Search results for "Fabry–Pérot interferometer"

showing 10 items of 25 documents

Er:Cr:YSGG laser with electrooptic PLZT ceramics Q-switching Fabry-Perot interferometer output mirror

2001

Summary form only given. Q-switching of Er:Cr:YSGG laser with transparent PLZT ceramics electro-optic modulators was reported previously. The extremely large quadratic EO effect in PLZT allows to build small size moderate control voltages. The high induced birefringence in PLZT results from an essential contribution to polarization (and consequently to the birefringence) of processes with longer relaxation times up to seconds, corresponding to the Er:Cr:YSGG laser operating rate. PLZT ceramics have also a high value of the refractive index (n /spl ap/ 2.2-2.3 for /spl lambda/ = 3 /spl mu/m, slightly depending on PLZT composition and temperature) and thus considerable Fresnel reflections R/s…

BirefringenceKerr effectMaterials sciencebusiness.industrychemistry.chemical_elementLaserQ-switchinglaw.inventionErbiumOpticschemistrylawSapphireOptoelectronicsbusinessRefractive indexFabry–Pérot interferometerTechnical Digest. Summaries of papers presented at the Conference on Lasers and Electro-Optics. Postconference Technical Digest (IEEE Cat. No.01CH37170)
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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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Development of a saturated absorption spectroscopy setup at IGISOL for characterisation of Fabry-Pérot interferometers

2016

A saturated absorption spectroscopy setup was developed and optimised for the characterisation of a home-built and a commercial Fabry-Pérot interferometer (FPI). The free spectral range of these FPIs has been determined with reliable statistical and systematic errors. These FPIs will be used for accurate wavelength determination of broad- and narrowband pulsed Ti:sapphire lasers used in resonance ionisation spectroscopy experiments. peerReviewed

Fabry-Pérot interferometerNuclear and High Energy PhysicsAbsorption spectroscopyChemistrybusiness.industrySaturated absorption spectroscopyCondensed Matter Physics01 natural sciencesAtomic and Molecular Physics and Optics010309 opticsrubidiumInterferometryOptics0103 physical sciencesAstronomical interferometerPhysical and Theoretical Chemistry010306 general physicsAbsorption (electromagnetic radiation)Spectroscopybusinesssaturation spectroscopyFabry–Pérot interferometerFree spectral rangeHyperfine Interactions
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Application of Thin ZnO ALD Layers in Fiber-Optic Fabry-Pérot Sensing Interferometers

2016

International audience; In this paper we investigated the response of a fiber-optic Fabry-Pérot sensing interferometer with thin ZnO layers deposited on the end faces of the optical fibers forming the cavity. Standard telecommunication single-mode optical fiber (SMF-28) segments were used with the thin ZnO layers deposited by Atomic Layer Deposition (ALD). Measurements were performed with the interferometer illuminated by two broadband sources operating at 1300 nm and 1550 nm. Reflected interference signal was acquired by an optical spectrum analyzer while the length of the air cavity was varied. Thickness of the ZnO layers used in the experiments was 50 nm, 100 nm, and 200 nm. Uncoated SMF…

Fabry-Pérot interferometerOptical fiberMaterials scienceinterferenceZnO layer02 engineering and technologylcsh:Chemical technologyInterference (wave propagation)01 natural sciencesBiochemistryArticleAnalytical Chemistrylaw.inventionAtomic layer depositionOpticslawAstronomical interferometerlcsh:TP1-1185Fiber[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Electrical and Electronic EngineeringInstrumentation[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]business.industry010401 analytical chemistry021001 nanoscience & nanotechnologyAtomic and Molecular Physics and Optics0104 chemical sciencesInterferometryAtomic Layer DepositionFabry-Pérot interferometer; Atomic Layer Deposition; ZnO layer; interference0210 nano-technologybusinessRefractive indexFabry–Pérot interferometer
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Monitoring the Growth of a Microbubble Generated Photothermally onto an Optical Fiber by Means Fabry-Perot Interferometry.

2021

In the present paper, we show the experimental measurement of the growth of a microbubble created on the tip of a single mode optical fiber, in which zinc nanoparticles were photodeposited on its core by using a single laser source to carry out both the generation of the microbubble by photothermal effect and the monitoring of the microbubble diameter. The photodeposition technique, as well as the formation of the microbubble, was carried out by using a single-mode pigtailed laser diode with emission at a wavelength of 658 nm. The microbubble’s growth was analyzed in the time domain by the analysis of the Fabry–Perot cavity, whose diameter was calculated with the number of interference frin…

Fabry–Perotoptical fiberMaterials scienceOptical fiberfabry-pérotmicrobubble02 engineering and technologycavitylcsh:Chemical technology01 natural sciencesBiochemistryAnalytical Chemistrylaw.invention010309 opticsOptics:FÍSICA [UNESCO]law0103 physical scienceslcsh:TP1-1185Electrical and Electronic EngineeringOscilloscopeInstrumentationLaser diodebusiness.industryCommunicationPhotothermal effectUNESCO::FÍSICASingle-mode optical fiber021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsInterferometry0210 nano-technologybusinessvibrometerLaser Doppler vibrometerFabry–Pérot interferometerSensors (Basel, Switzerland)
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Class-B two-photon Fabry–Pérot laser

1998

Abstract We study the stationary operation and stability properties of a class-B two-photon Fabry–Perot laser. We show that, differently from the one-photon laser, the intensity emitted by the two-photon laser is larger in a Fabry–Perot than in a ring cavity. The lasing solution loses stability through a subcritical Hopf bifurcation, as it occurs in the unidirectional ring laser. The stability domain in the parameter space is larger in the Fabry–Perot than in the ring cavity configuration.

Hopf bifurcationPhysicsDistributed feedback laserPhysics::Instrumentation and Detectorsbusiness.industryAstrophysics::Instrumentation and Methods for AstrophysicsPhysics::OpticsRing laserLaserAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsRound-trip gainlaw.inventionsymbols.namesakeOpticslawsymbolsLaser power scalingElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessLasing thresholdFabry–Pérot interferometerOptics Communications
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One- and two-photon lasers with injected signal in a high-Q fabry-Pérot cavity

2000

Explicit models are derived for good cavity one- and two-photon lasers with an injected signal in a Fabry-Perot cavity. The steady solutions and their stability properties are obtained analytically and compared with the corresponding ring cavity model ones. Only quantitative differences between both types of cavities are found. In particular we show that (i) the Fabry-Perot cavity reduces significantly the domain of self-pulsing with respect to the ring cavity, and for the two-photon laser case (ii) larger output can be extracted from a Fabry-Perot cavity than from a ring cavity under certain conditions, something impossible in free-running lasers. We conclude that ring cavity models are se…

Hopf bifurcationPhysicsPhysics::Instrumentation and Detectorsbusiness.industryAstrophysics::Instrumentation and Methods for AstrophysicsPhysics::OpticsLaserRing (chemistry)SignalAtomic and Molecular Physics and Opticslaw.inventionLongitudinal modesymbols.namesakeOpticslawOptical cavityDomain (ring theory)symbolsPhysics::Accelerator PhysicsAtomic physicsbusinessFabry–Pérot interferometerJournal of Modern Optics
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ALD thin ZnO layer as an active medium in a fiber-optic Fabry–Perot interferometer

2015

Abstract A novel optical fiber sensor of temperature using a thin ZnO layer fabricated by atomic layer deposition (ALD) is demonstrated for the first time. The thin ZnO layer was grown on the face of a standard optical telecommunication fiber SMF-28 and operates as a Fabry–Perot interferometer sensitive to temperature. The interferometer characterization was made in the temperature range extending from 50 to 300 °C with resolution equal to 1 °C. The output signal was analyzed by measurement of the shift of the maxima in spectral pattern. The sensitivity of temperature measurement is about 0.05 nm/°C. Furthermore, very good linearity of the sensor was achieved with correlation coefficient R2…

Materials science02 engineering and technology01 natural sciencesTemperature measurementAtomic layer depositionOptics0103 physical sciences[CHIM]Chemical SciencesFiberElectrical and Electronic EngineeringInstrumentationComputingMilieux_MISCELLANEOUS010302 applied physicsbusiness.industryMetals and AlloysAtmospheric temperature range021001 nanoscience & nanotechnologyCondensed Matter PhysicsSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsInterferometryFiber optic sensor0210 nano-technologybusinessLayer (electronics)Fabry–Pérot interferometer
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Infrared laser threshold magnetometry with a NV doped diamond intracavity etalon

2019

International audience; We propose a hybrid laser system consisting of a semiconductor external cavity laser associated to an intra-cavity diamond etalon doped with nitrogen-vacancy color centers. We consider laser emission tuned to the infrared absorption line that is enhanced under the magnetic field dependent nitrogen-vacancy electron spin resonance and show that this architecture leads to a compact solid-state magnetometer that can be operated at room-temperature. The sensitivity to the magnetic field limited by the photon shot-noise of the output laser beam is estimated to be less than 1 pT/ √ Hz. Unlike usual NV center infrared magnetometry, this method would not require an external f…

Materials scienceAbsorption spectroscopyMagnetometerInfraredPhysics::Optics02 engineering and technologyengineering.material01 natural scienceslaw.invention010309 opticsOptics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]law0103 physical sciencesPhysics::Atomic PhysicsAbsorption (electromagnetic radiation)[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryFar-infrared laserDiamond021001 nanoscience & nanotechnologyLaserAtomic and Molecular Physics and Optics[SPI.ELEC]Engineering Sciences [physics]/Electromagnetismengineering[SPI.OPTI]Engineering Sciences [physics]/Optics / Photonic0210 nano-technologybusinessFabry–Pérot interferometer
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Ultrahigh-Q Tunable Whispering-Gallery-Mode Microresonator

2009

Typical microresonators exhibit a large frequency spacing between resonances and a limited tunability. This impedes their use in a large class of applications which require a resonance of the microcavity to coincide with a predetermined frequency. Here, we experimentally overcome this limitation with highly prolate-shaped whispering-gallery-mode "bottle microresonators" fabricated from standard optical glass fibers. Our resonators combine an ultra-high quality factor of 360 million, a small mode volume, and near lossless fibre coupling, characteristic of whispering-gallery-mode resonators, with a simple and customizable mode structure enabling full tunability.

Materials sciencePhotonOptical fiberGeneral Physics and AstronomyFOS: Physical sciencesPhysics::OpticsPHOTONSOPTICAL MICROCAVITIESlaw.inventionStanding waveResonatorRESONATORSQuality (physics)OpticslawMICROSPHERE LASERPhysicsMode volumeTotal internal reflectionbusiness.industryCHIPCavity quantum electrodynamicsResonanceONE-ATOMChipFIBER TAPERAtom opticsCAVITYOptoelectronicsWhispering-gallery wavebusinessFabry–Pérot interferometerPhysics - OpticsOptics (physics.optics)GENERATIONPhysical Review Letters
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