A generalized adjoint optimization method for metasurfaces enabled by phase-convergence
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摘要:
本文构建了一种以相位调控机制为核心的超构器件通用伴随优化方法。该方法的核心在于建立了一个梯度-结构映射模型，将复数域的伴随梯度转化为物理可实现的结构更新量，从而在结构扰动与相位响应之间确立了稳定的迭代关系，最终实现对器件表面相位的逐点精确调控。其中伴随仿真始终采用单个电偶极子激励，无需针对不同设计任务重新构建伴随源；不同功能需求的差异完全可以通过结构更新映射的调整来实现，从而使该方法能够在统一仿真模型下高效处理多类型波前调控任务。在此基础上，完成了多类超构器件的数值设计验证。二维纳米柱超透镜实现了接近衍射极限的聚焦性能，衍射效率为 83.9%；基于线性相位梯度的超光栅实现了 30° 的输出偏折，+1 级衍射效率为 72.4%；设计的双焦点透镜汇聚效率达到 67.2%；全息超表面能够清晰重建中空三角形图案，对应能量集中度约为 60.3%。结果表明，所提出方法具有伴随源构建简单、计算效率高、结构类型适应性强等优势，可在统一框架下高效完成不同类型超构器件的逆向设计，为超构表面在成像、波前工程、紫外探测等领域的深入应用提供了一种可行方案。
Abstract:We propose a generalized adjoint-optimization method enabled by a phase-convergence mechanism. Central to this method is a gradient-to-structure mapping model that translates complex-valued adjoint gradients into physically realizable structural updates, establishing a stable iterative relation between structural perturbations and the resulting phase response. This mechanism ensures monotonic phase convergence at the device plane, enabling meta-element-level control of arbitrary phase profiles. Within this formulation, the adjoint simulation employs a single electric dipole excitation, independent of the desired metasurface function. Functional diversity is achieved solely by adjusting the update mapping rather than redefining the adjoint source or modifying the simulation model. This establishes a unified and computationally efficient inverse-design framework capable of handling multiple types of wavefront-shaping functionalities. As proof of concept, numerical validations are performed on diverse metadevices. Specifically, a 2D nanopillar metalens and a linear phase gradient metagrating achieved efficiencies of 83.9% and 72.4% (at 30° deflection), respectively. For arbitrary wavefront shaping, a bifocal lens showed a focusing efficiency of 67.2% and a holographic metasurface generated a hollow triangle pattern with 60.3% energy efficiency. Our results confirm that the proposed method features simplified source construction, high computational efficiency, and strong adaptability, providing a unified and viable framework for the engineering of metasurfaces in imaging, wavefront engineering, and ultraviolet detection.
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图 1 (a)超构单元结构及其(b)相位锁定机制。(a)单元结构示意图；(b)目标点相位负反馈更新示意图。
Figure 1. (a) Metasurface unit cell structure and (b) phase-locking mechanism
图 2 伴随优化流程图。其中相位参数θ(x,y)的推算除依赖 β(x,y)外，通常还需预先确定伴随仿真中偶极子源的位置，见式(9)。
Figure 2. Adjoint optimization flowchart. The parameter θ(x,y) is determined from β(x,y) once the dipole-source position in the adjoint simulation is specified; see Eq. (9).
图 3 两种伴随源策略下相位序列的收敛对比。(a) 恒定相位策略：单元相位（黑点）向固定目标（红色虚线）对齐。(b) 变相位策略：单元相位向自身均值（蓝色虚线）收敛
Figure 3. Comparison of convergence mechanisms under two different adjoint-source strategies. (a) Constant phase strategy: unit phases (black dots) align with a fixed target (red dashed line). (b) Variable phase strategy: unit phases converge toward their own mean (blue dashed line)
图 4 焦点相位在不同参数设置下的迭代与收敛情况。(a)(b) 为 α = 0时的θ扫描；(c)(d) 为θ = 0条件下的α扫描。相位均以 (−180°, 180°] 包裹
Figure 4. Iteration and convergence of the focal phase under different parameter settings. (a, b) θ sweeps with α = 0; (c, d) α sweeps with θ = 0. All phase values are wrapped to (−180°, 180°]
图 5 (a) xz平面中的归一化光强分布，虚线标识实际焦点的位置。(b) 目标焦点附近的电场归一化实部分布。(c) xy平面中的归一化光强分布。(d) 焦平面内焦点处沿 x 方向的归一化光强分布
Figure 5. (a) Normalized intensity distribution in the xz-plane, with the dashed line indicating actual focal position. (b) Normalized real part of the electric field in the vicinity of the target focus. (c) Normalized intensity distribution in the xy-plane. (d) Normalized intensity profile along the x direction in the focal plane
图 6 不同更新策略的优化对比。 (a) 归一化焦点电场强度，以蓝线最大值为基准；(b) 焦点电场相位, 范围为(−180°, 180°]。蓝色实线和橙色虚线分别对应实部与虚部梯度更新
Figure 6. Comparison of different optimization strategies. (a) Normalized focal electric field intensity, referenced to the maximum value of the blue solid line. (b) Focal electric field phase, wrapped to (−180°, 180°]. The blue solid and orange dashed lines indicate gradient updates based on the real and imaginary parts, respectively
图 7 超光栅器件。(a) 波前偏折分布，箭头示意偏折方向；(b) 出射场频谱分布，其中ux, uy为方向余弦。双焦点器件：(c) xz 平面归一化光强分布，虚线交点表示仿真得到的实际最大光强位置；(d) 焦平面（xy）的归一化光强分布。全息器件：(e) 目标中空三角形图案的光强分布，三角形外缘与孔径边界分别以实线和虚线表示；(f) 器件重建的全息图案。
Figure 7. Metagrating. (a) Deflected wavefront distribution, with the arrow indicating the deflection direction; (b) spatial spectrum of the transmitted field, where ux and uy denote the directional cosines. Bifocal lens: (c) Normalized intensity distribution in the xz-plane, where the intersection of the dashed lines marks the simulated position of maximum intensity; (d) normalized intensity distribution on the focal (xy) plane. Holographic metasurface: (e) Target intensity pattern of the hollow triangle, with its outer boundary and inner aperture indicated by solid and dashed lines, respectively; (f) reconstructed holographic pattern
表 1 传统方案与本文伴随源构造方案的定量对比
Table 1. Quantitative comparison of conventional and proposed adjoint-source constructions
指标 传统方案 本文方案 FDTD Yee
网格节点总数3.76 MNodes 2.62 MNodes
（模型相同）单轮仿真时间
（正向+伴随）174.4 s 121.5 s
（典型值，ξ=0°）稳定所需代数 18 19（典型值，ξ=0°） 优化后
目标焦点相位77.2° 2.8°，（ξ=0°）
90.9°，（ξ=90°）
178.2°，（ξ=180°）优化后目标
焦点强度
（归一化）1 1.13，（ξ=0°）
1.29，（ξ=90°）
0.95，（ξ=180°）优化后实际
焦点位置误差0.52 μm 0.35 μm，（ξ=0°）
0.30 μm，（ξ=90°）
0.68 μm，（ξ=180°）
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