Search results for "Fiber lasers"

showing 10 items of 24 documents

Influence of Cavity Loss Upon Performance of Q-Switched Erbium-Doped Fiber Laser

2013

Performance of an actively Q-switched erbium-doped fiber laser in function of intracavity loss is discussed. We show experimentally and theoretically (employing a distributed model that takes into account two contra-propagating laser waves) that the laser performance strongly depends on the intracavity loss of different kinds. We reveal in particular that the dominant source of smaller than expected pulse energy is the loss via excited-state absorption, inherent in erbium-doped fibers. We also discuss the other important processes involved in active Q-switching, such as passive losses and residual active fiber charge, the impact of which is clarified by a straightforward comparison of the m…

Materials sciencebusiness.industryPhysics::OpticsCharge (physics)LaserResidualAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionOpticslawFiber laserFiberLaser power scalingElectrical and Electronic EngineeringbusinessAbsorption (electromagnetic radiation)Erbium doped fiber lasersIEEE Photonics Technology Letters
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Q-switched mode locking noise-like pulse generation from a thulium-doped all-fiber laser based on nonlinear polarization rotation

2021

Abstract Q-switched mode locking (QML) noise-like pulse (NLP) emission from an all-fiber thulium-doped laser based on the nonlinear polarization rotation effect is reported. The QML emission is obtained in a cavity with net anomalous dispersion in a pump power interval in between the CW laser threshold and the threshold of the NLP regime. Highest-energy QML pulses were observed with a repetition rate of 812 kHz with a pump power of 520 mW at the optical wavelength of 1881.09 nm. A maximum overall energy of 460 nJ at an average output power of 6.4 mW was reached, which corresponds to a burst of mode-locked noise-like sub-pulses with 8.7 ns of pulse duration within a QML envelope of 11 µs. Th…

Nonlinear polarization rotationPhysicsQ-switched mode lockingbusiness.industryPhysics::Opticschemistry.chemical_elementPulse durationThulium-doped fiber lasersQC350-467Optics. LightÒpticaLaserNoise (electronics)Atomic and Molecular Physics and OpticsPulse (physics)law.inventionThuliumOpticschemistryMode-lockinglawFiber laserbusinessEnvelope (waves)Results in Optics
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Dissipative soliton resonance in a full polarization-maintaining fiber ring laser at different values of dispersion

2016

We investigated the dissipative solitons resonance in an ytterbium-doped fiber ring laser in which all the elements are polarization maintaining (PM). A semiconductor saturable absorber mirror was used as a mode-locker. The cavity included a normal dispersion single-mode fiber (SMF) and an anomalous dispersion photonic crystal fiber. The change of the length of the PM SMF allows the variation of the net-normal dispersion of the cavity in the range from 0.022 ps2 to 0.262 ps2. As the absolute value of the net-normal dispersion increases from 0.022 ps2 to 0.21 ps2, a square-shaped single pulse transformed to a single right-angle trapezoid-shaped pulse, and, at the dispersion of 0.262 ps2, to …

OnesMaterials scienceCiencias FísicasPhysics::OpticsPolarization-maintaining optical fiberRing laser02 engineering and technology01 natural sciencesGraded-index fiberMolecular physics//purl.org/becyt/ford/1 [https]010309 opticsDissipative soliton020210 optoelectronics & photonicsZero-dispersion wavelengthOpticsFiber laser0103 physical sciencesDispersion (optics)0202 electrical engineering electronic engineering information engineeringModal dispersionDispersion-shifted fiberÓpticabusiness.industryQuantitative Biology::Molecular Networksnonlinear opticsdissipative soliton resonanceSingle-mode optical fiber//purl.org/becyt/ford/1.3 [https]ÒpticaAtomic and Molecular Physics and Opticsfiber lasersPolarization mode dispersionDissipative systembusinessCIENCIAS NATURALES Y EXACTASLatin America Optics and Photonics Conference
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Q switching and mode locking pulse generation from an all-fiber ring laser by intermodal acousto-optic bandpass modulation

2018

Q-switched and mode-locked (QML) pulse generation from an all-fiber ring laser based on intermodal acousto-optic bandpass modulation is reported. The modulator relies on full-acousto-optic mode re-coupling cycle induced by a standing flexural acoustic wave, with a transmission response that is controlled by amplitude modulation of the acoustic wave signal. The Q factor of the cavity is controlled by a rectangular pulse wave with variable frequency and duty cycle, whereas mode locking is achieved by amplitude modulation derived from a standing flexural acoustic wave. The best QML pulses were obtained at 0.5 kHz repetition rate, with a pump power of 549.2 mW, at the optical wavelength of 1568…

Optical fiberMaterials scienceRing laser02 engineering and technologyFiber optics01 natural sciencesIndustrial and Manufacturing Engineeringlaw.invention010309 opticsFiber lasers020210 optoelectronics & photonicsOpticsBand-pass filterlaw0103 physical sciences0202 electrical engineering electronic engineering information engineeringInstrumentationAcousto-optic modulationbusiness.industryCondensed Matter PhysicsQ-switchingAtomic and Molecular Physics and OpticsUNESCO::FÍSICA::Óptica ::Fibras ópticasPulse (physics)Q-switched and mode-lockedAll fiberMode-lockingModulation:FÍSICA::Óptica ::Fibras ópticas [UNESCO]business
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Spatiotemporal pulse shaping with multimode nonlinear guided waves

2018

We experimentally and theoretically investigate complex temporal pulse reshaping that accompanies Kerr beam self-cleaning in multimode optical fibers. We also study the output beam shape dependence on initial conditions.

Optical fiberMaterials scienceand opticsPhysics::OpticsComputer Science::Human-Computer Interaction02 engineering and technologynonlinear fiber optics01 natural scienceslaw.invention010309 opticsOpticslawFiber laser0103 physical sciencesatomic and molecular physicsoptical and magnetic materialsComputingMilieux_MISCELLANEOUS[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]Multi-mode optical fiberbusiness.industryelectronic021001 nanoscience & nanotechnologyPulse shapingPulse (physics)fiber lasersNonlinear systempulse propagation and optical solitonstransverse effectsPhysics::Accelerator Physicsfiber lasers; nonlinear fiber optics; pulse propagation and optical solitons; transverse effects; electronic optical and magnetic materials; atomic and molecular physics and opticsPhotonics0210 nano-technologybusinessBeam (structure)
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Experimental study of an in-fiber acousto-optic tunable bandpass filter for single- and dual-wavelength operation in a thulium-doped fiber laser

2019

A tunable single- and dual-wavelength thulium-doped all-fiber laser is demonstrated based on the implementation of an in-fiber acousto-optic tunable bandpass filter (AOTBF). The AOTBF is fabricated to be operated in the 1.9 µm region, and takes advantage of the intermodal coupling effect produced by traveling flexural acoustic waves in an optical fiber. It exhibits a 3-dB bandwidth of 2.04 nm with an insertion loss of 4.75 dB. The tuning properties of the AO device allows a continuous-wave operation with characteristics of wide tuning range (211.5 nm), narrow linewidth (50 pm) and high signal-to-noise ratio (60 dB). In the dual-wavelength regime, the laser is capable of independent tuning o…

Optical fiberMaterials scienceoptical fibers02 engineering and technology01 natural scienceslaw.invention010309 opticsLaser linewidthOpticsFiber Bragg gratingBand-pass filterlawFiber laser0103 physical sciencesInsertion lossUNESCO::FÍSICA::Ópticabusiness.industry021001 nanoscience & nanotechnologyLaserAtomic and Molecular Physics and Opticsacousto-optic interactionfiber lasersWavelength:FÍSICA::Óptica [UNESCO]0210 nano-technologybusiness
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A laser-based system for a fast and accurate measurement of gain and linearity of photomultipliers

2018

This paper describes a method for the measurement of gain and linearity of photomultipliers (PMTs). Gain and linearity are two fundamental parameters to use properly a PMT in several physics experiments. In the developed system light is laser generated and adressed to the PMT through a set of optical fibers. The data acquisition system consists in a commercial 16 channel digitizer coupled to a custom front-end board. With the chosen digitizer the system is scalable to test up to 16 PMTs, with the aid of a light distribution system and a multi-channel version of the front-end board. Data analysis is performed by a custom acquisition software. A 1.5» Hamamatsu PMT is used to validate the syst…

PhotomultiplierOptical fiberMaterials scienceDistribution (number theory)Fiber Laservisible and IR photons (vacuum) (photomultipliers01 natural sciencesAnalogue electronic circuit030218 nuclear medicine & medical imaginglaw.invention03 medical and health sciences0302 clinical medicineData acquisitionOpticslawFront-end electronics for detector readout0103 physical sciencesPhoton detectors for UV visible and IR photons (vacuum) (photomultipliers HPDs others); Front-end electronics for detector readout; Analogue electronic circuits; Fiber LasersPhoton detectors for UVInstrumentationMathematical PhysicsFiber LasersData processing010308 nuclear & particles physicsbusiness.industrySettore FIS/01 - Fisica SperimentaleLinearityLaserPhoton detectors for UV visible and IR photons (vacuum) (photomultipliers HPDs others)HPDsAnalogue electronic circuitsothers)businessJournal of Instrumentation
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Dynamics of the transition from polarization disorder to antiphase polarization domains in vector fiber lasers

2014

We demonstrate that nonlinear polarization coupling in a fiber ring laser without polarization-selective elements, subject to the effects of average anomalous dispersion, Kerr effect, and nonlinear gain saturation, can lead to the antisynchronization of spatiotemporal chaos into a wide variety of ordered laminar states of orthogonal polarization temporal domains. These antiphase polarization domains include stable lattices of soliton trains with high duty cycle at repetition rates of hundreds of MHz, as well as sparse trains of coupled dark and bright solitary waves.

PhysicsKerr effectPolarization rotatorring lasersCondensed matter physicsOrthogonal polarization spectral imagingbusiness.industryRing laserLaminar flowFiber lasers; ring lasers; solitonsPolarization (waves)Atomic and Molecular Physics and OpticsFiber lasersOpticsDuty cycleFiber lasersolitonsbusiness
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Sub-200-kHz single soliton generation in a long ring Er-fiber laser with strict polarization control by using twisted fiber

2020

Abstract In the present work we demonstrate a novel single-soliton ultra-low pulse repetition frequency passively mode-locked erbium-doped fiber laser. We mitigate the residual linear birefringence of fiber by fiber twist to achieve a strict control of polarization. For mode-locking the nonlinear polarization rotation (NPR) was used. Special technique was applied to reduce the overdriving of NPR that allows the generation of single soliton in ultra-long cavity. The strict control of polarization yields a stable relation between the polarization state of the pulses propagating in the cavity and the regimes of generation. A 192.12-kHz train of soliton pulses was obtained with pulse duration o…

Pulse repetition frequencyPhysics::Optics02 engineering and technology01 natural sciences010309 optics020210 optoelectronics & photonicsOptics:FÍSICA [UNESCO]Fiber laser0103 physical sciences0202 electrical engineering electronic engineering information engineeringsolitonsultra-long laser cavityElectrical and Electronic EngineeringTwistmode-locked fiber lasersPhysicsbusiness.industrynonlinear opticsUNESCO::FÍSICAPulse durationNonlinear opticsNonlinear polarizationPolarization (waves)Atomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialsoverdriving nonlinear effectsSolitonbusiness
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Highly Efficient Holmium-Doped All-Fiber ∼2.07-μm Laser Pumped by Ytterbium-Doped Fiber Laser at ∼1.13 μm

2018

We report a 2.07-μm Holmium-doped all-fiber laser (HDFL) pumped by a 1.13-μm Ytterbium-doped fiber laser (YDFL). Home-made alumino–germano–silicate holmium-doped fiber (HDF) served here as an active medium, optimized in terms of chemical composition and co-dopants’ concentrations. Laser action at 2.07 μm was assessed in simple Fabry–Perot cavity, formed by a couple of home-made fiber Bragg gratings (FBGs), inscribed directly in the HDF; this allowed notable diminishing of intracavity loss of the 2.07-μm laser. HDF was in-core pumped by the 1.13-μm double-clad YDFL with a power of ∼12.5 W, in turn pumped in-clad by a laser diode (LD) operated at 0.97 μm with ∼24.5-W output. Using optimal len…

YtterbiumMaterials sciencechemistry.chemical_element02 engineering and technology01 natural scienceslaw.invention010309 opticsHolmium020210 optoelectronics & photonicsFiber Bragg gratinglawFiber laser0103 physical sciences0202 electrical engineering electronic engineering information engineeringElectrical and Electronic EngineeringLaser diodebusiness.industrySlope efficiencyLaserUNESCO::FÍSICA::Óptica ::Fibras ópticasAtomic and Molecular Physics and Opticschemistry:FÍSICA::Óptica ::Fibras ópticas [UNESCO]OptoelectronicsOptical fiber lasersQuantum efficiencybusinessHolmiumIEEE Journal of Selected Topics in Quantum Electronics
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