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Discretely tunable and multiwavelength erbium doped fibre lasers with Fabry-Perot etalon

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Abstrakty
EN
Modern WDM telecommunication systems require stable and calibrated laser sources. In this paper, we present examples of such lasers based on erbium doped fibres, i.e., discretely tunable and multiwavelength ring lasers. For the first case, tuning is possible due to a tunable Bragg grating overlapping spectrally the third telecommunication window (1550 nm). When a Fabry-Perot etalon is inserted into the cavity, discrete tunable operation with appropriate spacing between operating wavelengths is possible. Different free spectral ranges (FSR) of applied etalons ensured operation at a wavelength spacing 0.4 nm, 0.8 nm or 1.6 nm, respectively. When an acoustooptical Bragg frequency shifter was inserted together with the Fabry-Perot etalon, the stable simultaneous multiwavelength operation covering the erbium doped gain range was achieved.
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  • Institute of Telecommunication, Wrocław University of Technology, 27 Wybrzeże Wyspiańskiego Str., 50-370 Wrocław, Poland
Bibliografia
  • [1] E. Snitzer, “Proposed fiber cavities for optical lasers”, J. Appl. Phys. 32, 36-39 (1961).
  • [2] M.W. Maeda, J.S. Patel, D.A. Smith, C.L. Lin, M.A. Saifi, and A.V. Lehman, “An electronically tunable fiber laser with liquid - crystal etalon filter as the wavelength - tuning element”, IEEE Photonic. Tech. L. 2, 787 (1990).
  • [3] H. Schmuck, T. Pfeiffer, and G. Veith, “Widely tunable narrow linewidth erbium doped fibre ring laser”, Electron. Lett. 28, 2117 (1991).
  • [4] N. Park, J.W. Dawson, K.J. Vahala, and C. Miller, “All fiber, low threshold, widely tuneable single - frequency, erbium - doped fiber ring laser with a tandem fiber Fabry - Perot filter”, Appl. Phys. Lett. 59, 2369 (1991).
  • [5] A. Budnicki, Telecommunication Fiber Lasers, 2006. (in Polish)
  • [6] M.J.F. Digonnet, Rare - Earth - Doped Fiber Lasers and Amplifiers, ORC Press, 2001.
  • [7] S. Yamashita and K. Hotate, “Multiwavelength erbium - doped fiber laser using intracavity etalon and cooled by liquid nitrogen”, Electron. Lett. 32, 1298-1299 (1996).
  • [8] A. Budnicki, P. Kaczmarek, R. Lewicki, and K.M. Abramski, “Multiwavelength fiber laser with acoustooptical Bragg frequency shifter”, Proc. SPIE 5958, 59580S-1-59580S-6 (2005).
  • [9] R. Slavik and S. Larochelle, “Frequency shift in a fiber laser resonator”, Opt. Lett. 27, 28-30 (2002).
  • [10] M. Karasek and A. Bellmare, “Numerical analysis of multifrequency erbium - doped fiber ring laser employing periodic filter and frequency shifter”, IEE P-Optoelectron. 147, 115-119 (2000).
  • [11] S.K. Kim, M.J. Chu, and J.H. Lee, “Wideband multiwavelength erbium - doped fiber ring laser with frequency shifted feedback”, Opt. Commun. 190, 291-302 (2001).
  • [12] R. Slavik, S. Larochelle, and M. Karasek, “High - performance adjustable room temperature multiwavelength erbium - doped fiber ring laser in the C - band”, Opt. Commun. 206, 365-371 (2002).
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Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-article-BWAK-0017-0009
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