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R. Freund, H. Men, C. Nguyen, P. Parrilo and J. Peraire

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1 R. Freund, H. Men, C. Nguyen, P. Parrilo and J. Peraire
Design of Photonic Crystals with Multiple and Combined Band Gaps, plus Fabrication- Robust Design R. Freund, H. Men, C. Nguyen, P. Parrilo and J. Peraire MIT AFOSR, April 2011 MASSACHUSETTS INSTITUTE OF TECHNOLOGY

2 Wave Propagation in Periodic Media
For most l, beam(s) propagate through crystal without scattering (scattering cancels coherently). But for some l (~ 2a), no light can propagate: a band gap scattering ( from S.G. Johnson ) Rayleigh 1987 – Yablonovitch & John MASSACHUSETTS INSTITUTE OF TECHNOLOGY

3 S. G. Johnson et al., Appl. Phys. Lett. 77, 3490 (2000)
Photonic Crystals 3D Crystals Band Gap: Objective S. G. Johnson et al., Appl. Phys. Lett. 77, 3490 (2000) Applications By introducing “imperfections” one can develop: Waveguides Hyperlens Resonant cavities Switches Splitters Mangan, et al., OFC 2004 PDP24 MASSACHUSETTS INSTITUTE OF TECHNOLOGY

4 The Optimal Design Problem for Photonic Crystals
A photonic crystal with optimized 7th band gap. MASSACHUSETTS INSTITUTE OF TECHNOLOGY

5 The Optimal Design Problem for Photonic Crystals
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6 The Optimal Design Problem for Photonic Crystals
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7 The Optimal Design Problem for Photonic Crystals
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8 Previous Work There are some approaches proposed for solving the band gap optimization problem: Cox and Dobson (2000) first considered the mathematical optimization of the band gap problem and proposed a projected generalized gradient ascent method. Sigmund and Jensen (2003) combined topology optimization with the method of moving asymptotes (Svanberg (1987)). Kao, Osher, and Yablonovith (2005) used “the level set” method with a generalized gradient ascent method. However, these earlier proposals are gradient-based methods and use eigenvalues as explicit functions. They suffer from the low regularity of the problem due to eigenvalue multiplicity. MASSACHUSETTS INSTITUTE OF TECHNOLOGY

9 Our Approach Replace original eigenvalue formulation by a subspace method, and Convert the subspace problem to a convex semidefinite program (SDP) via semi-definite inclusion and linearization. MASSACHUSETTS INSTITUTE OF TECHNOLOGY

10 First Step: Standard Discretizaton
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11 Optimization Formulation: P0
Typically, MASSACHUSETTS INSTITUTE OF TECHNOLOGY

12 Parameter Dependence MASSACHUSETTS INSTITUTE OF TECHNOLOGY

13 Change of Decision Variables
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14 Reformulating the problem: P1
We demonstrate the reformulation in the TE case, This reformulation is exact, but non-convex and large-scale. We use a subspace method to reduce the problem size. MASSACHUSETTS INSTITUTE OF TECHNOLOGY

15 Subspace Method MASSACHUSETTS INSTITUTE OF TECHNOLOGY

16 Subspace Method, continued
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17 Subspace Method, continued
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18 Linear Fractional SDP :
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19 Solution Procedure The SDP optimization problems can be solved efficiently using modern interior-point methods [Toh et al. (1999)]. MASSACHUSETTS INSTITUTE OF TECHNOLOGY

20 Results: Optimal Structures
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21 Results: Computation Time
All computation performed on a Linux PC with Dual Core AMD Opteron 270, 2.0 GHz. The eigenvalue problem is solved by using the ARPACK software. MASSACHUSETTS INSTITUTE OF TECHNOLOGY

22 Mesh Adaptivity : Refinement Criteria
Interface elements 2:1 rule MASSACHUSETTS INSTITUTE OF TECHNOLOGY

23 Mesh Adaptivity : Solution Procedure
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24 Results: Optimization Process
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25 Results: Computation Time
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26 Multiple Band Gap Optimization
Multiple band gap optimization is a natural extension of the previous single band gap optimization that seeks to maximize the minimum of weighted gap-midgap ratios: MASSACHUSETTS INSTITUTE OF TECHNOLOGY

27 Multiple Band Gap Optimization
Even with other things being the same (e.g., discretization, change of variables, subspace construction), the multiple band gap optimization problem cannot be reformulated as a linear fractional SDP. We start with: where MASSACHUSETTS INSTITUTE OF TECHNOLOGY

28 Multiple Band Gap Optimization
This linearizes to: where MASSACHUSETTS INSTITUTE OF TECHNOLOGY

29 Solution Procedure MASSACHUSETTS INSTITUTE OF TECHNOLOGY

30 Sample Computational Results: 2nd and 5th TM Band Gaps
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31 Sample Computational Results: 2nd and 5th TM Band Gaps
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32 Optimized Structures TE polarization, Triangular lattice,
1st and 3rd band gaps TEM polarizations, Square lattice, Complete band gaps, 9th and 12th band gaps MASSACHUSETTS INSTITUTE OF TECHNOLOGY

33 Results: Pareto Frontiers of 1st and 3rd TE Band Gaps
TE polarization MASSACHUSETTS INSTITUTE OF TECHNOLOGY

34 Results: Computational Time
Square lattice Execution Time (minutes) MASSACHUSETTS INSTITUTE OF TECHNOLOGY

35 Future work Incorporate robust fabrication issues, see next slides….
Design of 3-dimensional photonic crystals, Incorporate robust fabrication issues, see next slides…. Metamaterial designs for cloaking devices, superlenses, and shockwave mitigation. Band-gap design optimization for other wave propagation problems, e.g., acoustic, elastic … Non-periodic structures, e.g., photonic crystal fibers. MASSACHUSETTS INSTITUTE OF TECHNOLOGY

36 Need for Fabrication Robustness
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37 Constructing Fabricable Solutions
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38 Constructing Fabricable Solutions, continued
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39 Quality of User-Constructed Solution
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40 Quality of User-Constructed Solution, continued
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41 Fabrication Robustness Paradigm
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42 Fabrication Robustness Paradigm, continued
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43 Basic Results MASSACHUSETTS INSTITUTE OF TECHNOLOGY

44 Fabrication Robustness: Basic Model
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45 Computable FR Problems via Special Structure
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46 Computable FR Problems via Special Structure, continued
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47 Computable FR Problems via Special Structure, continued
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