2021
DOI: 10.1364/oe.419091
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Stokes light induced modulation instability in high power continuous wave fiber amplifiers

Abstract: In this paper, Stokes light induced modulation instability (MI) in high power continuous wave (CW) fiber amplifiers is observed. The investigation shows that the Stokes light generated by inter-modal four wave mixing (IMFWM) and stimulated Raman scattering (SRS) in high power fiber amplifiers can be modulated by the signal light through XPM and cause MI. Then, a sideband will be generated around the second-order Raman frequency shift, which is amplified by SRS and shown as a train of pulses in time domain. It … Show more

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Cited by 10 publications
(6 citation statements)
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“…Based on the 130 mm coiling diameter of the amplifier YDF, the suppression of SRS is 24 dB relative to the intensity of the signal light in the 1090 nm laser, as shown in figure 5(a). When the coiling diameter of the amplifier YDF increased to 140 mm, a 34 dB suppression of SRS was obtained, achieving further suppression of SRS by the mode combination (11,01 → 11,01)dominated IMFWM; this was also be demonstrated in our previous work [30]. Figure 9 shows the output spectra of the 1080 nm fiber amplifier with a minimum coiling diameter of 150 mm.…”
Section: Discussionsupporting
confidence: 71%
“…Based on the 130 mm coiling diameter of the amplifier YDF, the suppression of SRS is 24 dB relative to the intensity of the signal light in the 1090 nm laser, as shown in figure 5(a). When the coiling diameter of the amplifier YDF increased to 140 mm, a 34 dB suppression of SRS was obtained, achieving further suppression of SRS by the mode combination (11,01 → 11,01)dominated IMFWM; this was also be demonstrated in our previous work [30]. Figure 9 shows the output spectra of the 1080 nm fiber amplifier with a minimum coiling diameter of 150 mm.…”
Section: Discussionsupporting
confidence: 71%
“…Firstly, the characteristic peaks of 1 st Raman effect have been observed when the output power reached 283 W. Then, two sidelobes around the signal wavelength appeared at 1067.9 nm and 1081.4 nm as the power scaled to 366 W, which manifested the appearance of SRSinduced XPM-MI [2]. The calculated gain spectra [2,19] of SRS-induced XPM-MI effect is plotted in Fig. 3(b).…”
Section: Resultsmentioning
confidence: 96%
“…The Brillouin scattering threshold can be effectively increased by broadening the spectral line at a single frequency and then amplifying so to suppress the SBS effect. The spectrum of the noise modulated laser is relatively continuous, which has advantages in suppressing nonlinear modulation effects such as self-phase modulation and cross-phase modulation [9].…”
Section: Introductionmentioning
confidence: 99%