• Advanced Photonics Nexus
  • Vol. 3, Issue 3, 036009 (2024)
Ming Shen1、2, Yanxin Li1、2, Qianying Li1、2, and Xuewen Shu1、2、*
Author Affiliations
  • 1Huazhong University of Science and Technology, Wuhan National Laboratory for Optoelectronics, Wuhan, China
  • 2Huazhong University of Science and Technology, School of Optical and Electronic Information, Wuhan, China
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    DOI: 10.1117/1.APN.3.3.036009 Cite this Article Set citation alerts
    Ming Shen, Yanxin Li, Qianying Li, Xuewen Shu. Random fiber laser using a cascaded fiber loop mirror[J]. Advanced Photonics Nexus, 2024, 3(3): 036009 Copy Citation Text show less
    (a) Schematic of the CFLM. Simulated (b) reflection spectrum and (c) spatial intensity distributions of the 10-CFLM.
    Fig. 1. (a) Schematic of the CFLM. Simulated (b) reflection spectrum and (c) spatial intensity distributions of the 10-CFLM.
    Simulated reflection spectra of the 10-CFLM at λ1 with (a1) fluctuating Lc, (a2) fluctuating k, and (a3) enlarged view of Fig. 1(b) for comparison. Experimentally measured (b1) transmission and (b2) reflection spectra of the 10-CFLM. (b3) Enlargement of panel (b2).
    Fig. 2. Simulated reflection spectra of the 10-CFLM at λ1 with (a1) fluctuating Lc, (a2) fluctuating k, and (a3) enlarged view of Fig. 1(b) for comparison. Experimentally measured (b1) transmission and (b2) reflection spectra of the 10-CFLM. (b3) Enlargement of panel (b2).
    Experimental setup. LD, laser diode; WDM, wavelength division multiplexer; EDF, erbium-doped fiber; CFLM, cascaded fiber loop mirror; ISO, isolator.
    Fig. 3. Experimental setup. LD, laser diode; WDM, wavelength division multiplexer; EDF, erbium-doped fiber; CFLM, cascaded fiber loop mirror; ISO, isolator.
    (a) Output spectra at the pump powers of 22 and 168 mW. Inset is the output spectrum right after the increase of pump power. (b) Output power versus pump power.
    Fig. 4. (a) Output spectra at the pump powers of 22 and 168 mW. Inset is the output spectrum right after the increase of pump power. (b) Output power versus pump power.
    Longitudinal mode envelopes under the pump powers of (a1) 22 mW and (a2) and (a3) 75 mW. (b) Averaged radio-frequency spectra at two different times at the pump power of 168 mW.
    Fig. 5. Longitudinal mode envelopes under the pump powers of (a1) 22 mW and (a2) and (a3) 75 mW. (b) Averaged radio-frequency spectra at two different times at the pump power of 168 mW.
    Variation of the Lévy index α with pump power.
    Fig. 6. Variation of the Lévy index α with pump power.
    Radio-frequency spectra with (a1) one and (a2) three FLMs. (b) Longitudinal mode envelopes with three FLMs at different times.
    Fig. 7. Radio-frequency spectra with (a1) one and (a2) three FLMs. (b) Longitudinal mode envelopes with three FLMs at different times.
    (a) Simulated phase of the electromagnetic field after a round trip as a function of frequency (offset from 193.55 THz). The red points are the solutions of phase conditions. (b) Adjacent longitudinal mode spacing counts from phase conditions. (c) Lasing modes count at different gains. Inset is the enlargement near the G of 4 dB. The simulation bandwidth is 2.5 GHz (20 pm).
    Fig. 8. (a) Simulated phase of the electromagnetic field after a round trip as a function of frequency (offset from 193.55 THz). The red points are the solutions of phase conditions. (b) Adjacent longitudinal mode spacing counts from phase conditions. (c) Lasing modes count at different gains. Inset is the enlargement near the G of 4 dB. The simulation bandwidth is 2.5 GHz (20 pm).
    Ming Shen, Yanxin Li, Qianying Li, Xuewen Shu. Random fiber laser using a cascaded fiber loop mirror[J]. Advanced Photonics Nexus, 2024, 3(3): 036009
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