216 research outputs found

    Designs of a Planar Waveguide Solar Concentrator

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    Solar energy, especially through the use of photovoltaic cells, is a promising sustainable energy source for human race. III-V multijunction photovoltaic cells with over 40% confirmed efficiency are among the best candidates for next generation solar cells. However, due to their complex fabrication process, these solar cells are currently too expensive for terrestrial 1 sun use. By using solar concentrators to replace sunlight collection area with cheap materials, total system cost is reduced and cell efficiency is increased. As a result, solar concentrators are viewed as an indispensable part in today’s multijunction photovoltaic cell systems. A novel planar waveguide solar concentrator is proposed in this work. Comparing to conventional solar concentrators, a waveguide is used to output homogenized light onto photovoltaic cells at its end surface. Such a planar structure is potentially easy to fabricate and is possible for novel sun tracking methods. It also benefits in terms of cell connections and heat management. The basic lens array-waveguide structure with the use of a tapered waveguide as a secondary concentrator shows over 90% efficiency under 800 geometric concentration under ideal cases. Optimizations are applied to the lens array, the couplers, and the secondary concentrator. The optimized structure has <1% geometry loss under 1000 geometric concentration and acceptance angles of 0.5˚~0.7˚ depending on the orientations due to structure asymmetry, which is verified by ZEMAX. As an integral part, solar tracking methods are reviewed and a two-axis tracking method realized by using a single-axis tracker and lateral translations is studied. Lateral translation is used for adjusting positions for seasonal sun movement. It has two-dimensional x-y tracking instead of horizontal movement x-only. A prototype system of 50 geometric concentration with >75% optical efficiency in simulation and >65% efficiency in experiment is presented as a practical example of the proposed tracking method

    νŽΈκ΄‘ 닀쀑화λ₯Ό μ΄μš©ν•˜μ—¬ ν–₯μƒλœ κΈ°λŠ₯을 μ œκ³΅ν•˜λŠ” λ„νŒŒκ΄€ 기반의 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄

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    ν•™μœ„λ…Όλ¬Έ (박사) -- μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› : κ³΅κ³ΌλŒ€ν•™ 전기·정보곡학뢀, 2021. 2. μ΄λ³‘ν˜Έ.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.λ³Έ λ°•μ‚¬ν•™μœ„ λ…Όλ¬Έμ—μ„œλŠ” νŽΈκ΄‘ 닀쀑화 기법을 μ΄μš©ν•˜μ—¬ λ„νŒŒκ΄€ 기반의 μ¦κ°•ν˜„μ‹€ κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄μ˜ μ„±λŠ₯을 ν–₯μƒμ‹œν‚€λŠ” κ΄‘ν•™ 섀계 및 이에 λŒ€ν•œ 뢄석에 λŒ€ν•΄ λ…Όμ˜ν•œλ‹€. λ³Έ μ—°κ΅¬λŠ” λ„νŒŒκ΄€ 기반 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄μ˜ κ°€μž₯ 큰 μž₯점인 μ†Œν˜• 폼 νŒ©ν„°λ₯Ό μœ μ§€ν•˜λ©΄μ„œ λ””μŠ€ν”Œλ ˆμ΄ μ„±λŠ₯을 κ°œμ„ ν•˜λŠ” 것에 쀑점을 λ‘”λ‹€. 이λ₯Ό μœ„ν•΄ κΈ°μ‘΄ κ΄‘ν•™ μ†Œμžμ— λΉ„ν•΄ 맀우 가볍고 얇은 νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμžκ°€ μƒˆλ‘­κ²Œ μ œμ•ˆλ˜λ©°, μ΄λŠ” μž…μ‚¬κ΄‘μ˜ νŽΈκ΄‘ μƒνƒœμ— 따라 독립적인 κ΄‘ 경둜 μ œμ–΄λ₯Ό κ°€λŠ₯μΌ€ ν•˜μ—¬ νŽΈκ΄‘ 닀쀑화λ₯Ό 톡해 ν–₯μƒλœ μ„±λŠ₯을 제곡 ν•  수 μžˆλ‹€. λ˜ν•œ μ‹€μ œ μ˜μƒμ˜ 빛은 κ·ΈλŒ€λ‘œ 투과 μ‹œν‚΄μœΌλ‘œμ¨ μ¦κ°•ν˜„μ‹€μ„ μœ„ν•œ μ†Œμžλ‘œ ν™œμš© κ°€λŠ₯ν•˜λ‹€. λ³Έ μ—°κ΅¬μ—μ„œ μ œμ•ˆν•˜λŠ” νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° κ΄‘ν•™ μ†ŒμžλŠ” κΈ°ν•˜ν•™μ  μœ„μƒ(geometric phase, GP)에 κΈ°λ°˜ν•˜μ—¬ λ™μž‘ν•œλ‹€. GP 기반의 κ΄‘ν•™μ†Œμžκ°€ μ„œλ‘œ μ§κ΅ν•˜λŠ” μ›ν˜• νŽΈκ΄‘ μž…μ‚¬κ΄‘μ— λŒ€ν•΄ 상보적인 κΈ°λŠ₯을 μˆ˜ν–‰ν•˜λŠ” 것을 μ΄μš©ν•˜μ—¬, 두 개 μ΄μƒμ˜ GP μ†Œμžμ™€ νŽΈκ΄‘ μ œμ–΄λ₯Ό μœ„ν•œ κ΄‘ν•™ 필름듀을 쀑첩 μ‹œν‚΄μœΌλ‘œμ¨ μ¦κ°•ν˜„μ‹€ κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμžλ₯Ό κ΅¬ν˜„ν•  수 μžˆλ‹€. 이듀 κ΄‘ν•™μ†ŒμžλŠ” 맀우 μ–‡κΈ° λ•Œλ¬Έμ—, λ³Έ μ—°κ΅¬μ—μ„œ μ œμž‘λœ νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμžμ˜ 총 λ‘κ»˜λŠ” 1 mm μˆ˜μ€€μœΌλ‘œ 폼 νŒ©ν„° μ œμ•½μœΌλ‘œλΆ€ν„° μžμœ λ‘­λ‹€. λ˜ν•œ ν‰ν‰ν•œ 필름 ν˜•νƒœμ΄λ―€λ‘œ, ν‰νŒν˜• λ„νŒŒκ΄€μ— λΆ€μ°©ν•˜κΈ° μ‰½λ‹€λŠ” 이점을 μ§€λ‹Œλ‹€. κ³ μ•ˆλœ νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμžλ₯Ό μ‚¬μš©ν•˜μ—¬ μ„Έ 가지 μœ ν˜•μ˜ μƒˆλ‘œμš΄ λ„νŒŒκ΄€ 기반의 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄ ꡬ쑰λ₯Ό μ œμ•ˆν•œλ‹€. 첫 λ²ˆμ§ΈλŠ” μž…μ‚¬κ΄‘μ˜ νŽΈκ΄‘ μƒνƒœμ— 따라 투λͺ… κ΄‘ν•™ μ°½ λ˜λŠ” 였λͺ© 렌즈둜 μž‘λ™ν•˜λŠ” νŽΈκ΄‘ μ˜μ‘΄ν˜• κ²°ν•©κΈ° 렌즈λ₯Ό μ μš©ν•˜μ—¬ 가상 μ˜μƒμ— λŒ€ν•΄ 이쀑 μ΄ˆμ λ©΄μ„ μ œκ³΅ν•˜λŠ” μ‹œμŠ€ν…œμ΄λ‹€. μ œμ•ˆλœ κ΅¬μ‘°λŠ” 기쑴의 λ„νŒŒκ΄€ 기반 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄κ°€ λ¬΄ν•œλŒ€ μœ„μΉ˜μ— 단일 μ΄ˆμ λ©΄μ„ μ œκ³΅ν•¨μœΌλ‘œμ¨ λ°œμƒν•˜λŠ” μ‹œκ°μ  ν”Όλ‘œ 및 νλ¦Ών•œ μ¦κ°•ν˜„μ‹€ μ˜μƒμ˜ 문제λ₯Ό μ™„ν™”ν•  수 μžˆλ‹€. 두 λ²ˆμ§Έλ‘œλŠ” μž…μ‚¬κ΄‘μ˜ νŽΈκ΄‘ μƒνƒœμ— 따라 κ΄‘ 경둜λ₯Ό 쒌츑 λ˜λŠ” 우츑으둜 μ œμ–΄ν•  수 μžˆλŠ” νŽΈκ΄‘ 격자λ₯Ό ν™œμš©ν•˜μ—¬ 가상 μ˜μƒμ˜ μ‹œμ•Όκ°μ„ 기쑴보닀 μ΅œλŒ€ 2λ°°κΉŒμ§€ ν™•μž₯ν•  수 μžˆλŠ” μ‹œμŠ€ν…œμ„ μ œμ•ˆν•œλ‹€. μ΄λŠ” 단일 λ„νŒŒκ΄€ 기반 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄μ—μ„œ μ˜μƒ κ²°ν•©κΈ° (imaging combiner)둜 ν™œμš©λ˜λŠ” 회절 μ†Œμžμ˜ 섀계 λ³€μˆ˜μ— μ˜ν•΄ μ œν•œλ˜λŠ” μ‹œμ•Όκ° ν•œκ³„μ μ„ λŒνŒŒν•  수 μžˆλŠ” ꡬ쑰둜 μ»΄νŒ©νŠΈν•œ 폼 νŒ©ν„°λ‘œ λ”μš± λͺ°μž…감 μžˆλŠ” λŒ€ν™”λ©΄ μ¦κ°•ν˜„μ‹€ μ˜μƒμ„ μ œκ³΅ν•  수 μžˆλ‹€. λ§ˆμ§€λ§‰μœΌλ‘œ μœ„μ—μ„œ μ œμ•ˆλœ 두 가지 νŽΈκ΄‘ μ˜μ‘΄ν˜• κ΄‘ν•™ μ†Œμžλ₯Ό λͺ¨λ‘ μ‚¬μš©ν•˜μ—¬ μ‹œμ  μ „ν™˜μ΄ κ°€λŠ₯ν•œ λ„νŒŒκ΄€ 기반의 망막 νˆ¬μ‚¬ν˜• λ””μŠ€ν”Œλ ˆμ΄ ꡬ쑰λ₯Ό μ œμ•ˆν•œλ‹€. νŽΈκ΄‘ 닀쀑화λ₯Ό 톡해 닀쀑 μ΄ˆμ λ“€μ„ μ„ νƒμ μœΌλ‘œ ν™œμ„±ν™”ν•¨μœΌλ‘œμ¨, ν™•μž₯된 μ‹œμ²­μ˜μ—­μ„ μ œκ³΅ν•˜λŠ” λ™μ‹œμ— 동곡 크기 λ³€ν™” λ˜λŠ” μ›€μ§μž„μ— μ˜ν•œ 이쀑 μ˜μƒ 문제λ₯Ό μ™„ν™”ν•  수 μžˆλ‹€. λ˜ν•œ 기계적 μ›€μ§μž„ 없이 μ‹œμ  κ°„μ˜ 고속 μ „ν™˜μ΄ κ°€λŠ₯ν•˜λ‹€λŠ” μž₯점을 μ§€λ‹ˆκ³  μžˆλ‹€. λ³Έ λ°•μ‚¬ν•™μœ„ λ…Όλ¬Έμ—μ„œ μ œμ‹œν•œ νŽΈκ΄‘ 닀쀑화λ₯Ό ν™œμš©ν•œ μƒˆλ‘œμš΄ κ²°ν•©κΈ° κ΄‘ν•™ μ†Œμž 및 κ΄‘ν•™ ꡬ쑰듀은 λ„νŒŒκ΄€ 기반 κ·Όμ•ˆ λ””μŠ€ν”Œλ ˆμ΄μ˜ ν–₯μƒλœ μ„±λŠ₯을 μ œκ³΅ν•˜λŠ” ν•΄κ²°μ±… 및 μƒˆλ‘œμš΄ κ°€λŠ₯μ„±μœΌλ‘œ μ œμ‹œν•  수 μžˆμ„ 것이라 κΈ°λŒ€λœλ‹€.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

    Designs of a Planar Waveguide Solar Concentrator

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    Solar energy, especially through the use of photovoltaic cells, is a promising sustainable energy source for human race. III-V multijunction photovoltaic cells with over 40% confirmed efficiency are among the best candidates for next generation solar cells. However, due to their complex fabrication process, these solar cells are currently too expensive for terrestrial 1 sun use. By using solar concentrators to replace sunlight collection area with cheap materials, total system cost is reduced and cell efficiency is increased. As a result, solar concentrators are viewed as an indispensable part in today’s multijunction photovoltaic cell systems. A novel planar waveguide solar concentrator is proposed in this work. Comparing to conventional solar concentrators, a waveguide is used to output homogenized light onto photovoltaic cells at its end surface. Such a planar structure is potentially easy to fabricate and is possible for novel sun tracking methods. It also benefits in terms of cell connections and heat management. The basic lens array-waveguide structure with the use of a tapered waveguide as a secondary concentrator shows over 90% efficiency under 800 geometric concentration under ideal cases. Optimizations are applied to the lens array, the couplers, and the secondary concentrator. The optimized structure has <1% geometry loss under 1000 geometric concentration and acceptance angles of 0.5˚~0.7˚ depending on the orientations due to structure asymmetry, which is verified by ZEMAX. As an integral part, solar tracking methods are reviewed and a two-axis tracking method realized by using a single-axis tracker and lateral translations is studied. Lateral translation is used for adjusting positions for seasonal sun movement. It has two-dimensional x-y tracking instead of horizontal movement x-only. A prototype system of 50 geometric concentration with >75% optical efficiency in simulation and >65% efficiency in experiment is presented as a practical example of the proposed tracking method

    Integrated Optical Interferometers with Micromachined Diaphragms for Pressure Sensing

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    Optical pressure sensors have been fabricated which use an integrated optical channel waveguide that is part of an interferometer to measure the pressure-induced strain in a micromachined silicon diaphragm. A silicon substrate is etched from the back of the wafer leaving a rectangular diaphragm. On the opposite side of the wafer, ring resonator and Mach-Zehnder interferometers are formed with optical channel waveguides made from a low pressure chemical vapor deposited film of silicon oxynitride. The interferometer's phase is altered by pressure-induced stress in a channel segment positioned over the long edge of the diaphragm. The phase change in the ring resonator is monitored using a link-insensitive swept frequency laser diode, while in the Mach-Zehnder it is determined using a broad band super luminescent diode with subsequent wavelength separation. The ring resonator was found to be highly temperature sensitive, while the Mach-Zehnder, which had a smaller optical path length difference, was proportionally less so. The quasi-TM mode was more sensitive to pressure, in accord with calculations. Waveguide and sensor theory, sensitivity calculations, a fabrication sequence, and experimental results are presented

    Planar waveguides obtained on commercial glass substrates by sol-gel and laser irradiation methods

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    The aim of the thesis is the fundamental study, design, fabrication and characterisation of photonic structures for spatial optic and, particulary, the interconnexion of optical devices. The research explored technologies and substrates for the fabrication of photonic structures based on the guided propogation of light and its application to research and development of integrated optical devices and improving the functionality of communication systems, which realises intelligent optical operations based on Fourier spatial transformed and image formation properties.At the same time, aims to explore new technologies for fabrication ofphotonic structures; which are repeatibility and not contaminants; and the product of well-defined charactericstics and low price

    Development of microfabricated optical chemical sensor platforms using polymer processing technology

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    This work describes the design and fabrication of enhanced polymer waveguide platforms for absorption-based optical chemical sensors and the use of soft lithographic techniques for the fabrication of optical sensor chips. The design of the enhanced polymer waveguide platforms was based on a previously reported theoretical model that was verified experimentally in this work. The platforms were fabricated by micro-injection moulding and subsequently coated with sol-gelderived sensing layers doped with a colorimetric indicator compound. The sensor response to both gaseous ammonia and solution pH was examined using a LEDbased prototype sensor head. Soft lithographic patterning techniques, based on the use of a poly(dimethylsiloxane) (PDMS) patterning element, were employed to produce a variety of sol-gel-based structures with applications in optical sensing. These included discrete sensor spots, surface corrugation grating couplers and ridge waveguides. As a proof of principle, these techniques were applied to the development of an integrated optical oxygen sensor based on the quenching of fluorescence from a sol-gel-encapsulated ruthenium complex that was deposited as a sensor spot onto a ridge waveguide. This work highlights the feasibility of using rapid prototyping technology to fabricate sensitive, mass-producible sensor platforms that employ generic configurations, thereby facilitating their use in a broad range of applications

    Bending Loss Mitigation by Surface Plasmon Resonance

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    Surface plasmon resonance can be used to confine a wave within a thin metal film. The resultant wave is very well-confined by the extreme refractive index difference between the metal and the ambient medium. Such confinement can be used to guide waves under extreme conditions such as subwavelength channels or through extremely tight bends where radiation losses would normally dissipate the wave. A nichrome thin film was deposited and etched as a shadow alongside a series of multi-mode SU-8 slab waveguides with extremely sharp angled bends. Light from a Helium-Neon laser was coupled into these waveguides and the power transmitted was measured and compared to a sample without a nichrome thin film. A total attenuation of signal was found in the non-metallic sample, while a steady signal was successfully transmitted through the sample with the thin film
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