644 research outputs found

    Photo-effects on Current Transport in Back-gate Graphene Field-effect Transistor

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    Graphene, which has attracted wide attention because of its two-dimensional structure and high carrier mobility, is a promising candidate for potential application in optics and electronics. In this dissertation, the photonic effects on current transport in back-gate graphene field-effect transistor is investigated. Chemical vapor deposition (CVD) on metal provides a promising way for large area, controllability and high quality graphene film. The transfer and back-gate transistor fabrication processes are proposed in this dissertation. The theoretical analysis of photodetector based on back-gate graphene field-effect transistor has been done. It is shown that the photo-electronic current consists of current contributions from photovoltaic, photo-thermoelectric and photo-bolometric effects. A maximum external responsivity close to 0.0009A/W is achieved at 30ΞΌW laser power source and 633nm wavelength. The photodiode based on graphene/silicon Schottky barrier is also. A computed 238.8 W-1 photocurrent to dark current ratio normalized by the power source (633nm wavelength and 10mW laser) is obtained. An equivalent circuit model of the graphene/silicon Schottky barrier diode compatible with SPICE simulation is developed and simulated photo-response characteristics are presented using analog behavior modeling which are in close agreement with the theoretical analysis. Besides the optical applications, graphene based-transistors can also be used in applications related to space electronics. The irradiation effects including oxide trap charge and graphene layer traps charges are investigated. A semi-empirical model of graphene back-gate transistors before and after irradiation is predicted

    Electronic, optical, mechanical and thermoelectric properties of graphene

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    Graphene, a two-dimensional allotrope of graphite with sp2 bonded carbon atoms, is arranged in honeycomb structure. Its quasi one-dimensional form is graphene nanoribbon (GNR). Graphene related materials have been found to display excellent electronic, chemical, mechanical properties along with uniquely high thermal conductivity, electrical conductivity and high optical transparency. With excellent electrical characteristics such as high carrier transport properties, quantum Hall effect at room temperature and unusual magnetic properties, graphene has applications in optoelectronic devices. Electronically, graphene is a zero bandgap semiconductor making it essential to tailor its structure for obtaining specific band structure. Narrow GNRs are known to open up bandgap and found to exhibit variations for different chiralities i.e., armchair and zigzag. Doping graphene, with p- or n- type elements, is shown to exhibit bandgap in contrast to pristine graphene. In this study, optical properties including dielectric functions, absorption coefficient, transmittance, and reflectance, as a function of wavelength and incident energy, are studied. Refractive index and extinction coefficient of pristine graphene are presented. A key optical property in the infrared region, emissivity, is studied as a function of wavelength for various multilayered configurations having graphene as one of the constituent layers. Application of such a structure is in the fabrication of a Hot Electron Bolometer (a sensor that operates on the basis of temperature-dependent electrical resistance). Graphene is found to have very high elastic modulus and intrinsic strength. Nanoindentation of graphene sheet is simulated to study the force versus displacement curves. Effects of variation of diameter of indenter, speed of indentation and number of layers of graphene on the mechanical properties are presented. Shrinking size of electronic devices has led to an acute need for thermal management. This prompted the study of thermoelectric (TE) effects in graphene based systems. TE devices are finding applications in power generation and solid state refrigeration. This study involves analyzing the electronic, thermal and electrical transport properties of these systems. Electronic thermal conductivity, of graphene based systems (ΞΊe), is found to be negligible as compared to its phonon-induced lattice thermal conduction (ΞΊp). Variations in ΞΊp of graphene and GN Rs are evaluated as a function of their width and length of their edges, chiralities, temperature, and number of layers. The interdependence of transport parameters, i.e., electrical conductivity (Οƒ), thermoelectric power (TEP) or Seebeck coefficient (S), and ΞΊ of graphene are discussed. The thermoelectric performance of these materials is determined mainly by a parameter called Figure-of-Merit. Effective methods to optimize the value of Figure-of-Merit are explored. Reducing the thermal conductivity and increasing the power factor of these systems are found to improve the Figure-of-Merit significantly. This involves correlation of structure and transport properties. Effects of doping on Οƒ, ΞΊ and Hall coefficient are discussed

    Solid State Circuits Technologies

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    The evolution of solid-state circuit technology has a long history within a relatively short period of time. This technology has lead to the modern information society that connects us and tools, a large market, and many types of products and applications. The solid-state circuit technology continuously evolves via breakthroughs and improvements every year. This book is devoted to review and present novel approaches for some of the main issues involved in this exciting and vigorous technology. The book is composed of 22 chapters, written by authors coming from 30 different institutions located in 12 different countries throughout the Americas, Asia and Europe. Thus, reflecting the wide international contribution to the book. The broad range of subjects presented in the book offers a general overview of the main issues in modern solid-state circuit technology. Furthermore, the book offers an in depth analysis on specific subjects for specialists. We believe the book is of great scientific and educational value for many readers. I am profoundly indebted to the support provided by all of those involved in the work. First and foremost I would like to acknowledge and thank the authors who worked hard and generously agreed to share their results and knowledge. Second I would like to express my gratitude to the Intech team that invited me to edit the book and give me their full support and a fruitful experience while working together to combine this book

    Hybrid Nanomaterials

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    Two of the hottest research topics today are hybrid nanomaterials and flexible electronics. As such, this book covers both topics with chapters written by experts from across the globe. Chapters address hybrid nanomaterials, electronic transport in black phosphorus, three-dimensional nanocarbon hybrids, hybrid ion exchangers, pressure-sensitive adhesives for flexible electronics, simulation and modeling of transistors, smart manufacturing technologies, and inorganic semiconductors

    A Double-Voltage-Controlled Effective Thermal Conductivity Model of Graphene for Thermoelectric Cooling

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    Β© 1963-2012 IEEE. Graphene provides a new opportunity for thermoelectric study based on its unique heat transfer behavior controllable by a gate voltage. In this paper, an effective thermal conductivity model of graphene for thermoelectric cooling is proposed. The model is based on a double-voltage-control mechanism. According to the law of Fourier heat conduction, an effective thermal conductivity model of the proposed thermoelectric cooling device is derived taking a tunable external voltage into account. Then, a gate voltage is used which can change graphene's thermoelectric characteristics. To verify the correctness and effectiveness of the proposed model, a circuit simulation model using HSPICE is built based on the thermoelectric duality. The simulation results from HSPICE and the calculated results from the mathematic model show good agreements with each other. This paper provides a novel precisely controlling method for thermoelectric cooling

    Thermoelectric Power in Graphene

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    λΉ„κ³΅μœ  화학적 도핑을 μ΄μš©ν•œ 단일측 κ·Έλž˜ν•€ μ†Œμžμ˜ μ „μžνŠΉμ„± μ΅œμ ν™”

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    ν•™μœ„λ…Όλ¬Έ(박사) -- μ„œμšΈλŒ€ν•™κ΅λŒ€ν•™μ› : μžμ—°κ³Όν•™λŒ€ν•™ ν™”ν•™λΆ€, 2022. 8. 홍병희.2004λ…„ κ·Έλž˜ν•€μ€ ν…Œμ΄ν”„λ₯Ό μ΄μš©ν•œ (κ³ λ°°ν–₯ μ—΄λΆ„ν•΄μ„±) 흑연(highly oriented pyrolytic graphite; HOPG)μœΌλ‘œλΆ€ν„°μ˜ 박리λ₯Ό 톡해 졜초 λ°œκ²¬λ˜μ—ˆλ‹€. 이후 μˆ˜λ§Žμ€ 연ꡬ듀에 μ˜ν•΄ κ·Έλž˜ν•€μ΄ μš°μˆ˜ν•œ 열적, 기계적, 전기적, 광학적 νŠΉμ„±μ„ μ§€λ…”μŒμ΄ μ•Œλ €μ‘Œλ‹€. 2009년에 이λ₯΄λŸ¬ 화학기상증착(chemical vapor deposition; CVD) 방식을 μ΄μš©ν•œ λ‹€κ²°μ • κ·Έλž˜ν•€μ˜ λŒ€λ©΄μ  합성이 μ‹€ν—˜μ μœΌλ‘œ κ°€λŠ₯ν•΄μ‘Œκ³ , 이둜써 κ·Έλž˜ν•€μ΄ λ‹€μ–‘ν•œ 뢄야에 μ‘μš©λ  수 μžˆλŠ” 발판이 λ§ˆλ ¨λ˜μ—ˆλ‹€. 특히 κ·Έλž˜ν•€μ˜ μ‘μš©λΆ„μ•Ό 쀑 μ „κΈ°μ „μžνŠΉμ„±μ„ μ΄μš©ν•œ λΆ„μ•Όκ°€ 각광을 λ°›κ³  μžˆλ‹€. κ·Έλž˜ν•€μ€ 높은 μ „μžμ΄λ™λ„, 전기전도도 및 열전도도λ₯Ό μ§€λ‹Œ 재료이며, λ°€μ ‘κ²°ν•©(tight-binding; TB) 근사 λͺ¨ν˜•μ„ μ΄μš©ν•˜μ—¬ κ³„μ‚°ν•œ, 결함이 μ—†λŠ” 단결정 단측 κ·Έλž˜ν•€μ˜ λ°΄λ“œκ°­(band gap)은 0μž„μ΄ λ°ν˜€μ‘Œλ‹€. 재료의 μ „μžνŠΉμ„± μ‘°μ ˆμ€ μ „μžμ†Œμžλ‘œμ˜ μ‘μš©μ— ν•„μˆ˜μ  곡정이고, 도핑은 μ „μžνŠΉμ„± μ‘°μ ˆμ— 주둜 μ“°μ΄λŠ” 방법 쀑 ν•˜λ‚˜μ΄λ‹€. κ·Έλž˜ν•€μ— 도핑 처리λ₯Ό ν•¨μœΌλ‘œμ¨ λ°΄λ“œκ°­, 전기전도도 및 μΌν•¨μˆ˜μ™€ 같은 μ „κΈ°μ „μžνŠΉμ„±μ„ μ‘°μ ˆν•  수 μžˆλ‹€. κ·Έλž˜ν•€μ— λŒ€ν•œ 도핑 λ°©λ²•μœΌλ‘œλŠ” μ›μž μΉ˜ν™˜, 전계 인가, λΆ„μžλ‚˜ κΈˆμ† λ‚˜λ…Έμž…μž λ“±μ˜ 물리적 흑착 등이 μžˆλ‹€. 이 쀑 물리적 흑착 방식은 결함 없이 κ°„λ‹¨ν•˜κ³  μš°μˆ˜ν•œ 도핑 효과λ₯Ό 얻을 수 μžˆμ–΄ κ·Έλž˜ν•€ 도핑 λ°©λ²•μœΌλ‘œ 널리 μ‚¬μš©λ˜κ³  μžˆλ‹€. λ³Έ λ…Όλ¬Έμ—μ„œλŠ” 화학기상증착 λ°©μ‹μœΌλ‘œ ν•©μ„±ν•œ κ·Έλž˜ν•€μ˜ μ „μžνŠΉμ„± μ΅œμ ν™” 방법 및 μ „μžμ†Œμžλ‘œμ˜ μ‘μš©μ— κ΄€ν•œ 연ꡬλ₯Ό λ‹€λ£¨μ—ˆλ‹€. κ·Έλž˜ν•€μ˜ μ „μžνŠΉμ„± μ΅œμ ν™” λ°©μ‹μœΌλ‘œ 물리적 흑착을 ν†΅ν•œ λΉ„κ³΅μœ  화학적 도핑을 νƒν•˜μ˜€μœΌλ©°, λ„ν•‘λœ κ·Έλž˜ν•€μ˜ μ „μžμ†Œμžλ‘œμ˜ μ‘μš© κ°€λŠ₯성에 λŒ€ν•˜μ—¬ ν™•μΈν•˜μ˜€λ‹€. 제1μž₯μ—μ„œλŠ” κ·Έλž˜ν•€μ˜ 물리적 νŠΉμ„± 쀑 μ „κΈ°μ „μžνŠΉμ„±μ— μ΄ˆμ μ„ 맞좰 μ„€λͺ…ν•˜μ˜€λ‹€. λ˜ν•œ, 연ꡬ에 μ‚¬μš©ν•œ 도핑 방법과 λ„ν•‘λœ κ·Έλž˜ν•€μ˜ μ „ν•˜ μ΄λ™ν˜„μƒμ— κ΄€ν•˜μ—¬ μ†Œκ°œν•˜μ˜€λ‹€. 제2μž₯μ—μ„œλŠ” κ·Έλž˜ν•€μ˜ ν•©μ„±, 전사 및 도핑 방법에 κ΄€ν•˜μ—¬ μ„œμˆ ν•˜μ˜€λ‹€. 연ꡬ에 μ‚¬μš©λœ κ·Έλž˜ν•€μ€ 화학기상증착 λ°©μ‹μœΌλ‘œ ν•©μ„±λ˜μ—ˆμœΌλ©°, ν•©μ„±λœ κ·Έλž˜ν•€μ€ ꡬ리 식각 및 전사 곡정을 톡해 μ†Œμž 연ꡬλ₯Ό μœ„ν•œ μ‹œνŽΈμœΌλ‘œ μ œμž‘λ˜μ—ˆλ‹€. κ·Έλž˜ν•€μ€ μžκΈ°μ‘°λ¦½λ‹¨μΈ΅(self-assembled monolayer; SAM)을 ν˜•μ„±ν•˜λŠ” λΆ„μž μ™Έ λ‹€μ–‘ν•œ λ‚˜λ…Έλ¬Όμ§ˆμ„ μ΄μš©ν•œ 물리적 흑착 방식에 μ˜ν•΄ 화학적 λ„ν•‘λœλ‹€. 라만 뢄광뢄석을 톡해 ν•©μ„± 및 도핑 μ§ν›„μ˜ κ·Έλž˜ν•€ μ‹œνŽΈμ˜ ν’ˆμ§ˆμ„ ν‰κ°€ν•˜μ˜€κ³ , 3 μ „κ·Ή μ‹œμŠ€ν…œμ„ μ΄μš©ν•œ μ „κ³„νš¨κ³Ό νŠΈλžœμ§€μŠ€ν„°λ₯Ό μ œμž‘ν•˜μ—¬ κ·Έλž˜ν•€μ˜ μ „μžνŠΉμ„±μ„ λΆ„μ„ν•˜μ˜€λ‹€. 제3μž₯μ—μ„œλŠ” 화학기상증착 λ°©μ‹μœΌλ‘œ ν•©μ„±ν•œ κ·Έλž˜ν•€μ— λ‹€μ–‘ν•œ λ‚˜λ…Έλ¬Όμ§ˆμ„ μ°¨λ‘€λ‘œ μ œκ³΅ν•¨μœΌλ‘œμ¨ 화학적 도핑 효과의 λ³€ν™”λ₯Ό λ‚˜νƒ€λ‚Έ μ „μžμ†Œμž 연ꡬλ₯Ό κΈ°μˆ ν•˜μ˜€λ‹€. κ·Έλž˜ν•€ ν‘œλ©΄μ— 금 λ‚˜λ…Έμž…μžλ₯Ό 물리적 흑착 λ°©μ‹μœΌλ‘œ λ„ν•‘ν•˜μ—¬ λΉ„κ³΅μœ  κΈ°λŠ₯ν™”ν•˜κ³ , 이λ₯Ό μ΄μš©ν•œ κ·Έλž˜ν•€μ„ μ „κ³„νš¨κ³Ό νŠΈλžœμ§€μŠ€ν„° μ†Œμžλ‘œ μ œμž‘ν•˜μ˜€λ‹€. μ œμž‘λœ μ†Œμžμ— μ‘΄μž¬ν•˜λŠ” 금 λ‚˜λ…Έμž…μžμ— 4-λ¨ΈμΊ…ν† λ²€μ‘°μ‚°(4-mercaptobenzoic acid; 4-MBA) λΆ„μžλ₯Ό ν‘μ°©μ‹œν‚΄μœΌλ‘œμ¨ μžκΈ°μ‘°λ¦½λ‹¨μΈ΅μ„ ν˜•μ„±μΌ€ ν•œλ‹€. μ΄λ•Œ μˆ˜μ€ μ΄μ˜¨μ„ μ£Όμž…ν•˜λ©΄ μžκΈ°μ‘°λ¦½λ‹¨μΈ΅μ„ ν˜•μ„±ν•œ 4-MBA λΆ„μžμ˜ μΉ΄λ³΅μ‹œκΈ°(carboxyl group)κ°€ λ¦¬κ°„λ“œλ‘œ μž‘μš©ν•˜μ—¬ μˆ˜μ€ μ΄μ˜¨μ„ ν¬νšν•˜λ©΄μ„œ ν‚¬λ ˆμ΄νŠΈ(chelate) 볡합체λ₯Ό κ΅¬μ„±ν•œλ‹€. 각 λ‹¨κ³„μ˜ κ·Έλž˜ν•€ μ „κ³„νš¨κ³Ό νŠΈλžœμ§€μŠ€ν„° μ†Œμžμ˜ μ „μžνŠΉμ„± 뢄석을 톡해, 각 λ‚˜λ…Έλ¬Όμ§ˆ μš”μ†Œμ— μ˜ν•΄ κ·Έλž˜ν•€ ν‘œλ©΄μ˜ 도핑 νš¨κ³Όκ°€ λ―Έμ„Έ 쑰정됨을 μ•Œ 수 μžˆλ‹€. λ³Έ 연ꡬλ₯Ό 톡해 κ·Έλž˜ν•€ μ „κ³„νš¨κ³Ό νŠΈλžœμ§€μŠ€ν„°μ˜ 화학적 κΈ°λŠ₯화에 λŒ€ν•œ κ°€λŠ₯성을 ν™•μΈν•˜μ˜€λ‹€. 제4μž₯μ—μ„œλŠ” 화학기상증착 λ°©μ‹μœΌλ‘œ ν•©μ„±ν•œ κ·Έλž˜ν•€μ— n-μ•Œν‚¬μ•„λ―Ό(n-alkylamine; H2NCn) λΆ„μžλ₯Ό λ„μž…ν•¨μœΌλ‘œμ¨, nν˜• λ„ν•‘λœ κ·Έλž˜ν•€μ„ μ΄μš©ν•œ μ—΄μ „μ†Œμž μ„±λŠ₯의 ν–₯상에 κ΄€ν•˜μ—¬ κΈ°μˆ ν•˜μ˜€λ‹€. n-μ•Œν‚¬μ•„λ―Ό λΆ„μžλŠ” κ·Έλž˜ν•€ ν‘œλ©΄μ—μ„œ μžκΈ°μ‘°λ¦½λ‹¨μΈ΅μ„ ν˜•μ„±ν•˜κ³  λΉ„κ³΅μœ  κΈ°λŠ₯ν™”λ₯Ό 톡해 μ „μžλ₯Ό κ·Έλž˜ν•€μ— μ œκ³΅ν•œλ‹€. νƒ„μ†Œμ‚¬μŠ¬ 길이가 각기 λ‹€λ₯Έ n-μ•Œν‚¬μ•„λ―Ό λΆ„μžλ₯Ό μ΄μš©ν•˜μ—¬ λ„ν•‘ν•œ κ·Έλž˜ν•€μ„ 3 μ „κ·Ή μ‹œμŠ€ν…œμ„ 톡해 λΆ„μ„ν•¨μœΌλ‘œμ¨, μ„œλ‘œ λ‹€λ₯Έ 길이의 λΆ„μžλ₯Ό 톡해 κ·Έλž˜ν•€ μ‹œνŽΈμ˜ μ „ν•˜μš΄λ°˜μž λ†λ„μ˜ 쑰절이 κ°€λŠ₯함을 ν™•μΈν•˜μ˜€λ‹€. n-μ•Œν‚¬μ•„λ―Ό λΆ„μžμ˜ μžκΈ°μ‘°λ¦½λ‹¨μΈ΅μ΄ ν˜•μ„±λœ 각 κ·Έλž˜ν•€ μ‹œνŽΈ μœ„λ‘œ μ‚°ν™”κ°ˆλ₯¨(Ga2O3) 박막측 및 갈λ₯¨-인듐 κ³΅μœ΅ν•©κΈˆ(eutectic Ga-In alloy; EGaIn) λ²Œν¬μΈ΅μ„ μ°¨λ‘€λ‘œ μ μΈ΅ν•˜μ—¬ μ—΄μ „μ†Œμžλ₯Ό μ œμž‘ν•˜μ˜€λ‹€. n-μ•Œν‚¬μ•„λ―Ό λΆ„μžμ˜ λΉ„κ³΅μœ  접합에 μ˜ν•΄ μœ λ„ κ°­ μƒνƒœ(induced-gap state)κ°€ κ·Έλž˜ν•€ μ—΄μ „μ†Œμž(SLG//H2NCn//Ga2O3/EGaIn)에 λ„μž…λ˜μ—ˆλ‹€. 금 박막측과 n-μ•ŒμΌ€μΈμ‹Έμ΄μ˜¬λ ˆμ΄νŠΈ(n-alkanethiolates; SCn) λΆ„μžμ˜ μ ‘ν•©μœΌλ‘œ κ΅¬μ„±λœ μ’…λž˜μ˜ μ—΄μ „μ†Œμž(Au/SCn//Ga2O3/EGaIn)μ™€μ˜ 비ꡐλ₯Ό 톡해, μƒκΈ°ν•œ λ°©μ‹μœΌλ‘œ μ œμž‘λœ κ·Έλž˜ν•€ μ—΄μ „μ†Œμžκ°€ μš°μˆ˜ν•œ μ—΄μ „νŠΉμ„±μ„ μ§€λ‹ˆκ³  μžˆμŒμ„ 증λͺ…ν•˜μ˜€λ‹€.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 178λ°•

    Photo Thermal Effect Graphene Detector Featuring 105 Gbit s-1 NRZ and 120 Gbit s-1 PAM4 Direct Detection

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    The challenge of next generation datacom and telecom communication is to increase the available bandwidth while reducing the size, cost and power consumption of photonic integrated circuits. Silicon (Si) photonics has emerged as a viable solution to reach these objectives. Graphene, a single-atom thick layer of carbon5, has been recently proposed to be integrated with Si photonics because of its very high mobility, fast carrier dynamics and ultra-broadband optical properties. Here, we focus on graphene photodetectors for high speed datacom and telecom applications. High speed graphene photodetectors have been demonstrated so far, however the most are based on the photo-bolometric (PB) or photo-conductive (PC) effect. These devices are characterized by large dark current, in the order of milli-Amperes , which is an impairment in photo-receivers design, Photo-thermo-electric (PTE) effect has been identified as an alternative phenomenon for light detection. The main advantages of PTE-based photodetectors are the optical power to voltage conversion, zero-bias operation and ultra-fast response. Graphene PTE-based photodetectors have been reported in literature, however high-speed optical signal detection has not been shown. Here, we report on an optimized graphene PTE-based photodetector with flat frequency response up to 65 GHz. Thanks to the optimized design we demonstrate a system test leading to direct detection of 105 Gbit s-1 non-return to zero (NRZ) and 120 Gbit s-1 4-level pulse amplitude modulation (PAM) optical signal
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