Results
First, look at the modes polarized in the z direction.
Surface 1
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Notice that your plot may look different from the plot above, as the plot shows the real part of the boundary mode electric field. The computed complex electric field can have a different phase factor than for the plot above. Thus, the field can either show minima (a blue color) or maxima (a red color) at the locations for the waveguide cores. However, since this is a symmetric mode, it will have the same field values for both waveguide cores.
Another consequence of the arbitrary phase factor is that the magnitude for the displayed real part of the electric field in your plot can be different from what is shown in the plot above.
When adding two mode fields having arbitrary phases, the resulting superposition field will, of course, also have a random shape. To remove this arbitrariness, later, in the last part of this example model, the Port input power and the Mode phase parameters for the exciting ports will be used to ensure that the superposition field approximates a target field.
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From the Settings window for Surface, locate the Expression section and enter ewbe.tEbm1y in the Expression text field, to plot the mode field polarized in the y direction.
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Derived Values
You will need to copy the effective indices for the different modes and use them in the boundary mode analyses for the different ports.
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Locate the Expressions section in the Settings window for Global Evaluation and enter ewbe.neff_1 in the Expression cell for the first table row. The variable ewbe.neff_1 is the effective index for the first port.
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Now, copy all information in the table to the clipboard. Then paste that information into your favorite text editor, so you can easily enter the values later in the boundary mode analysis steps.
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