Optiwave software can be used in different industries and applications, including Fiber Optic Communication, Sensing, Pharma/Bio, Military & Satcom, Test & Measurement, Fundamental Research, Solar Panels, Components / Devices, etc..
OptiSystem is a comprehensive software design suite that enables users to plan, test, and simulate optical links in the transmission layer of modern optical networks.
OptiSPICE is the first circuit design software for analysis of integrated circuits including interactions of optical and electronic components. It allows for the design and simulation of opto-electronic circuits at the transistor level, from laser drivers to transimpedance amplifiers, optical interconnects and electronic equalizers.
OptiFDTD is a powerful, highly integrated, and user friendly CAD environment that enables the design and simulation of advanced passive and non-linear photonic components.
OptiBPM is a comprehensive CAD environment used for the design of complex optical waveguides. Perform guiding, coupling, switching, splitting, multiplexing, and demultiplexing of optical signals in photonic devices.
OptiFiber The optimal design of a given optical communication system depends directly on the choice of fiber parameters. OptiFiber uses numerical mode solvers and other models specialized to fibers for calculating dispersion, losses, birefringence, and PMD.
Emerging as a de facto standard over the last decade, OptiGrating has delivered powerful and user friendly design software for modeling integrated and fiber optic devices that incorporate optical gratings.
OptiConverge is a collaborative integration framework that seamlessly combines two or more Optiwave products (e.g., OptiSystem, OptiSPICE, OptiFDTD, etc.) and other third party products into unified solutions. Designed to streamline complex workflows, it empowers users to achieve their goals faster by harnessing the collective power of our trusted Optiwave tools.
Optiwave software can be used in different industries and applications, including Fiber Optic Communication, Sensing, Pharma/Bio, Military & Satcom, Test & Measurement, Fundamental Research, Solar Panels, Components / Devices, etc..
OptiSystem is a comprehensive software design suite that enables users to plan, test, and simulate optical links in the transmission layer of modern optical networks.
OptiSPICE is the first circuit design software for analysis of integrated circuits including interactions of optical and electronic components. It allows for the design and simulation of opto-electronic circuits at the transistor level, from laser drivers to transimpedance amplifiers, optical interconnects and electronic equalizers.
OptiFDTD is a powerful, highly integrated, and user friendly CAD environment that enables the design and simulation of advanced passive and non-linear photonic components.
OptiBPM is a comprehensive CAD environment used for the design of complex optical waveguides. Perform guiding, coupling, switching, splitting, multiplexing, and demultiplexing of optical signals in photonic devices.
OptiFiber The optimal design of a given optical communication system depends directly on the choice of fiber parameters. OptiFiber uses numerical mode solvers and other models specialized to fibers for calculating dispersion, losses, birefringence, and PMD.
Emerging as a de facto standard over the last decade, OptiGrating has delivered powerful and user friendly design software for modeling integrated and fiber optic devices that incorporate optical gratings.
OptiConverge is a collaborative integration framework that seamlessly combines two or more Optiwave products (e.g., OptiSystem, OptiSPICE, OptiFDTD, etc.) and other third party products into unified solutions. Designed to streamline complex workflows, it empowers users to achieve their goals faster by harnessing the collective power of our trusted Optiwave tools.
Home » Tutorials » Effects of PMD on Pulse Propagation
Compatibility:
Polarization mode dispersion (PMD) can cause serious problems in high bit-rate transmissions. In this lesson, the PMD emulator component is used to demonstrate the distortions in the transmitted signal, caused by first and second order PMD effects. The system showed in Figure 1 is utilized in the simulations.
Figure 1: PMD system layout
The system simulates the transmission of a sequence of pulses for a 10 Gb/s bit rate in a high PMD fiber with differential group delay of 71 ps, depolarization rate of 10.8°/GHz, and polarization chromatic dispersion of 1.3ps/GHz. In the simulations, attenuation and dispersion are set to zero. The input signal is a sequence of NRZ pulses showed in Figure 2.
Figure 2: Input sequence of pulses
Simulations are carried out for two different polarizations of the optical input signal. Figure 3(a) shows the output signal for an input state of polarization (SOP) aligned with one of the two principal states of polarization, azimuth = 0 and ellipticity = 0. In Figure 3(b), the output signal is the same, but the input SOP is aligned with the other axis, azimuth = 90 and ellipticity = 0.
Figure 3: (a) Simulation results for input signals with azimuth = 0,
ellipticity = 0
Figure 3: (b) Simulation results for input signals with azimuth = 90, ellipticity = 0
In both cases, the main second order effect is due to the depolarization rate coefficient, since the polarization chromatic dispersion is too small to create a substantial deformation of the output signal.
The presence of power over-shoots on the sequences of “1”s, and the presence of energy on the “0”s are due to the imperfect cancellation of the pulses coupled on the orthogonal axis. The results found in the simulations are in agreement with the results presented in [1].
References:
[1]Cristian Francia, Frank Bruyere, Denis Penninckx, and Michel Chbat. ” PMD Second-Order Effects on Pulse Propagation in Single-Model Optical Fibers”. IEEE Photonics Technology Letters, December 1998.
[2]L. E. Nelson, R. M. Jopson, H. Kogelnik, and G. J. Foschini. “Measurement of Depolarization and Scaling Associated with Second Order Polarization Mode Dispersion in Optical Fibers”. IEEE Photonics Technology Letters, December 1999.