From f448ebd98e5c56a2a64fc80dd9a1db7db2d224d9 Mon Sep 17 00:00:00 2001 From: Ardavan Oskooi Date: Fri, 20 Jan 2023 14:30:56 -0800 Subject: [PATCH] Additional results and updates to adjoint-optimization tutorial involving waveguide mode converter (#2373) * additional results and updates to adjoint-optimization tutorial * switch from imposed constraint to measured minimum feature size in plot axis * revert plot axis to imposed constraint from measured value * add values in table for measured linewidth and linespacing for all designs * mention that support for 2D constraints is for arbitrary rather than just circular shapes --- doc/docs/Python_Tutorials/Adjoint_Solver.md | 149 ++++++++++++------ doc/docs/images/mode_converter_designs.png | Bin 0 -> 45986 bytes .../mode_converter_worst_case_refl_tran.png | Bin 0 -> 47460 bytes 3 files changed, 100 insertions(+), 49 deletions(-) create mode 100644 doc/docs/images/mode_converter_designs.png create mode 100644 doc/docs/images/mode_converter_worst_case_refl_tran.png diff --git a/doc/docs/Python_Tutorials/Adjoint_Solver.md b/doc/docs/Python_Tutorials/Adjoint_Solver.md index 40db53823..f28998deb 100644 --- a/doc/docs/Python_Tutorials/Adjoint_Solver.md +++ b/doc/docs/Python_Tutorials/Adjoint_Solver.md @@ -4,10 +4,9 @@ Meep contains an adjoint-solver module for efficiently computing the gradient of an arbitrary function of the mode coefficients -($\mathcal{S}$-parameters), DFT fields, local density of states -(LDOS), and "far" fields with respect to $\varepsilon$ on a discrete -spatial grid (a -[`MaterialGrid`](../Python_User_Interface.md#materialgrid) class +($S$-parameters), DFT fields, local density of states (LDOS), and +"far" fields with respect to $\varepsilon$ on a discrete spatial grid +(a [`MaterialGrid`](../Python_User_Interface.md#materialgrid) class object) at multiple frequencies over a broad bandwidth. Regardless of the number of degrees of freedom for the grid points, just **two** distinct timestepping runs are required. The first run is the @@ -35,7 +34,10 @@ Python using [autograd](https://github.com/HIPS/autograd) as well as The adjoint solver supports inverse design and [topology optimization](https://en.wikipedia.org/wiki/Topology_optimization) by providing the functionality to wrap an optimization library around the -gradient computation. This is demonstrated in several tutorials below. +gradient computation. The adjoint solver also supports enforcing +minimum feature sizes on the optimal design in 1D (line width and +spacing) and 2D (arbitrary-shaped holes and islands). This is +demonstrated in several tutorials below. [TOC] @@ -43,67 +45,76 @@ Broadband Waveguide Mode Converter with Minimum Feature Size ------------------------------------------------------------ This example demonstrates some of the advanced functionality of the -adjoint solver including worst-case (minimax) optimization, multiple -objective functions, and constraints on the minimum line width and -line spacing. The design problem involves a broadband waveguide mode -converter with minimum feature size in 2D. This is based on -[M.F. Schubert et al., ACS Photonics, Vol. 9, pp. 2327-36, +adjoint solver including worst-case (minimax) optimization across +multiple wavelengths, multiple objective functions, and design +constraints on the minimum line width and line spacing. The design +problem involves a broadband waveguide mode converter in 2D with +minimum feature size. This is based on [M.F. Schubert et al., ACS +Photonics, Vol. 9, pp. 2327-36, (2022)](https://doi.org/10.1021/acsphotonics.2c00313). The mode converter must satisfy two separate design objectives: (1) minimize the reflectance $R$ into the fundamental mode of the input -port ($\mathcal{S}_{11}$) and (2) maximize the transmittance $T$ into -the second-order mode of the output port ($\mathcal{S}_{21}$). There -are different ways to define this multi-objective and multi-wavelength +port ($S_{11}$) and (2) maximize the transmittance $T$ into the +second-order mode of the output port ($S_{21}$). There are different +ways to define this multi-objective and multi-wavelength optimization. The approach taken here is *worst-case* optimization whereby we minimize the maximum (the worst case) of $R$ and $1-T$ -across all six wavelengths (in the O-band for -telecommunications). This is known as *minimax* optimization. +across six wavelengths in the $O$-band for telecommunications. This is +known as *minimax* optimization. The fundamental mode launched from +the input port has $E_z$ polarization given a 2D cell in the $xy$ +plane. The challenge with minimax optimization is that the $\max$ objective function is not everywhere differentiable. This property would seem to preclude the use of gradient-based optimization algorithms for this -problem which involves 12 independent functions ($R$ and $1-T$ for +problem which involves twelve independent functions ($R$ and $1-T$ for each of six wavelengths). Fortunately, there is a workaround: the -problem can be reformulated as a differentiable problem using -a so-called "epigraph" formulation: introducing -a new "dummy" optimization variable $t$ and -adding each independent function $f_k(x)$ as a new nonlinear constraint $t \ge f_k(x)$. See -the [NLopt +problem can be reformulated as a differentiable problem using a +so-called "epigraph" formulation: introducing a new "dummy" +optimization variable $t$ and adding each independent function +$f_k(x)$ as a new nonlinear constraint $t \ge f_k(x)$. See the [NLopt documentation](https://nlopt.readthedocs.io/en/latest/NLopt_Introduction/#equivalent-formulations-of-optimization-problems) for an overview of this approach. The minimax/epigraph approach is also covered in the [near-to-far field tutorial](https://nbviewer.org/github/NanoComp/meep/blob/master/python/examples/adjoint_optimization/06-Near2Far-Epigraph.ipynb). -In this example, we use a minimum feature size of 150 nm for the line -width *and* line spacing. The implementation of these constraints is -based on [A.M. Hammond et al., Optics Express, Vol. 29, pp. 23916-38 +In this example, we use a minimum feature size of 150 nm for the +linewidth *and* linespacing. The implementation of these constraints +in the adjoint-solver module is based on [A.M. Hammond et al., Optics +Express, Vol. 29, pp. 23916-38 (2021)](https://doi.org/10.1364/OE.431188). There are five important items to note in the set up of the optimization problem: -- The lengthscale constraint is activated only in the final epoch. It is - often helpful to mostly binarize the design before this final epoch. This is because - the lengthscale constraint forces binarization which could induce - large changes in an initial greyscale design and irrevocably spoil - the performance of the final design. - -- The initial value of the epigraph variable of the final epoch (in - which the linewidth constraint is imposed) should take into account - the value of the constraint itself to ensure a feasible starting - point. - -- The edge of the design region is padded by a filter radius (rather +1. The lengthscale constraint is activated only in the final epoch. It + is often helpful to binarize the design before this final + epoch. This is because the lengthscale constraint forces + binarization which could induce large changes in an initial + greyscale design and thus irrevocably spoil the performance of the + final design. + +2. The initial value of the epigraph variable of the final epoch (in + which the minimum feature size constraint is imposed) should take + into account the value of the constraint itself. This ensures a + feasible starting point for the [method of moving asymptotes (MMA) + optimization + algorithm](https://nlopt.readthedocs.io/en/latest/NLopt_Algorithms/#mma-method-of-moving-asymptotes-and-ccsa), + (which is based on the conservative convex separable approximation + (CCSA) algorithm). + +3. The edge of the design region is padded by a filter radius (rather than e.g., a single pixel) to produce measured lengthscales of the final design that are consistent with the imposed constraint. -- The hyperparameters of the lengthscale constraint function (`glc` in - the script below), need to be chosen carefully to produce final - designs which do not significantly degrade the performance of the - unconstrained designs at the start of the final epoch. +4. The hyperparameters of the lengthscale constraint function (`a1`, + `b1`, and `c0` in the `glc` function of the script below), need to + be chosen carefully to produce final designs which do not + significantly degrade the performance of the unconstrained designs + at the start of the final epoch. -- Damping of the design weights is used for the early epochs in which +5. Damping of the design weights is used for the early epochs in which the design is mostly greyscale to induce binarization. Subpixel averaging of the design weights is used in the later epochs in which the $\beta$ parameter of the thresholding function is large and thus @@ -114,7 +125,7 @@ optimization problem: A schematic of the final design and the simulation layout is shown below. The minimum lengthscale of the final design, measured using a [ruler](https://github.com/NanoComp/photonics-opt-testbed/tree/main/ruler), -is 163 nm. This value is consistent with the imposed lengthscale since +is 165 nm. This value is consistent with the imposed lengthscale since it is approximately within one design pixel (10 nm). ![](../images/mode_converter_sim_layout.png#center) @@ -126,15 +137,56 @@ transmittance is -2.1 dB at a wavelength of 1.265 μm. ![](../images/mode_converter_refl_tran_spectra.png#center) -Finally, a plot of the objective function history is shown. The +A plot of the objective-function history (worst case or maximum value +across the six wavelengths) for this design is also shown. The "spikes" present in the plot are a normal feature of nonlinear-optimization algorithms. The algorithm may take too large a step which turns out to make the objective function worse. This means the algorithm then has to "backtrack" and take a smaller step. This -occurs in the CCSA algorithm by increasing a penalty term. +occurs in the CCSA algorithm by increasing a penalty term. Also, even +though the worst-case objective function is constant during most of +the first epoch which may indicate the optimizer is making no +progress, in fact the optimizer is working to improve the objective +function at the other (non worst-case) wavelengths. ![](../images/mode_converter_objfunc_hist.png#center) +Finally, here are additional designs generated using constraints on +the minimum feature size of 50 nm, 70 nm, 90 nm, and 225 nm. The +designs with smaller minimum feature sizes are clearly distinguishable +from the designs with the larger ones. + +![](../images/mode_converter_designs.png#center) + +The table below shows a comparison of the imposed constraint on the +minimum feature size of the optimizer versus the measured minimum +linewidth and linespacing for the five designs presented in this +tutorial. There is fairly consistent agreement in the constraint and +measured values except for the design with the largest minimum feature +size (225 nm vs. 277 nm). For cases in which the measured minimum +feature size is significantly *larger* than the constraint used in the +optimization, this could be an indication that the final design can be +improved by a better choice of the hyperparameters in the feature-size +constraint function. Generally, one should expect the constraint and +measured values to agree within a length of about one to two +design-region pixels (10 nm, in this example). + +| constraint (nm) | measured linewidth (nm) | measured linespacing (nm) | +|:---------------:|:-----------------------:|:-------------------------:| +| 50 | 85 | 60 | +| 70 | 103 | 85 | +| 90 | 109 | 134 | +| 150 | 221 | 165 | +| 225 | 277 | 681 | + +Finally, a plot of the worst-case reflectance and transmittance versus +the imposed constraint on the minimum feature size is shown below for +the five designs. The general trend of decreasing performance (i.e., +increasing reflectance and decreasing transmittance) with increasing +minimum feature size is evident. + +![](../images/mode_converter_worst_case_refl_tran.png#center) + The script is [python/examples/adjoint_optimization/mode_converter.py](https://github.com/NanoComp/meep/tree/master/python/examples/adjoint_optimization/mode_converter.py). The runtime of this script using three Intel Xeon 2.0 GHz processors is @@ -703,13 +755,12 @@ if __name__ == '__main__': ) ``` -Compact Notebook Tutorials Demonstrating Main Features ------------------------------------------------------- +Compact Notebook Tutorials of Basic Features +-------------------------------------------- -As an alternative to the first example which combined multiple +As an alternative to the first tutorial which combined multiple features into a single demonstration, there are six notebook tutorials -that demonstrate various standalone features of the adjoint -solver. +that demonstrate various basic features of the adjoint solver. - [Introduction](https://nbviewer.jupyter.org/github/NanoComp/meep/blob/master/python/examples/adjoint_optimization/01-Introduction.ipynb) diff --git a/doc/docs/images/mode_converter_designs.png b/doc/docs/images/mode_converter_designs.png new file mode 100644 index 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