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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.
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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 Friends
I am trying to model rough surface geometry with the incident light of s and p polarization. After that I want to find out reflectance and transmittance for both polarizations. Also light is incident at oblique angles.
Would it be okay if I set (Ez,Hx,Hy) and (Hz,Ex,Ey) for s and p polarizations. What are the components of poynting vector which should be calculated?
Please find the attached file in which schematic diagram is given.
Hello Sumeet,
Based on the diagram you attached it would appear that your incidence plane is XY (propagation in XY and interface normal is Y). You are correct, if this is the case then the S (E field perpendicular to the incidence plane) would be the Ez group while the P( E fields parallel to the incident plane) would be the Ex/Ey group.
S – Ez, Hx, Hy
P – Ex, Ey, Hz
In regards to your question about the Poynting vector calculation things get a bit trickier.
S = E x H
which leads to
S = (EyHz-EzHy)x+(EzHx-ExHz)y+(ExHy-EyHx)z
If you have a source that is purely S or purely P polarized then you can neglect the field components of P when working on S, etc. This yields
S (S polarization) = -(EzHy)x+(EzHx)y
S (P polarization) = (EyHz)x-(ExHz)y
Note this separation cannot be done if your source contains field components of both polarizations.
In OptiFDTD the Poynting vector for an observation area is calculated along the direction normal to the plane. This means to get the polarizations above you should create an observation plane perpendicular to x and one perpendicular to y and get the fields from these. From there you can calculate the above equations.
Scott
Thanks Mr Newman