Abstract:This paper presents an accurate theoretical model for the study of concatenation of optical multiplexers/demultiplexers (MUXs/DMUXs) in transparent multiwavelength optical networks. The model is based on a semianalytical technique for the evaluation of the error probability of the network topology. The error-probability evaluation takes into account arbitrary pulse shapes, arbitrary optical MUX/DMUX, and electronic low-pass filter transfer functions, and non-Gaussian photocurrent statistics at the output of th… Show more
“…These power values are further used for the computation of total power output. In the comparison of model and experimental results, it is observed that Equation (31) is comparable to Equation (11) with n equal to 'l i ', and 'a i ' is equal to '1/m' for computing wavelength dependent output power of wavelength 'λ i ' not equal to 'λ c ', where tolerance limits were taken as 0.5 dBm. For wavelength λ i = λ c , 'a i ' is equal to '1.5/m'.…”
Abstract-This paper mathematically models the operation of Arrayed Waveguide Grating (AWG) based multiplexer (mux) and demultiplexer (demux) used in optical networks. In WDM networks, the optical mux and demux play a crucial role of managing the aggregation and segregation of wavelengths for networking applications. A simple and intuitive model of AWG based mux design is discussed in this work. This model assumes that the device is linear, in which the principle of superposition is valid, and the primary emphasis is given to the optical power gain of the individual wavelengths. By using this model, one can exactly estimate the individual and overall power associated with each of the multiplexed wavelengths. The developed model was evaluated with experimental results using AWG based multiplexers. The experiments were repeated for different test cases with various power input levels and multiplexer configurations. It was found that the developed model provided a good approximation to the actual AWG mux/demux.
“…These power values are further used for the computation of total power output. In the comparison of model and experimental results, it is observed that Equation (31) is comparable to Equation (11) with n equal to 'l i ', and 'a i ' is equal to '1/m' for computing wavelength dependent output power of wavelength 'λ i ' not equal to 'λ c ', where tolerance limits were taken as 0.5 dBm. For wavelength λ i = λ c , 'a i ' is equal to '1.5/m'.…”
Abstract-This paper mathematically models the operation of Arrayed Waveguide Grating (AWG) based multiplexer (mux) and demultiplexer (demux) used in optical networks. In WDM networks, the optical mux and demux play a crucial role of managing the aggregation and segregation of wavelengths for networking applications. A simple and intuitive model of AWG based mux design is discussed in this work. This model assumes that the device is linear, in which the principle of superposition is valid, and the primary emphasis is given to the optical power gain of the individual wavelengths. By using this model, one can exactly estimate the individual and overall power associated with each of the multiplexed wavelengths. The developed model was evaluated with experimental results using AWG based multiplexers. The experiments were repeated for different test cases with various power input levels and multiplexer configurations. It was found that the developed model provided a good approximation to the actual AWG mux/demux.
“…In a TON, signal distortion and noise accumulation, due to optical nodes concatenation, can also impair significantly the TON performance [12,13]. It was shown that it is necessary to choose suitably the filter bandwidth in order to maximize the TON performance when signal distortion and incoherent homodyne crosstalk are present [14].…”
Section: R G Leiria and A V T Cartaxomentioning
confidence: 99%
“…Several works have studied the cascadability of optical MUX/DEMUX and OADM based on AWG [12,15]. However, high channel spacing [15] and an approximated AWG transfer function [12] have been considered.…”
Section: R G Leiria and A V T Cartaxomentioning
confidence: 99%
“…However, high channel spacing [15] and an approximated AWG transfer function [12] have been considered.…”
A transparent optical network (TON) composed by optical add-drop multiplexers based on arrayed waveguide grating (AWG) with fabrication errors is optimized for10 Gbit/s per channel and channel spacing of 25 GHz. The optimization takes into account the effect of inter-symbol interference, amplified spontaneous emission noise accumulation, and coherent and incoherent homodyne crosstalk. Numerical results reveal that AWG fabrication errors can have a high influence on the TON performance; however, in all investigated situations, they do not affect the AWG parameters values corresponding to the optimum AWG frequency response. This surprising behavior is due to the fabrication errors affect mainly the AWG response outside the passband for the required AWG crosstalk level. It is shown that the optimum AWG frequency response is a flat-top response with a mean amplitude response outside the passband lower than −30 dB and the switch isolation should exceed 30 dB.
“…A comprehensive study of the aforementioned effects are included in the model presented in Ref. [10]. Other extensive studies have been performed for sample WDM optical systems or networks operating at 2.5 Gbps and 10 Gbps that provided a better understanding of the impact of optical filter cascades (amplitude and phase) on the performance and are presented in Refs.…”
A technique to separate the phase-induced penalty of a cascade of optical filters into dispersion, dispersion slope, and higher-order terms is introduced and its impact on the proper design and engineering of high-speed Dense Wavelength Division Multiplexed (WDM) optical systems and networks is demonstrated. As the currently deployed fiber optic systems and networks strive for higher speeds to respond to the growing global needs for more bandwidth, the impact of physical layer impairments (such as optical filter dispersion slope) which were not significant at lower speeds are now becoming increasingly important and worth looking at. In this article we demonstrate that at speeds of 40 Gbps and beyond, where the next generation systems will be operating, optical filter dispersion slope is at least as important as filter dispersion. As a result, separating the above contributions and accounting for each using the described modeling technique proves to be an effective way for designing and engineering such systems.
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