• Photonics Research
  • Vol. 7, Issue 11, 1287 (2019)
Pan Wang1, Shunyu Yao1, Philippe Grelu2, Xiaosheng Xiao1, and Changxi Yang1、*
Author Affiliations
  • 1State Key Laboratory of Precision Measurement Technology and Instruments, Department of Precision Instruments, Tsinghua University, Beijing 100084, China
  • 2Laboratoire ICB UMR 6303 CNRS, Université Bourgogne Franche-Comté, F-21078 Dijon Cedex, France
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    DOI: 10.1364/PRJ.7.001287 Cite this Article Set citation alerts
    Pan Wang, Shunyu Yao, Philippe Grelu, Xiaosheng Xiao, Changxi Yang. Pattern formation in 2-μm Tm Mamyshev oscillators associated with the dissipative Faraday instability[J]. Photonics Research, 2019, 7(11): 1287 Copy Citation Text show less
    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. 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).
    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 g0=12.8, Esat=19.4 nJ, and ΔΩ=7.0 nm.
    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 g0=12.8, Esat=19.4  nJ, andΔΩ=7.0  nm.
    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 g0=16.2, Esat=19.4 nJ, and ΔΩ=7.0 nm.
    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 g0=16.2, Esat=19.4  nJ, andΔΩ=7.0  nm.
    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 g0=16.2, Esat=19.4 nJ, and ΔΩ=5.4 nm.
    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 g0=16.2, Esat=19.4  nJ, andΔΩ=5.4  nm.
    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 g0=16.2, Esat=19.4 nJ, and ΔΩ=4.6 nm.
    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 g0=16.2, Esat=19.4  nJ, andΔΩ=4.6  nm.
    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. 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.
    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 g0=16.2, Esat=19.4 nJ, and ΔΩ=4.2 nm.
    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 g0=16.2, Esat=19.4  nJ, andΔΩ=4.2  nm.
    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 g0=16.2, Esat=19.4 nJ, and ΔΩ=2.8 nm.
    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 g0=16.2, Esat=19.4  nJ, andΔΩ=2.8  nm.
    Temporal and phase profiles of the RWs’ generation after the longer-wavelength filter. The remaining parameters are g0=16.2, Esat=19.4 nJ, and ΔΩ=2.0 nm.
    Fig. 9. Temporal and phase profiles of the RWs’ generation after the longer-wavelength filter. The remaining parameters are g0=16.2, Esat=19.4  nJ, andΔΩ=2.0  nm.
    Influence of the frequency detuning between the filters on RWs generation: histogram on log scale showing the statistics distribution of the pulse intensity for ΔΩ values of (a) 4.6 nm; (b) 5.4 nm; (c) 4.2 nm; (d) 2.8 nm; and (e) 2.0 nm; (f) PDF and number of events versus the frequency detuning between the filters. The remaining parameters are g0=16.2 and Esat=19.4 nJ.
    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 ΔΩ values of (a) 4.6 nm; (b) 5.4 nm; (c) 4.2 nm; (d) 2.8 nm; and (e) 2.0 nm; (f) PDF and number of events versus the frequency detuning between the filters. The remaining parameters are g0=16.2 and Esat=19.4  nJ.
    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 g0=16.8, Esat=16.4 nJ, and ΔΩ=5.4 nm.
    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 g0=16.8, Esat=16.4  nJ, andΔΩ=5.4  nm.
    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. 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.
    Spatiotemporal dynamics of irregular pattern formation: (a) temporal and (b) spectral evolution over 300 roundtrips at the output of OC1 (the remaining parameters are g0=16.8, Esat=16.4 nJ, and ΔΩ=3.6 nm); (b) temporal and (d) spectral evolution over 300 roundtrips at the output of OC1 (the remaining parameters are g0=16.8, Esat=16.4 nJ, and ΔΩ=2.4 nm).
    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 g0=16.8, Esat=16.4  nJ, andΔΩ=3.6  nm); (b) temporal and (d) spectral evolution over 300 roundtrips at the output of OC1 (the remaining parameters are g0=16.8, Esat=16.4  nJ, andΔΩ=2.4  nm).
    Influence of the frequency detuning between the filters on RWs’ generation: histogram on log scale showing the statistics distribution of the pulse intensity for ΔΩ values of (a) 3.7 nm; (b) 2.6 nm; and (c) 2.2 nm; (d) PDF and number of events versus the frequency detuning between the filters. The remaining parameters are g0=16.8 and Esat=16.4 nJ.
    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 ΔΩ values of (a) 3.7 nm; (b) 2.6 nm; and (c) 2.2 nm; (d) PDF and number of events versus the frequency detuning between the filters. The remaining parameters are g0=16.8 and Esat=16.4  nJ.
    Pan Wang, Shunyu Yao, Philippe Grelu, Xiaosheng Xiao, Changxi Yang. Pattern formation in 2-μm Tm Mamyshev oscillators associated with the dissipative Faraday instability[J]. Photonics Research, 2019, 7(11): 1287
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