2008
DOI: 10.1109/lpt.2008.922974
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Single-Longitudinal-Mode Erbium-Doped Fiber Ring Laser Based on High Finesse Fiber Bragg Grating Fabry–PÉrot Etalon

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Cited by 113 publications
(62 citation statements)
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“…However, such techniques often employ a combination of components or the requirement to modify their characteristics, thus adding complexity to their operation and control. For example, as reported in [3], stable wavelength output was achieved by the use of an apodised FBG with the addition of an intra-cavity high finesse FBG Fabry-Perot etalon. The modification of the FBG as well as the fact that the fibre system used relatively low pumping power decreased the likelihood of spontaneous noise fluctuations within the gain media.…”
Section: Introductionmentioning
confidence: 91%
“…However, such techniques often employ a combination of components or the requirement to modify their characteristics, thus adding complexity to their operation and control. For example, as reported in [3], stable wavelength output was achieved by the use of an apodised FBG with the addition of an intra-cavity high finesse FBG Fabry-Perot etalon. The modification of the FBG as well as the fact that the fibre system used relatively low pumping power decreased the likelihood of spontaneous noise fluctuations within the gain media.…”
Section: Introductionmentioning
confidence: 91%
“…Secondly, an ultranarrow mode selecting mechanism should be utilized to eliminate the multi-longitudinal-mode oscillation and mode competition, caused by the long cavity length and hence the narrow longitudinal mode spacing. Such an ultranarrow bandpass filter can be obtained by using a phase shifted fiber Bragg grating (FBG) [6], an SA based Sagnac loop [13], or an FBG-based Fabry-Perot (F-P) filter [14,15]. Although the FBG based F-P filter has been utilized in the ring cavity of fiber laser to realize the SLM operation [14,15], no single to dual wavelength switching can be achieved.…”
Section: Introductionmentioning
confidence: 99%
“…Such an ultranarrow bandpass filter can be obtained by using a phase shifted fiber Bragg grating (FBG) [6], an SA based Sagnac loop [13], or an FBG-based Fabry-Perot (F-P) filter [14,15]. Although the FBG based F-P filter has been utilized in the ring cavity of fiber laser to realize the SLM operation [14,15], no single to dual wavelength switching can be achieved. However, either no SA element is used for stabilizing the output power [14], or a segment of gain fiber and a pump diode are employed to function as the SA element [15].…”
Section: Introductionmentioning
confidence: 99%
“…For example, optical systems that require wavelengths to be evenly spaced, such as WDM, need a laser source where the output wavelength can be discretely tuned [1]. Several tunable fibre laser structures have been reported [2][3][4][5][6][7][8], most of them are based on erbium-doped fibre amplifiers (EDFAs) and employ one or a combination of components or techniques for wavelength selection or tuning, including Fibre Bragg Gratings (FGB) [2 -4], etalon based filters like Fabry-Perot cavity [5 -6] and acousto-optic based tunable filters [7]. *E-mail: dmichel@our.ecu.edu.au This paper proposes and demonstrates a novel continuously linear-cavity tunable fibre laser employing an Opto-VLSI processor as the wavelength selection mechanism.…”
Section: Introductionmentioning
confidence: 99%