Search results for "Doped Fiber"

showing 10 items of 11 documents

ASE narrow‐band noise pulsing in erbium‐doped fiber amplifier and its effect on self‐phase modulation

2019

In this paper, we report a study of the features of polarized and unpolarized narrow-band amplified spontaneous emission (ASE) in a low-doped erbium fiber at 976-nm pumping. We demonstrate that ASE noise can be treated as a train of Gaussian-like pulses with random magnitudes, widths, and inter-pulse intervals. ASE noise can also provide a statistical analysis of these three parameters. We also present the data that reveal ASE noise’s role in optical spectrum broadening through self-phase modulation of light propagating in a communication fiber. In particular, the data show that the ASE noise derivative defines the broadening’s spectral shape.

Amplified spontaneous emissionMaterials scienceSpectral shape analysischemistry.chemical_elementPhysics::OpticsLaser02 engineering and technology01 natural sciencesASE010309 opticsErbiumOpticsFiber Bragg grating0103 physical sciencesComputer Science::Networking and Internet ArchitectureFiberSelf-phase modulationbusiness.industryFiber Optic021001 nanoscience & nanotechnologyDoped FiberAtomic and Molecular Physics and OpticsUNESCO::FÍSICA::Óptica ::Fibras ópticaschemistryModulation:FÍSICA::Óptica ::Fibras ópticas [UNESCO]0210 nano-technologybusinessNoise (radio)
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Long- and short-term stability of all polarization-maintaining thulium doped passively mode-locked fiber lasers with emission wavelengths at 1.95 µm …

2023

In this work, we compare the operation of a passively modelocked polarization-maintaining emission in two thulium-doped fiber lasers pumped at 1561 nm, with emission at wavelengths of 1.951 μm in one case and 2.07 μm in the other. We obtained a sequence of light pulses at 15.6 MHz, whose temporal width was 81 ps at 1.95 μm, and a sequence of light pulses at 13.1 MHz, whose temporal width was 94 ps at 2.07 μm. Finally, we also measured the long-term stability of this setup during a 24-h operation, as well as the short-term stability in a simulated harsh environment. The results confirm the superior performance of fiber laser systems with a fully polarization-maintaining design.

Fluid Flow and Transfer Processespassive mode-lockingProcess Chemistry and TechnologyPOLARIZACIONGeneral EngineeringFísicaÒpticathulium doped fibersfiber lasersComputer Science ApplicationsFIBRAS DOPADAS CON TULIOpolarization-maintainingLASER DE FIBRAGeneral Materials ScienceInstrumentation
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Optical Soliton Molecules in Fiber Lasers

2006

Recent experiments demonstrate that fiber laser cavities are able to support various multisoliton complexes, analogous to soliton molecules, which could have impact on optical information transmission or storage. These advances are guided by the concept of dissipative soliton.

Information transmissionMaterials sciencebusiness.industryFiber nonlinear opticsPhysics::Optics01 natural sciences3. Good health010309 opticsDissipative solitonNonlinear Sciences::Exactly Solvable and Integrable SystemsOpticsFiber laser0103 physical sciencesLaser mode lockingOptoelectronicsMoleculeSoliton010306 general physicsbusinessNonlinear Sciences::Pattern Formation and SolitonsErbium doped fiber lasersComputingMilieux_MISCELLANEOUS
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Influence of Ce codoping and H2 pre-loading on Er/Yb-doped fiber: Radiation response characterized by Confocal Micro-Luminescence

2011

International audience; Confocal microscopy luminescence measurements were applied to study the X-ray radiation response of Er/Yb-doped optical fibers in connection with H2 pre-loading and with the addition of another lanthanide element (Cerium) in the core composition. Laser excitations at 488 nm and 325 nm allow deriving the emission and absorption pattern of Er3+, the latter derived from the dips appearing in a wide luminescence band related to defects in silica. We found that the luminescence spectrum of the X-irradiated Er/Yb-doped core fiber evidences an increase in the emission intensity around 520 and 660 nm; in contrast, no changes are induced by radiation neither after H2 pre-load…

LanthanideMaterials sciencePhotoluminescenceOptical fiberOptica fiber; Er/Yb doping; Ce doping; confocal micro-luminescencechemistry.chemical_elementlaw.inventionOpticsMicro-luminescencelawRare earthMaterials ChemistryEr/Yb dopingFiberAbsorption (electromagnetic radiation)Ce dopingconfocal micro-luminescence[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]business.industrySilicaErbium doped fibersCondensed Matter PhysicsLaserOptica fiberElectronic Optical and Magnetic MaterialsCeriumchemistryCeramics and CompositesOptoelectronicsDefectsLuminescencebusiness
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Cladding-Pumped Erbium/Ytterbium Co-Doped Fiber Amplifier for C-Band Operation in Optical Networks

2021

Space-division multiplexing (SDM) attracts attention to cladding-pumped optical amplifiers, but they suffer from a low pump power conversion efficiency. To address this issue, ytterbium (Yb3+) and erbium (Er3+) co-doping is considered as an effective approach. However, it changes the gain profile of Er3+-doped fiber amplifiers and induces the gain difference between optical wavelengths in the C-band, significantly limiting the effective band of the dense wavelength-division multiplexed (DWDM) system. This paper is devoted to a detailed study of a cladding-pumped Er3+/Yb3+ co-doped fiber amplifier (EYDFA) through numerical simulations aiming to identify a configuration, before assembling a s…

Materials scienceActive laser mediumchemistry.chemical_elementOptical power02 engineering and technologyNoise figure01 natural scienceslcsh:Technologyoptical fiber networkAbsolute gain010309 opticsErbiumlcsh:Chemistry020210 optoelectronics & photonicsWavelength-division multiplexing0103 physical sciences0202 electrical engineering electronic engineering information engineering:NATURAL SCIENCES:Physics [Research Subject Categories]General Materials Scienceerbium/ytterbium co-dopingInstrumentationlcsh:QH301-705.5wavelength division multiplexingcladding-pumped optical amplifierFluid Flow and Transfer ProcessesOptical amplifierbusiness.industrylcsh:TProcess Chemistry and TechnologyAmplifierGeneral Engineeringsimulationbit error ratelcsh:QC1-999Computer Science Applicationschemistrylcsh:Biology (General)lcsh:QD1-999lcsh:TA1-2040Optoelectronicsdoped fiber amplifiersbusinesslcsh:Engineering (General). Civil engineering (General)lcsh:Physics
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Tunable dual-wavelength operation of an all- fiber thulium-doped fiber laser based on tunable fiber Bragg gratings

2018

Tunable dual-wavelength emission of a Tm-doped fiber laser based on two fiber Bragg gratings (FBGs) is experimentally demonstrated. By using two FBGs with central wavelengths at 2069.30 and 2069.44 nm, stable dual-wavelength laser generation in the 2 ?m wavelength region is achieved by adjusting the differential loss of the two wavelengths in the laser cavity. Strain applied on the FBG allows independent tuning of the simultaneously generated wavelengths with separation between the laser lines in a range from 0.54 to 9 nm. The laser has output power fluctuations less than 0.093% for an output power of 77.3 mW.

Materials scienceDual-wavelength fiber laserschemistry.chemical_elementPhysics::Optics02 engineering and technology01 natural scienceslaw.invention010309 optics020210 optoelectronics & photonicsOpticsFiber Bragg gratinglawFiber laser0103 physical sciences0202 electrical engineering electronic engineering information engineeringRange (particle radiation)business.industryDopingLaserAtomic and Molecular Physics and OpticsUNESCO::FÍSICA::Óptica ::Fibras ópticasElectronic Optical and Magnetic MaterialsWavelengthThuliumchemistry:FÍSICA::Óptica ::Fibras ópticas [UNESCO]Optical cavitybusinessThulium-Doped FiberTunable fiber lasersFiber bragg gratings
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Flat supercontinuum generation pumped by amplified noise-like pulses from a figure-eight erbium-doped fiber laser

2017

The conditions to obtain noise-like pulses (NLPs) from a figure-eight fiber laser (F8L) and their application for supercontinuum (SC) generation in the anomalous dispersion regime are reported. The F8L is designed to remove the undesired low-intensity background radiation from pulse emission, generating NLPs with a 3 dB spectral bandwidth of 17.43 nm at the fundamental repetition frequency of 0.8 MHz. After amplification, NLPs reach a maximum average power of 9.2 mW and 123.32 nm spectral bandwidth. By controlling the amplifier pump power, flat SC generation is demonstrated through both a 800 m long spool of SMF-28 fiber and a piece of 5 m long highly nonlinear optical fiber. The results de…

Materials sciencePhysics and Astronomy (miscellaneous)business.industryAmplifierBandwidth (signal processing)02 engineering and technology01 natural sciencesNonlinear optical fiberUNESCO::FÍSICA::Óptica ::Fibras ópticasSupercontinuum010309 optics020210 optoelectronics & photonics:FÍSICA::Óptica ::Fibras ópticas [UNESCO]Fiber laser0103 physical sciences0202 electrical engineering electronic engineering information engineeringOptoelectronicsbusinessInstrumentationErbium doped fiber laserssupercontinuum generationnonlinear effects
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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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Application of WGM Resonances to the Measurement of the Temperature Increment of Ho and Ho-Yb Doped Optical Fibers Pumped at 1125 and 975 nm

2021

Optical fiber characterization using whispering gallery mode resonances of the fiber itself has been demonstrated to be a powerful technique. In this work, we exploit the thermal sensitivity of whispering gallery mode resonances to characterize the pump-induced temperature increment in holmium doped and holmium-ytterbium codoped optical fibers. The technique relies on the measurement of the resonances’ wavelength shift due to temperature variation as a function of the pump power. Holmium doped fibers were pumped to the second excited level 5I6 of the Ho3+ ion using a laser diode at 1125 nm and ytterbium-holmium codoped fibers to the 2F5/2 level of the Yb3+ ion by a laser diode at 975 nm. Ou…

YtterbiumOptical fiberMaterials sciencechemistry.chemical_element02 engineering and technologylcsh:Chemical technology01 natural sciencesBiochemistrydoped fibersAnalytical Chemistrylaw.invention010309 optics020210 optoelectronics & photonicslaw2 μm fiber lasers:FÍSICA [UNESCO]0103 physical sciences0202 electrical engineering electronic engineering information engineeringlcsh:TP1-1185FiberElectrical and Electronic Engineeringwhispering gallery modesInstrumentationLaser diodebusiness.industryCommunicationDopingUNESCO::FÍSICAytterbium2 um fiber lasersAtomic and Molecular Physics and OpticschemistryExcited stateOptoelectronicsfiber characterizationholmiumWhispering-gallery waveHolmiumbusiness
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