2013
DOI: 10.1016/j.optlastec.2012.08.020
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Tunable single-polarization single-longitudinal-mode erbium-doped fiber ring laser employing a CMFBG filter and saturable absorber

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Cited by 45 publications
(24 citation statements)
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“…To attain SLM operation, various filters are usually incorporated in the fiber ring cavity. So far, a lot of all fiber filters, such as fiber bragg gratings (FBGs) [7], chirped moire FBGs [8], and a Fabry-Perot interferometer [9] have been inserted into the fiber laser cavity to achieve SLM lasing oscillations. However, several disadvantages including high loss, bulky systems and a risk of system instability still exist due to the multiple cavity filtering components.…”
Section: Introductionmentioning
confidence: 99%
“…To attain SLM operation, various filters are usually incorporated in the fiber ring cavity. So far, a lot of all fiber filters, such as fiber bragg gratings (FBGs) [7], chirped moire FBGs [8], and a Fabry-Perot interferometer [9] have been inserted into the fiber laser cavity to achieve SLM lasing oscillations. However, several disadvantages including high loss, bulky systems and a risk of system instability still exist due to the multiple cavity filtering components.…”
Section: Introductionmentioning
confidence: 99%
“…More importantly, the short-length cavity can result in broad spectral linewidth. Another approach is a long-length ring cavity to offer higher output power without special requirements for the gain media [6]. However, since a fiber ring laser usually has a long cavity with closely spaced longitudinal modes, an ultranarrow bandpass filter (BPF) must be incorporated to eliminate multilongitudinal-mode oscillation and mode hopping [7].…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, to achieve stable SLM operation, several techniques have been proposed to ensure a long-term stable performance in EDFL, for instance, introducing a passive multiplering cavity or a compound ring resonator composed of a dual-coupler fiber ring to guarantee SLM laser oscillation [9], using an unpumped EDF as a dynamic narrow-bandwidth filter [10], and utilizing selfinjection feedback to control the lasing frequency [11]. At the same time, in order to realize a singlepolarization (SP) fiber laser, several methods have been proposed, such as utilizing polarizationdependent losses of the fiber laser [12], an inline broadband polarizer [6], injection locking [13], and PM-FBG [14].…”
Section: Introductionmentioning
confidence: 99%
“…A narrow linewidth ring laser always exhibits a long cavity length, so its longitudinal interval is extremely narrow, which is easy to arouse mode-hopping. Several methods have been investigated and reported to be implemented stable narrow linewidth fiber lasers by suppressing the multi-longitudinal-mode operation and mode hopping for example inserting an unpumped doped fiber which acts as a saturable absorber, an intra-cavity Fabry-Pérot etalon in the fiber cavity or a fiber loop which works as a filter etc [11][12][13][14] . However, short length linear cavity fiber lasers have recently demonstrated the potential to meet all the requirements thanks to their compactness, simplicity, and robustness.…”
Section: Introductionmentioning
confidence: 99%
“…OSA. Usually, the laser linewidth can be measured by the delayed homodyne method [14] . The characteristic of longitudinal mode is confirmed by a scanning Fabry-Pérot interferometer (FSR= 8.8…”
Section: Introductionmentioning
confidence: 99%