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利用TOAD实现10Gbit/s全光非归零码到归零码的转换 被引量:7

10 Gbit/s All-Optical Non-Return-to-Zero to Returnto-Zero Conversion Based on Terahertz Optical Asymmetric Demultiplexer
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摘要 利用从非归零(NRZ)信号中全光提取的时钟,采用太赫兹光非对称解复用器(TOAD)实现了10 Gbit/s非归零码到归零(RZ)码的码型转换。非归零信号采用半导体光放大器(SOA)进行时钟分量增强并用平面波导阵列(AWG)滤出相应的伪归零(PRZ)信号,然后采用半导体光放大器注入锁模光纤环形激光器进行时钟提取,提取的时钟信号和待转换的非归零信号分别作为抽运光和探测光输入太赫兹光非对称解复用器,在其中进行码型转换。转换后输出的归零信号的质量仅由恢复的时钟信号和非归零信号的质量决定,受太赫兹光非对称解复用器中半导体光放大器增益恢复时间的影响极小。实验测得转换后的归零信号消光比为8.7 dB,码型效应非常低,其光谱明显展宽,并且出现谱间隔为0.08 nm的多峰结构,与10 Gbit/s的比特速率相对应。该方法对时钟信号的码型效应有一定的容忍度。 10 Gbit/s all-optical non-return-to-zero (NRZ) to return-to-zero (RZ) conversion is demonstrated based on terahertz optical asymmetric demultiplexer (TOAD) using all-optically recovered clock from the NRZ signal. The clock component is enhanced in an semiconductor optical amplifier (SOA) and the pseudo-return-to-zero (PRZ) signal is filtered. The PRZ signal is input into an injection mode-locked fiber ring laser for clock recovery. The recovered clock and the NRZ signal are input into TOAD as pump signal and probe signal, respectively, and format conversion is performed. The quality of the converted RZ signal is determined by that of the recovered clock and the NRZ signal, whereas hardly influenced by the gain recovery time of the SOA. In the experimental demonstration, the obtained RZ signal has an extinction ratio of 8.7 dB and low pattern dependency. After conversion, the spectrum broadens obviously and shows multimode structure with spectral interval of 0.08 nm, which matches with the bit rate of 10 Gbit/s. Furthermore, this format conversion method has some tolerance on the pattern dependency o{ the clock signal.
出处 《中国激光》 EI CAS CSCD 北大核心 2005年第11期1510-1514,共5页 Chinese Journal of Lasers
关键词 光通信 码型转换 太赫兹光非对称解复用器 半导体光放大器 时钟提取 optical communication format conversion terahertz optical asymmetric demultiplexer, semiconductor optical amplifier clock recovery
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参考文献15

  • 1Lei Xu, Bing C. Wang, Varghese Baby et al.. All-optical data format conversion between RZ and NRZ based on a Mach-Zehnder interferometric wavelength converter [J]. IEEE Photon. Technol. Lett. , 2003, 15(2):308-310.
  • 2S. Bigo, O. Leclerc, E. Desurvire. All-optical fiber signal processing and regeneration for soliton communications [J]. IEEE J. Sel. Top. Quantum Electron. , 1997, 3(5) : 1208-1223.
  • 3余建军,管克俭,陈树强,杨伯君.利用非线性光学环路镜实现非归零码脉冲到归零码脉冲的变换[J].光电子.激光,1999,10(4):317-320. 被引量:4
  • 4H. K. Lee, K. H. Kim, J. T. Ahna al.. All-optical format conversion from NRZ to RZ signals using a walk-off balanced nonlinear fibre loop mirror [J]. Electron. Lett. , 1996, 32(25) :2335-2336.
  • 5M. Owen, M. F. C. Stephens, R. V. Penty et al.. All-optical 3R regeneration and format conversion in an integrated SOA/DFB laser [C]. OFC'2000, 76-78.
  • 6H. Kawaguchi. All-optical demultiplexing and format conversion using an ultrafast bistable laser diode [C]. LFNM'2001, 56-60.
  • 7C. W. Chow, C. S. Wong, H. K. Tsang. All-optical format and wavelength conversion using polarization switching in a FP laser diode[C]. LEOS ' 2002, 629 -630.
  • 8David Norte, Alan E. Willner. Experimental demonstrations of all-optical conversions between the RZ and NRZ data formats incorporating noninverting wavelength shifting leading to format transparency [J]. IEEE Photon. Technol. Lett. , 1996, 8(5):712-714.
  • 9C. Gosset, G.-H. Duan. Extinction ratio improvement and wavelength conversion based on four-wave mixing in a semiconductor optical amplifier [J].IEEE Photon. Technol. Lett. , 2001, 13(2):139-141.
  • 10A. T. Clausen, K. S. Jepsen, H. N. Poulsenet al.. Interface for 10 Gbit/s bit-synchronisation and format and wavelength conversion with 3R regenerative capabilities [J]. Electron.Lett., 1998, 34(16):1554-1555.

二级参考文献27

  • 1Kao Y H, Goltser I V, Islan M Net al.. Ultrafast optical logic gate using a semiconductor laser amplifier operating at transparency in a loop mirror. CLEO '97,CTuJ4, 1997. 94-95.
  • 2Obermann K, Kindt S, Breuer D et al.. Performance analysis of wavelength converters based on cross-gain modulation in semiconductor-optical amplifiers. J Lightwave Technol , 1998, 16(1):78-84.
  • 3Tang J M, Shore K A. Analysis of the characteristics of TOAD's subject to frequency-detuned control and signal picosecond pulses. IEEE J Quant Electron , 1999, 35(11) ; 1704- 1712.
  • 4Uskov A, Mork J, Mark J. Wave mixing in semiconductor laser amplifiers due to carrier heating and spectral-hole burning. IEEE J Ouant Electron , 1994, 30(8):1769-1781.
  • 5Mork J, Mecozzi A. Theory of the ultrafast optical response of active semiconductor waveguides. J Opt Soc Am (B), 1996, 13(8):1803-1816.
  • 6Yu B Y, Toliver P, Runser R Jet al.. Packet-switched optical networks. IEEE Micro, January/February, 1998.28-38.
  • 7Glesk I, Solokoff J P, Prucnal P R. All-optical address recognition and self-routing in a 250 Gbit/s packet-switched network. Electron Lett , 1994, 30(16):1322-1323.
  • 8Zhou Xiang, Ye Peida, Guan K J nal.. A novel OTDM frame synchronization scheme based on a terahertz optical asymmetric de-multiplexer with feedback. IEEE Photon Technol Lett , 1999, 11(1):125-127.
  • 9Deng K L, Glesk I, Kang K Iet al.. Unbalanced TOAD for optical data and clock separation in self-clocked transparent OTDM networks. IEEE Photon Technol Lett , 1997, 9(6):830-833.
  • 10Robinson B S, Hall K K. Experimental analysis of switching windows in semiconductor based all-optical switches. Conference on Lasers and Electro-Optics, San Francisco, 2000. 331-332.

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