61 research outputs found

    Metamaterial

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    In-depth analysis of the theory, properties and description of the most potential technological applications of metamaterials for the realization of novel devices such as subwavelength lenses, invisibility cloaks, dipole and reflector antennas, high frequency telecommunications, new designs of bandpass filters, absorbers and concentrators of EM waves etc. In order to create a new devices it is necessary to know the main electrodynamical characteristics of metamaterial structures on the basis of which the device is supposed to be created. The electromagnetic wave scattering surfaces built with metamaterials are primarily based on the ability of metamaterials to control the surrounded electromagnetic fields by varying their permeability and permittivity characteristics. The book covers some solutions for microwave wavelength scales as well as exploitation of nanoscale EM wavelength such as visible specter using recent advances of nanotechnology, for instance in the field of nanowires, nanopolymers, carbon nanotubes and graphene. Metamaterial is suitable for scholars from extremely large scientific domain and therefore given to engineers, scientists, graduates and other interested professionals from photonics to nanoscience and from material science to antenna engineering as a comprehensive reference on this artificial materials of tomorrow

    Tatsuo Itoh : discurs llegit a la cerimรฒnia d'investidura celebrada a la Sala d'Actes del Rectorat el dia 14 d'octubre de l'any 2015

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    Tatsuo Itoh va ser investit doctor honoris causa per la UAB per les seves rellevants contribucions a l'enginyeria de radiofreqรผรจncia/microones i de les telecomunicacions.Nomenament 19/03/2015. A proposta de l'Escola d'Enginyeria. L'acte d'investidura va tenir lloc el 14 d'octubre de 201

    Design and realization for radar cross section reduction of patch antennas using shorted stubs metamaterial absorbers

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    This thesis is devoted to analyzing of the Radar Cross Section (RCS) of rectangular patch antenna using Metamaterial Absorber (MMA) and the analysis of its reducing techniques. The addressed theme has a great complexity and it covers various areas that include designing and optimization of target geometrical model of rectangular patch antenna structures and making it compatible with respect to metamaterial geometry. Analyses have been made to optimize and validate the structure performances that include numerical methods for electromagnetic field computation, MMA behavior, characterization, extraction of parameters, antenna radiation performance analyses, simulation, fabrication, testing, and optimization with back validating the designs. The MMA structure finds its applications in antenna designing for the reduction of Monostatic and Bistatic RCS in stealth platform for lower detectable objects. However, there is still more emphasis needed to devote for in-band frequency response for low RCS of the antenna. Therefore, making these assumptions, we have been proposing novel designs of single-band, dual-band, and triple-band MMA structures. These structures provide significant scattering characteristics and offering flexibility to the designer to control and tune the resonant frequency, based on the specific applications as compared to that of the other MMAs in the microwave regime of the Electromagnetic (EM) spectrum. To explore the research scope, a three dimensional Frequency Selective Surface (FSS) structure has been analyzed and its simulation responses with respect to parametric analyses have been made. The research investigation further extended to Electronic Band Gap (EBG) Structure and Defected Ground Structure (DGS). A hybrid structure of patch antenna is proposed and designed for an inset feed rectangular microstrip patch antenna operating at 2.45 GHz in the Industrial, Scientific, and Medical (ISM) band. This hybrid structure claims the size reduction, bandwidth, and gains enhancement. The main focus of this research work is limited to determine the potential and practical feasibility of MMAโ€™s to enhance the stealth performance of rectangular patch antennas. For this purpose, Monostatic and Bistatic RCS simulation and measurements are carried out in an anechoic chamber and practical methods for Radar Cross Section reduction are discussed and analyzed

    1-D broadside-radiating leaky-wave antenna based on a numerically synthesized impedance surface

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    A newly-developed deterministic numerical technique for the automated design of metasurface antennas is applied here for the first time to the design of a 1-D printed Leaky-Wave Antenna (LWA) for broadside radiation. The surface impedance synthesis process does not require any a priori knowledge on the impedance pattern, and starts from a mask constraint on the desired far-field and practical bounds on the unit cell impedance values. The designed reactance surface for broadside radiation exhibits a non conventional patterning; this highlights the merit of using an automated design process for a design well known to be challenging for analytical methods. The antenna is physically implemented with an array of metal strips with varying gap widths and simulation results show very good agreement with the predicted performance

    Beam scanning by liquid-crystal biasing in a modified SIW structure

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    A fixed-frequency beam-scanning 1D antenna based on Liquid Crystals (LCs) is designed for application in 2D scanning with lateral alignment. The 2D array environment imposes full decoupling of adjacent 1D antennas, which often conflicts with the LC requirement of DC biasing: the proposed design accommodates both. The LC medium is placed inside a Substrate Integrated Waveguide (SIW) modified to work as a Groove Gap Waveguide, with radiating slots etched on the upper broad wall, that radiates as a Leaky-Wave Antenna (LWA). This allows effective application of the DC bias voltage needed for tuning the LCs. At the same time, the RF field remains laterally confined, enabling the possibility to lay several antennas in parallel and achieve 2D beam scanning. The design is validated by simulation employing the actual properties of a commercial LC medium

    Inverse Design of Three-Dimensional Frequency Selective Structures and Metamaterials using Multi-Objective Lazy Ant Colony Optimization

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    With the rise of big data and the โ€œinternet of things,โ€ wireless signals permeate todayโ€™s environment more than ever before. As the demand for information and security continues to expand, the need for filtering a crowded signal space will become increasingly important. Although existing devices can achieve this with additional components, such as in-line filters and low noise amplifiers, these approaches introduce additional bulk, cost and complexity. An alternative, low-cost solution to filtering these signals can be achieved through the use of Frequency Selective Surfaces (FSSs), which are commonly used in antennas, polarizers, radomes, and intelligent architecture. FSSs typically consist of a doubly-periodic array of unit cells, which acts as a spatial electromagnetic filter that selectively rejects or transmits electromagnetic waves, based on the unit cellโ€™s geometry and material properties. Unlike traditional analog filters, spatial filters must also account for the polarization and incidence angle of signals; thus, an ideal FSS maintains a given frequency response for all polarizations and incidence angles. Traditional FSS designs have ranged from planar structures with canonical shapes to miniaturized and multi-layer designs using fractals and other space-filling geometries. More recently, FSS research has expanded into three-dimensional (3D) designs, which have demonstrated enhanced fields of view over traditional planar and multi-layer designs. To date, nearly all FSSs still suffer from significant shifts in resonant frequencies or onset of grating lobes at incidence angles beyond 60 degrees in one or more polarizations. Additionally, while recent advances in additive manufacturing techniques have made fully 3D FSS designs increasingly popular, design tools to exploit these fabrication methods to develop FSSs with ultra-wide Fields of View (FOV) do not currently exist. In this dissertation, a Multi-Objective Lazy Ant Colony Optimization (MOLACO) scheme will be introduced and applied to the problem of 3D FSS design for extreme FOVs. The versatility of this algorithm will further be demonstrated through application to the design of meander line antennas, optical antennas, and phase-gradient metasurfaces

    Fiber Optic Sensors and Fiber Lasers

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    The optical fiber industry is emerging from the market for selling simple accessories using optical fiber to the new optical-IT convergence sensor market combined with high value-added smart industries such as the bio industry. Among them, fiber optic sensors and fiber lasers are growing faster and more accurately by utilizing fiber optics in various fields such as shipbuilding, construction, energy, military, railway, security, and medical.This Special Issue aims to present novel and innovative applications of sensors and devices based on fiber optic sensors and fiber lasers, and covers a wide range of applications of optical sensors. In this Special Issue, original research articles, as well as reviews, have been published

    ๋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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