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    ํŽธ๊ด‘ ๋‹ค์ค‘ํ™”๋ฅผ ์ด์šฉํ•˜์—ฌ ํ–ฅ์ƒ๋œ ๊ธฐ๋Šฅ์„ ์ œ๊ณตํ•˜๋Š” ๋„ํŒŒ๊ด€ ๊ธฐ๋ฐ˜์˜ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2021. 2. ์ด๋ณ‘ํ˜ธ.This dissertation presents the studies on the optical design method that enhances the display performance of see-through waveguide-based near-eye displays (WNEDs) using the polarization multiplexing technique. The studies focus on the strategies to improve the crucial display performances without compromising a small form factor, the most attractive merit of the WNEDs. To achieve this goal, thin and lightweight polarization-dependent optical elements are devised and employed in the WNED structure. The polarization-dependent devices can allow multiple optical functions or optical paths depending on the polarization state of the input beam, which can break through the limitation of the waveguide system with the polarization multiplexing. To realize the function-selective eyepiece for AR applications, the proposed devices should operate as an optically transparent window for the real scene while performing specific optical functions for the virtual image. The proposed devices are manufactured in a combination structure in which polarization-dependent optical elements are stacked. The total thickness of the stacked structure is about 1 mm, and it can be attached to the waveguide surface without conspicuously increasing the form factor of the optical system. Using the proposed polarization-dependent devices, the author proposes three types of novel WNED systems with enhanced performance. First, the author suggests a compact WNED with dual focal planes. Conventional WNEDs have an inherent limitation that the focal plane of the virtual image is at an infinite distance because they extract a stream of collimated light at the out-coupler. By using the polarization-dependent eyepiece lens, an additional focal plane can be generated with the polarization multiplexing in addition to infinity depth. The proposed configuration can provide comfortable AR environments by alleviating visual fatigue caused by vergence-accommodation conflict. Second, the novel WNED configuration with extended field-of-view (FOV) is presented. In the WNEDs, the maximum allowable FOV is determined by the material properties of the diffraction optics and the substrate. By using the polarization-dependent steering combiner, the FOV can be extended up to two times, which can provide more immersive AR experiences. In addition, this dissertation demonstrates that the distortion for the real scene caused by the stacked structure cannot severely disturb the image quality, considering the acuity of human vision. Lastly, the author presents a retinal projection-based WNED with switchable viewpoints by simultaneously adopting the polarization-dependent lens and grating. The proposed system can convert the viewpoint according to the position of the eye pupil without mechanical movement. The polarization-dependent viewpoint switching can resolve the inherent problem of a narrow eyebox in retinal projection displays without employing the bulky optics for mechanical movement. In conclusion, the dissertation presents the practical optical design and detailed analysis for enhanced WNED based on the polarization multiplexing technique through various simulations and experiments. The proposed approaches are expected to be utilized as an innovative solution for compact wearable displays.๋ณธ ๋ฐ•์‚ฌํ•™์œ„ ๋…ผ๋ฌธ์—์„œ๋Š” ํŽธ๊ด‘ ๋‹ค์ค‘ํ™” ๊ธฐ๋ฒ•์„ ์ด์šฉํ•˜์—ฌ ๋„ํŒŒ๊ด€ ๊ธฐ๋ฐ˜์˜ ์ฆ๊ฐ•ํ˜„์‹ค ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด์˜ ์„ฑ๋Šฅ์„ ํ–ฅ์ƒ์‹œํ‚ค๋Š” ๊ด‘ํ•™ ์„ค๊ณ„ ๋ฐ ์ด์— ๋Œ€ํ•œ ๋ถ„์„์— ๋Œ€ํ•ด ๋…ผ์˜ํ•œ๋‹ค. ๋ณธ ์—ฐ๊ตฌ๋Š” ๋„ํŒŒ๊ด€ ๊ธฐ๋ฐ˜ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด์˜ ๊ฐ€์žฅ ํฐ ์žฅ์ ์ธ ์†Œํ˜• ํผ ํŒฉํ„ฐ๋ฅผ ์œ ์ง€ํ•˜๋ฉด์„œ ๋””์Šคํ”Œ๋ ˆ์ด ์„ฑ๋Šฅ์„ ๊ฐœ์„ ํ•˜๋Š” ๊ฒƒ์— ์ค‘์ ์„ ๋‘”๋‹ค. ์ด๋ฅผ ์œ„ํ•ด ๊ธฐ์กด ๊ด‘ํ•™ ์†Œ์ž์— ๋น„ํ•ด ๋งค์šฐ ๊ฐ€๋ณ๊ณ  ์–‡์€ ํŽธ๊ด‘ ์˜์กดํ˜• ๊ฒฐํ•ฉ๊ธฐ ๊ด‘ํ•™ ์†Œ์ž๊ฐ€ ์ƒˆ๋กญ๊ฒŒ ์ œ์•ˆ๋˜๋ฉฐ, ์ด๋Š” ์ž…์‚ฌ๊ด‘์˜ ํŽธ๊ด‘ ์ƒํƒœ์— ๋”ฐ๋ผ ๋…๋ฆฝ์ ์ธ ๊ด‘ ๊ฒฝ๋กœ ์ œ์–ด๋ฅผ ๊ฐ€๋Šฅ์ผ€ ํ•˜์—ฌ ํŽธ๊ด‘ ๋‹ค์ค‘ํ™”๋ฅผ ํ†ตํ•ด ํ–ฅ์ƒ๋œ ์„ฑ๋Šฅ์„ ์ œ๊ณต ํ•  ์ˆ˜ ์žˆ๋‹ค. ๋˜ํ•œ ์‹ค์ œ ์˜์ƒ์˜ ๋น›์€ ๊ทธ๋Œ€๋กœ ํˆฌ๊ณผ ์‹œํ‚ด์œผ๋กœ์จ ์ฆ๊ฐ•ํ˜„์‹ค์„ ์œ„ํ•œ ์†Œ์ž๋กœ ํ™œ์šฉ ๊ฐ€๋Šฅํ•˜๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ ์ œ์•ˆํ•˜๋Š” ํŽธ๊ด‘ ์˜์กดํ˜• ๊ฒฐํ•ฉ๊ธฐ ๊ด‘ํ•™ ์†Œ์ž๋Š” ๊ธฐํ•˜ํ•™์  ์œ„์ƒ(geometric phase, GP)์— ๊ธฐ๋ฐ˜ํ•˜์—ฌ ๋™์ž‘ํ•œ๋‹ค. GP ๊ธฐ๋ฐ˜์˜ ๊ด‘ํ•™์†Œ์ž๊ฐ€ ์„œ๋กœ ์ง๊ตํ•˜๋Š” ์›ํ˜• ํŽธ๊ด‘ ์ž…์‚ฌ๊ด‘์— ๋Œ€ํ•ด ์ƒ๋ณด์ ์ธ ๊ธฐ๋Šฅ์„ ์ˆ˜ํ–‰ํ•˜๋Š” ๊ฒƒ์„ ์ด์šฉํ•˜์—ฌ, ๋‘ ๊ฐœ ์ด์ƒ์˜ GP ์†Œ์ž์™€ ํŽธ๊ด‘ ์ œ์–ด๋ฅผ ์œ„ํ•œ ๊ด‘ํ•™ ํ•„๋ฆ„๋“ค์„ ์ค‘์ฒฉ ์‹œํ‚ด์œผ๋กœ์จ ์ฆ๊ฐ•ํ˜„์‹ค ๊ฒฐํ•ฉ๊ธฐ ๊ด‘ํ•™ ์†Œ์ž๋ฅผ ๊ตฌํ˜„ํ•  ์ˆ˜ ์žˆ๋‹ค. ์ด๋“ค ๊ด‘ํ•™์†Œ์ž๋Š” ๋งค์šฐ ์–‡๊ธฐ ๋•Œ๋ฌธ์—, ๋ณธ ์—ฐ๊ตฌ์—์„œ ์ œ์ž‘๋œ ํŽธ๊ด‘ ์˜์กดํ˜• ๊ฒฐํ•ฉ๊ธฐ ๊ด‘ํ•™ ์†Œ์ž์˜ ์ด ๋‘๊ป˜๋Š” 1 mm ์ˆ˜์ค€์œผ๋กœ ํผ ํŒฉํ„ฐ ์ œ์•ฝ์œผ๋กœ๋ถ€ํ„ฐ ์ž์œ ๋กญ๋‹ค. ๋˜ํ•œ ํ‰ํ‰ํ•œ ํ•„๋ฆ„ ํ˜•ํƒœ์ด๋ฏ€๋กœ, ํ‰ํŒํ˜• ๋„ํŒŒ๊ด€์— ๋ถ€์ฐฉํ•˜๊ธฐ ์‰ฝ๋‹ค๋Š” ์ด์ ์„ ์ง€๋‹Œ๋‹ค. ๊ณ ์•ˆ๋œ ํŽธ๊ด‘ ์˜์กดํ˜• ๊ฒฐํ•ฉ๊ธฐ ๊ด‘ํ•™ ์†Œ์ž๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ ์„ธ ๊ฐ€์ง€ ์œ ํ˜•์˜ ์ƒˆ๋กœ์šด ๋„ํŒŒ๊ด€ ๊ธฐ๋ฐ˜์˜ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด ๊ตฌ์กฐ๋ฅผ ์ œ์•ˆํ•œ๋‹ค. ์ฒซ ๋ฒˆ์งธ๋Š” ์ž…์‚ฌ๊ด‘์˜ ํŽธ๊ด‘ ์ƒํƒœ์— ๋”ฐ๋ผ ํˆฌ๋ช… ๊ด‘ํ•™ ์ฐฝ ๋˜๋Š” ์˜ค๋ชฉ ๋ Œ์ฆˆ๋กœ ์ž‘๋™ํ•˜๋Š” ํŽธ๊ด‘ ์˜์กดํ˜• ๊ฒฐํ•ฉ๊ธฐ ๋ Œ์ฆˆ๋ฅผ ์ ์šฉํ•˜์—ฌ ๊ฐ€์ƒ ์˜์ƒ์— ๋Œ€ํ•ด ์ด์ค‘ ์ดˆ์ ๋ฉด์„ ์ œ๊ณตํ•˜๋Š” ์‹œ์Šคํ…œ์ด๋‹ค. ์ œ์•ˆ๋œ ๊ตฌ์กฐ๋Š” ๊ธฐ์กด์˜ ๋„ํŒŒ๊ด€ ๊ธฐ๋ฐ˜ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด๊ฐ€ ๋ฌดํ•œ๋Œ€ ์œ„์น˜์— ๋‹จ์ผ ์ดˆ์ ๋ฉด์„ ์ œ๊ณตํ•จ์œผ๋กœ์จ ๋ฐœ์ƒํ•˜๋Š” ์‹œ๊ฐ์  ํ”ผ๋กœ ๋ฐ ํ๋ฆฟํ•œ ์ฆ๊ฐ•ํ˜„์‹ค ์˜์ƒ์˜ ๋ฌธ์ œ๋ฅผ ์™„ํ™”ํ•  ์ˆ˜ ์žˆ๋‹ค. ๋‘ ๋ฒˆ์งธ๋กœ๋Š” ์ž…์‚ฌ๊ด‘์˜ ํŽธ๊ด‘ ์ƒํƒœ์— ๋”ฐ๋ผ ๊ด‘ ๊ฒฝ๋กœ๋ฅผ ์ขŒ์ธก ๋˜๋Š” ์šฐ์ธก์œผ๋กœ ์ œ์–ดํ•  ์ˆ˜ ์žˆ๋Š” ํŽธ๊ด‘ ๊ฒฉ์ž๋ฅผ ํ™œ์šฉํ•˜์—ฌ ๊ฐ€์ƒ ์˜์ƒ์˜ ์‹œ์•ผ๊ฐ์„ ๊ธฐ์กด๋ณด๋‹ค ์ตœ๋Œ€ 2๋ฐฐ๊นŒ์ง€ ํ™•์žฅํ•  ์ˆ˜ ์žˆ๋Š” ์‹œ์Šคํ…œ์„ ์ œ์•ˆํ•œ๋‹ค. ์ด๋Š” ๋‹จ์ผ ๋„ํŒŒ๊ด€ ๊ธฐ๋ฐ˜ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด์—์„œ ์˜์ƒ ๊ฒฐํ•ฉ๊ธฐ (imaging combiner)๋กœ ํ™œ์šฉ๋˜๋Š” ํšŒ์ ˆ ์†Œ์ž์˜ ์„ค๊ณ„ ๋ณ€์ˆ˜์— ์˜ํ•ด ์ œํ•œ๋˜๋Š” ์‹œ์•ผ๊ฐ ํ•œ๊ณ„์ ์„ ๋ŒํŒŒํ•  ์ˆ˜ ์žˆ๋Š” ๊ตฌ์กฐ๋กœ ์ปดํŒฉํŠธํ•œ ํผ ํŒฉํ„ฐ๋กœ ๋”์šฑ ๋ชฐ์ž…๊ฐ ์žˆ๋Š” ๋Œ€ํ™”๋ฉด ์ฆ๊ฐ•ํ˜„์‹ค ์˜์ƒ์„ ์ œ๊ณตํ•  ์ˆ˜ ์žˆ๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ ์œ„์—์„œ ์ œ์•ˆ๋œ ๋‘ ๊ฐ€์ง€ ํŽธ๊ด‘ ์˜์กดํ˜• ๊ด‘ํ•™ ์†Œ์ž๋ฅผ ๋ชจ๋‘ ์‚ฌ์šฉํ•˜์—ฌ ์‹œ์  ์ „ํ™˜์ด ๊ฐ€๋Šฅํ•œ ๋„ํŒŒ๊ด€ ๊ธฐ๋ฐ˜์˜ ๋ง๋ง‰ ํˆฌ์‚ฌํ˜• ๋””์Šคํ”Œ๋ ˆ์ด ๊ตฌ์กฐ๋ฅผ ์ œ์•ˆํ•œ๋‹ค. ํŽธ๊ด‘ ๋‹ค์ค‘ํ™”๋ฅผ ํ†ตํ•ด ๋‹ค์ค‘ ์ดˆ์ ๋“ค์„ ์„ ํƒ์ ์œผ๋กœ ํ™œ์„ฑํ™”ํ•จ์œผ๋กœ์จ, ํ™•์žฅ๋œ ์‹œ์ฒญ์˜์—ญ์„ ์ œ๊ณตํ•˜๋Š” ๋™์‹œ์— ๋™๊ณต ํฌ๊ธฐ ๋ณ€ํ™” ๋˜๋Š” ์›€์ง์ž„์— ์˜ํ•œ ์ด์ค‘ ์˜์ƒ ๋ฌธ์ œ๋ฅผ ์™„ํ™”ํ•  ์ˆ˜ ์žˆ๋‹ค. ๋˜ํ•œ ๊ธฐ๊ณ„์  ์›€์ง์ž„ ์—†์ด ์‹œ์  ๊ฐ„์˜ ๊ณ ์† ์ „ํ™˜์ด ๊ฐ€๋Šฅํ•˜๋‹ค๋Š” ์žฅ์ ์„ ์ง€๋‹ˆ๊ณ  ์žˆ๋‹ค. ๋ณธ ๋ฐ•์‚ฌํ•™์œ„ ๋…ผ๋ฌธ์—์„œ ์ œ์‹œํ•œ ํŽธ๊ด‘ ๋‹ค์ค‘ํ™”๋ฅผ ํ™œ์šฉํ•œ ์ƒˆ๋กœ์šด ๊ฒฐํ•ฉ๊ธฐ ๊ด‘ํ•™ ์†Œ์ž ๋ฐ ๊ด‘ํ•™ ๊ตฌ์กฐ๋“ค์€ ๋„ํŒŒ๊ด€ ๊ธฐ๋ฐ˜ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด์˜ ํ–ฅ์ƒ๋œ ์„ฑ๋Šฅ์„ ์ œ๊ณตํ•˜๋Š” ํ•ด๊ฒฐ์ฑ… ๋ฐ ์ƒˆ๋กœ์šด ๊ฐ€๋Šฅ์„ฑ์œผ๋กœ ์ œ์‹œํ•  ์ˆ˜ ์žˆ์„ ๊ฒƒ์ด๋ผ ๊ธฐ๋Œ€๋œ๋‹ค.Abstract i Contents iii List of Tables vi List of Figures vii Chapter. 1 Introduction 1 1.1 Augmented reality near-eye display 1 1.2 Key performance parameters of near-eye displays 4 1.3 Basic scheme of waveguide-based near-eye displays 22 1.4 Motivation and purpose of this dissertation 33 1.5 Scope and organization 37 Chapter 2 Dual-focal waveguide-based near-eye display using polarization-dependent combiner lens 39 2.1 Introduction 39 2.2 Optical design for polarization-dependent combiner lens 42 2.2.1 Design and principle of polarization-dependent combiner lens 42 2.2.2 Prototype implementation 48 2.3 Waveguide-based augmented reality near-eye display with dual-focal plane using polarization-dependent combiner lens 51 2.3.1 Implementation of the prototype and experimental results 51 2.3.2 Performance analysis and discussion 57 2.4 Conclusion 69 Chapter 3 Extended-field-of-view waveguide-based near-eye display via polarization-dependent steering combiner 70 3.1 Introduction 70 3.2 Optical design for polarization-dependent steering combiner 73 3.2.1 Principle of polarization grating 73 3.2.2 Principle of polarization-dependent steering combiner 76 3.2.3 Analysis and verification experiment for real-scene distortion 77 3.3 Waveguide-based augmented reality near-eye display with extended-field-of-view 81 3.3.1 Field-of-view for volume grating based waveguide technique 81 3.3.2 Implementation of the prototype and experimental results 84 3.3.3 Performances analysis and discussion 87 3.4 Conclusion 92 Chapter 4 Viewpoint switchable retinal-projection-based near-eye display with waveguide configuration 93 4.1 Introduction 93 4.2 Polarization-dependent switchable eyebox 97 4.2.1 Optical devices for polarization-dependent switching of viewpoints 97 4.2.2 System configuration for proposed method 100 4.2.3 Design of waveguide and imaging combiner 105 4.3 Compact retinal projection-based near-eye display with switchable viewpoints via waveguide configuration 114 4.3.1 Implementation of the prototype and experimental results 114 4.3.2 Performance analysis and discussion 118 4.4 Conclusion 122 Chapter 5. Conclusion 123 Bibliography 127 Appendix 135Docto

    ๋น„๋“ฑ๋ฐฉ์„ฑ ๊ด‘ํ•™ ์†Œ์ž๋ฅผ ์ด์šฉํ•œ ๊ด‘ ์‹œ์•ผ๊ฐ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2019. 2. ์ด๋ณ‘ํ˜ธ.Near-eye display is considered as a promising display technique to realize augmented reality by virtue of its high sense of immersion and user-friendly interface. Among the important performances of near-eye display, a field of view is the most crucial factor for providing a seamless and immersive experience for augmented reality. In this dissertation, a transmissive eyepiece is devised instead of a conventional reflective eyepiece and it is discussed how to widen the field of view without loss of additional system performance. In order to realize the transmissive eyepiece, the eyepiece should operate lens to virtual information and glass to real-world scene. Polarization multiplexing technique is used to implement the multi-functional optical element, and anisotropic optical elements are used as material for multi-functional optical element. To demonstrate the proposed idea, an index-matched anisotropic crystal lens has been presented that reacts differently depending on polarization. With the combination of isotropic material and anisotropic crystal, the index-matched anisotropic crystal lens can be the transmissive eyepiece and achieve the large field of view. Despite the large field of view by the index-matched anisotropic crystal lens, many problems including form factor still remain to be solved. In order to overcome the limitations of conventional optics, a metasurface is adopted to the augmented reality application. With a stunning optical performance of the metasurface, a see-through metasurface lens is proposed and designed for implementing wide field of view near-eye display. The proposed novel eyepieces are expected to be an initiative study not only improving the specification of the existing near-eye display but opening the way for a next generation near-eye display.๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด๋Š” ๋†’์€ ๋ชฐ์ž…๊ฐ๊ณผ ์‚ฌ์šฉ์ž ์นœํ™”์ ์ธ ์ธํ„ฐํŽ˜์ด์Šค๋กœ ์ธํ•ด ์ฆ๊ฐ• ํ˜„์‹ค์„ ๊ตฌํ˜„ํ•˜๋Š” ๊ฐ€์žฅ ํšจ๊ณผ์ ์ธ ๊ธฐ์ˆ ๋กœ ์ตœ๊ทผ ํ™œ๋ฐœํ•œ ์—ฐ๊ตฌ๊ฐ€ ๊ณ„์†๋˜๊ณ  ์žˆ๋‹ค. ์ด๋Ÿฌํ•œ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด์˜ ์ค‘์š”ํ•œ ์„ฑ๋Šฅ ์ค‘ ์‹œ์•ผ๊ฐ์€ ๋งค๋„๋Ÿฝ๊ณ  ๋ชฐ์ž…๊ฐ ์žˆ๋Š” ๊ฒฝํ—˜์„ ์‚ฌ์šฉ์ž์—๊ฒŒ ์ „ํ•ด์คŒ์œผ๋กœ์จ ๊ฐ€์žฅ ์ค‘์š”ํ•œ ๊ด‘ํ•™์  ํ‰๊ฐ€์ง€ํ‘œ ์ค‘์— ํ•˜๋‚˜์ด๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ๊ธฐ์กด์˜ ๋ฐ˜์‚ฌํ˜• ์•„์ดํ”ผ์Šค (eyepiece) ๋ฅผ ๋Œ€์‹ ํ•˜๋Š” ํˆฌ๊ณผํ˜• ์•„์ดํ”ผ์Šค๋ฅผ ์ œ์•ˆํ•œ๋‹ค. ์ด๋Ÿฌํ•œ ํˆฌ๊ณผํ˜• ์•„์ดํ”ผ์Šค๋ฅผ ๊ตฌํ˜„ํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ์™ธ๋ถ€ ์ •๋ณด์— ๋Œ€ํ•ด์„œ๋Š” ํˆฌ๋ช…ํ•œ ์œ ๋ฆฌ์™€ ๊ฐ™์ด ํˆฌ๊ณผ์‹œํ‚ค๋ฉฐ, ๋™์‹œ์— ๊ฐ€์ƒ ์ •๋ณด๋Š” ๋ Œ์ฆˆ๋กœ ์ž‘๋™ํ•˜์—ฌ ๋จผ ๊ฑฐ๋ฆฌ์— ๋„์šธ ์ˆ˜ ์žˆ๋Š” ๊ด‘ํ•™์†Œ์ž๋ฅผ ๊ฐœ๋ฐœํ•˜์—ฌ์•ผ ํ•œ๋‹ค. ์ด๋Ÿฌํ•œ ํˆฌ๊ณผํ˜• ์•„์ดํ”ผ์Šค๋ฅผ ๊ตฌํ˜„ํ•˜๊ธฐ ์œ„ํ•ด์„œ ํŽธ๊ด‘์— ๋”ฐ๋ผ ๋‹ค๋ฅด๊ฒŒ ๋ฐ˜์‘ํ•˜๋Š” ๊ตด์ ˆ๋ฅ  ์ •ํ•ฉ ์ด๋ฐฉ์„ฑ ๊ฒฐ์ • ๋ Œ์ฆˆ (index-matched anisotropic crystal lens) ๋ฅผ ์ œ์•ˆํ•˜์˜€๋‹ค. ์ด๋ฐฉ์„ฑ ๊ฒฐ์ • ๊ตฌ์กฐ (anisotropic crystal)๋กœ ์ด๋ฃจ์–ด์ง„ ๋ Œ์ฆˆ์™€ ์ด๋ฅผ ๋‘˜๋Ÿฌ์‹ผ ๋“ฑ๋ฐฉ์„ฑ ๋ฌผ์งˆ (isotropic crytal) ๋กœ ์ด๋ฃจ์–ด์ง„ ๊ตด์ ˆ๋ฅ  ์ •ํ•ฉ ์ด๋ฐฉ์„ฑ ๊ฒฐ์ • ๋ Œ์ฆˆ๋Š” ํŽธ๊ด‘์— ๋”ฐ๋ผ ๋‹ค๋ฅด๊ฒŒ ์ž‘๋™ํ•œ๋‹ค. ์ด๋Ÿฌํ•œ ํˆฌ๊ณผํ˜• ์•„์ดํ”ผ์Šค๋Š” ๊ธฐ์กด์˜ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด์— ๋น„ํ•ด ๋„“์€ ์‹œ์•ผ๊ฐ์„ ์ œ๊ณตํ•  ์ˆ˜ ์žˆ์ง€๋งŒ ์ด๋ฐฉ์„ฑ ๊ฒฐ์ • ๊ตฌ์กฐ์˜ ๋‚ฎ์€ ๊ตด์ ˆ๋ฅ  ์ฐจ์ด๋กœ ์ธํ•ด ์‹œ์Šคํ…œ์˜ ํฌ๊ธฐ๊ฐ€ ์ปค์ง€๋Š” ๋‹จ์ ์„ ๊ฐ€์ง€๊ณ  ์žˆ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์ด๋Ÿฌํ•œ ๋‹จ์ ์„ ๊ฐœ์„ ํ•˜๊ธฐ ์œ„ํ•ด ๋ฉ”ํƒ€ ํ‘œ๋ฉด์„ ์ฆ๊ฐ• ํ˜„์‹ค ๋””์Šคํ”Œ๋ ˆ์ด ๋ถ„์•ผ์— ์ ์šฉํ•˜์˜€๋‹ค. ๋ฉ”ํƒ€ ํ‘œ๋ฉด์˜ ๊ธฐ์กด ๊ด‘ํ•™ ์†Œ์ž๋ฅผ ๋Šฅ๊ฐ€ํ•˜๋Š” ๋†€๋ผ์šด ๊ด‘ํ•™ ์„ฑ๋Šฅ์„ ์ด์šฉํ•˜์—ฌ ๋„“์€ ์‹œ์•ผ๊ฐ์„ ๊ฐ€์ง€๋Š” ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด๋ฅผ ๊ตฌํ˜„ํ•˜๊ธฐ ์œ„ํ•ด ํˆฌ๋ช… ๋ฉ”ํƒ€ ๋ Œ์ฆˆ๋ฅผ ์ œ์•ˆํ•˜์˜€๋‹ค. ํŽธ๊ด‘์— ๋”ฐ๋ผ ๋‹ค๋ฅด๊ฒŒ ๋ฐ˜์‘ํ•˜๋Š” ํˆฌ๋ช… ๋ฉ”ํƒ€๋ Œ์ฆˆ๋Š” ๋„“์€ ์‹œ์•ผ๊ฐ๊ณผ ๊ฒฝ๋Ÿ‰ํ™” ์‹œ์Šคํ…œ ๊ตฌํ˜„์ด ๊ฐ€๋Šฅํ•˜๋ฉฐ ์ด๋ฅผ ์ž…์ฆํ•˜๊ธฐ ์œ„ํ•ด ํˆฌ๋ช… ๋ฉ”ํƒ€๋ Œ์ฆˆ์˜ ์„ค๊ณ„ ๋ฐฉ๋ฒ• ๋ฟ ์•„๋‹ˆ๋ผ ์‹ค์ œ ๊ตฌํ˜„์„ ํ†ตํ•œ ๊ฐ€๋Šฅ์„ฑ์„ ์ž…์ฆํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ ์ƒˆ๋กœ์šด ์•„์ดํ”ผ์Šค์— ๋Œ€ํ•œ ๊ฐœ๋…์€ ๊ธฐ์กด์˜ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด์˜ ์‚ฌ์–‘ ๊ฐœ์„ ์— ์œ ์šฉํ•˜๊ฒŒ ์‚ฌ์šฉ๋  ๋ฟ ์•„๋‹ˆ๋ผ ์ฐจ์„ธ๋Œ€ ๊ทผ์•ˆ ๋””์Šคํ”Œ๋ ˆ์ด๋ฅผ ์œ„ํ•œ ์„ ๋„์ ์ธ ์—ญํ• ์„ ํ•  ๊ฒƒ์œผ๋กœ ๊ธฐ๋Œ€๋œ๋‹ค.Abstract Contents List of Tables List of Figures Near-eye displays with wide field of view using anisotropic optical elements Chapter 1 Introduction 1.1 Near-eye displays for augmented reality 1.2 Optical performances of near-eye display 1.3 State-of-the-arts of near-eye display 1.4 Motivation and contribution of this dissertation Chapter 2 Transmissive eyepiece for wide field of view near-eye display 2.1 Transmissive eyepiece for near-eye display Chapter 3 Near-eye display using index-matched anisotropic crystal lens 3.1 Introduction 3.2 Index-matched anisotropic crystal lens 3.2.1 Principle of the index-matched anisotropic crystal lens 3.2.2 Aberration analysis of index-matched anisotropic crystal lens 3.2.3 Implementation 3.3 Near-eye displays using index-matched anisotropic crystal lens 3.3.1 Near-eye display using index-matched anisotropic crystal lens 3.3.2 Flat panel type near-eye display using IMACL 3.3.3 Polarization property of transparent screen 3.4 Conclusion Chapter 4 Near-eye display using metasurface lens 4.1 Introduction 4.2 See-through metasurface lens 4.2.1 Metasurface lens 4.3 Full-color near-eye display using metasurface lens 4.3.1 Full-color near-eye display using metasurface lens 4.3.2 Holographic near-eye display using metasurface lens for aberration compensation 4.4 Conclusion Chapter 5 Conclusion Bibliography AppendixDocto

    Deformable Beamsplitters: Enhancing Perception with Wide Field of View, Varifocal Augmented Reality Displays

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    An augmented reality head-mounted display with full environmental awareness could present data in new ways and provide a new type of experience, allowing seamless transitions between real life and virtual content. However, creating a light-weight, optical see-through display providing both focus support and wide field of view remains a challenge. This dissertation describes a new dynamic optical element, the deformable beamsplitter, and its applications for wide field of view, varifocal, augmented reality displays. Deformable beamsplitters combine a traditional deformable membrane mirror and a beamsplitter into a single element, allowing reflected light to be manipulated by the deforming membrane mirror, while transmitted light remains unchanged. This research enables both single element optical design and correct focus while maintaining a wide field of view, as demonstrated by the description and analysis of two prototype hardware display systems which incorporate deformable beamsplitters. As a user changes the depth of their gaze when looking through these displays, the focus of virtual content can quickly be altered to match the real world by simply modulating air pressure in a chamber behind the deformable beamsplitter; thus ameliorating vergenceโ€“accommodation conflict. Two user studies verify the display prototypesโ€™ capabilities and show the potential of the display in enhancing human performance at quickly perceiving visual stimuli. This work shows that near-eye displays built with deformable beamsplitters allow for simple optical designs that enable wide field of view and comfortable viewing experiences with the potential to enhance user perception.Doctor of Philosoph

    Geometric model and calibration method for a solid-state LiDAR

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    This paper presents a novel calibration method for solid-state LiDAR devices based on a geometrical description of their scanning system, which has variable angular resolution. Determining this distortion across the entire Field-of-View of the system yields accurate and precise measurements which enable it to be combined with other sensors. On the one hand, the geometrical model is formulated using the well-known Snellโ€™s law and the intrinsic optical assembly of the system, whereas on the other hand the proposed method describes the scanned scenario with an intuitive camera-like approach relating pixel locations with scanning directions. Simulations and experimental results show that the model fits with real devices and the calibration procedure accurately maps their variant resolution so undistorted representations of the observed scenario can be provided. Thus, the calibration method proposed during this work is applicable and valid for existing scanning systems improving their precision and accuracy in an order of magnitude.Peer ReviewedPostprint (published version

    Roadmap on digital holography [Invited]

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    This Roadmap article on digital holography provides an overview of a vast array of research activities in the field of digital holography. The paper consists of a series of 25 sections from the prominent experts in digital holography presenting various aspects of the field on sensing, 3D imaging and displays, virtual and augmented reality, microscopy, cell identification, tomography, label-free live cell imaging, and other applications. Each section represents the vision of its author to describe the significant progress, potential impact, important developments, and challenging issues in the field of digital holography

    Bio-Inspired Multi-Spectral Image Sensor and Augmented Reality Display for Near-Infrared Fluorescence Image-Guided Surgery

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    Background: Cancer remains a major public health problem worldwide and poses a huge economic burden. Near-infrared (NIR) fluorescence image-guided surgery (IGS) utilizes molecular markers and imaging instruments to identify and locate tumors during surgical resection. Unfortunately, current state-of-the-art NIR fluorescence imaging systems are bulky, costly, and lack both fluorescence sensitivity under surgical illumination and co-registration accuracy between multimodal images. Additionally, the monitor-based display units are disruptive to the surgical workflow and are suboptimal at indicating the 3-dimensional position of labeled tumors. These major obstacles have prevented the wide acceptance of NIR fluorescence imaging as the standard of care for cancer surgery. The goal of this dissertation is to enhance cancer treatment by developing novel image sensors and presenting the information using holographic augmented reality (AR) display to the physician in intraoperative settings. Method: By mimicking the visual system of the Morpho butterfly, several single-chip, color-NIR fluorescence image sensors and systems were developed with CMOS technologies and pixelated interference filters. Using a holographic AR goggle platform, an NIR fluorescence IGS display system was developed. Optoelectronic evaluation was performed on the prototypes to evaluate the performance of each component, and small animal models and large animal models were used to verify the overall effectiveness of the integrated systems at cancer detection. Result: The single-chip bio-inspired multispectral logarithmic image sensor I developed has better main performance indicators than the state-of-the-art NIR fluorescence imaging instruments. The image sensors achieve up to 140 dB dynamic range. The sensitivity under surgical illumination achieves 6108 V/(mW/cm2), which is up to 25 times higher. The signal-to-noise ratio is up to 56 dB, which is 11 dB greater. These enable high sensitivity fluorescence imaging under surgical illumination. The pixelated interference filters enable temperature-independent co-registration accuracy between multimodal images. Pre-clinical trials with small animal model demonstrate that the sensor can achieve up to 95% sensitivity and 94% specificity with tumor-targeted NIR molecular probes. The holographic AR goggle provides the physician with a non-disruptive 3-dimensional display in the clinical setup. This is the first display system that co-registers a virtual image with human eyes and allows video rate image transmission. The imaging system is tested in the veterinary science operating room on canine patients with naturally occurring cancers. In addition, a time domain pulse-width-modulation address-event-representation multispectral image sensor and a handheld multispectral camera prototype are developed. Conclusion: The major problems of current state-of-the-art NIR fluorescence imaging systems are successfully solved. Due to enhanced performance and user experience, the bio-inspired sensors and augmented reality display system will give medical care providers much needed technology to enable more accurate value-based healthcare

    Liquid Crystal on Silicon Devices: Modeling and Advanced Spatial Light Modulation Applications

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    Liquid Crystal on Silicon (LCoS) has become one of the most widespread technologies for spatial light modulation in optics and photonics applications. These reflective microdisplays are composed of a high-performance silicon complementary metal oxide semiconductor (CMOS) backplane, which controls the light-modulating properties of the liquid crystal layer. State-of-the-art LCoS microdisplays may exhibit a very small pixel pitch (below 4 ?m), a very large number of pixels (resolutions larger than 4K), and high fill factors (larger than 90%). They modulate illumination sources covering the UV, visible, and far IR. LCoS are used not only as displays but also as polarization, amplitude, and phase-only spatial light modulators, where they achieve full phase modulation. Due to their excellent modulating properties and high degree of flexibility, they are found in all sorts of spatial light modulation applications, such as in LCOS-based display systems for augmented and virtual reality, true holographic displays, digital holography, diffractive optical elements, superresolution optical systems, beam-steering devices, holographic optical traps, and quantum optical computing. In order to fulfil the requirements in this extensive range of applications, specific models and characterization techniques are proposed. These devices may exhibit a number of degradation effects such as interpixel cross-talk and fringing field, and time flicker, which may also depend on the analog or digital backplane of the corresponding LCoS device. The use of appropriate characterization and compensation techniques is then necessary

    Advancements in Optical See-through Near-Eye Display

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    With the development of optical design and manufacturing, the optical see-through near-eye display becomes a promising research topic in recent decades, which can be applied in medical devices, education, aviation, entertainment etย al. Typical products include Head-mounted Displays (HMDs) and Augmented Reality (AR) glasses. The optical display system of AR devices mainly consists of a miniature projecting module and an optical imaging module. In this chapter, the display systems used by AR glasses on the market, including various mini-display screens and optical imaging elements, have been systematically summarized. Therein, the differences in optical combinators are the key part to distinguish various AR display systems. Thus, it is essential to figure out the advantages and disadvantages of each optical imaging technology applied in this area. Besides, the characteristics of the projectors are crucial to the quality of the images
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