2016
DOI: 10.1109/lpt.2016.2586098
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A Single Longitudinal Mode Fiber Ring Laser Based on Cascaded Microfiber Knots Filter

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Cited by 15 publications
(6 citation statements)
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“…Similarly, the light oscillates counterclockwise in MKR 2 and is partially output from port 13 through coupling region IV. According to the resonance principle, the signal light can exist stably in the ring only when its frequency matches the two MKRs, while the other signal light is suppressed in output range, and the phase matching condition of CMKR can be expressed as: [86]…”
Section: Combined With Vernier Effectmentioning
confidence: 99%
See 1 more Smart Citation
“…Similarly, the light oscillates counterclockwise in MKR 2 and is partially output from port 13 through coupling region IV. According to the resonance principle, the signal light can exist stably in the ring only when its frequency matches the two MKRs, while the other signal light is suppressed in output range, and the phase matching condition of CMKR can be expressed as: [86]…”
Section: Combined With Vernier Effectmentioning
confidence: 99%
“…Similarly, the light oscillates counterclockwise in MKR 2 and is partially output from port 13 through coupling region IV. According to the resonance principle, the signal light can exist stably in the ring only when its frequency matches the two MKRs, while the other signal light is suppressed in output range, and the phase matching condition of CMKR can be expressed as: [ 86 ] R1R2badbreak=m0.28em+0.28em12m0.28em+0.28emN0.28em+0.28em12;mgoodbreak=0,1,2,$$\begin{equation}\frac{{{R_1}}}{{{R_2}}} = \frac{{m\; + {\mathrm{\;}}\frac{1}{2}}}{{m\; + {\mathrm{\;}}N\; + {\mathrm{\;}}\frac{1}{2}}};m = 0,1,2, \ldots \end{equation}$$where R 1 and R 2 are the radiuses of MKR 1 and MKR 2 , respectively. In particular, when N = 1 every m ‐th resonance peak of MKR 1 will overlap with every ( m + 1)‐th resonance peak of MKR 2 , so that a periodic cursor envelope can be formed.…”
Section: Mkr and Its Improved Structurementioning
confidence: 99%
“…Besides, cascaded interferometers can significantly enhance the spectral shift range through the Vernier effect. The use of cascaded interferometers as filters for interval-adjustable FRLs has been proposed in recent years [32][33][34]. However, to the best of our knowledge, FRL sensor operated under the principle of Vernier effect has not been widely proposed.…”
Section: Introductionmentioning
confidence: 99%
“…Single longitudinal mode (SLM) fiber lasers are highly desired due to the significant potential for use in various applications, ranging from optical sensing and wavelength division multiplexing (WDM) communications systems to interferometry, data storage, spectroscopy, and coherent signal generation. The attractiveness of SLM fiber lasers is in their output, which has very narrow linewidth and a high output power, thus making them particularly useful for applications requiring dense wavelength transmissions over long distances [1][2][3][4].…”
Section: Introductionmentioning
confidence: 99%
“…SLM fiber lasers typically employ etalon-like devices in the laser cavity as a part of their design, as well as various filters, such as cascaded microfiber knots filters (CMKFs) and tunable Fabry-Perot (FP) filters; as well as saturable absorbers (SAs), such as graphene [1][2][3][4][5][6][7][8][9][10]. These approaches are all able to generate the desired SLM outputs, but each technique has various advantages and disadvantages.…”
Section: Introductionmentioning
confidence: 99%