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Descend through FDTD to a closed-form optimum

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A three-layer coating matches free space to a substrate of εr = 12 over 8–12 GHz. Each layer is 5.5 mm (11 cells) thick; the three permittivities are the design variables and the objective is the band-mean power reflection. The transfer-matrix method gives the exact optimum, so the question is whether gradient descent through a time-domain solve lands there.

1.1 % largest layer-permittivity gap to the optimum
0.1 % closed-form reflection above the optimum
60 Adam steps
Reflection of the coating from rfx FDTD and the transfer matrix, the three layer permittivities over the Adam iterations, and the band-mean reflection against the transfer-matrix optimum

What happened

From the geometric-ladder start (1.861 / 3.464 / 6.447) the layer permittivities settle at 1.922 / 4.670 / 4.707 against the optimum 1.943 / 4.652 / 4.720, although the closed-form optimizer started from a different point. Evaluated with the transfer matrix, the design’s band-mean |R|² is 0.03434 against the optimum’s 0.03430, −14.6 dB, 3.0 dB below the start. FDTD and transfer-matrix |R|² of the final design differ by at most 1.5×10⁻³ over the 15 frequencies the cost uses (8.20–11.78 GHz).

How the gradient was checked

Against central differences at the start to 5.5×10⁻⁴, and against a 1.5× longer record to 4.8×10⁻⁴.

A one-dimensional stack at normal incidence; it shows the optimizer and the gradient work together, not the accuracy of a 3-D radome.

Downloads

Run it

Terminal window
python examples/inverse_design/multilayer_ar_coating.py

CPU, minutes; the showcase script scripts/showcase/ar_coating.py records every iterate.

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