93 research outputs found

    Doubly resonant photonic crystal cavity using merged bound states in the continuum

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    In this work, a doubly resonant photonic crystal (PhC) cavity using the merged bound states in the continuum (BICs) is proposed to obtain a higher second harmonic generation (SHG) efficiency. Firstly by scanning geometry parameters the accidental BICs and a band-edge mode outside the light cone can be obtained. Then as the lattice constant or the thickness of the slab is adjusted the accidental BICs will merge. A supercell with large and small holes is constructed and the band-edge mode outside the light cone can be mode-matched with the merged BICs mode. Finally the heterostructure PhC cavity is designed. The merged BICs show a high quality factor for the photonic crystal with finite size. Consequently, the SHG efficiency of the lattice constant near merged BICs of ~6000% W-1 is higher than the one of the isolated BIC

    Logic functions, devices, and circuits based on parametric nonlinear processes

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    Second-harmonic generation and parametric down-conversion processes have been studied as the basis of all-optical logic gates. All possibilities that are obtainable with both the low and high conversion efficiencies of such processes have been analyzed here. XOR and AND gates are also experimentally proven by using 1-ps pulses at 800 nm within a beta-BaB(2)O(4) crystal, reaching conversion efficiencies of as high as 80%. Based on these phenomena, complex algebraic operations are proposed for performing several different logic functionalities particularly concerning network switching and arithmetic calculation

    Distributed Quantum Computation Architecture Using Semiconductor Nanophotonics

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    In a large-scale quantum computer, the cost of communications will dominate the performance and resource requirements, place many severe demands on the technology, and constrain the architecture. Unfortunately, fault-tolerant computers based entirely on photons with probabilistic gates, though equipped with "built-in" communication, have very large resource overheads; likewise, computers with reliable probabilistic gates between photons or quantum memories may lack sufficient communication resources in the presence of realistic optical losses. Here, we consider a compromise architecture, in which semiconductor spin qubits are coupled by bright laser pulses through nanophotonic waveguides and cavities using a combination of frequent probabilistic and sparse determinstic entanglement mechanisms. The large photonic resource requirements incurred by the use of probabilistic gates for quantum communication are mitigated in part by the potential high-speed operation of the semiconductor nanophotonic hardware. The system employs topological cluster-state quantum error correction for achieving fault-tolerance. Our results suggest that such an architecture/technology combination has the potential to scale to a system capable of attacking classically intractable computational problems.Comment: 29 pages, 7 figures; v2: heavily revised figures improve architecture presentation, additional detail on physical parameters, a few new reference

    Photonic based Radar: Characterization of 1x4 Mach-Zehnder Demultiplexer

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    This work is based on a research activity which aims to implement an optical transceiver for a photonic-assisted fullyโ€“digital radar system based on optic miniaturized optical devices both for the optical generation of the radiofrequency (RF) signal and for the optical sampling of the received RF signal. The work is more focused on one very critical block of receiver which is used to parallelize optical samples. Parallelization will result in samples which will be lower in repetition rate so that we can use commercial available ADCs for further processing. This block needs a custom design to meet all the system specifications. In order to parallelize the samples a 1x4 switching matrix (demux) based on Mach Zehnder (MZ) interferometer has been proposed. The demux technique is Optical Time Division Demultiplexing. In order to operate this demux according to the requirements the characterization of device is needed. We need to find different stable control points (coupler bias and MZ bias) of demux to get output samples with high extinction ratio. A series of experiments have been performed to evaluate the matrix performance, issues and sensitivity. The evaluated results along with the whole scheme has been discussed in this document

    ๋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
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