Volume 47 Issue 1
Jan.  2018
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Chen Jiao, Tong Zhengrong, Zhang Weihua, Xue Lifang. Temperature tunable multiwavelength fiber laser by using compounded filter[J]. Infrared and Laser Engineering, 2018, 47(1): 105001-0105001(7). doi: 10.3788/IRLA201847.0105001
Citation: Chen Jiao, Tong Zhengrong, Zhang Weihua, Xue Lifang. Temperature tunable multiwavelength fiber laser by using compounded filter[J]. Infrared and Laser Engineering, 2018, 47(1): 105001-0105001(7). doi: 10.3788/IRLA201847.0105001

Temperature tunable multiwavelength fiber laser by using compounded filter

doi: 10.3788/IRLA201847.0105001
  • Received Date: 2017-06-05
  • Rev Recd Date: 2017-08-03
  • Publish Date: 2018-01-25
  • A stable multiwavelength erbium-doped fiber laser was proposed and experimentally demonstrated by using a compounded fiber filter, which was composed of a Mach-Zehnder interferometer(MZI) and a birefringence fiber filter-Lyot filter. The MZI was fabricated by using the fiber fusion splicer to splice a section of SMF to form two cascaded spherical structures. The Lyot filter was incorporating a segment of polarization maintaining fiber(PMF) and two polarization controllers(PCs), which provided nonlinear polarization rotation(NPR) and birefringent filter effect to suppress the mode competition and generate multiwavelength. Using cascaded spherical-shape structures MZI and the Lyot filter as mode restricting elements respectively, the transmission spectrum of cascaded spherical-shape structures MZI was modulated by the Lyot filter, which determined the period of the compounded structure. In the experiments, 9-wavelength operation with a side-mode suppression ratio (SMSR) of~40 dB was achieved, and the space of wavelength was 0.68 nm defined by the Lyot filter. When the stability of proposed structure was observed for 2 hours every 10 minutes, the fluctuation of the central wavelength's output power was less than 0.67 dB. Furthermore, when the two spherical-shape structures MZI was fixed on a furnace and the temperature varied from 30℃ to 110℃, the spectrum of output wavelength can be tuned within the range of 6.69 nm.
  • [1] Luo Yiyang, Xia Li, Sun Qizhen, et al. Multi-wavelength fiber laser based on self-seed light amplification and wavelength-dependent gain[J]. Optics Communications, 2015, 338:336-339.
    [2] Gao Xuesong, Gao Chunqing, Song Xueyong, et al. Theoretical analysis and experimental study of output characteristics of Er3+ doped ring cavity fiber laser[J]. Infrared and Laser Engineering, 2006, 35(5):573-578. (in Chinese)
    [3] Cheng Jianqun, Chen Weicheng, Chen Guojie. Switchable quadruple-wavelength Erbium-doped fiber laser based on a chirped fiber grating and polarization-maintaining fiber[J]. Optics Laser Technology, 2016, 78:71-73.
    [4] Harith Ahmad, Nor Ahya Hassan, Siti Nabila Aidit, et al. Generation of tunable multi-wavelength EDFL by using graphene thin film as nonlinear medium and stabilizer[J]. Optics Laser Technology, 2016, 81:67-69.
    [5] Estudillo-Ayala J M, Jauregui-Vazquez D, Haus J W, et al. Multi-wavelength fiber laser based on a fiber Fabry-Perot interferometer[J]. Applied Physics, 2015, 121(4):407-412.
    [6] Hu Kai, Wei Y, Sun Binzi, et al. Flexibly switchable multi-wavelength fiber optical parametric oscillator based on a Lyot-Sagnac Filter[J]. Laser Physics, 2012, 22(12):1842-1846.
    [7] Gao W Q, Liao M S, Deng D H, et al. Raman comb lasing in a ring cavity with high-birefringence fiber loop mirror[J]. Optics Communications, 2013, 300:225-229.
    [8] Wang Feng, Bi Weihong, Fu Xinghu, et al. Dual-wavelength Er3+-doped photonic crystal fiber laser based on superimposed fiber gratings[J]. Infrared and Laser Engineering, 2016, 45(8):0822001. (in Chinese)
    [9] Huang Ligang, Chang Pengfa, Song Xiaobo, et al. Tunable in-fiber Mach-Zehnder interferometer driven by unique acoustic transducer and its application in tunable multi-wavelength laser[J]. Optics Express, 2016, 24(3):2406-2412.
    [10] Gutierrez-Gutierrez J, Rojas-Laguna R, Estudillo-Ayala J M, et al. Switchable and multi-wavelength linear fiber laser based on Fabry-Perot and Mach-Zehnder interferometers[J]. Optics Communications, 2016, 374:39-44.
    [11] Li Yuan, Quan Mingran, Tian Jiajun, et al. Tunable multiwavelength erbium-doped fiber laser based on nonlinear optical loop mirror and birefringence fiber filter[J]. Applied Physics B, 2015, 119:363-370.
    [12] Zhou Yingwu, Sun Guoyong. Widely tunable erbium-doped fiber laser based on superimposed core-cladding-mode and Sagnac interferences[J]. IEEE Photonics Journal, 2012, 4(5):1503-1509.
    [13] Tom D P Allsop, Reeves R, Webb D J, et al. A high sensitivity refractometer based upon a long period grating Mach-Zehnder interferometer[J]. Review of Scientific Instruments, 2002, 73(4):1702-1705.
    [14] Fan Jingli, Zhang Jiangshan, Lu Ping, et al. A single-mode fiber sensor based on core-offset inter-modal interferometer[J]. Optics Communications, 2014, 320(2):33-37.
    [15] Zhang Z X, Ye Z Q, Xu Kun, et al. Tunable nonlinear-polarization-rotation based on multi-wavelength fiber laser with in-line fiber filter[C]//Optical Fiber Communication Optoelectronic Exposition Conference, 2008.
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Temperature tunable multiwavelength fiber laser by using compounded filter

doi: 10.3788/IRLA201847.0105001
  • 1. Key Laboratory of Film Electronic and Communication Devices,School of Electrical and Electronic Engineering,Tianjin University of Technology,Tianjin 300384,China

Abstract: A stable multiwavelength erbium-doped fiber laser was proposed and experimentally demonstrated by using a compounded fiber filter, which was composed of a Mach-Zehnder interferometer(MZI) and a birefringence fiber filter-Lyot filter. The MZI was fabricated by using the fiber fusion splicer to splice a section of SMF to form two cascaded spherical structures. The Lyot filter was incorporating a segment of polarization maintaining fiber(PMF) and two polarization controllers(PCs), which provided nonlinear polarization rotation(NPR) and birefringent filter effect to suppress the mode competition and generate multiwavelength. Using cascaded spherical-shape structures MZI and the Lyot filter as mode restricting elements respectively, the transmission spectrum of cascaded spherical-shape structures MZI was modulated by the Lyot filter, which determined the period of the compounded structure. In the experiments, 9-wavelength operation with a side-mode suppression ratio (SMSR) of~40 dB was achieved, and the space of wavelength was 0.68 nm defined by the Lyot filter. When the stability of proposed structure was observed for 2 hours every 10 minutes, the fluctuation of the central wavelength's output power was less than 0.67 dB. Furthermore, when the two spherical-shape structures MZI was fixed on a furnace and the temperature varied from 30℃ to 110℃, the spectrum of output wavelength can be tuned within the range of 6.69 nm.

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