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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.
OptiInstrument addresses the needs of researchers, scientists, photonic engineers, professors and students who are working with instruments.
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.
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.
Download our 30-day Free Evaluations, lab assignments, and other freeware here.Â
Dear sir/madam,
I tried to make a simulation of a cfbg in optigrating. It doesn’t matter much what the specifications of this cfbg are. I want to apply a temperature difference in the middle of the grating length so that the spectrum shifts on the left side and there is a dip at the temperature difference, this all works fine when I apply a temperature difference with the user function at temperature. However, I am now using a temperature difference where the beginning of the fibre has a high temperature and the end has a low temperature (see picture). Actually, it should be a low temperature at the beginning and then to a high temperature. Then I get a peak instead of a dip. It looks like the grating length is the opposite as the length in the temperature function. Is that true?
Yours sincerely,
Quinten
Hi Quinten,
The x axis is not reversed. I believe the reason for the confusion is that the direction of the applied linear period chirp is the opposite of what you might expect. The equation OptiGrating uses for linear chirp is Lambda(z) = Lamba0 – Delta*(z-L/2)/L, where Delta is the specified chirp rate (Eq. 21 in the OptiGrating User Reference). If you set the chirp parameter to a positive number, the period will decrease along the length of the grating instead of increase. If you set it to a negative number (-10 in your case), the period will increase along the length of the grating, and if you leave everything else the same, the effect will be reversed, as you expected (the dip you saw in reflection becomes a peak, and the peak in transmission becomes a dip, see images below).
Amine