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arXiv 2610.09527physics.optics

从导模理论看增强现实波导的角分辨率极限

Angular resolution limit of augmented reality waveguides from guided mode theory

Guohua Wei

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中文总结 AI 辅助

从导模理论推导AR波导角分辨率极限,发现薄波导和较小TIR角使分辨率变差,500微米厚度下多数TIR范围劣于1弧分,窄线宽激光显示受影响,而LED显示不受限。

中文摘要 AI 辅助

我们从导模理论推导了增强现实(AR)波导合束器的角分辨率极限。有限厚度的平板仅支持一组离散的全内反射(TIR)角,这导致角分辨率随波导变薄和TIR角减小而变差。在500微米厚度下,在大部分可用的TIR范围内,分辨率劣于1弧分(60 ppd)的视力目标,而要在TIR<42°时达到1弧分,则需要厚度超过1毫米的基底。该极限会被大于约0.1纳米的光源线宽或大于约100纳米的跨瞳孔复制周期的厚度变化所抹除,但仅会被瞳孔截断部分消除,且完全不受出耦合损耗影响。因此,基于LED和微型LED的显示器因其宽光谱而不受影响,而基于窄线宽激光的显示器在薄且均匀的波导中则受此极限约束。

英文摘要

We derive the angular resolution limit of an augmented-reality (AR) waveguide combiner from guided mode theory. A slab of finite thickness supports only a discrete set of total-internal-reflection (TIR) angles, giving an angular resolution that worsens with thinner waveguides and smaller TIR angles. At 500 $μ$m thickness the resolution is worse than the 1 arcmin (60 ppd) acuity target over most of the usable TIR range, and reaching 1 arcmin for TIR < 42$^\circ$ requires a substrate thicker than 1 mm. The limit is washed out by a source linewidth above $\sim$0.1 nm or a thickness variation above $\sim$100 nm across the pupil-replication period, but only partially by pupil truncation and not at all by out-coupling loss. LED- and micro-LED-based displays are therefore unaffected with their broad spectrum, whereas a narrow-linewidth laser-based display in a thin, uniform waveguide is subject to this limit.

发表机构

  • Reality Labs, Meta(Meta现实实验室)

机构由 AI 辅助整理,请以论文原文为准。

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