Photonics Research, Volume. 7, Issue 11, 1287(2019)
Pattern formation in 2-μm Tm Mamyshev oscillators associated with the dissipative Faraday instability
Fig. 1. Schematic diagram of the 2-μm fiber ring cavity in a Mamyshev oscillator configuration. OC, optical coupler; TDF, Tm-doped gain fiber; filter 1, longer-wavelength super-Gaussian spectral filter; filter 2, shorter-wavelength super-Gaussian spectral filter; passive fiber, the commercial normal dispersion fiber (NDF).
Fig. 2. Spatiotemporal dynamics of single pulse operation: (a) temporal spectral evolution during per cavity roundtrip. A, B, C, D, E, and F represent the TDF1, passive fiber1, filter1 + OC1, TDF2, passive fiber2, and filter2 + OC2; (b) temporal (blue) and frequency chirping (red) profiles after the interaction with the longer-wavelength filter; (c) spectral pulse profile (blue) after the longer-wavelength filter (red); (d) spectral evolution over 300 roundtrips at the output of OC1 (color scale for the optical intensity, in dB). The cavity parameters are
Fig. 3. Spatiotemporal dynamics of soliton pair molecule operation: (a) temporal evolution during per cavity roundtrip. A, B, C, D, E, and F represent the TDF1, passive fiber1, filter1 + OC1, TDF2, passive fiber2, and filter2 + OC2; (b) temporal and frequency chirping profiles after the longer-wavelength filter; (c) spectral profiles after the longer-wavelength filter; (d) spectral evolution over 300 roundtrips at the output of OC1. The remaining parameters are
Fig. 4. Spatiotemporal dynamics of random pulse train operation: (a) temporal and (c) spectral evolution over 300 roundtrips at the output of OC1; (b) temporal and (d) spectral evolution during per cavity roundtrip. A, B, C, D, E, and F represent the TDF1, passive fiber1, filter1 + OC1, TDF2, passive fiber2, and filter2 + OC2. The remaining parameters are
Fig. 5. Spatiotemporal dynamics of regular pattern formation: (a) temporal and (c) spectral evolution over 300 roundtrips at the output of OC1; (b) temporal and (d) spectral evolution during per cavity roundtrip. A, B, C, D, E, and F represent the TDF1, passive fiber1, filter1 + OC1, TDF2, passive fiber2, and filter2 + OC2. The remaining parameters are
Fig. 6. Spatiotemporal profiles of regular pattern formation: single pulse temporal profiles (a) before and (b) after the interaction with the longer-wavelength filter; (c) pulse train temporal and phase profiles after the longer-wavelength filter; (d) spectral profile after the longer-wavelength filter.
Fig. 7. Spatiotemporal dynamics of irregular pattern formation: (a) temporal and (c) spectral evolution over 300 roundtrips at the output of OC1; (b) temporal and (d) spectral evolution during per cavity roundtrip. A, B, C, D, E, and F represent the TDF1, passive fiber1, filter1 + OC1, TDF2, passive fiber2, and filter2 + OC2. The remaining parameters are
Fig. 8. Spatiotemporal dynamics of irregular pattern formation: (a) temporal and (c) spectral evolution over 300 roundtrips at the output of OC1; (b) temporal and (d) spectral evolution during per cavity roundtrip. A, B, C, D, E, and F represent the TDF1, passive fiber1, filter1 + OC1, TDF2, passive fiber2, and filter2 + OC2. The remaining parameters are
Fig. 9. Temporal and phase profiles of the RWs’ generation after the longer-wavelength filter. The remaining parameters are
Fig. 10. Influence of the frequency detuning between the filters on RWs generation: histogram on log scale showing the statistics distribution of the pulse intensity for
Fig. 11. Spatiotemporal dynamics of regular pattern formation in the near-zero dispersion fiber ring setup (see text): (a) temporal and (c) spectral evolution over 300 roundtrips at the output of OC1; (b) temporal and (d) spectral evolution during per cavity roundtrip. A, B, C, D, E, and F represent the TDF1, passive fiber1, filter1+OC1, TDF2, passive fiber2, and filter2+OC2. The remaining parameters are
Fig. 12. Spatiotemporal profiles of regular pattern formation: single pulse temporal profiles (a) before and (b) after the interaction with the longer-wavelength filter; (c) pulse train temporal and phase profiles after the longer-wavelength filter; (d) spectral profile after the longer-wavelength filter.
Fig. 13. Spatiotemporal dynamics of irregular pattern formation: (a) temporal and (b) spectral evolution over 300 roundtrips at the output of OC1 (the remaining parameters are
Fig. 14. Influence of the frequency detuning between the filters on RWs’ generation: histogram on log scale showing the statistics distribution of the pulse intensity for
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Pan Wang, Shunyu Yao, Philippe Grelu, Xiaosheng Xiao, Changxi Yang, "Pattern formation in 2-μm Tm Mamyshev oscillators associated with the dissipative Faraday instability," Photonics Res. 7, 1287 (2019)
Category: Lasers and Laser Optics
Received: Jun. 6, 2019
Accepted: Sep. 11, 2019
Published Online: Oct. 28, 2019
The Author Email: Changxi Yang (cxyang@tsinghua.edu.cn)