299 research outputs found

    AN EXTENDED GREEN-SASAO HIERARCHY OF CANONICAL TERNARY GALOIS FORMS AND UNIVERSAL LOGIC MODULES

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    A new extended Green-Sasao hierarchyย of families and forms with a new sub-familyย for many-valued Reed-Muller logic is introduced. Recently, two familiesย of binaryย canonicalย Reed-Mullerย forms, called Inclusive Formsย (IFs) and Generalized Inclusive Formsย (GIFs) have been proposed, where the second familyย was the first to include all minimum Exclusive Sum-Of-Products (ESOPs). In this paper, we propose, analogously to the binary case, two general families of canonical ternary Reed-Muller forms, called Ternary Inclusive Forms (TIFs) and their generalizationย of Ternary Generalized Inclusive Forms (TGIFs), where the second family includes minimum Galois Field Sum-Of-Products (GFSOPs) over ternary Galois fieldย GF(3). One of the basic motivations in this work is the application of these TIFs and TGIFs to find the minimum GFSOPย for many-valuedย input-output functions within logic synthesis, where a GFSOPย minimizer based on IF polarityย can be used to minimize the many-valued GFSOP expression for any given function. The realization of the presented S/D trees using Universal Logic Modules (ULMs) is also introduced, whereULMs are complete systems that can implement all possible logic functions utilizing the corresponding S/D expansions of many-valuedShannon and Davio spectral transforms.ย  ย 

    Doctor of Philosophy

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    dissertationThe synthesis, characterization, and nonclassical optical properties of photonic crystals (PCs) created from naturally occurring biological templates was studied. Biotemplated PCs were created from several different natural structures using sol-gel chemistry methods. PCs were characterized using a combination of reflection spectroscopy, SEM image analysis, three-dimensional structure modeling, photonic band structure calculations, and density of optical states calculations. The effect our PCs had on the density of optical states (DOS) was probed using time correlated single photon counting spectroscopy. By carefully controlling the sol-gel chemistry used in the templating process, it is possible to synthesize hollow silica inverse, solid silica inverse, hollow titania inverse, solid titania inverse, and solid titania replicate structures. The inverse-type structures have the advantage of being accessible through a single templating step, while the titania replica is capable of a predicted full photonic band gap. Each structure was investigated using methods mentioned above. The reliability of reflectance spectroscopy was investigated. It was found that in certain cases, a continuum of structural parameters yield reflections that match photonic band structure calculations. Methods to improve this situation are discussed. When applied to titania inverse opals, it was found that the refractive index could be determined to ยฑ0.05 and the volume fraction to ยฑ0.5%. Accurately determining the refractive index of inverse opals is useful in estimating the refractive index of other PCs made from the same sol-gel. Calculation of the DOS using a combination of MIT's photonic bands package and house-written software was applied to biotemplated photonic crystals. It was found that even partial band gap photonic crystals can greatly modify the DOS. Finally, the rate of spontaneous emission of quantum dots embedded in photonic crystals was measured to indirectly probe the DOS. Three different models were used to extract the lifetime from radiative decay curves. It was found that a log-normal distribution of lifetimes was the most meaningful model. The radiative lifetime of quantum dots embedded in titania photonic crystals replicated from Lamprocyphus augustus was modified by up to a factor of ten, an amount unprecedented in the photonic crystal literature

    New Data Structures and Algorithms for Logic Synthesis and Verification

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    The strong interaction between Electronic Design Automation (EDA) tools and Complementary Metal-Oxide Semiconductor (CMOS) technology contributed substantially to the advancement of modern digital electronics. The continuous downscaling of CMOS Field Effect Transistor (FET) dimensions enabled the semiconductor industry to fabricate digital systems with higher circuit density at reduced costs. To keep pace with technology, EDA tools are challenged to handle both digital designs with growing functionality and device models of increasing complexity. Nevertheless, whereas the downscaling of CMOS technology is requiring more complex physical design models, the logic abstraction of a transistor as a switch has not changed even with the introduction of 3D FinFET technology. As a consequence, modern EDA tools are fine tuned for CMOS technology and the underlying design methodologies are based on CMOS logic primitives, i.e., negative unate logic functions. While it is clear that CMOS logic primitives will be the ultimate building blocks for digital systems in the next ten years, no evidence is provided that CMOS logic primitives are also the optimal basis for EDA software. In EDA, the efficiency of methods and tools is measured by different metrics such as (i) the result quality, for example the performance of a digital circuit, (ii) the runtime and (iii) the memory footprint on the host computer. With the aim to optimize these metrics, the accordance to a specific logic model is no longer important. Indeed, the key to the success of an EDA technique is the expressive power of the logic primitives handling and solving the problem, which determines the capability to reach better metrics. In this thesis, we investigate new logic primitives for electronic design automation tools. We improve the efficiency of logic representation, manipulation and optimization tasks by taking advantage of majority and biconditional logic primitives. We develop synthesis tools exploiting the majority and biconditional expressiveness. Our tools show strong results as compared to state-of-the-art academic and commercial synthesis tools. Indeed, we produce the best results for several public benchmarks. On top of the enhanced synthesis power, our methods are the natural and native logic abstraction for circuit design in emerging nanotechnologies, where majority and biconditional logic are the primitive gates for physical implementation. We accelerate formal methods by (i) studying properties of logic circuits and (ii) developing new frameworks for logic reasoning engines. We prove non-trivial dualities for the property checking problem in logic circuits. Our findings enable sensible speed-ups in solving circuit satisfiability. We develop an alternative Boolean satisfiability framework based on majority functions. We prove that the general problem is still intractable but we show practical restrictions that can be solved efficiently. Finally, we focus on reversible logic where we propose a new equivalence checking approach. We exploit the invertibility of computation and the functionality of reversible gates in the formulation of the problem. This enables one order of magnitude speed up, as compared to the state-of-the-art solution. We argue that new approaches to solve EDA problems are necessary, as we have reached a point of technology where keeping pace with design goals is tougher than ever

    Prospects for Declarative Mathematical Modeling of Complex Biological Systems

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    Declarative modeling uses symbolic expressions to represent models. With such expressions one can formalize high-level mathematical computations on models that would be difficult or impossible to perform directly on a lower-level simulation program, in a general-purpose programming language. Examples of such computations on models include model analysis, relatively general-purpose model-reduction maps, and the initial phases of model implementation, all of which should preserve or approximate the mathematical semantics of a complex biological model. The potential advantages are particularly relevant in the case of developmental modeling, wherein complex spatial structures exhibit dynamics at molecular, cellular, and organogenic levels to relate genotype to multicellular phenotype. Multiscale modeling can benefit from both the expressive power of declarative modeling languages and the application of model reduction methods to link models across scale. Based on previous work, here we define declarative modeling of complex biological systems by defining the operator algebra semantics of an increasingly powerful series of declarative modeling languages including reaction-like dynamics of parameterized and extended objects; we define semantics-preserving implementation and semantics-approximating model reduction transformations; and we outline a "meta-hierarchy" for organizing declarative models and the mathematical methods that can fruitfully manipulate them

    Cellular Automata

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    Modelling and simulation are disciplines of major importance for science and engineering. There is no science without models, and simulation has nowadays become a very useful tool, sometimes unavoidable, for development of both science and engineering. The main attractive feature of cellular automata is that, in spite of their conceptual simplicity which allows an easiness of implementation for computer simulation, as a detailed and complete mathematical analysis in principle, they are able to exhibit a wide variety of amazingly complex behaviour. This feature of cellular automata has attracted the researchers' attention from a wide variety of divergent fields of the exact disciplines of science and engineering, but also of the social sciences, and sometimes beyond. The collective complex behaviour of numerous systems, which emerge from the interaction of a multitude of simple individuals, is being conveniently modelled and simulated with cellular automata for very different purposes. In this book, a number of innovative applications of cellular automata models in the fields of Quantum Computing, Materials Science, Cryptography and Coding, and Robotics and Image Processing are presented

    Computation with spin foam models of quantum gravity

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    The focus of this thesis is the study of spin foam models of quantum gravity on a computer. These models include the standard Barrett-Crane (BC) spin foam model, as well as the new Engle-Pereira-Rovelli (EPR) and Freidel-Krasnov (FK) models. New numerical algorithms are developed and implemented, based on the existing Christensen-Egan (CE) algorithm, to allow computations with the BC model in the presence of a cosmological constant (implemented through g-deformation) and to allow computations with the recently proposed EPR and FK models. For the first time, we show that the inclusion of a positive cosmological constant, a long standing open problem for spin foams, curiously changes the behavior of the BC model, rendering the expectation values of its observables discontinuous in the limit of zero cosmological constant. Also, unlike previous work, this investigation was carried out on large triangulations, which are closer to large semiclassical space-times. Efficient numerical algorithms are described and implemented, for the first time, allowing the evaluation of the EPR and FK spin foam vertex amplitudes. An initial application of these algorithms is the study of the effective single vertex large spin asymptotics of the new models. Their asymptotic behavior is found to be qualitatively similar to that of the BC model. The leading asymptotic behavior does not exhibit the oscillatory character expected by analogy with the Ponzano-Regge model. Two important tests of the spin foam semiclassical limit are wave packet propagation and evaluation of the graviton propagator matrix elements. These tests are generalized to encompass the three major spin foam models. The wave packet propagation test is carried out in greater generality than previously. The results indicate that conjectures about good semiclassical behavior of the new spin foam models may have been premature

    Computation with spin foam models of quantum gravity

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    The focus of this thesis is the study of spin foam models of quantum gravity on a computer. These models include the standard Barrett-Crane (BC) spin foam model, as well as the new Engle-Pereira-Rovelli (EPR) and Freidel-Krasnov (FK) models. New numerical algorithms are developed and implemented, based on the existing Christensen-Egan (CE) algorithm, to allow computations with the BC model in the presence of a cosmological constant (implemented through g-deformation) and to allow computations with the recently proposed EPR and FK models. For the first time, we show that the inclusion of a positive cosmological constant, a long standing open problem for spin foams, curiously changes the behavior of the BC model, rendering the expectation values of its observables discontinuous in the limit of zero cosmological constant. Also, unlike previous work, this investigation was carried out on large triangulations, which are closer to large semiclassical space-times. Efficient numerical algorithms are described and implemented, for the first time, allowing the evaluation of the EPR and FK spin foam vertex amplitudes. An initial application of these algorithms is the study of the effective single vertex large spin asymptotics of the new models. Their asymptotic behavior is found to be qualitatively similar to that of the BC model. The leading asymptotic behavior does not exhibit the oscillatory character expected by analogy with the Ponzano-Regge model. Two important tests of the spin foam semiclassical limit are wave packet propagation and evaluation of the graviton propagator matrix elements. These tests are generalized to encompass the three major spin foam models. The wave packet propagation test is carried out in greater generality than previously. The results indicate that conjectures about good semiclassical behavior of the new spin foam models may have been premature

    Quantum formulation for nanoscale optical and material chirality: symmetry issues, space and time parity, and observables

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    To properly represent the interplay and coupling of optical and material chirality at the photon-molecule or photon-nanoparticle level invites a recognition of quantum facets in the fundamental aspects and mechanisms of light-matter interaction. It is therefore appropriate to cast theory in a general quantum form, one that is applicable to both linear and nonlinear optics as well as various forms of chiroptical interaction including chiral optomechanics. Such a framework, fully accounting for both radiation and matter in quantum terms, facilitates the scrutiny and identification of key issues concerning spatial and temporal parity, scale, dissipation and measurement. Furthermore it fully provides for describing the interactions of light beams with a vortex character, and it leads to the complete identification of symmetry conditions for materials to provide for chiral discrimination. Quantum considerations also lend a distinctive perspective to the very different senses in which other aspects of chirality are recognized in metamaterials. Duly attending to the symmetry principles governing allowed or disallowed forms of chiral discrimination supports an objective appraisal of the experimental possibilities and developing applications

    ๋น„๊ณต์œ  ํ™”ํ•™์  ๋„ํ•‘์„ ์ด์šฉํ•œ ๋‹จ์ผ์ธต ๊ทธ๋ž˜ํ•€ ์†Œ์ž์˜ ์ „์žํŠน์„ฑ ์ตœ์ ํ™”

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ์ž์—ฐ๊ณผํ•™๋Œ€ํ•™ ํ™”ํ•™๋ถ€, 2022. 8. ํ™๋ณ‘ํฌ.2004๋…„ ๊ทธ๋ž˜ํ•€์€ ํ…Œ์ดํ”„๋ฅผ ์ด์šฉํ•œ (๊ณ ๋ฐฐํ–ฅ ์—ด๋ถ„ํ•ด์„ฑ) ํ‘์—ฐ(highly oriented pyrolytic graphite; HOPG)์œผ๋กœ๋ถ€ํ„ฐ์˜ ๋ฐ•๋ฆฌ๋ฅผ ํ†ตํ•ด ์ตœ์ดˆ ๋ฐœ๊ฒฌ๋˜์—ˆ๋‹ค. ์ดํ›„ ์ˆ˜๋งŽ์€ ์—ฐ๊ตฌ๋“ค์— ์˜ํ•ด ๊ทธ๋ž˜ํ•€์ด ์šฐ์ˆ˜ํ•œ ์—ด์ , ๊ธฐ๊ณ„์ , ์ „๊ธฐ์ , ๊ด‘ํ•™์  ํŠน์„ฑ์„ ์ง€๋…”์Œ์ด ์•Œ๋ ค์กŒ๋‹ค. 2009๋…„์— ์ด๋ฅด๋Ÿฌ ํ™”ํ•™๊ธฐ์ƒ์ฆ์ฐฉ(chemical vapor deposition; CVD) ๋ฐฉ์‹์„ ์ด์šฉํ•œ ๋‹ค๊ฒฐ์ • ๊ทธ๋ž˜ํ•€์˜ ๋Œ€๋ฉด์  ํ•ฉ์„ฑ์ด ์‹คํ—˜์ ์œผ๋กœ ๊ฐ€๋Šฅํ•ด์กŒ๊ณ , ์ด๋กœ์จ ๊ทธ๋ž˜ํ•€์ด ๋‹ค์–‘ํ•œ ๋ถ„์•ผ์— ์‘์šฉ๋  ์ˆ˜ ์žˆ๋Š” ๋ฐœํŒ์ด ๋งˆ๋ จ๋˜์—ˆ๋‹ค. ํŠนํžˆ ๊ทธ๋ž˜ํ•€์˜ ์‘์šฉ๋ถ„์•ผ ์ค‘ ์ „๊ธฐ์ „์žํŠน์„ฑ์„ ์ด์šฉํ•œ ๋ถ„์•ผ๊ฐ€ ๊ฐ๊ด‘์„ ๋ฐ›๊ณ  ์žˆ๋‹ค. ๊ทธ๋ž˜ํ•€์€ ๋†’์€ ์ „์ž์ด๋™๋„, ์ „๊ธฐ์ „๋„๋„ ๋ฐ ์—ด์ „๋„๋„๋ฅผ ์ง€๋‹Œ ์žฌ๋ฃŒ์ด๋ฉฐ, ๋ฐ€์ ‘๊ฒฐํ•ฉ(tight-binding; TB) ๊ทผ์‚ฌ ๋ชจํ˜•์„ ์ด์šฉํ•˜์—ฌ ๊ณ„์‚ฐํ•œ, ๊ฒฐํ•จ์ด ์—†๋Š” ๋‹จ๊ฒฐ์ • ๋‹จ์ธต ๊ทธ๋ž˜ํ•€์˜ ๋ฐด๋“œ๊ฐญ(band gap)์€ 0์ž„์ด ๋ฐํ˜€์กŒ๋‹ค. ์žฌ๋ฃŒ์˜ ์ „์žํŠน์„ฑ ์กฐ์ ˆ์€ ์ „์ž์†Œ์ž๋กœ์˜ ์‘์šฉ์— ํ•„์ˆ˜์  ๊ณต์ •์ด๊ณ , ๋„ํ•‘์€ ์ „์žํŠน์„ฑ ์กฐ์ ˆ์— ์ฃผ๋กœ ์“ฐ์ด๋Š” ๋ฐฉ๋ฒ• ์ค‘ ํ•˜๋‚˜์ด๋‹ค. ๊ทธ๋ž˜ํ•€์— ๋„ํ•‘ ์ฒ˜๋ฆฌ๋ฅผ ํ•จ์œผ๋กœ์จ ๋ฐด๋“œ๊ฐญ, ์ „๊ธฐ์ „๋„๋„ ๋ฐ ์ผํ•จ์ˆ˜์™€ ๊ฐ™์€ ์ „๊ธฐ์ „์žํŠน์„ฑ์„ ์กฐ์ ˆํ•  ์ˆ˜ ์žˆ๋‹ค. ๊ทธ๋ž˜ํ•€์— ๋Œ€ํ•œ ๋„ํ•‘ ๋ฐฉ๋ฒ•์œผ๋กœ๋Š” ์›์ž ์น˜ํ™˜, ์ „๊ณ„ ์ธ๊ฐ€, ๋ถ„์ž๋‚˜ ๊ธˆ์† ๋‚˜๋…ธ์ž…์ž ๋“ฑ์˜ ๋ฌผ๋ฆฌ์  ํก์ฐฉ ๋“ฑ์ด ์žˆ๋‹ค. ์ด ์ค‘ ๋ฌผ๋ฆฌ์  ํก์ฐฉ ๋ฐฉ์‹์€ ๊ฒฐํ•จ ์—†์ด ๊ฐ„๋‹จํ•˜๊ณ  ์šฐ์ˆ˜ํ•œ ๋„ํ•‘ ํšจ๊ณผ๋ฅผ ์–ป์„ ์ˆ˜ ์žˆ์–ด ๊ทธ๋ž˜ํ•€ ๋„ํ•‘ ๋ฐฉ๋ฒ•์œผ๋กœ ๋„๋ฆฌ ์‚ฌ์šฉ๋˜๊ณ  ์žˆ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ํ™”ํ•™๊ธฐ์ƒ์ฆ์ฐฉ ๋ฐฉ์‹์œผ๋กœ ํ•ฉ์„ฑํ•œ ๊ทธ๋ž˜ํ•€์˜ ์ „์žํŠน์„ฑ ์ตœ์ ํ™” ๋ฐฉ๋ฒ• ๋ฐ ์ „์ž์†Œ์ž๋กœ์˜ ์‘์šฉ์— ๊ด€ํ•œ ์—ฐ๊ตฌ๋ฅผ ๋‹ค๋ฃจ์—ˆ๋‹ค. ๊ทธ๋ž˜ํ•€์˜ ์ „์žํŠน์„ฑ ์ตœ์ ํ™” ๋ฐฉ์‹์œผ๋กœ ๋ฌผ๋ฆฌ์  ํก์ฐฉ์„ ํ†ตํ•œ ๋น„๊ณต์œ  ํ™”ํ•™์  ๋„ํ•‘์„ ํƒํ•˜์˜€์œผ๋ฉฐ, ๋„ํ•‘๋œ ๊ทธ๋ž˜ํ•€์˜ ์ „์ž์†Œ์ž๋กœ์˜ ์‘์šฉ ๊ฐ€๋Šฅ์„ฑ์— ๋Œ€ํ•˜์—ฌ ํ™•์ธํ•˜์˜€๋‹ค. ์ œ1์žฅ์—์„œ๋Š” ๊ทธ๋ž˜ํ•€์˜ ๋ฌผ๋ฆฌ์  ํŠน์„ฑ ์ค‘ ์ „๊ธฐ์ „์žํŠน์„ฑ์— ์ดˆ์ ์„ ๋งž์ถฐ ์„ค๋ช…ํ•˜์˜€๋‹ค. ๋˜ํ•œ, ์—ฐ๊ตฌ์— ์‚ฌ์šฉํ•œ ๋„ํ•‘ ๋ฐฉ๋ฒ•๊ณผ ๋„ํ•‘๋œ ๊ทธ๋ž˜ํ•€์˜ ์ „ํ•˜ ์ด๋™ํ˜„์ƒ์— ๊ด€ํ•˜์—ฌ ์†Œ๊ฐœํ•˜์˜€๋‹ค. ์ œ2์žฅ์—์„œ๋Š” ๊ทธ๋ž˜ํ•€์˜ ํ•ฉ์„ฑ, ์ „์‚ฌ ๋ฐ ๋„ํ•‘ ๋ฐฉ๋ฒ•์— ๊ด€ํ•˜์—ฌ ์„œ์ˆ ํ•˜์˜€๋‹ค. ์—ฐ๊ตฌ์— ์‚ฌ์šฉ๋œ ๊ทธ๋ž˜ํ•€์€ ํ™”ํ•™๊ธฐ์ƒ์ฆ์ฐฉ ๋ฐฉ์‹์œผ๋กœ ํ•ฉ์„ฑ๋˜์—ˆ์œผ๋ฉฐ, ํ•ฉ์„ฑ๋œ ๊ทธ๋ž˜ํ•€์€ ๊ตฌ๋ฆฌ ์‹๊ฐ ๋ฐ ์ „์‚ฌ ๊ณต์ •์„ ํ†ตํ•ด ์†Œ์ž ์—ฐ๊ตฌ๋ฅผ ์œ„ํ•œ ์‹œํŽธ์œผ๋กœ ์ œ์ž‘๋˜์—ˆ๋‹ค. ๊ทธ๋ž˜ํ•€์€ ์ž๊ธฐ์กฐ๋ฆฝ๋‹จ์ธต(self-assembled monolayer; SAM)์„ ํ˜•์„ฑํ•˜๋Š” ๋ถ„์ž ์™ธ ๋‹ค์–‘ํ•œ ๋‚˜๋…ธ๋ฌผ์งˆ์„ ์ด์šฉํ•œ ๋ฌผ๋ฆฌ์  ํก์ฐฉ ๋ฐฉ์‹์— ์˜ํ•ด ํ™”ํ•™์  ๋„ํ•‘๋œ๋‹ค. ๋ผ๋งŒ ๋ถ„๊ด‘๋ถ„์„์„ ํ†ตํ•ด ํ•ฉ์„ฑ ๋ฐ ๋„ํ•‘ ์งํ›„์˜ ๊ทธ๋ž˜ํ•€ ์‹œํŽธ์˜ ํ’ˆ์งˆ์„ ํ‰๊ฐ€ํ•˜์˜€๊ณ , 3 ์ „๊ทน ์‹œ์Šคํ…œ์„ ์ด์šฉํ•œ ์ „๊ณ„ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ๋ฅผ ์ œ์ž‘ํ•˜์—ฌ ๊ทธ๋ž˜ํ•€์˜ ์ „์žํŠน์„ฑ์„ ๋ถ„์„ํ•˜์˜€๋‹ค. ์ œ3์žฅ์—์„œ๋Š” ํ™”ํ•™๊ธฐ์ƒ์ฆ์ฐฉ ๋ฐฉ์‹์œผ๋กœ ํ•ฉ์„ฑํ•œ ๊ทธ๋ž˜ํ•€์— ๋‹ค์–‘ํ•œ ๋‚˜๋…ธ๋ฌผ์งˆ์„ ์ฐจ๋ก€๋กœ ์ œ๊ณตํ•จ์œผ๋กœ์จ ํ™”ํ•™์  ๋„ํ•‘ ํšจ๊ณผ์˜ ๋ณ€ํ™”๋ฅผ ๋‚˜ํƒ€๋‚ธ ์ „์ž์†Œ์ž ์—ฐ๊ตฌ๋ฅผ ๊ธฐ์ˆ ํ•˜์˜€๋‹ค. ๊ทธ๋ž˜ํ•€ ํ‘œ๋ฉด์— ๊ธˆ ๋‚˜๋…ธ์ž…์ž๋ฅผ ๋ฌผ๋ฆฌ์  ํก์ฐฉ ๋ฐฉ์‹์œผ๋กœ ๋„ํ•‘ํ•˜์—ฌ ๋น„๊ณต์œ  ๊ธฐ๋Šฅํ™”ํ•˜๊ณ , ์ด๋ฅผ ์ด์šฉํ•œ ๊ทธ๋ž˜ํ•€์„ ์ „๊ณ„ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ ์†Œ์ž๋กœ ์ œ์ž‘ํ•˜์˜€๋‹ค. ์ œ์ž‘๋œ ์†Œ์ž์— ์กด์žฌํ•˜๋Š” ๊ธˆ ๋‚˜๋…ธ์ž…์ž์— 4-๋จธ์บ…ํ† ๋ฒค์กฐ์‚ฐ(4-mercaptobenzoic acid; 4-MBA) ๋ถ„์ž๋ฅผ ํก์ฐฉ์‹œํ‚ด์œผ๋กœ์จ ์ž๊ธฐ์กฐ๋ฆฝ๋‹จ์ธต์„ ํ˜•์„ฑ์ผ€ ํ•œ๋‹ค. ์ด๋•Œ ์ˆ˜์€ ์ด์˜จ์„ ์ฃผ์ž…ํ•˜๋ฉด ์ž๊ธฐ์กฐ๋ฆฝ๋‹จ์ธต์„ ํ˜•์„ฑํ•œ 4-MBA ๋ถ„์ž์˜ ์นด๋ณต์‹œ๊ธฐ(carboxyl group)๊ฐ€ ๋ฆฌ๊ฐ„๋“œ๋กœ ์ž‘์šฉํ•˜์—ฌ ์ˆ˜์€ ์ด์˜จ์„ ํฌํšํ•˜๋ฉด์„œ ํ‚ฌ๋ ˆ์ดํŠธ(chelate) ๋ณตํ•ฉ์ฒด๋ฅผ ๊ตฌ์„ฑํ•œ๋‹ค. ๊ฐ ๋‹จ๊ณ„์˜ ๊ทธ๋ž˜ํ•€ ์ „๊ณ„ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ ์†Œ์ž์˜ ์ „์žํŠน์„ฑ ๋ถ„์„์„ ํ†ตํ•ด, ๊ฐ ๋‚˜๋…ธ๋ฌผ์งˆ ์š”์†Œ์— ์˜ํ•ด ๊ทธ๋ž˜ํ•€ ํ‘œ๋ฉด์˜ ๋„ํ•‘ ํšจ๊ณผ๊ฐ€ ๋ฏธ์„ธ ์กฐ์ •๋จ์„ ์•Œ ์ˆ˜ ์žˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ๋ฅผ ํ†ตํ•ด ๊ทธ๋ž˜ํ•€ ์ „๊ณ„ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ์˜ ํ™”ํ•™์  ๊ธฐ๋Šฅํ™”์— ๋Œ€ํ•œ ๊ฐ€๋Šฅ์„ฑ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ œ4์žฅ์—์„œ๋Š” ํ™”ํ•™๊ธฐ์ƒ์ฆ์ฐฉ ๋ฐฉ์‹์œผ๋กœ ํ•ฉ์„ฑํ•œ ๊ทธ๋ž˜ํ•€์— n-์•Œํ‚ฌ์•„๋ฏผ(n-alkylamine; H2NCn) ๋ถ„์ž๋ฅผ ๋„์ž…ํ•จ์œผ๋กœ์จ, nํ˜• ๋„ํ•‘๋œ ๊ทธ๋ž˜ํ•€์„ ์ด์šฉํ•œ ์—ด์ „์†Œ์ž ์„ฑ๋Šฅ์˜ ํ–ฅ์ƒ์— ๊ด€ํ•˜์—ฌ ๊ธฐ์ˆ ํ•˜์˜€๋‹ค. n-์•Œํ‚ฌ์•„๋ฏผ ๋ถ„์ž๋Š” ๊ทธ๋ž˜ํ•€ ํ‘œ๋ฉด์—์„œ ์ž๊ธฐ์กฐ๋ฆฝ๋‹จ์ธต์„ ํ˜•์„ฑํ•˜๊ณ  ๋น„๊ณต์œ  ๊ธฐ๋Šฅํ™”๋ฅผ ํ†ตํ•ด ์ „์ž๋ฅผ ๊ทธ๋ž˜ํ•€์— ์ œ๊ณตํ•œ๋‹ค. ํƒ„์†Œ์‚ฌ์Šฌ ๊ธธ์ด๊ฐ€ ๊ฐ๊ธฐ ๋‹ค๋ฅธ n-์•Œํ‚ฌ์•„๋ฏผ ๋ถ„์ž๋ฅผ ์ด์šฉํ•˜์—ฌ ๋„ํ•‘ํ•œ ๊ทธ๋ž˜ํ•€์„ 3 ์ „๊ทน ์‹œ์Šคํ…œ์„ ํ†ตํ•ด ๋ถ„์„ํ•จ์œผ๋กœ์จ, ์„œ๋กœ ๋‹ค๋ฅธ ๊ธธ์ด์˜ ๋ถ„์ž๋ฅผ ํ†ตํ•ด ๊ทธ๋ž˜ํ•€ ์‹œํŽธ์˜ ์ „ํ•˜์šด๋ฐ˜์ž ๋†๋„์˜ ์กฐ์ ˆ์ด ๊ฐ€๋Šฅํ•จ์„ ํ™•์ธํ•˜์˜€๋‹ค. n-์•Œํ‚ฌ์•„๋ฏผ ๋ถ„์ž์˜ ์ž๊ธฐ์กฐ๋ฆฝ๋‹จ์ธต์ด ํ˜•์„ฑ๋œ ๊ฐ ๊ทธ๋ž˜ํ•€ ์‹œํŽธ ์œ„๋กœ ์‚ฐํ™”๊ฐˆ๋ฅจ(Ga2O3) ๋ฐ•๋ง‰์ธต ๋ฐ ๊ฐˆ๋ฅจ-์ธ๋“ ๊ณต์œตํ•ฉ๊ธˆ(eutectic Ga-In alloy; EGaIn) ๋ฒŒํฌ์ธต์„ ์ฐจ๋ก€๋กœ ์ ์ธตํ•˜์—ฌ ์—ด์ „์†Œ์ž๋ฅผ ์ œ์ž‘ํ•˜์˜€๋‹ค. n-์•Œํ‚ฌ์•„๋ฏผ ๋ถ„์ž์˜ ๋น„๊ณต์œ  ์ ‘ํ•ฉ์— ์˜ํ•ด ์œ ๋„ ๊ฐญ ์ƒํƒœ(induced-gap state)๊ฐ€ ๊ทธ๋ž˜ํ•€ ์—ด์ „์†Œ์ž(SLG//H2NCn//Ga2O3/EGaIn)์— ๋„์ž…๋˜์—ˆ๋‹ค. ๊ธˆ ๋ฐ•๋ง‰์ธต๊ณผ n-์•Œ์ผ€์ธ์‹ธ์ด์˜ฌ๋ ˆ์ดํŠธ(n-alkanethiolates; SCn) ๋ถ„์ž์˜ ์ ‘ํ•ฉ์œผ๋กœ ๊ตฌ์„ฑ๋œ ์ข…๋ž˜์˜ ์—ด์ „์†Œ์ž(Au/SCn//Ga2O3/EGaIn)์™€์˜ ๋น„๊ต๋ฅผ ํ†ตํ•ด, ์ƒ๊ธฐํ•œ ๋ฐฉ์‹์œผ๋กœ ์ œ์ž‘๋œ ๊ทธ๋ž˜ํ•€ ์—ด์ „์†Œ์ž๊ฐ€ ์šฐ์ˆ˜ํ•œ ์—ด์ „ํŠน์„ฑ์„ ์ง€๋‹ˆ๊ณ  ์žˆ์Œ์„ ์ฆ๋ช…ํ•˜์˜€๋‹ค.Since its first discovery as a flake-form from mechanical exfoliation of highly-oriented pyrolytic graphite (HOPG) using tape in 2004, numerous studies have shown that graphene has outstanding and extraordinary thermal, mechanical, electrical, electronic and optical properties. In 2009, large-area synthesis of polycrystalline graphene using a chemical vapor deposition (CVD) method became experimentally possible, thereby establishing a foothold for the graphene to be applied to various fields. In particular, the field of application using electrical and electronic characteristics of graphene is in the spotlight. Graphene is a remarkable material with high electron mobility, electrical conductivity and thermal conductivity. Furthermore, the pristine single-layer graphene (SLG) has zero gap, a theoretical value calculated by a tight-binding (TB) approximation model. Engineering the electronic properties of materials is an essential process for application to electronic devices, and doping is one of the methods mainly used to control electronic properties. By doping graphene, electrical and electronic characteristics such as band gap, electrical conductivity, and work function (WF) can be modified and controlled. Doping methods for graphene include atomic substitution, applying electric field, physisorption (physical adsorption) of molecules and metal nanoparticles, etc. Among those methods, the physisorption is widely used as a graphene doping method because it can obtain a simple and superior doping effect without crystallographic defects. This paper describes researches on optimization methods of the electronic properties of graphene synthesized by CVD method and its applications of electronic devices. Noncovalent chemical doping by the physisorption was selected as the optimization method of the electronic properties of graphene, and the possibility of application of the doped graphene to an electronic device was verified. Chapter 1 delineates the physical properties of graphene, focusing on the electrical and electronic properties. In addition, the doping method used in the study and the charge transfer phenomenon of doped graphene were introduced. Chapter 2 gives a detailed description of the procedure such as the synthesis, transfer, and doping methods of graphene. Graphene used in these researches was synthesized by CVD method, and the synthesized graphene was manufactured as electronic device specimens through copper etching and transfer processes. Graphene is chemically doped by the physisorption method using various nanomaterials such as molecules forming self-assembled monolayers (SAM). Through Raman spectroscopy, the quality of graphene specimens immediately after synthesis and doping process was evaluated. Moreover, the electronic properties of graphene were analyzed by a 3-electrode system using field-effect transistor (FET) devices Chapter 3 depicts a study on electronic devices showing changes in chemical doping effects by sequentially providing various nanomaterials to graphene synthesized by CVD method. Gold nanoparticles were used as dopants on the surface of graphene by physisorption for a noncovalent functionalization, and the doped graphene was manufactured as FET devices. SAM is formed by adsorbing 4-mercaptobenzoic acid (4-MBA) molecules onto gold nanoparticles on the manufactured graphene device. And then, if mercury ions are injected, a carboxyl group of 4-MBA molecules constructing SAM acts as a ligand to capture mercury ions, thereby assembling a chelate complex. Through the analyses of the electronic properties of the graphene FET devices in each step, it can be seen that the doping effect of the graphene surface is finely adjusted by each nanomaterial element. Through this study, the possibility of chemical functionalization of graphene FET devices was exactly clarified. Chapter 4 describes the improvement in the performance of graphene thermoelectric devices using n-type doping by introducing n-alkylamine (H2NCn) molecules onto SLG film synthesized by CVD method. The n-alkylamine molecules form SAM on the surface of graphene and provide electrons to graphene through noncovalent functionalization. Graphene doped by n-alkylamine molecules with different lengths of carbon chain was manufactured as FET devices and analyzed by a 3-electrode system. Graphene FET devices were proved clearly that the concentration of charge carriers of graphene specimens could be regulated by chemical doping method using each molecule. Graphene thermoelectric devices was manufactured by sequentially stacking a gallium oxide (Ga2O3) thin film layer and a eutectic gallium-indium alloy (EGaIn) bulk layer onto the n-alkylamine SAM formed on each graphene specimen. An induced-gap state was introduced into the graphene layer in graphene thermoelectric devices (SLG//H2NCn//Ga2O3/EGaIn) by noncovalent junctions of n-alkylamine molecules. Through comparison with thermoelectric devices with a conventional structure (Au/SCn/Ga2O3/EGaIn) composed of the junction of gold thin film layer and n-alkanethiolates (SCn) molecules, it was shown that the graphene thermoelectric devices produced by the above method have improved and outstanding thermoelectric properties.Cover 1 Abstract 3 Table of Contents 6 List of Tables 8 List of Figures 9 Chapter 1. Introduction to Graphene 12 1. 1. Discovery and Advancement of Graphene 12 1. 2. Crystal Structure of Graphene 16 1. 3. Band Structure of Graphene 25 1. 4. Group Theory to Analyze Graphene 40 1. 5. Chemical Doping of Graphene 47 1. 6. Properties of Doped Graphene 50 Chapter 2. Experimental 54 2. 1. Graphene Synthesis by Chemical Vapor Deposition 54 2. 2. Pre-treatment Process for Graphene Transfer 65 2. 3. Graphene Transfer Process 66 2. 4. Graphene Doping by Physisorption 69 2. 5. Raman Spectroscopic Analyses for Graphene 70 2. 6. Electronic Analyses for Graphene Field-effect Transistor 80 Chapter 3. Gold Nanoparticle-Mediated Noncovalent Functionalization of Graphene for Field-Effect Transistors 94 3. 1. Abstract 94 3. 2. Introduction 95 3. 3. Experimental 96 3. 4. Results and Discussion 101 3. 5. Conclusion 123 Chapter 4. Enhanced Thermopower of Saturated Molecules by Noncovalent Anchor-Induced Electron Doping of Single-Layer Graphene 124 4. 1. Abstract 124 4. 2. Introduction 125 4. 3. Experimental 128 4. 4. Results and Discussion 138 4. 5. Conclusion 157 Bibliography 158 Abstract in Korean 178๋ฐ•
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