Modeling a Scatterer Near an Optical Waveguide

August 25, 2020

The dielectric slab waveguide is one of the conceptual building blocks in photonic structure design. Although most real structures are more complex than just a two-dimensional dielectric slab, we can still learn a lot about modeling from this case. Here, we will look at the case of a small lossy scatterer in the proximity of an optical waveguide, show how this interacts with the fields, and compute reflection and transmission along the waveguide, as well as losses and scattering.

Background

The schematic of the example case is shown below. A dielectric slab waveguide has a small circular metallic object nearby that will interact with the fields, lead to some losses within the material, and cause scattering of light into all directions. For the example of a waveguide without the nearby object, this case would reduce to a perfect dielectric slab waveguide, which is discussed in this model.

A dielectric slab waveguide in 2D, with parts including a lossy material, dielectric core, and dielectric cladding.
Schematic of a 2D dielectric slab waveguide with a lossy material in proximity to the core.

We will consider the case of a waveguide that is wide enough to support multiple modes, although we will restrict ourselves to just the example of the electric field polarized out of the modeling plane. (We can reasonably assume that either the electric or the magnetic field is polarized purely out-of-plane, and that there is no coupling between these two, as long as all materials are isotropic.) This simplifies our analysis a little bit.

A schematic showing the different ways the incident light guided along a waveguide can behave.
The incident light guided along the waveguide can be reflected, transmitted, absorbed, and scattered.

Before starting our modeling, it is worth doing a bit of manual bookkeeping, thinking of where the light is coming from, and where it is going. We will consider light propagating along the waveguide toward the scatterer, and that this incident light is the first, fundamental, mode. Due to the scatterer, some fraction of the incident light will be:

  1. Transmitted forward and of the same fundamental mode
  2. Transmitted forward, but converted into the second mode
  3. Reflected backward, and into the fundamental mode
  4. Reflected backward, and into the second mode
  5. Absorbed by the lossy metallic inclusion
  6. Scattered into other directions

Computing the transmission into the four possible guided modes of the waveguide (items 1–4) requires solely that we introduce four different numerical ports into the model, two on either side. As already discussed in a previous blog post, it is possible to introduce multiple interior slit port boundary conditions at boundaries within the modeling space. Modeling the absorption into the lossy material simply involves integrating the loss within the metallic object. It is the last quantity, the computation of the scattered light, that requires some special attention.

Computing Scattered Light

In general, the scattered light from the object near the waveguide can go in any direction. We do know, however, that light propagating along the axis of the waveguide must be one of the guided modes. So, if we draw a boundary normal to the propagation direction of light within the waveguide and integrate the power flow crossing this boundary, we know that this integral will be the sum of the guided light plus whatever scattered light is propagating nearly but not exactly parallel to the waveguide. The light that is guided along the waveguides is computed by the port transmittances and reflectances. So if we subtract this away, we are left with the scattered fraction. Now, since we are integrating across an interior boundary, we will want to make use of the up() or down() operators to evaluate the flux only on one side of the boundary. To integrate these accurately, we use a boundary layer mesh.

We can insert additional interior boundaries that are tangential to the waveguide, and also monitor the power flow across them. They will form a rectangular box along with the previous two boundaries. Integrating the power flowing out of this box gives us the total of all scattering and all light leaving as a guided mode.

The computational model for the optical waveguide scattering problem, with parts labeled.
Schematic of our computational model.

Along with monitoring the scattered light, we also need to make sure that the light that is propagating out of the modeling domain does not get reflected back. We do so via the usage of perfectly matched layers (PML), which do a very good job of absorbing most outgoing radiation with their default settings. However, for the PML’s adjacent to the waveguide, we can get a little bit better performance by adjusting the characteristic wavelength in the PML settings to be based upon the propagation constant of the first guided mode of the waveguide, because we do know that most of the power is still carried in this mode. This setting is shown in the screenshot below.

A screenshot of the settings for adjusting the perfectly matched layer (PML) wavelength in COMSOL Multiphysics.
Manual adjustment of the PML wavelength settings.

Simulation results showing a lossy dielectric scatterer near an optical waveguide.
Sample results showing a lossy metallic scatterer near a dielectric slab waveguide.

The results of our model are shown in the image above, and the model file is available for download via the link below. Whenever you are modeling a scatterer near a dielectric waveguide you will want to use the combination of modeling techniques developed here.

Try It Yourself

Get the model discussed in this blog post by clicking the button below, which will take you to the Application Gallery (note that you must be logged into COMSOL Access with a valid software license to download MPH-files).

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Tesfay Abraha
Tesfay Abraha
September 1, 2020

Thanks. very nice program

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