33 research outputs found

    Electrical resistance of individual defects at a topological insulator surface

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    Three-dimensional topological insulators host surface states with linear dispersion, which manifest as a Dirac cone. Nanoscale transport measurements provide direct access to the transport properties of the Dirac cone in real space and allow the detailed investigation of charge carrier scattering. Here, we use scanning tunnelling potentiometry to analyse the resistance of different kinds of defects at the surface of a (Bi0.53Sb0.47)2Te3 topological insulator thin film. The largest localized voltage drop we find to be located at domain boundaries in the topological insulator film, with a resistivity about four times higher than that of a step edge. Furthermore, we resolve resistivity dipoles located around nanoscale voids in the sample surface. The influence of such defects on the resistance of the topological surface state is analysed by means of a resistor network model. The effect resulting from the voids is found to be small compared to the other defects

    Thermoelectric Limitations of Graphene Nanodevices at Ultrahigh Current Densities.

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    Graphene is atomically thin, possesses excellent thermal conductivity, and is able to withstand high current densities, making it attractive for many nanoscale applications such as field-effect transistors, interconnects, and thermal management layers. Enabling integration of graphene into such devices requires nanostructuring, which can have a drastic impact on the self-heating properties, in particular at high current densities. Here, we use a combination of scanning thermal microscopy, finite element thermal analysis, and operando scanning transmission electron microscopy techniques to observe prototype graphene devices in operation and gain a deeper understanding of the role of geometry and interfaces during high current density operation. We find that Peltier effects significantly influence the operational limit due to local electrical and thermal interfacial effects, causing asymmetric temperature distribution in the device. Thus, our results indicate that a proper understanding and design of graphene devices must include consideration of the surrounding materials, interfaces, and geometry. Leveraging these aspects provides opportunities for engineered extreme operation devices

    Spatial control of electron & hole states in InAs/GaSb heterostructures

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    Single nanowire transistors employing three separately controlled electrostatic gates were fabricated to investigate band gap modulation in InAs-GaSb heterostructures. The aim is to show hybridization between electron and hole states over the heterojunction. Electric and thermoelectric characterization at low temperatures suggests that transport can be tuned from electrons in InAs to holes GaSb and that the relative band alignment can be altered from an inverted to a small effective gap. The band gap modulation is speculated to be caused by quantum confinement induced by the gates

    Thermoelectric Limitations of Graphene Nanodevices at Ultrahigh Current Densities

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    Graphene is atomically thin, possesses excellent thermal conductivity, and is able to withstand high current densities, making it attractive for many nanoscale applications such as field-effect transistors, interconnects, and thermal management layers. Enabling integration of graphene into such devices requires nanostructuring, which can have a drastic impact on the self-heating properties, in particular at high current densities. Here, we use a combination of scanning thermal microscopy, finite element thermal analysis, and operando scanning transmission electron microscopy techniques to observe prototype graphene devices in operation and gain a deeper understanding of the role of geometry and interfaces during high current density operation. We find that Peltier effects significantly influence the operational limit due to local electrical and thermal interfacial effects, causing asymmetric temperature distribution in the device. Thus, our results indicate that a proper understanding and design of graphene devices must include consideration of the surrounding materials, interfaces, and geometry. Leveraging these aspects provides opportunities for engineered extreme operation devices

    ๋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•

    Van Der Waals heterostructures:Fabrication and nanoscale and thermal characterisation via SPM methods

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    Since the dawn of two-dimensional (2D) era, graphene and the plethora of other atomically thin layered materials cousins, including their combinations in heterostructures, have revolutionized material science and established themselves as promising candidates for the next-generation of nanoscale devices. However, the landscape of opportunities and possible combinations is so vast, that many promising research topics remain widely unexplored. The aim of this work is to address some of these questions, contributing to the progress and understanding in three different areas: fabrication of novel 2D materials and their heterostructures; electronic properties and doping mechanisms in these at the nanoscale; and characterization of the nanoscale thermal and thermoelectric properties of 2D materials. Starting with the fabrication procedures, different techniques for mechanical exfoliation and polymeric dry transfer of 2D materials and heterostructures were explored. This research route led to the establishment of a new fabrication facility at the National Physical laboratory (NPL), and to the production of a wide variety of samples, from exfoliated flakes to complex heterostructures and devices. A selection of the produced samples was employed during this thesis to investigate the electronic and thermal properties of 2D materials via spectroscopic and advanced scanning probe microscopy (SPM) techniques. Regarding the electronic response of graphene, two routes were undertaken: first, the electronic response of different types of graphene towards humidity acting as a p-dopant was studied for the first time using Raman spectroscopy. Second, a procedure improving current methods of quantitative probe calibration in Kelvin probe force microscopy (KPFM) was developed, establishing the determination of reliable and consistent work-function values with high-resolution. This method was then employed to study the electronic properties and doping of encapsulated graphene heterostructures, providing quantitative values of the work-function of the system, as well as demonstrating the capability of KPFM as an excellent visualisation and characterisation technique for buried layers otherwise inaccessible by other methods. Finally, various thermal properties of 2D materials were studied via advanced SPM techniques: Scanning thermal microscopy (SThM) that was used for the determination of the thickness dependence of the thermal conductance of exfoliated InSe, and scanning thermal gate microscopy (STGM) that was employed to explore the thermovoltage, and thus Seebeck coefficient, variation in encapsulated graphene heterostructures with patterned constrictions. The main highlights of the work developed during this thesis are: (1) the formulated need and subsequent realisation of various approaches towards the fabrication of 2D materials and heterostructures. For this, shared expertise with other researchers and institutions, and access to different fabrication facilities were essential; and (2) the exploitation of the potential of spectroscopic and advanced SPM methods in providing reliable characterisation of the 2D material and heterostructureโ€™s properties with nanoscale resolution. The findings of this thesis have provided new insights in a varied number of areas, and hold promise for different future applications: from single material thermocouples to graphene-gas sensors, including improved fabrication procedures for 2D materials, or even, probe-calibration and characterisation methods

    Proximity Effects in Epitaxial Graphene on SiC and their Impact on Atomic-Scale Charge Transport

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    Es gibt erste Ansรคtze, die Nรคhe des zweidimensionalen Materials Graphen zu bestimmten Materialien auszunutzen, um die Eigenschaften von Graphen gezielt zu verรคndern. Um diese Ansรคtze jedoch in vorteilhafte Werkzeuge zur gezielten Beeinflussung der Eigenschaften von epitaktischem Graphen umzuwandeln, mรผssen zunรคchst die Proximity-Effekte in unverรคndertem Graphen auf SiC untersucht und die zugrundeliegenden Kopplungsmechanismen verstanden werden. Ein direkter Einfluss der Nรคhe zum Substrat zeigt sich in den Ladungstransporteigenschaften von epitaktischem Graphen, da charakteristische GrรถรŸen wie die Ladungstrรคgerdichte und die Ladungstrรคgerbeweglichkeit stark beeinflusst werden. In dieser Arbeit wird ein umfassender Zugang verwendet, der auf der Verknรผpfung von lokalen strukturellen, elektronischen und Transporteigenschaften basiert, um die Auswirkungen der Nรคhe des SiC-Substrates auf epitaktisches Graphen zu untersuchen. Dies ermรถglicht es, lokale Variationen in der Kopplung zu identifizieren und Zugang zu den grundlegenden Mechanismen der Substrat-Graphen-Wechselwirkung zu erhalten.Approaches to exploit the proximity of the two-dimensional material graphene to certain materials in order to specifically tune grapheneโ€™s properties start to emerge. However, to turn these approaches into truly beneficial tools to engineer epitaxial grapheneโ€™s properties, it is first necessary to investigate proximity effects in pristine graphene on SiC and to understand the coupling mechanisms behind them. A direct influence of the proximity to the substrate is seen in the charge transport properties of epitaxial graphene, as characteristic quantities such as the charge carrier density and the charge carrier mobility are significantly affected. In this thesis, a comprehensive approach based on linking local structural, electronic as well as transport properties is used to investigate proximity effects of the SiC substrate on epitaxial graphene. This allows to identify local variations in the coupling and to gain access to the fundamental mechanisms of the substrate-graphene interaction.2021-10-2

    Novel Multiphysics Phenomena in a New Generation of Energy Storage and Conversion Devices

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    The swelling demand for storing and using energy at diverse scales has stimulated the exploration of novel materials and design strategies applicable to energy storage systems. The most popular electrochemical energy storage systems are batteries, fuel cells and capacitors. Supercapacitors, also known as ultracapacitors, or electrochemical capacitors have emerged to be particularly promising. Besides exhibiting high cycle life, they combine the best attributes of capacitors (high power density) and batteries (high energy storage density). Consequently, they are expected to be in high demand for applications requiring peak power such as hybrid electric vehicles and uninterruptible power supplies (UPS). This dissertation aims to make advancements on the following two topics in supercapacitor research with the aid of modeling and experimental tools: applying various thermophysical effects to design supercapacitor devices with novel functionalities and studying degradation mechanisms upon continuous cycling of conventional supercapacitors. The prime drawback of conventional supercapacitors is their low energy density. Most research in the last decade has focused on synthesizing novel electrode materials. Although such novel electrodes lead to high energy density, they often involve complicated synthesis process and result in high cost and low power density. A new concept of inducing pseudocapacitance developed in recent years is by introducing redox additives in the electrolyte that engage in redox reactions at the electrode/electrolyte interface during charge/discharge. The first section of this dissertation reports the performance of fabricated solid-state supercapacitors composed of redox-active gel electrolyte (PVA-K3Fe(CN)6-K4Fe(CN)6). The electrochemical performance has been studied extensively using cyclic voltammetry, constant current charge/discharge and impedance spectroscopy techniques, and then the results are compared with similar devices composed of conventional gel electrolytes such as PVA-H3PO4 and PVA-KOH on the basis of capacitance, internal resistance and stable voltage window. The second section explores the utility of the thermogalvanic property of the same redox-active gel electrolyte, PVA-K3Fe(CN)6-K4Fe(CN)6 in the construction of a thermoelectric supercapacitor. The integrated device is capable of being electrically charged by applying a temperature gradient across its two electrodes. In the absence of available temperature gradient, the device can be discharged electrically through an external circuit. Therefore, such a device can be used to harvest waste heat from intermittent heat sources. An equivalent circuit elucidating the mechanisms of energy conversion and storage applicable to thermally chargeable supercapacitors is developed. A fitting analysis aids in the evaluation of model circuit parameters providing good agreement with experimental voltage and current measurements. The latter part of the dissertation investigates the factors influencing aging in conventional supercapacitors. In the first part, a new imaging technique based on the electroreflectance property of gold has been developed and applied to characterize the aging characteristics of a microsupercapacitor device. Previous aging studies were performed through traditional electrical characterization techniques such as cyclic voltammetry, constant charge/discharge, and electrochemical impedance spectroscopy. These methods, although simple, measure an average of the structuresโ€™ internal performance, providing little or no information about microscopic details inside the device. The electroreflectance imaging method, developed in this work is demonstrated as a high-resolution imaging technique to investigate charge distribution, and thus to infer aging characteristics upon continuous cycling at high scan rates. The technique can be used for non-intrusive spatial analysis of other electrochemical systems in the future. In addition, we investigate heat generation mechanisms that are responsible for accelerated aging in supercapacitors. A modeling framework has been developed for heat generation rates and resulting temperature evolution in porous electrode supercapacitors upon continuous cycling. Past thermal models either neglected spatial variations of heat generation within the cell or considered electrodes as flat plates that led to inaccuracies. Here, expressions for spatiotemporal variation of heat generation rate are rigorously derived on the basis of porous electrode theory. Detailed numerical simulations of temperature evolution are performed for a real-world device, and the results resemble past measurements both qualitatively and quantitatively. In the last chapter of the thesis, a rare thermoelectric effect called the Nernst effect has been investigated in single-layer periodic graphene with the aid of a modified Boltzmann transport equation. Detailed formulations of the transport coefficients from the BTE solution are developed in order to relate the Nernst coefficient to the amount of impurity density, temperature, band gap and applied magnetic field. Detailed knowledge of the variation of the thermoelectric and thermomagnetic properties of graphene shown in this work will prove helpful for improving the performance of magnetothermoelectric coolers and sensors

    Spin-dependent phenomena and device concepts explored in (Ga,Mn)As

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    Over the past two decades, the research of (Ga,Mn)As has led to a deeper understanding of relativistic spin-dependent phenomena in magnetic systems. It has also led to discoveries of new effects and demonstrations of unprecedented functionalities of experimental spintronic devices with general applicability to a wide range of materials. In this article we review the basic material properties that make (Ga,Mn)As a favorable test-bed system for spintronics research and discuss contributions of (Ga,Mn)As studies in the general context of the spin-dependent phenomena and device concepts. Special focus is on the spin-orbit coupling induced effects and the reviewed topics include the interaction of spin with electrical current, light, and heat.Comment: 47 pages, 41 figure
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