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利用一种无源非线性脉冲整形方法, 实现了在普通正色散(ND)光纤中产生三角形光脉冲, 此方法依赖于脉冲预啁啾和脉冲在ND光纤中传输时群速度色散与自相位调制的相互作用. 实验研究表明, 在较宽的脉冲预啁啾值范围内, 通过优化脉冲输入功率和脉冲传输的ND光纤长度, 均可得到典型的三角形光脉冲: 脉冲时域形状前后沿的变化率接近恒定、整个脉冲具有线性频率啁啾. 另外, 在不同的脉冲预啁啾下, 要得到高质量的三角形光脉冲, 均需要较高的脉冲输入功率; 并且脉冲预啁啾较大时, 三角形脉冲的形成对ND光纤长度和脉冲输入功率有较大的容差, 易获得三角形光脉冲.Generation of triangular optical pulses in conventional normal dispersive (ND) fiber is experimentally realized using a passive nonlinear pulse shaping method based on a combination of pulse pre-chirping, group-velocity dispersion and self-phase modulation in a section of ND fiber. It is found that by optimizing the parameters of launching pulse power level and ND fiber length, high-quality triangular optical pulses with nearly constant gradients of leading and trailing edges and linear frequency chirp profiles can be obtained for a wide range of different pulse pre-chirping values. For different pulse pre-chirpings, high launch power is required for triangular optical pulse generation. The tolerance of triangular pulse formation to ND fiber length and launch power level is improved with the increase of pulse pre-chirping, which means that it is easy to obtain triangular pulses for higher pulse pre-chirping.
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Keywords:
- triangular optical pulse /
- normal dispersive fiber /
- nonlinear effects /
- pre-chirping
[1] Kravtsov K, Deng Y, Prucnal P R 2009 IEEE J. Quantum Electron. 45 396
[2] Camerlingo A, Parmigiani F, Xian F 2010 IEEE Photon. Technol. Lett. 22 628
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[9] Parmigiani F, Ibsen M, Ng T T 2009 IEEE Photon. Technol. Lett. 21 1837
[10] Li J, Olsson B E, Karlsson M 2005 J. Lightwave Technol. 23 2654
[11] Latkin A I, Boscolo S, Bhamber R S 2009 J. Opt. Soc. Am. B 26 1492
[12] Bhamber R S, Latkin A I, Boscolo S 2008 ECOC Brussels Belgium Th.1.B.2
[13] Agrawal G P 2007 Nonlinear Fiber Optics (New York: Academic Press)
[14] Park Y, Asghari M H, Ahn T J 2007 Opt. Express 15 9584
[15] Boscolo S, Latkin A I, Turitsyn S K 2008 IEEE J. Quantum Electron. 44 1196
[16] Latkin A I, Boscolo S, Turitsyn S K 2008 Proc. OFC Paper OTuB7
[17] Wang H, Latkin A I, Boscolo S 2009 CLEO-Europe Paper CD.P.32 TUE
[18] Wang H, Latkin A I, Boscolo S 2010 J. Opt. 12 035205
[19] Dudley J M, Barry L P, Bollond P G 1998 Opt. Fiber Technol. 4 237
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[1] Kravtsov K, Deng Y, Prucnal P R 2009 IEEE J. Quantum Electron. 45 396
[2] Camerlingo A, Parmigiani F, Xian F 2010 IEEE Photon. Technol. Lett. 22 628
[3] Lu Y X, Yang X, Sun S 2009 Acta Phys. Sin. 58 2467 (in Chinese) [吕玉祥, 杨星, 孙帅 2009 58 2467]
[4] Parmigiani F, Petropoulos P, Ibsen M 2006 IEEE Photon. Technol. Lett. 18 829
[5] Finot C, Dudley J M, Kibler B 2009 IEEE J. Quantum Electron. 45 1482
[6] Kanaka R P, Masayuki K 2011 New J. Phys. 13 023030
[7] Deng Y X, Tu C H, Lu F Y 2009 Acta Phys. Sin. 58 3173 (in Chinese) [邓一鑫, 涂成厚, 吕福云 2009 58 3173]
[8] Parmigiani F, Ng T T, Ibsen M 2008 IEEE Photon. Technol. Lett. 20 1992
[9] Parmigiani F, Ibsen M, Ng T T 2009 IEEE Photon. Technol. Lett. 21 1837
[10] Li J, Olsson B E, Karlsson M 2005 J. Lightwave Technol. 23 2654
[11] Latkin A I, Boscolo S, Bhamber R S 2009 J. Opt. Soc. Am. B 26 1492
[12] Bhamber R S, Latkin A I, Boscolo S 2008 ECOC Brussels Belgium Th.1.B.2
[13] Agrawal G P 2007 Nonlinear Fiber Optics (New York: Academic Press)
[14] Park Y, Asghari M H, Ahn T J 2007 Opt. Express 15 9584
[15] Boscolo S, Latkin A I, Turitsyn S K 2008 IEEE J. Quantum Electron. 44 1196
[16] Latkin A I, Boscolo S, Turitsyn S K 2008 Proc. OFC Paper OTuB7
[17] Wang H, Latkin A I, Boscolo S 2009 CLEO-Europe Paper CD.P.32 TUE
[18] Wang H, Latkin A I, Boscolo S 2010 J. Opt. 12 035205
[19] Dudley J M, Barry L P, Bollond P G 1998 Opt. Fiber Technol. 4 237
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