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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.
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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 » Semiconductor Laser Modulation Response
Compatibility:
When using a directly modulated laser for high-speed transmission systems, the modulation frequency can be no larger than the frequency of the relaxation oscillations. The relaxation oscillation depends on both carrier lifetime and photon lifetime. The approximate expression of this dependence is given by:
The relaxation oscillation frequency increases with the laser bias current.
In this lesson, we will demonstrate the performance of the high speed system while using the modulation frequency and increasing resonance frequency (through the improvement in the system performance) with the laser bias current. The project is depicted in Figure 1.
Figure 1: Project layout
For the default parameters of our laser rate equation model Ith = 33.45mA, Tsp = 1ns, Tph = 3ps , and if we assume modulation peak current I = 40mA, and IB = 40mA , the corresponding resonance frequency in accordance with the above equation will be about 1.3 GHz.
Discussion of the numerical parameters: bit rate is 1.3 Gb/s and sequence length 128 bits, therefore, the time window is about 98.5 ns. Samples per bit are 512, therefore, the sample rate is 670 GHz. The default resolution therefore is 10 MHz.
In Figure 2 and Figure 3, the influence of the increased modulation frequency above the resonance one on system performance will be demonstrated. In Figure 2, 1.3 Gb/s (10Gb/s) transmission is studied. The parameters of the laser rate equations are the default ones (I = IB = 40mA) as previously described.
Figure 2: Increase in modulation frequency above resonance
Clearly, modulation with the frequency well above the resonance one leads to unacceptable system performance.
In Figure 3, the influence of the bias current on the resonance frequency, and therefore on system performance, for a fixed bit rate will be demonstrated. We use 1.3 Gb/s transmission, keep all other parameters the same, and use IB = 20mA.
Figure 3: Reduction of bias current
If you compare Figure 3 with Figure 2 (with 1.3 Gb/s transmission and IB = 40mA ),
it is clearly demonstrated that the reduction of the bias current below its threshold
value leads to a decrease in system performance.
In this lesson we have shown the dependence of the performance of the high speed system on the modulation frequency and the laser bias current.
References
[1]G.P. Agrawal, Fiber-Optic Communication Systems, John Wiley & Sons, Inc, second edition, 1997.