Design and Implementation of All-optical Demultiplexer using Four-Wave Mixing (FWM) in a Highly Nonlinear Fiber (HNLF)

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International Journal of Scientific and Research Publications, Volume 4, Issue 5, May 2014 1 Design and Implementation of All-optical Demultiplexer using Four-Wave Mixing (FWM) in a Highly Nonlinear Fiber (HNLF) Thet Htet Nhin Department of Electronic Engineering, Mandalay Technological University, Myanmar Abstract- All-optical demultiplexer of 10Gb/s channel dropped out of 40Gb/s data stream is demonstrated by using the method of four-wave mixing (FWM) and an optical filter. Demultiplexing of optical time division multiplexed (OTDM) signal is based on the effect of nonlinearities in a highly nonlinear fiber (HNLF).We describe our experiment of all-optical demultiplexer and bit error rate (BER) measurements. Index Terms- Optical time division multiplexing (OTDM), four-wave mixing (FWM), wavelength conversion, optical components. I. INTRODUCTION Demultiplexing is based on the effect of four-wave mixing (FWM) in a highly nonlinear fiber.most common demultiplexers are cross-phase modulation (XPM) in a fiber [1]-[3], SOA [2], nonlinear optical loop mirror (NOLM) [4]-[5], mach-zehnder interferometer (MZI) [6].Other method is four-wave mixing (FWM) in a dispersion shifted fiber (DSF) or an SOA [7]-[8], electroabsorption modulator (EAM). In this paper, we demonstrate a new research for all-optical demultiplexer using a highly nonlinear fiber with four-wave mixing (FWM) method.this method is induced by beating between two or more channels cause the generation of one or more new frequencies at the expense of power depletion of the original channels.very low bit error rate (BER) (<10-12 ) is illustrated with 10Gb/s demultiplexed channel from 40Gb/s data stream.the main part of our proposed system is that we utilize an optical band pass filter that is choosed the desired channel to demultiplex.this research results in higher and amplified output signal received. II. PRINCIPLE OF DEMULTIPLEXER BY FOUR-WAVE MIXING Figure1:Proposed block diagram of 40Gb/s to 10Gb/s all-optical demultiplexer The operation principle of the proposed design work is illustrated in Fig [1].It includes signal transmission, signal amplification and demultiplexing. In signal transmission, four 10Gb/s channels are aggregated to 40Gb/s data stream.the clock signal and the data stream are amplified in an erbium doped fiber amplifier.to demultiplex the desired channel by means of four-wave mixing based on fiber and optical bandpass filter. In spectrum broadening, dispersion is done by highly nonlinear fiber after passing 0.4Km long. At the output of the HNLF, an optical bandpass filter (OBPF) is used to choose the demultiplexed channel.

International Journal of Scientific and Research Publications, Volume 4, Issue 5, May 2014 2 III. SIMULATION SETUP AND RESULTS Fig2: Simulation setup of the proposed system The simulation setup is shown in fig [2].A continuous wave laser diode emitted in optical pulses at a 1538 nm wavelength with a repetition bit rate of 10GHz.The data which is transmitted from 10 Gb/s PRBS is combined with CW laser output in an Mazchender modulator.the output data of modulator is tuned by appropriate four optical delay to get four channels within a 100ps time slot.with the help of power combiner, 40Gb/s data stream is evolved. The clock signals were generated by combining optical pulses and sine generator in an electroabsorption modulator well known as optical intensity modulator.the combined signals were amplified in an erbium-doped fiber amplifier (EDFA) with 15 db gain.the amplified output signal is launched into the 0.4km long highly nonlinear fiber with a dispersion of -0.08ps/nm/km and a dispersion slope of 0.032 ps/nm 2 /km.nonlinear interaction of the two signals occurred in the applied fiber.the peak power of the clock signal into the fiber was 1.659mW, while the power of the signal was 1.039mW.Due to the effects of FWM, the generation of side bands were appeared according to the following equations M= N 2 (N-1) / 2 Where N is the number of channels and M is the number of newly generated side bands.fig [3] shows an example of mixing of two waves at frequency ω 1 and ω 2. After passing through the fiber, the optical spectrum was broadened.so, the desired 10Gb/s channel of 40Gb/s data stream was demultiplexed by using a 0.33-nm optical BPF adjusted to a center wavelength of 1542nm.The demultiplexed channel was used to various receiver operations such as optical spectrum analyzer, optical oscilloscope and BER tester.

International Journal of Scientific and Research Publications, Volume 4, Issue 5, May 2014 3 Table 1. Simulation parameters in the proposed system Signal Wavelength 1538nm Laser Power 11dBm Clock Wavelength 1540nm Laser Power 9dBm SMF Length 0.3km Attenuation 0.2dB/km Dispersion -80ps/nm/km at o=1540nm EDFA Gain 15dB HNLF Wavelength 1550nm Fiber Length 0.4km Attenuation 0.2dB/km Dispersion Slope 0.032ps/nm 2 /km Nonlinear coefficient γ 12.6W -1 km -1 BPF Bandwidth 0.33nm Fig[4] shows the spectrum of the combination of clock and data signals before highly nonlinear and after highly nonlinear fiber.after passing fiber, the optical spectrum was broadened.to demultiplex the desired channel without containing the amplified spontaneous emission (ASE) noise, the proper choosing of optial bandpass filter is important. Fig4: (a) The spectrum of the combined signal before fiber, and (b) The broadened spectrum induced by FWM effect after fiber Fig[5] shows the input signal waveforms and the demultiplexed output waveforms.as a result, the peak power of output waveforms is better than that of the input. But, there has a few zero level noise that is the effect of other channels.there is still need to regenerate the peak power of 1 level. (a) (b) (c) (d)

International Journal of Scientific and Research Publications, Volume 4, Issue 5, May 2014 4 (e) (f) (g) (h) F Fig[6] Fig 5:Input is the eye signals patterns of(a)ch for each 1,(b)CH demultiplexed 2,(c)CH 3,(d)CH channels. 4,Output signals of (e)ch 1,(f)CH 2,(g)CH 3,(h)CH 4 Fig6: (a)-(d) Demultiplexed 10Gb/s channels Eye patterns of the demultiplexed 10Gb/s channels are shown in Fig.6.As seen in Fig.7, the power penalty of the demultiplexed channels are about <1 db at standard BER of 10-9. Fig7:BER measurements for 40-10Gb/s demultiplexing

International Journal of Scientific and Research Publications, Volume 4, Issue 5, May 2014 5 IV. CONCLUSION In this paper, we have showned a new method for OTDM demultiplexing based on FWM in a highly nonlinear fiber.40gb/s data channel was demultiplexed to 10Gb/s with <1dB power penalty successfully.. According to the simulation results, regeneration of 1s in output signal is required for better demultiplexing. ACKNOWLEDGMENT The author is greatly thankful to all her teachers from Department of Electronic Engineering, Mandalay Technological University. REFERENCES [1]Bengt -Erik Olsson and Daniel J.Blumenthal,"All-Optical Demultiplexing Using Fiber Cross-Phase Modulation (XPM) and Optical Filtering,"IEEEPhotonics Technology Lett.,vol.13,NO.8,AUGUST 2001. [2]E.Tangdiongga,Y.Liu,H.deWaardt,G.D.Khoe, Fellow and H.J.S.Dorren,"320-to-40-Gb/s Demultiplexing Using a Single SOA assisted by an Optical Filter,"IEEE Photonic Technology Lett.vol.18,NO.8,APRIL 15,2006. [3]Jianjun Yu and Palle Jeppesen,"Simultaneous All-Optical Demultiplexing and Regeneration Based on Self-Phase and Cross-Phase Modulation in a Dispersion Shifted Fiber,"IEEE JournalofLightwaveTechnology,vol,19,NO.7,July 2001. [4]K.J.Blow,N. J. Doran, and P. B. Nelson, Demonstration of the nonlinear fiber loop mirror as an ultrafast all-optical demultiplexer, Electronic. Lett., vol.26, pp.962-964,1990. [5]Y.Liang, J. W. Lou, J. K. Andersen, J. C. Stocker, O.Boyraz, and M.N. Islam, Polarization-insensitive nonlinear optical loop mirror demultiplexing with twisted fiber, Opt. Lett., vol.24,pp.726-728,1999.ach-ze [6]M. Vaa, B. Mikkelsen, K. S. Jepsen, and K. E. Stubkjaer, Bit error rate assessment of 80 Gb/s all-optical demultiplexing by a monolithically integrated M ach- Zehnder interferometer with semiconductor optical amplifiers, in ECOC 97,Edinburgh, Scotland, U.K., pp.we1b-4-1438. [7]P. A. Andrekson, N. A. Olsson, and J. R. Simpson, 16 Gb/s all-optical demultiplexing using four-wave mixing, Electron. Lett., vol. 27, pp.922-924, 1991. [8]Nazmi A. Mohammed, Four-wave-mixing based wavelength conversion using different types of ibers, International Journal of Engineering Science and Technology ( IJEST )., VOL. 4, No.01 January 2012. AUTHOR First Author Thet Htet Nhin, Bachelor of Engineering (Electronics), Mandalay Technological University, Myanmar and thethtet87@gmail.com.