A Two-Mirror Faceted Projection System for EUV Lithography
physics.optics, cs.LG, physics.app-ph, physics.class-ph, physics.comp-ph
Submitted: 2026-09-10
Updated: 2026-09-10
License: http://creativecommons.org/licenses/by/4.0/
The gist: We propose an all-reflective two-mirror projection system for extreme ultraviolet (EUV) lithography operating at exposure wavelengths of 13.5 nm (Mo/Si) and 11.2 nm (Ru/Be), delivering a fourfold (4
Terminology
Abstract
We propose an all-reflective two-mirror projection system for extreme ultraviolet (EUV) lithography operating at exposure wavelengths of 13.5 nm (Mo/Si) and 11.2 nm (Ru/Be), delivering a fourfold (4 times) demagnification of the periodic mask pattern at a numerical aperture approaching unity (NA about 0.993). In contrast to conventional EUV projection objectives that incorporate 6--10 aspheric mirrors with an overall optical throughput of less than 15%, the proposed design redirects each accepted discrete spatial diffraction order scattered by the mask onto the wafer via a dedicated pair of planar mirror facets. The number of reflections is strictly fixed at two for all accepted orders, retaining 50 -- 60% of the power leaving the mask in each accepted order. We derive a spatial geometry providing rigorous optical path length equalization across all diffraction orders, thereby removing order-dependent propagation phase shifts. Individually optimized 30-bilayer Bragg multilayer coatings are designed for each facet using the transfer matrix method combined with global evolutionary optimization algorithms. The architecture is generalized to a three-dimensional vector formulation with a two-dimensionally periodic mask. Utilizing inverse lithography technology, Fourier parameterization, and a differentiable electromagnetic modal waveguide solver, we solve the synthesis problem for binary absorber masks (La absorber on a Ru/Be/Sr multilayer mirror). We demonstrate simulated aerial images of sub-10-nm features on the wafer (isolated peaks with a full width at half maximum (FWHM) of approximately 5.4 nm and line pairs with a critical dimension of 6 nm) and find that the two peaks remain resolved for the tested wafer defocus values from 0 to 5 nm along the z-axis.
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