21 research outputs found

    Eight-input optical programmable logic array enabled by parallel spectrum modulation

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    Despite over 40 years' development of optical logic computing, the studies have been still struggling to support more than four operands, since the high parallelism of light has not been fully leveraged blocked by the optical nonlinearity and redundant input modulation in existing methods. Here, we propose a scalable multi-input optical programmable logic array (PLA) with minimal logical input, enabled by parallel spectrum modulation. By making full use of the wavelength resource, an eight-input PLA is experimentally demonstrated, and there are 2^256 possible combinations of generated logic gates. Various complex logic fuctions, such as 8-256 decoder, 4-bit comparator, adder and multiplier are experimentally demonstrated via leveraging the PLA. The scale of PLA can be further extended by fully using the dimensions of wavelength and space. As an example, a nine-input PLA is implemented to realize the two-dimensional optical cellular automaton for the first time and perform Conway's Game of Life to simulate the evolutionary process of cells. Our work significantly alleviates the challenge of extensibility of optical logic devices, opening up new avenues for future large-scale, high-speed and energy-efficient optical digital computing

    Design of Ultrafast All-Optical Pseudo Binary Random Sequence Generator, 4-bit Multiplier and Divider using 2 x 2 Silicon Micro-ring Resonators

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    All-optical devices are essential for next generation ultrafast, ultralow-power and ultrahigh bandwidth information processing systems. Silicon microring resonators (SiMRR) provide a versatile platform for all-optical switching and CMOS-compatible computing, with added advantages of high Q-factor, tunability, compactness, cascadability and scalability. A detailed theoretical analysis of ultrafast all-optical switching 2 x 2 SiMRRs has been carried out incorporating the effects of two photon absorption induced free-carrier injection and thermo optic effect. The results have been used to design simple and compact all-optical 3-bit and 4-bit pseudo-random binary sequence generators and the first reported designs of all-optical 4 x 4-bit multiplier and divider. The designs have been optimized for low-power, ultrafast operation with high modulation depth, enabling logic operations at 45 Gbps.Comment: 13 pages, 4 figures. Submitted at Journal (Optik) for publicatio

    Adiabatic technique based low power synchronous counter design

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    The performance of integrated circuits is evaluated by their design architecture, which ensures high reliability and optimizes energy. The majority of the system-level architectures consist of sequential circuits. Counters are fundamental blocks in numerous very large-scale integration (VLSI) applications. The T-flip-flop is an important block in synchronous counters, and its high-power consumption impacts the overall effectiveness of the system. This paper calculates the power dissipation (PD), power delay product (PDP), and latency of the presented T flip-flop. To create a 2-bit synchronous counter based on the novel T flip-flops, a performance matrix such as PD, latency, and PDP is analyzed. The analysis is carried out atย 100 and 10 MHz frequencies with varying temperatures and operating voltages. It is observed that the presented counter design has a lesser power requirement and PDP compared to the existing counter architectures. The proposed T-flip-flop design at the 45 nm technology node shows an improvement of 30%, 76%, and 85% in latency, PD, and PDP respectively to the 180 nm node at 10 MHz frequency. Similarly, the proposed counter at the 45 nm technology node shows 96% and 97% improvement in power dissipation, delay, and PDP respectively compared to the 180 nm at 10 MHz frequency

    Doctor of Philosophy

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    dissertationRecent breakthroughs in silicon photonics technology are enabling the integration of optical devices into silicon-based semiconductor processes. Photonics technology enables high-speed, high-bandwidth, and high-fidelity communications on the chip-scale-an important development in an increasingly communications-oriented semiconductor world. Significant developments in silicon photonic manufacturing and integration are also enabling investigations into applications beyond that of traditional telecom: sensing, filtering, signal processing, quantum technology-and even optical computing. In effect, we are now seeing a convergence of communications and computation, where the traditional roles of optics and microelectronics are becoming blurred. As the applications for opto-electronic integrated circuits (OEICs) are developed, and manufacturing capabilities expand, design support is necessary to fully exploit the potential of this optics technology. Such design support for moving beyond custom-design to automated synthesis and optimization is not well developed. Scalability requires abstractions, which in turn enables and requires the use of optimization algorithms and design methodology flows. Design automation represents an opportunity to take OEIC design to a larger scale, facilitating design-space exploration, and laying the foundation for current and future optical applications-thus fully realizing the potential of this technology. This dissertation proposes design automation for integrated optic system design. Using a buildingblock model for optical devices, we provide an EDA-inspired design flow and methodologies for optical design automation. Underlying these flows and methodologies are new supporting techniques in behavioral and physical synthesis, as well as device-resynthesis techniques for thermal-aware system integration. We also provide modeling for optical devices and determine optimization and constraint parameters that guide the automation techniques. Our techniques and methodologies are then applied to the design and optimization of optical circuits and devices. Experimental results are analyzed to evaluate their efficacy. We conclude with discussions on the contributions and limitations of the approaches in the context of optical design automation, and describe the tremendous opportunities for future research in design automation for integrated optics

    Optical Communication

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    Optical communication is very much useful in telecommunication systems, data processing and networking. It consists of a transmitter that encodes a message into an optical signal, a channel that carries the signal to its desired destination, and a receiver that reproduces the message from the received optical signal. It presents up to date results on communication systems, along with the explanations of their relevance, from leading researchers in this field. The chapters cover general concepts of optical communication, components, systems, networks, signal processing and MIMO systems. In recent years, optical components and other enhanced signal processing functions are also considered in depth for optical communications systems. The researcher has also concentrated on optical devices, networking, signal processing, and MIMO systems and other enhanced functions for optical communication. This book is targeted at research, development and design engineers from the teams in manufacturing industry, academia and telecommunication industries

    ๋ณต์†Œ, ๋ฌด์งˆ์„œ ๋ฐ ๊ด‘ํ•™์  ๋น„์„ ํ˜• ํผํ…์…œ์—์„œ์˜ ๋Œ€์นญ์„ฑ ๋ถ•๊ดด๋ฅผ ํ†ตํ•œ ๋น›์˜ ํ๋ฆ„ ์ œ์–ด

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์ „๊ธฐยท์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2015. 8. ๋ฐ•๋‚จ๊ทœ.๋งค์งˆ ๋‚ด ๋น›์˜ ํ๋ฆ„์€ ํ†ต์ƒ์ ์œผ๋กœ ๊ฑฐ์‹œ์  ๋งฅ์Šค์›ฐ ๋ฐฉ์ •์‹์— ์˜ํ•ด ์ •์˜๋œ๋‹ค. ๋™์งˆ์„ฑ ๋ฐ ๋“ฑ๋ฐฉ์„ฑ์„ ๊ฐ€์ง€๊ณ , ์„ ํ˜•์ ์ด๋ฉฐ, ์‹œ๊ฐ„์— ๋Œ€ํ•ด ์ผ์ •ํ•œ ๊ด‘ํ•™ ๋งค์งˆ ๋ณ€์ˆ˜๋ฅผ ๊ฐ–๋Š” ์ด์ƒ์ ์ธ ๋งค์งˆ์—์„œ๋Š” ๊ด‘ํŒŒ์˜ ์–‘์ƒ์ด ํŽ˜๋ฅด๋งˆ์˜ ์›๋ฆฌ์˜ ์ง์ ‘์ ์ธ ์˜ˆ์ธ ์ง„๋™ํ•˜๋Š” ์ „์ž๊ธฐ์žฅ์˜ ์ง์ง„ ํ˜•ํƒœ๋กœ, ๊ฐ„๋‹จํ•˜๋ฉฐ ์ง๊ด€์ ์ด๋‹ค. ์ด๋Ÿฌํ•œ ํ‰๋ฉดํŒŒ์  ํŠน์„ฑ์€ ๊ธฐํ•˜ ๊ด‘ํ•™์˜ ๋ฐ”ํƒ•์ด๋ฉฐ, ์Šˆ๋ขฐ๋”ฉ๊ฑฐ ๋ฐฉ์ •์‹ ํ˜•ํƒœ์˜ ํŒŒ๋™ ๋ฐฉ์ •์‹์ด ๊ฐ–๋Š” ๋‹ค์–‘ํ•œ ๋Œ€์นญ์„ฑ (๋ณ‘์ง„ ๋Œ€์นญ, ํ‚ค๋ž„ ๋Œ€์นญ, ์—๋ฅด๋ฏธํŠธ ๋Œ€์นญ, ๋กœ๋ Œ์ธ  ๋Œ€์นญ ๋ฐ ์‹œ๊ฐ„ ๋ฐ˜์ „ ๋Œ€์นญ)์˜ ๋ณด์กด์—์„œ ๊ทธ ์›๋ฆฌ์„ ์ฐพ์„ ์ˆ˜ ์žˆ๋‹ค. ๋ Œ์ฆˆ, ๊ฑฐ์šธ ๋ฐ ํ”„๋ฆฌ์ฆ˜๊ณผ ๊ฐ™์€ ๊ณ ์ „์ ์ธ ๋ฐฉ์‹์—์„œ์กฐ์ฐจ, ๋น›์˜ ํ๋ฆ„์„ ์กฐ์ ˆํ‚ค ์œ„ํ•ด์„œ๋Š” ์ผ๋ถ€ ๊ด‘ํ•™์  ๋Œ€์นญ์„ฑ์˜ ๋ถ•๊ดด๋ฅผ ํ•„์š”๋กœ ํ•œ๋‹ค. ๋น„๊ท ์งˆ ๋งค์งˆ์—์„œ์˜ ๋ณ‘์ง„ ๋Œ€์นญ์˜ ๋ถ•๊ดด๋Š” ๊ตด์ ˆ, ๋ฐ˜์‚ฌ, ํšŒ์ ˆ๊ณผ ๊ฐ™์€ ์‚ฐ๋ž€ ๊ธฐ๋ฐ˜ ๋น› ์ œ์–ด๋ฅผ ์œ„ํ•œ ๊ณ ์ „์ ์ธ ๋ฐฉ๋ฒ•์ด๋‹ค. ์ „ํŒŒ ์‹œ์˜ ๋น› ์—๋„ˆ์ง€์˜ ์†Œ๋ชจ ๋˜๋Š” ์ฆํญ์€ ํŒŒ๋™ ๋ฐฉ์ •์‹์˜ ๋น„์—๋ฅด๋ฏธํŠธ ํ—ค๋ฐ€ํ† ๋‹ˆ์•ˆ์— ์˜ํ•ด ์ •๋Ÿ‰ํ™”๋œ๋‹ค. ํ‚ค๋ž„ ๋ถ„์ž๋กœ ์ด๋ฃจ์–ด์ง„ ๋งค์งˆ์€ ๊ด‘ํ•™ ํ™œ์„ฑ, ์ฆ‰ ๋น›์˜ ํŽธ๊ด‘์„ ๋Œ๋ฆด ์ˆ˜ ์žˆ๋„๋ก ํ•œ๋‹ค. ์ฒœ๋ฌธํ•™์—์„œ ๋ณ„ ๋ฐ ์€ํ•˜ ์›€์ง์ž„์˜ ๊ด€์ฐฐ์— ์ด์šฉ๋˜๋Š” ๊ด‘ํ•™์  ๋„ํ”Œ๋Ÿฌ ํšจ๊ณผ๋Š” ๋กœ๋ Œ์ธ  ๋Œ€์นญ์„ฑ์„ ๋ถ•๊ดด์‹œํ‚ค๋Š” ๊ด‘์›์˜ ์‹œ๊ฐ„์— ๋”ฐ๋ฅธ ๋ณ€ํ™”์— ๊ธฐ๋ฐ˜ํ•œ๋‹ค. ๋น„์ง๊ด€์ ์ธ ์ด๋ก ์  ๊ฒฐ๊ณผ๋ฌผ ๋ฐ ํ–ฅ์ƒ๋œ ๊ณต์ • ๊ธฐ์ˆ ์„ ํฌํ•จํ•˜๋Š” ๊ด‘ํ•™ ๋ถ„์•ผ์˜ ์ตœ๊ทผ ์„ฑ๊ณผ๋“ค์€ ์ด์ œ ๋น„๊ณ ์ „์ ์ธ ๋น›์˜ ํ๋ฆ„์„ ์ด๋Œ์–ด๋‚ด๊ธฐ ์œ„ํ•œ ๊ด‘ํ•™์  ํผํ…์…œ ์ œ์–ด์˜ ์ƒˆ๋กœ์šด ์˜์—ญ์„ ๊ฐœ์ฒ™ํ•˜๊ณ  ์žˆ๋‹ค. ๋ฉ”ํƒ€ ๋ฌผ์งˆ ๊ฐœ๋…๊ณผ ์—ฐ๊ณ„๋œ ๋‚˜๋…ธ ์Šค์ผ€์ผ ๊ธฐ์ˆ ์€ ๋‹จ๋ฐฉํ–ฅ ๋น› ์ „ํŒŒ, ๋ณ€ํ˜•๋œ ์Šค๋„ฌ์˜ ๋ฒ•์น™, ์Œ๊ตด์ ˆ์œจ, ํˆฌ๋ช… ๋งํ† , ์™„์ „ ํก์ˆ˜์ฒด์™€ ๊ฐ™์€ ํŠน์ดํ•œ ๋น›์˜ ํ๋ฆ„์„ ์ง€์›ํ•˜๋Š”, ์ด๋ก ์ ์œผ๋กœ ์ฆ๋ช…๋œ ์ธ์กฐ ๋งค์งˆ์˜ ์„ค๊ณ„๋ฅผ ๊ฐ€๋Šฅ์ผ€ ํ•œ๋‹ค. ๊ด‘ ์ฆํญ ๊ธฐ์ˆ ์˜ ๋ฐœ์ „์€ ์–‘์ž์—ญํ•™์  ๊ฐœ๋…์ธ ํŒจ๋ฆฌํ‹ฐ-์‹œ๊ฐ„ ๋Œ€์นญ์„ฑ์˜ ๊ตฌํ˜„์— ์ ์šฉ๋˜์–ด, ๋ณต์†Œ ํผํ…์…œ์—์„œ์˜ ์ƒˆ๋กœ์šด ์ข…๋ฅ˜์˜ ๊ด‘ํ•™์„ ํƒ„์ƒ์‹œ์ผฐ๋‹ค. ์ด๋Ÿฌํ•œ ์„ฑ์ทจ๋ฌผ๋“ค์€ ๋งฅ์Šค์›ฐ ๋ฐฉ์ •์‹์—์„œ์˜ ๋” ๋„“๊ณ  ๊ธ‰๊ฒฉํ•œ ํ˜•ํƒœ์˜ ๋Œ€์นญ์„ฑ ๋ถ•๊ดด์— ๊ธฐ๋ฐ˜ํ•˜๊ธฐ ๋•Œ๋ฌธ์—, ์˜๋„๋œ ๋น›์˜ ํ๋ฆ„ ์กฐ์ ˆ์„ ์œ„ํ•ด์„œ๋Š” ๋‹ค์–‘ํ•œ ๋Œ€์นญ์„ฑ ๋ถ•๊ดด์— ๊ด€ํ•œ ์‹ฌ๋„์žˆ๋Š” ์—ฐ๊ตฌ๊ฐ€ ํ•„์š”ํ•˜๋‹ค. ๋ณธ ํ•™์œ„ ๋…ผ๋ฌธ์—์„œ๋Š” ๋ณต์†Œ, ๋ถˆ๊ทœ์น™, ๋น„์„ ํ˜• ๊ด‘ํ•™ ํผํ…์…œ๊ณผ ๊ฐ™์€ ๋‹ค์–‘ํ•œ ํ”Œ๋žซํผ์—์„œ์˜ ๋Œ€์นญ์„ฑ ๋ถ•๊ดด์— ๋Œ€ํ•˜์—ฌ ์‚ดํŽด๋ณด๊ณ ์ž ํ•œ๋‹ค. ๋ณธ ์—ฐ๊ตฌ๋Š” ํŒจ๋ฆฌํ‹ฐ-์‹œ๊ฐ„ ๋Œ€์นญ์„ฑ, ํ‚ค๋ž„ ํŠน์„ฑ, ์ธ๊ณผ์œจ, ์ดˆ๋Œ€์นญ, ์ƒ๋ฌผ ๋ชจ๋ฐฉ ๊ธฐ์ˆ , ๋ชจ๋“œ ๊ฒฝ๊ณ„ ๊ด‘ํ•™ ๋ฐ ๋Š๋ฆฐ ๋น› ์›๋ฆฌ์™€ ์—ฐ๊ณ„๋œ ๋น›์˜ ํŠน์ดํ•œ ํ๋ฆ„์— ์ง‘์ค‘ํ•œ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์ง„์ด ์ด๋Œ์–ด๋‚ธ ๋น„์ง๊ด€์ ์ธ ๊ฐœ๋… ๋ฐ ๊ด‘์†Œ์ž์˜ ์ƒˆ๋กœ์šด ์„ค๊ณ„ ๊ธฐ๋ฒ• ๊ด€๋ จ ๊ฒฐ๊ณผ๋“ค์€ ๋น„๊ณ ์ „์ ์ธ ๋น›์˜ ํ๋ฆ„์— ๊ธฐ๋ฐ˜ํ•œ ๋ฏธ๋ž˜ ๊ด‘ํ•™ ๋ฐœ์ „์— ๋„์›€์ด ๋  ๊ฒƒ์ด๋‹ค.The flow of light in matters is usually defined by macroscopic Maxwells equations. In ideal media with homogeneous, isotropic, linear, and time-invariant optical material parameters, the aspect of light wave dynamics is simple and intuitive: propagating straight with oscillated electromagnetic fields, as the direct example of Fermats principle. This planewave dynamics, the basis of geometric optics, originates from the conservation of various symmetries of the Schrodinger-like wave equation, including translational and chiral symmetry, Hermitian symmetry, Lorentz reciprocity, and time-reversal symmetry. To control the flow of light even in a classical manner such as lens, mirror, and prism, some parts of the symmetries in optics should be broken. Breaking the translational symmetry with inhomogeneous materials is the traditional method of controlling light by scattering such as refraction, reflection, and diffraction. The dissipation or amplification of optical energy during the propagation is quantified by the non-Hermitian Hamiltonian of the wave equation. The materials composed of chiral molecules allow the rotation of the polarization of light, i.e. optical activity. The optical Doppler effect, which has been employed in astronomy for the observation of the motion of stars and galaxies, is based on the time-varying position of light sources, breaking Lorentz reciprocity. Recent achievements in optics, including counterintuitive theoretical results and improved fabrication technologies, have now been pioneering unprecedented regimes of controlling optical potentials which derive non-classical flow of light. Nano-scale technologies linked with the concept of metamaterials have opened a path to the design of theoretically-demonstrated artificial media supporting extraordinary light flows: such as unidirectional light flow, modified Snells law, negative index, cloaking, and perfect absorption. The development of optical amplification techniques has been applied to the realization of the quantum-mechanical notion of parity-time symmetry: stimulating a new class of optics in complex potentials. Because these achievements have been based on broader and drastic forms of symmetry breaking in Maxwells equations, in-depth investigation of various symmetry breakings is now imperative to realize designer manipulation of light flow. In this dissertation, we explore symmetry breakings in various platforms: complex, disordered, and nonlinear optical potentials. The investigation is focused on unconventional flows of light linked with the notions of parity-time symmetry, chirality, causality, supersymmetry, biomimetics, mode junction photonics, and slow-light. We believe that our results including counterintuitive concepts and novel design methods for optical devices will be the foundation of future development in optics based on non-classical flow of light.Table of Contents Abstract i Table of Contents iv List of Figures viii Chapter 1 Introduction ๏ผ‘ 1.1 Why should we break the symmetry of light? ๏ผ‘ 1.2 Outline of the dissertation ๏ผ’ Chapter 2 Parity-Time Symmetric Optics ๏ผ” 2.1 Introduction to PT-symmetric optics ๏ผ• 2.2 PT-symmetric waves in the spatial domain ๏ผ‘๏ผ‘ 2.2.1 2-level chirped system ๏ผ‘๏ผ‘ 2.2.2 N-level photonic molecule ๏ผ’๏ผ” 2.3 PT-symmetric waves in momentum domains ๏ผ”๏ผ“ 2.3.1 Optical chirality in low-dimensional eigensystems ๏ผ”๏ผ” 2.3.2 Interpretation of PT-symmetry in k-space ๏ผ–๏ผ“ 2.4 Conclusion ๏ผ—๏ผ• Chapter 3 Disordered Optics ๏ผ—๏ผ– 3.1 Introduction to disordered optics ๏ผ—๏ผ— 3.2 Supersymmetric bandgap in disorder ๏ผ—๏ผ˜ 3.2.1 Wave dynamics in random-walk potentials ๏ผ—๏ผ™ 3.2.2 Supersymmetric transformation for isospectrality ๏ผ˜๏ผ“ 3.2.3 Bloch-wave family with tunable disorder ๏ผ˜๏ผ– 3.3 Biomimetic disordered surface ๏ผ™๏ผ‘ 3.4 Conclusion ๏ผ™๏ผ˜ Chapter 4 All-Optical Devices with Nonlinearity ๏ผ™๏ผ™ 4.1 Introduction to all-optical devices ๏ผ‘๏ผ๏ผ 4.2 Mode junction photonics ๏ผ‘๏ผ๏ผ‘ 4.2.1 Photonic Junction Diode ๏ผ‘๏ผ๏ผ• 4.2.2 Multi-Junction Half Adder ๏ผ‘๏ผ‘๏ผ“ 4.3 Slow-light enhanced optical functionalities ๏ผ‘๏ผ‘๏ผ• 4.3.1 Multiband slow light ๏ผ‘๏ผ‘๏ผ– 4.3.2 Optical A/D converter ๏ผ‘๏ผ’๏ผ– 4.3.3 All-optical A/D converter ๏ผ‘๏ผ“๏ผ— 4.3.4 Travelling-wave all-optical isolator ๏ผ‘๏ผ”๏ผ“ 4.4 Conclusion ๏ผ‘๏ผ”๏ผ™ Chapter 5 Conclusion ๏ผ‘๏ผ•๏ผ Appendix A Eigenvalues in PT-Meta-molecules ๏ผ‘๏ผ•๏ผ’ Appendix B Supplements for Section 2.3.1 ๏ผ‘๏ผ•๏ผ— B.1 Planewave solution of a PT-symmetric optical material ๏ผ‘๏ผ•๏ผ— B.2 Density of optical chirality for complex eigenmodes ๏ผ‘๏ผ•๏ผ˜ B.3 Effect of imperfect PT symmetry on the modal chirality ๏ผ‘๏ผ•๏ผ™ B.3.1 Broken symmetry in the real part of permittivity ๏ผ‘๏ผ•๏ผ™ B.3.2 Broken anti-symmetry in the imaginary part of the permittivity ๏ผ‘๏ผ–๏ผ‘ B.4 Transfer between RCP and LCP modes in the PT-symmetric chiral material ๏ผ‘๏ผ–๏ผ’ B.4.1 Propagation of complex eigenmodes ๏ผ‘๏ผ–๏ผ’ B.4.2 Strength of chiral conversion CCS before the EP ๏ผ‘๏ผ–๏ผ“ B.5 The state of polarization (SOP) at the EP: Optical spin black hole ๏ผ‘๏ผ–๏ผ” B.6 Giant chiral conversion in the resonant structure ๏ผ‘๏ผ–๏ผ• B.7 Detailed information of fabrication and experiment in THz chiral polar metamaterials ๏ผ‘๏ผ–๏ผ– B.7.1 Fabrication process of THz chiral polar metamaterials ๏ผ‘๏ผ–๏ผ– B.7.2 THz-TDS system for the measurement of intermodal chirality ๏ผ‘๏ผ–๏ผ— B.8 Realization of PT-symmetric permittivity in metamaterial platforms ๏ผ‘๏ผ–๏ผ— B.9 Design parameters of chiral waveguides ๏ผ‘๏ผ—๏ผ‘ B.10 Low-dimensional linear polarization ๏ผ‘๏ผ—๏ผ‘ Appendix C Detailed Derivation for Section 2.3.2 ๏ผ‘๏ผ—๏ผ“ C.1 Detailed derivation of Eq. (2.20) ๏ผ‘๏ผ—๏ผ“ C.2 Serial calculation of discretized coupled mode equations ๏ผ‘๏ผ—๏ผ• Appendix D Analytical Methods for Section 3.2 ๏ผ‘๏ผ—๏ผ— D.1 Details of the FDM and FGH method ๏ผ‘๏ผ—๏ผ— D.2 Calculation of the Hurst exponent ๏ผ‘๏ผ—๏ผ— Appendix E Supplements for Section 4.2 ๏ผ‘๏ผ—๏ผ™ E.1 Details of the device structures and numerical method used in the study ๏ผ‘๏ผ—๏ผ™ E.2 Coupled mode theory for the di-atomic photonic junction diode ๏ผ‘๏ผ˜๏ผ‘ E.2.1 Analytical model and coupled mode equations ๏ผ‘๏ผ˜๏ผ‘ E.2.2. Solution of resonator field (a1, a2, a3) ๏ผ‘๏ผ˜๏ผ“ E.2.3 Implementation of Kerr nonlinearity and calculation of diode throughput ๏ผ‘๏ผ˜๏ผ• Bibliography ๏ผ‘๏ผ˜๏ผ— Abstract in Korean ๏ผ’๏ผ๏ผ“Docto

    Towards Brillouin Enabled Photonic Switching and Quantum Memories

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    Cumulative index to NASA Tech Briefs, 1970-1975

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    Tech briefs of technology derived from the research and development activities of the National Aeronautics and Space Administration are presented. Abstracts and indexes of subject, personal author, originating center, and tech brief number for the 1970-1975 tech briefs are presented
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