cond-mat.supr-con)Nonlinear systemModulationHarmonicHigh temperature superconductorElectrical and Electronic EngineeringMicrowave
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Second-harmonic generation in surface periodically poled lithium niobate waveguides:On the role of multiphoton absorption

2008

Second harmonic generation is investigated in lithium niobate channels realized by proton exchange and quasi-phase-matched by surface periodic-poling. The reduction in conversion efficiency at high powers is interpreted in terms of multi-photon absorption via two-color terms, yielding an estimate of the dominating three-photon process.

Surface (mathematics)Materials sciencePhysics and Astronomy (miscellaneous)Protonbusiness.industryLithium niobateEnergy conversion efficiencyGeneral EngineeringGeneral Physics and AstronomySecond-harmonic generationFOS: Physical sciencesPhysics::Opticschemistry.chemical_compoundchemistryOptoelectronicslithium niobate channel multi-photon absorptionbusinessAbsorption (electromagnetic radiation)Physics - OpticsOptics (physics.optics)
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Frequency doubling in surface periodically poled lithium niobate waveguides: Competing effects

2007

We fabricated α-phase pro ton-exchanged (PE) lithium niobate (LN) channel waveguides quasi phase-matched (QPM) via surface periodic poling (SPP) and carried out the first experimental demonstration of second harmonic generation (SHG) in such devices.[1] Experiments were performed by employing an optical parametric amplifier/oscillator producing 25 ps pulses in the range 1.1-1.6 μm with a line-width less than 2cm−1 and a repetition rate of 10Hz. SHG measurements were performed either at a fixed wavelength by varying the fundamental frequency (FF) input power or by scanning the FF wavelength, ratioing the second harmonic (SH) output to the FF input to obtain the conversion efficiency. By repe…

Surface (mathematics)Optical amplifierMaterials sciencebusiness.industryLithium niobateSecond-harmonic generationPhysics::OpticsWaveguide (optics)Power (physics)chemistry.chemical_compoundTransverse planeOpticschemistryPeriodic polingbusiness
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