Search results for "Mode-locking"

showing 10 items of 60 documents

Effect of slow gain dynamics in mode-locked fiber lasers: Chirped soliton molecules

2012

We theoretically and experimentally demonstrate the pivotal role of the gain dynamics in the formation of chirped soliton molecules in mode-locked lasers. Such molecules are characterized by an increasing separation from leading to trailing pulses.

Materials sciencebusiness.industryDynamics (mechanics)Physics::OpticsSoliton (optics)Laserlaw.inventionOpticsMode-lockinglawFiber laserOptoelectronicsMoleculePhysics::Atomic PhysicsbusinessNonlinear Sciences::Pattern Formation and Solitons
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Doubly active Q switching and mode locking of an all-fiber laser

2009

Simultaneous and independent active Q switching and active mode locking of an erbium-doped fiber laser is demonstrated using all-fiber modulation techniques. A magnetostrictive rod attached to the output fiber Bragg grating modulates the Q factor of the Fabry-Perot cavity, whereas active mode locking is achieved by amplitude modulation with a Bragg-grating-based acousto-optic device. Fully modulated Q-switched mode-locked trains of optical pulses were obtained for a wide range of pump powers and repetition rates. For a Q-switched repetition rate of 500 Hz and a pump power of 100 mW, the laser generates trains of 12-14 mode-locked pulses of about 1 ns each, within an envelope of 550 ns, an o…

Materials sciencebusiness.industryLaserQ-switchingAtomic and Molecular Physics and Opticslaw.inventionAmplitude modulationOpticsFiber Bragg gratingMode-lockingModulationlawQ factorFiber laserbusiness
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Mode locking of an all-fiber laser by acousto-optic superlattice modulation

2009

Active mode locking of an erbium-doped all-fiber laser with a Bragg-grating-based acousto-optic modulator is demonstrated. The fiber Bragg grating was acoustically modulated by a standing longitudinal elastic wave, which periodically modulates the sidebands at twice the acoustic frequency. The laser has a Fabry-Perot configuration in which cavity loss modulation is achieved by tuning the output fiber Bragg grating to one of the acoustically induced sidebands. Optical pulses at 9 MHz repetition rate, 120 mW peak power, and 780 ps temporal width were obtained. The output results to be stable and has a timing jitter below 40 ps. The measured linewidth, 2.8 pm, demonstrates that these pulses ar…

Materials sciencebusiness.industryPhysics::OpticsLaserAtomic and Molecular Physics and Opticslaw.inventionLaser linewidthOpticsMode-lockingFiber Bragg gratingModulationlawFiber laserbusinessFrequency modulationJitter
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Multi-gigahertz repetition-rate-selectable passive harmonic mode locking of a fiber laser

2013

We demonstrate a passive harmonically mode-locked erbium-doped fiber laser that operates at selectable harmonics spanning from the 6th to the 928th, which corresponds to repetition rates ranging from 153 MHz to 22.2 GHz. The noteworthy laser output stability is attested by supermode suppression levels as large as 41 dB. The influence of a continuous wave background on harmonics stability is tested.

Materials sciencebusiness.industryPhysics::OpticsRangingEquipment DesignLasers Solid-StateLaserAtomic and Molecular Physics and OpticsFeedbacklaw.inventionEquipment Failure AnalysisOpticsMode-lockinglawQuantum dot laserFiber laserHarmonicsHarmonicFiber Optic TechnologyContinuous wavebusinessOptics Express
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Actively mode-locked fiber laser with an acousto-optic in-fiber superlattice modulator

2009

All-fiber lasers permit the development of efficient, robust and compact coherent light sources. However, all-fiber active mode-locking is a challenging objective and very few all-fiber techniques have been published [1–3]. The development of a low-insertion-loss acoustically-induced superlattice modulator that works in the MHz range has demonstrated its suitability to perform active mode-locking of an all-fiber laser. While travelling extensional acoustic waves launched along a fiber Bragg grating (FBG) produce stationary side bands and a frequency shift [4,5], we found that the excitation of a standing extensional acoustic wave should produce no frequency shift, but the amplitude modulati…

Materials sciencebusiness.industryPhysics::Opticschemistry.chemical_elementAcoustic waveLaserlaw.inventionErbiumAmplitude modulationOpticschemistryFiber Bragg gratingMode-lockingModulationlawOptical cavityOptoelectronicsbusinessCLEO/Europe - EQEC 2009 - European Conference on Lasers and Electro-Optics and the European Quantum Electronics Conference
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Actively mode-locked fibre ring laser based on in-fibre acousto-optic amplitude modulation

2011

Recent advances in the development of all-fibre amplitude modulators have led to the implementation of a series of different actively mode-locked fibre lasers [1–4]. In-fibre acousto-optic modulation based on intermodal coupling induced my a standing flexural acoustic wave permits the implementation of broad bandwidth (1.5 nm), high modulation depth (0.72), low-insertion-loss (0.75 dB) all-fibre amplitude modulators that operate in the MHz frequency range. The experimental characterization of a laser with the configuration depicted in Fig. 1 (a) as a function of the radio frequency voltage that controls the modulator (see Fig. 1 (b)), the length of the Erbium doped fibre (EDF), and the opti…

Materials sciencebusiness.industryRing laserFibre optic gyroscopeLaserlaw.inventionSubwavelength-diameter optical fibreAmplitude modulationOpticsMode-lockingFiber Bragg gratinglawFiber laserOptoelectronicsbusiness2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)
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Relative phase locking of pulses in a passively mode-locked fiber laser

2003

In a passively mode-locked fiber ring laser, we report the experimental observation of relative phase locking of pulses in a wide variety of cases. Relative phase locking is observed in bunches of N pulses separated by more than 20 pulse widths as well as in close pulse pairs. In the latter case, the phase relationship between the two pulses is measured to be ±π/2, which is related to theoretical predictions formerly obtained from a Ginzburg-Landau distributed model. We have developed a simplified numerical model adapted to our laser, which keeps its essential features while significantly reducing the number of free parameters. The agreement with the experiment is excellent. © 2003 Optical …

Materials sciencebusiness.industryStatistical and Nonlinear PhysicsLaserPulse shapingAtomic and Molecular Physics and Opticslaw.inventionPulse (physics)BunchesOpticsMode-lockinglawFiber laserSelf-phase modulationbusinessBandwidth-limited pulse
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Actively mode-locked fiber ring laser by intermodal acousto-optic modulation

2010

We report an actively mode-locked fiber ring laser. A simple and low-insertion-loss acousto-optic modulator driven by standing flexural waves, which couples core-to-cladding modes in a standard single-mode optical fiber, is used as an active mechanism for mode locking. Among the remarkable features of the modulator, we mention its high modulation depth (72%), broad bandwidth (187 GHz), easy tunability in the optical wavelength, and low insertion losses (0.7 dB). The narrowest optical pulses obtained were of 95 ps time width, 21 mW peak power, repetition rate of 4.758 MHz, and 110 mW of pump power.

Mode volumeOptical fiberMaterials sciencebusiness.industryPhysics::OpticsPolarization-maintaining optical fiberAtomic and Molecular Physics and Opticslaw.inventionOpticsMode-lockinglawFiber optic sensorFiber laserDispersion-shifted fiberOptoelectronicsPlastic optical fiberbusiness
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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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phase-locked soliton pairs in a fiber ring laser

2002

We have experimentally observed the formation of stable pulse pairs with a π/2 phase difference in a passively mode-locked stretched-pulse fiber ring laser. We have developed a simplified theoretical model that, keeping the essential features of the experiment, reduces greatly the number of free parameters and solved it numerically. The agreement with the experimental results is excellent.

Optical fiberMaterials scienceMode-lockinglawFiber laserPhase (waves)Dispersion-shifted fiberSoliton (optics)Ring laserPolarization-maintaining optical fiberMolecular physicslaw.inventionNonlinear Guided Waves and Their Applications
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