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Lasers & Sources
Nonlinearity enhances operation of fiber ring laser
Parametric four-wave mixing in nonlinear fiber allows continuous wave or mode-locked fiber ring lasers to achieve ultrastable, superior performance for high-power multiwavelength output.
15 January 2007, SPIE Newsroom. DOI: 10.1117/2.1200701.0562
Fiber lasers, especially multiwavelength erbium-doped fiber lasers (MW-EDFLs), have attracted considerable interest for potential applications in optical test and measurement, and optical wavelength-division-multiplexing communication and sensing systems.1 Compared with compact semiconductor-based lasers, EDFLs are competitive because of their all-fiber structure as well as their capacity to provide high power and ultrashort pulse width.2 They can be used in applications that require multiple wavelength sources, with small, equal wavelength spacing, a large number of peaks within a broad band, and high output uniformity across the channels. These requirements pose a very challenging task for building a cost-effective multiwavelength EDFL for continuous wave (CW) or pulsed operation.
Previously, due to the homogeneously broadened gain property, many MW-EDFLs were developed with wavelength spacing larger than homogeneous linewidth (∼3.5nm) to overcome gain competition. Although a MW-EDFL with 16 wavelengths has been accomplished by cooling an erbium-doped fiber (EDF) to 77K using liquid nitrogen, the increased complexity and cost make it impractical for real applications. Many different approaches have also been explored for developing MW-EDFLs, including using polarization or spatial hole burning, using independent gain media, frequency shifting, and phase modulation.3–7
Here, we demonstrate a novel room-temperature-operated MW-EDFL with wavelength spacing less than homogeneous broadening linewidth, based on interchannel four-wave mixing (FWM).8 The gain-clamping effect in EDF is compensated by the parametric FWM between multiwavelength channels in a highly nonlinear fiber section that is inserted into the fiber ring cavity.
First, we implemented a stable CW MW-EDFL based on highly nonlinear photonic crystal fiber (HNL-PCF) and sampled-fiber Bragg grating (SFBG), as described in Figure 1. We initiated multiple wavelength operation, as shown in Figure 2, by adjusting the polarization controller and a specific SFBG with 0.8nm wavelength spacing. We then used an FWM-induced dynamic gain-flattening mechanism to stabilize the output. The FWM processes suppress the homogeneous line broadening of the EDFL and stabilize the multiple wavelength oscillation. By tuning the intracavity polarization controller and then the FWM efficiency, the number of concurrent lasing wavelengths can be changed from two to five, and the peak power differences for the main oscillation wavelengths are less than 2.0dB.
Figure 1. Schematic diagram of the multiwavelength erbium-doped fiber laser. PC: Polarization controller. FBG: Fiber Bragg grating. HNL-PCF: Highly nonlinear photonic crystal fiber. EDFA: Erbium-doped fiber amplifier. (Click to enlarge all images.)
Figure 2. The multipeak transmission spectrum of sampled fiber Bragg grating (SFBG) and the interchannel parametric four-wave mixing (FWM) lead to stable multiwavelength output.
We further extend the idea of FWM-induced self-stable operation of MW-EDFL to the multiwavelength mode-locking fiber ring laser to generate ultrashort, ultrafast, multiwavelength and synchronized pulse sources, as shown in Figure 3. By using 1km conventional highly nonlinear fiber (HNLF), two and four wavelengths anchored on the International Telecommunications Union standards (ITU-T) with 100GHz channel spacing are successfully mode-locked at 10GHz simultaneously, without gain competition.
Figure 3. Experimental setup for multiwavelength mode-locked erbium-doped fiber ring laser (ML-EDFL). EDF: Erbium-doped fiber. WDM: Wavelength division multiplexing. LD: Laser diode. HNLF: Highly nonlinear fiber. DWDM: Dense WDM. ODL: Optical delay line. VOA: Variable optical attenuator. RF: Radio frequency. OSA: Optical spectrum analyzer.
Moreover, we implement a much more compact cavity structure with 60m HNL-PCF to achieve the extremely small channel spacing of 0.5nm operation of 10GHz dual-wavelength mode locking with the help of fiber birefringence. This is the densest 10GHz mode-locked fiber laser reported, to the best of our knowledge, and the system can easily be scaled to provide more wavelengths. Figure 4 shows the spectrum and pulse train of two mode-locked wavelengths. The amplitude fluctuation and timing jitter are measured to be less than 1% and 100fs, respectively. The supermode suppression ratio is higher than 60dB. The time-bandwidth products vary between 0.39 ∼ 0.41, hence our laser generates nearly transform-limited pulses. Also, the channel spacing can be designed according to the repetition rate and the fiber birefringence evolution.
Figure 4. Dual-wavelength mode-locking performance. (a) Optical spectrum. (b) Direct pulse train output.
In conclusion, we proposed and demonstrated a novel room-temperature MW-EDFL that uses FWM throughout the length of the HNLF to suppress homogeneous gain broadening. The optimal combination of nonlinearity and dispersion of the HNL-PCF enables efficient FWM generation and eliminates the interchannel saturation effect. It is a promising start to building a simple structure incorporating a laser cavity and nonlinear fiber, which can easily generate more wavelengths with dense channel spacing.
Ping Shum, Ming Tang, Fu Songnian, Hui Dong
Network Technology Research Centre (NTRC), Nanyang Technological University
Yandong Gong, Xiufeng Yang
Institute for Infocomm Research
Photonics Research Centre, The Hong Kong Polytechnic University
Hong Kong, China
5. C.-L. Zhao, X. Yang, C. Lu, J. H. Ng, X. Guo, P. R. Chaudhuri, X. Dong, Switchable multi-wavelength erbium-doped fiber lasers by using cascaded fiber bragg gratings written in high birefringence fiber,
no. 230pp. 313-317, 2004.