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    Self-Assembly of Electric Circuits

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    Self-Assembly of Electric Circuit

    ์ „์ž ์žฅ์น˜ ๋‚ด ๊ตญ๋ถ€์  ์ „๊ณ„ ํ–ฅ์ƒ์„ ์œ„ํ•œ ๋‚˜๋…ธ ๊ตฌ์กฐ์ฒด

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€, 2021.8. ์กฐ์žฌ์˜.The goal of this dissertation is to investigate effect of nanostructures for local electric field enhancement in electronic devices and to provide experimental and theoretical bases for their practical use. Resistive random access memory (RRAM) is a data storage device that can be modulated its resistance states by external electrical stimuli. The electric field generated by the applied potential difference between the two electrodes acts as the driving force to switch the resistance states, so controlling the electric field within the device can lead to improved operational performance and reliability of the device. Even though considerable progress has been made through significant efforts to control the electric field within the device, selectively enhancing the electric field in the intended position for stable and uniform resistive switching behavior is still challenging. Engineered metal structures in the RRAM can efficiently manipulate the electric field. As the radius of the metal structures decreases, the charge density increases, generating electric field enhancements in confined region. To minimize the radius of the metal structure and thus to greatly increase the electric field in a local area, we introduced a nanoscale metal structure into the RRAM. First, pyramid-structured metal electrode with a sharp tip was used to achieve a tip-enhanced electric field, and the effect of the enhanced electric field on the resistive switching behaviors of the device was investigated. Based on numerical simulation and experimental results, we confirmed that pyramidal electrode with a tip radius of tens of nanometers can selectively enhance the electric field at the tip. The tip-enhanced electric field can facilitate the thermochemical reaction in transition metal oxide-based RRAMs and efficiency of charge injection and transport in organic-based RRAMs, as well as provide position selectivity during formation of conductive filament. The resulting RRAM exhibited reliable resistive switching behavior and highly improved device performance compared with conventional RRAM with planar electrode. As another approach to enhance the electric field within the resistive switching layer, we prepared spherical nanostructures via self-assembled block copolymer (BCP)/metal compound micelles. BCP and metal precursors were dissolved in aqueous media for use as BCP/metal compound micelles. These micelles were used as complementary resistive switch (CRS) layers of the memory device and the mechanism of CRS behavior was investigated. The spherical metal nanostructures can improve the electric fields, promoting a resistive switching mechanism based on electrochemical metallization. The resulting CRS memory exhibited reliable resistive switching behavior with four distinct threshold voltages in both cycle-to-cycle and cell-to-cell tests. Also, the conduction and resistive switching mechanism are experimentally demonstrated through the the analysis of the currentโ€“voltage data plot and detemination of the temperature coefficient of resistance. Overall, we pursued efficient engineering of metal nanostructures capable of manipulating electric fields for improving the operational performance and reliability of memory devices. There is no doubt that the commercialized RRAM will become popular in the near future after overcoming all the challenges of RRAM through continuous interest and research. We believe that these results will not only contribute to the significant advancement of all electronic devices, including RRAM, but will also help promote research activities in the electronic device field.๋ณธ ๋…ผ๋ฌธ์˜ ๋ชฉ์ ์€ ๋‚˜๋…ธ ๊ตฌ์กฐ์ฒด๋ฅผ ํ†ตํ•œ ์ „์ž ์žฅ์น˜ ๋‚ด ๊ตญ๋ถ€์  ์ „๊ณ„ ํ–ฅ์ƒ ํšจ๊ณผ๋ฅผ ์กฐ์‚ฌํ•˜๊ณ , ์ด์˜ ์‹ค์ œ ์‚ฌ์šฉ์„ ์œ„ํ•œ ์‹คํ—˜ ๋ฐ ์ด๋ก ์  ๊ธฐ๋ฐ˜์„ ์ œ๊ณตํ•˜๋Š” ๊ฒƒ์ด๋‹ค. ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ (resistive random access memory) ๋Š” ์™ธ๋ถ€ ์ „๊ธฐ ์ž๊ทน์— ์˜ํ•ด ์ €ํ•ญ ์ƒํƒœ๋ฅผ ๋ณ€ํ™” ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ๋ฐ์ดํ„ฐ ์ €์žฅ ์žฅ์น˜์ด๋‹ค. ๋‘ ์ „๊ทน ์‚ฌ์ด์— ์ธ๊ฐ€๋œ ์ „์œ„์ฐจ์— ์˜ํ•ด ์ƒ์„ฑ๋œ ์ „๊ธฐ์žฅ์€ ์ €ํ•ญ ์ƒํƒœ๋ฅผ ์ „ํ™˜์‹œํ‚ค๋Š” ๊ตฌ๋™๋ ฅ์œผ๋กœ์จ ์ž‘์šฉํ•˜๋ฏ€๋กœ, ์ „์ž ์žฅ์น˜ ๋‚ด์—์„œ ์ „๊ธฐ์žฅ์„ ์ œ์–ดํ•˜๋ฉด ์žฅ์น˜์˜ ์„ฑ๋Šฅ๊ณผ ์‹ ๋ขฐ์„ฑ์„ ํ–ฅ์ƒ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋‹ค. ์žฅ์น˜ ๋‚ด์—์„œ ์ „๊ธฐ์žฅ์„ ์ œ์–ดํ•˜๋ ค๋Š” ๋งŽ์€ ๋…ธ๋ ฅ์„ ํ†ตํ•ด ์ƒ๋‹นํ•œ ์ง„์ „์ด ์žˆ์—ˆ์ง€๋งŒ, ์•ˆ์ •์ ์ด๊ณ  ๊ท ์ผํ•œ ์ €ํ•ญ ๋ณ€ํ™” ๊ฑฐ๋™์„ ์œ„ํ•ด ์˜๋„๋œ ์œ„์น˜์—์„œ ์ „๊ธฐ์žฅ์„ ์„ ํƒ์ ์œผ๋กœ ํ–ฅ์ƒ์‹œํ‚ค๋Š” ์ผ์€ ์•„์ง ๋„์ „์  ๊ณผ์ œ์ด๋‹ค. ๊ตฌ์กฐํ™”๋œ ๊ธˆ์†์„ ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ์— ์ ‘๋ชฉ์‹œํ‚ด์œผ๋กœ์จ ์ „๊ธฐ์žฅ์„ ํšจ์œจ์ ์œผ๋กœ ์กฐ์ž‘ํ•  ์ˆ˜ ์žˆ๋‹ค. ๊ธˆ์† ๊ตฌ์กฐ์ฒด์˜ ๋ฐ˜๊ฒฝ์ด ๊ฐ์†Œํ•จ์— ๋”ฐ๋ผ ์ „ํ•˜ ๋ฐ€๋„๊ฐ€ ์ฆ๊ฐ€ํ•˜์—ฌ ๊ตญ๋ถ€์  ์˜์—ญ์—์„œ ์ „๊ธฐ์žฅ์ด ํ–ฅ์ƒ๋œ๋‹ค. ์ด ๋…ผ๋ฌธ์—์„œ๋Š” ๊ธˆ์† ๊ตฌ์กฐ์ฒด์˜ ๋ฐ˜๊ฒฝ์„ ์ตœ์†Œํ™”ํ•˜์—ฌ ๊ตญ๋ถ€์ ์œผ๋กœ ์ „๊ธฐ์žฅ์„ ํฌ๊ฒŒ ํ–ฅ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•ด ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ์— ๋‚˜๋…ธ์Šค์ผ€์ผ์˜ ๊ธˆ์† ๊ตฌ์กฐ์ฒด๋ฅผ ๋„์ž…ํ•˜์˜€๋‹ค. ์ฒซ ๋ฒˆ์งธ๋กœ, ํŒ ๊ฐ•ํ™” (tip-enhanced) ์ „๊ธฐ์žฅ ํšจ๊ณผ๋ฅผ ๋‹ฌ์„ฑํ•˜๊ธฐ ์œ„ํ•ด ๋‚ ์นด๋กœ์šด ํŒ์„ ๊ฐ€์ง€๋Š” ํ”ผ๋ผ๋ฏธ๋“œ ๊ธˆ์† ๊ตฌ์กฐ์ฒด๋ฅผ ์ „๊ทน์œผ๋กœ ์‚ฌ์šฉํ•˜์˜€์œผ๋ฉฐ, ๊ฐ•ํ™”๋œ ์ „๊ธฐ์žฅ์ด ์†Œ์ž์˜ ์ €ํ•ญ ๋ณ€ํ™” ๊ฑฐ๋™์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์„ ์กฐ์‚ฌํ•˜์˜€๋‹ค. ์œ ํ•œ์š”์†Œ๋ชจ๋ธ๋ง๊ณผ ์‹คํ—˜๊ฒฐ๊ณผ๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ, ์ˆ˜์‹ญ ๋‚˜๋…ธ ๋ฏธํ„ฐ์˜ ํŒ ๋ฐ˜๊ฒฝ์„ ๊ฐ€์ง€๋Š” ํ”ผ๋ผ๋ฏธ๋“œ ๊ตฌ์กฐ์ฒด ์ „๊ทน์ด ํŒ ๋ถ€๊ทผ์—์„œ ์ „๊ธฐ์žฅ์„ ๊ตญ์†Œ์ ์œผ๋กœ ํ–ฅ์ƒ์‹œํ‚ฌ ์ˆ˜ ์žˆ์Œ์„ ํ™•์ธํ•˜์˜€๋‹ค. ํŒ ๊ฐ•ํ™” ์ „๊ธฐ์žฅ์€ ์ „์ด ๊ธˆ์† ์‚ฐํ™”๋ฌผ-๊ธฐ๋ฐ˜ ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ์—์„œ ์—ดํ™”ํ•™ (thermochemical) ๋ฐ˜์‘์„ ์ด‰์ง„์‹œํ‚ค๊ณ  ์œ ๊ธฐ-๊ธฐ๋ฐ˜ ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ์—์„œ ์ „ํ•˜ ์ฃผ์ž… (charge injection) ๋ฐ ์ˆ˜์†ก (transport) ํšจ์œจ์„ฑ์„ ํ–ฅ์ƒ์‹œํ‚ฌ ๋ฟ ์•„๋‹ˆ๋ผ, ์„ ํƒ์ ์ธ ์œ„์น˜์—์„œ๋งŒ ์ „๋„์„ฑ ํ•„๋ผ๋ฉ˜ํŠธ (conductive filament)๋ฅผ ํ˜•์„ฑ์‹œํ‚ฌ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๊ทธ ๊ฒฐ๊ณผ ํ”ผ๋ผ๋ฏธ๋“œ ๊ตฌ์กฐ์ฒด ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ๋Š” ์ข…๋ž˜์˜ ํ‰ํŒ ๊ตฌ์กฐ์ฒด ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ์— ๋น„ํ•ด ์•ˆ์ •์ ์ธ ์ €ํ•ญ ๋ณ€ํ™” ๊ฑฐ๋™๊ณผ ํ–ฅ์ƒ๋œ ์žฅ์น˜ ์„ฑ๋Šฅ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ์ €ํ•ญ ๋ณ€ํ™” ์ธต ๋‚ด์˜ ์ „๊ธฐ์žฅ์„ ํ–ฅ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•œ ๋˜ ๋‹ค๋ฅธ ์ ‘๊ทผ๋ฒ•์œผ๋กœ, ์ž๊ธฐ์กฐ๋ฆฝ (self-assembled)๋œ ๋ธ”๋ก๊ณต์ค‘ํ•ฉ์ฒด (block copolymer)/๊ธˆ์† ๋ณตํ•ฉ์ฒด ๋ฏธ์…€ (micelle)์„ ์ด์šฉํ•˜์—ฌ ๊ตฌํ˜•์˜ ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด๋ฅผ ์†Œ์ž์˜ ์ค‘๊ฐ„์ธต์œผ๋กœ ๋„์ž…ํ•˜์˜€๋‹ค. ๋ธ”๋ก๊ณต์ค‘ํ•ฉ์ฒด ๋ฐ ๊ธˆ์†์ „๊ตฌ์ฒด๋ฅผ ๋ณตํ•ฉ์ฒด ๋ฏธ์…€๋กœ ์‚ฌ์šฉํ•˜๊ธฐ ์œ„ํ•ด ์„ ํƒ์  ์šฉ๋งค์— ์šฉํ•ด์‹œ์ผฐ๋‹ค. ํ•ด๋‹น ๋ฏธ์…€์„ ๋ฉ”๋ชจ๋ฆฌ ์†Œ์ž์˜ ์ƒ๋ณด์  ์ €ํ•ญ ๋ณ€ํ™” (complementary resistive switch) ์ธต์œผ๋กœ ์‚ฌ์šฉํ•˜์˜€์œผ๋ฉฐ, ์ƒ๋ณด์  ์ €ํ•ญ ๋ณ€ํ™” ๊ฑฐ๋™์˜ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ์กฐ์‚ฌํ•˜์˜€๋‹ค. ๊ตฌํ˜•์˜ ๊ธˆ์† ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด๋Š” ์ „๊ธฐ์žฅ์„ ํ–ฅ์ƒ์‹œ์ผœ ์ „๊ธฐํ™”ํ•™์  ๊ธˆ์†ํ™” (electrochemical metallization)์— ๊ธฐ๋ฐ˜ํ•œ ์ €ํ•ญ ๋ณ€ํ™” ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ์ด‰์ง„์‹œํ‚ฌ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๊ทธ ๊ฒฐ๊ณผ ์ƒ๋ณด์  ์ €ํ•ญ ๋ณ€ํ™” ๋ฉ”๋ชจ๋ฆฌ๋Š” ์‚ฌ์ดํด ๋ฐ ์…€๊ฐ„ ๋ฐ˜๋ณต ์‹œํ—˜ ๋ชจ๋‘์—์„œ 4๊ฐœ์˜ ์ž„๊ณ„ ์ „์••์œผ๋กœ ์•ˆ์ •์ ์ธ ์ €ํ•ญ ๋ณ€ํ™” ๋™์ž‘์„ ๋‚˜ํƒ€๋‚ด์—ˆ๋‹ค. ๋˜ํ•œ ์ „๋ฅ˜-์ „์•• ์ž๋ฃŒ ํ”Œ๋กฏ (plot) ๋ถ„์„๊ณผ ์ €ํ•ญ์˜ ์˜จ๋„ ๊ณ„์ˆ˜ ๊ฒฐ์ •์„ ํ†ตํ•ด ์žฅ์น˜์˜ ์ „๋„ ๋ฐ ์ €ํ•ญ ๋ณ€ํ™” ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ์‹คํ—˜์ ์œผ๋กœ ์ž…์ฆํ•˜์˜€๋‹ค. ์ „๋ฐ˜์ ์œผ๋กœ ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์žฅ์น˜ ๋‚ด ์ „๊ธฐ์žฅ์„ ์ฆํญ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ๊ธˆ์† ๋‚˜๋…ธ๊ตฌ์กฐ์ฒด์˜ ํšจ์œจ์ ์ธ ์—”์ง€๋‹ˆ์–ด๋ง์„ ํ†ตํ•ด ๋ฉ”๋ชจ๋ฆฌ ์žฅ์น˜์˜ ์„ฑ๋Šฅ๊ณผ ์‹ ๋ขฐ์„ฑ ํ–ฅ์ƒ์„ ์ถ”๊ตฌํ•˜์˜€๋‹ค. ์ง€์†์ ์ธ ๊ด€์‹ฌ๊ณผ ์—ฐ๊ตฌ๋ฅผ ํ†ตํ•ด ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ์˜ ๋ชจ๋“  ๊ณผ์ œ๋ฅผ ๊ทน๋ณตํ•œ ํ›„, ์ƒ์šฉํ™”๋œ ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ๊ฐ€ ๊ฐ€๊นŒ์šด ๋ฏธ๋ž˜์— ๋Œ€์ค‘ํ™”๋  ๊ฒƒ์ž„์„ ๋ฏฟ์–ด ์˜์‹ฌ์น˜ ์•Š๋Š”๋‹ค. ์šฐ๋ฆฌ๋Š” ์ด ๊ฒฐ๊ณผ๊ฐ€ ์ €ํ•ญ๋ณ€ํ™”๋ฉ”๋ชจ๋ฆฌ๋ฅผ ํฌํ•จํ•œ ๋ชจ๋“  ์ „์ž ์žฅ์น˜์˜ ํš๊ธฐ์ ์ธ ๋ฐœ์ „์— ๊ธฐ์—ฌํ•  ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ์ „์ž ์žฅ์น˜ ๋ถ„์•ผ์˜ ์—ฐ๊ตฌ ํ™œ๋™์„ ์ด‰์ง„ํ•˜๋Š” ๋ฐ์—๋„ ๋„์›€์ด ๋  ๊ฒƒ์ด๋ผ๊ณ  ๋ฏฟ๋Š”๋‹ค.Chapter 1. Introduction 1 1.1. Background 1 1.1.1. Necessity of new memory devices 1 1.1.2. Resistive random access memory 2 1.2. Motivation 4 1.3. Dissertation Overview 6 1.4. References 9 Chapter 2. Tip-Enhanced Electric Field-Driven Efficient Charge Injection and Transport in Organic Material-Based Resistive Memories 19 2.1. Introduction 21 2.2. Experimental 24 2.3. Results and Discussion 27 2.4. Conclusions 37 2.5. References 38 Chapter 3. Facilitation of the Thermochemical Mechanism in NiO-Based Resistive Switching Memories via Tip-Enhanced Electric Fields 52 3.1. Introduction 54 3.2. Experimental 57 3.3. Results and Discussion 60 3.4. Conclusions 66 3.5. References 67 Chapter 4. Facile Achievement of Complementary Resistive Switching Behaviors via Self-Assembled Block Copolymer Micelles 82 4.1. Introduction 83 4.2. Experimental 86 4.3. Results and Discussion 89 4.4. Conclusions 96 4.5. References 97 Chapter 5. Conclusion 109 Abstract in Korean 112๋ฐ•

    Design of bias circuit for charge pump in 130nm BiCMOS technology

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    El presente trabajo muestra el diseรฑo de un circuito de polarizaciรณn en la tecnologรญa de 130nm BiCMOS con las herramientas de diseรฑo de Cadence. El circuito de polarizaciรณn es parte de un circuito Charge Pump (CP), el cual a su vez es parte de un circuito PLL (Phased Locked Loop) que se utilizarรก en una implementaciรณn de seรฑal mixta de un Recuperador de Datos (CDR). Al inicio del trabajo se presenta una descripciรณn general de los mรณdulos analรณgicos y digitales que conforman el proyecto. La topologรญa de diseรฑo propuesta refleja la enorme dependencia del circuito de polarizaciรณn con el circuito CP. Un circuito replica permite โ€œseguirโ€ las variaciones de carga y descarga de corriente del circuito CP para compensar mediante un OTA (Operational Transconductance Amplifier) el nivel de voltaje requerido en los transistores del circuito diferencial del CP. El proceso de diseรฑo, la generaciรณn de esquemรกticos y bancos de pruebas son mostrados durante los primeros capรญtulos del trabajo. La verificaciรณn del diseรฑo pre-layout a travรฉs del proceso de esquinas, asรญ como el uso el uso de las herramientas de verificaciรณn de reglas de diseรฑo post-layout son mostradas durante los capรญtulos finales.The present work shows the design of a Bias circuit in 130 nm of BiCMOS process using Cadence tools. The Bias circuit is part of a Charge Pump (CP) circuit, which in turn is one block of a PLL (Phased Locked Loop) that will be used in a mixed-signal implementation of a Clock and Data Recovery (CDR) circuit. This PLL-based CDR is the project of the generation 2018 of the Specialty in System on a Chip at ITESO. A general description of the analog and digital modules that make up this project is shown at the beginning of this work. As it is described in detail in this work, the proposed design topology reveals the enormous dependence of the polarization circuit to the CP circuit. The replica method used in the Bias circuit allows to "follow" the current variations of CP charge/discharge process to compensate through an OTA (Operational Transconductance Amplifier) the level of voltage required by the tail transistors of CP circuit. The design procedure, the generation of schematics and test benches are shown during the first chapters of this work. The verification of the pre-layout design through the corners process, as well as the use of the post-layout design rules verification tools, are shown during the final chapters of this work.Consejo Nacional de Ciencia y Tecnologรญ

    High-throughput large-area plastic nanoelectronics

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    Large-area electronics (LAE) manufacturing has been a key focus of both academic and industrial research, especially within the last decade. The growing interest is born out of the possibility of adding attractive properties (flexibility, light weight or minimal thickness) at low cost to well-established technologies, such as photovoltaics, displays, sensors or enabling the realisation of emerging technologies such as wearable devices and the Internet of Things. As such there has been great progress in the development of materials specifically designed to be employed in solution processed (plastic) electronics, including organic, transparent metal oxide and nanoscale semiconductors, as well as progress in the deposition methods of these materials using low-cost high-throughput printing techniques, such as gravure printing, inkjet printing, and roll-to-roll vacuum deposition. Meanwhile, industry innovation driven by Mooreโ€™s law has pushed conventional silicon-based electronic components to the nanoscale. The processes developed for LAE must strive to reach these dimensions. Given that the complex and expensive patterning techniques employed by the semiconductor industry so far are not compatible with LAE, there is clearly a need to develop large-area high throughput nanofabrication techniques. This thesis presents progress in adhesion lithography (a-Lith), a nanogap electrode fabrication process that can be applied over large areas on arbitrary substrates. A-Lith is a self-alignment process based on the alteration of surface energies of a starting metal electrode which allows the removal of any overlap of a secondary metal electrode. Importantly, it is an inexpensive, scalable and high throughput technique, and, especially if combined with low temperature deposition of the active material, it is fundamentally compatible with large-area fabrication of nanoscale electronic devices on flexible (plastic) substrates. Herein, I present routes towards process optimisation with a focus on gap size reduction and yield maximisation. Asymmetric gaps with sizes below 10 nm and yields of > 90 % for hundreds of electrode pairs generated on a single substrate are demonstrated. These large width electrode nanogaps represent the highest aspect ratio nanogaps (up to 108) fabricated to date. As a next step, arrays of Schottky nanodiodes are fabricated by deposition of a suitable semiconductor from solution into the nanogap structures. Of principal interest is the wide bandgap transparent semiconductor, zinc oxide (ZnO). Lateral ZnO Schottky diodes show outstanding characteristics, with on-off ratios of up to 106 and forward current values up to 10 mA for obtained upon combining a-Lith with low-temperature solution processing. These unique devices are further investigated for application in rectifier circuits, and in particular for potential use in radio frequency identification (RFID) tag technology. The ZnO diodes are found to surpass the 13.56 MHz frequency bernchmark used in commercial applications and approach the ultra-high frequency (UHF) band (hundreds of megahertz), outperforming current state of the art printed diodes. Solution processed fullerene (C60) is also shown to approach the UHF band in this co-planar device configuration, highlighting the viability of a-Lith for enabling large-area flexible radio frequency nanoelectronics. Finally, resistive switching memory device arrays based on a-Lith patterned nanogap aluminium symmetric electrodes are demonstrated for the first time. These devices are based either on empty aluminium nanogap electrodes, or with the gap filled with a solution-processed semiconductor, the latter being ZnO, the semiconducting polymer poly(9,9-dioctylfluorene-alt-benzothiadiazole) (F8BT) or carbon nanotube/polyfluorene blends. The switching mechanism, retention time and switching speed are investigated and compared with published data. The fabrication of arrays of these devices illustrates the potential of a-Lith as a simple technique for the realisation of large-area high-density memory applications.Open Acces

    Threshold Switching and Self-Oscillation in Niobium Oxide

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    Volatile threshold switching, or current controlled negative differential resistance (CC-NDR), has been observed in a range of transition metal oxides. Threshold switching devices exhibit a large non-linear change in electrical conductivity, switching from an insulating to a metallic state under external stimuli. Compact, scalable and low power threshold switching devices are of significant interest for use in existing and emerging technologies, including as a selector element in high-density memory arrays and as solid-state oscillators for hardware-based neuromorphic computing. This thesis explores the threshold switching in amorphous NbOx and the properties of individual and coupled oscillators based on this response. The study begins with an investigation of threshold switching in Pt/NbOx/TiN devices as a function device area, NbOx film thickness and temperature, which provides important insight into the structure of the self-assembled switching region. The devices exhibit combined threshold-memory behaviour after an initial voltage-controlled forming process, but exhibit symmetric threshold switching when the RESET and SET currents are kept below a critical value. In this mode, the threshold and hold voltages are shown to be independent of the device area and film thickness, and the threshold power, while independent of device area, is shown to decrease with increasing film thickness. These results are shown to be consistent with a structure in which the threshold switching volume is confined, both laterally and vertically, to the region between the residual memory filament and the electrode, and where the memory filament has a core-shell structure comprising a metallic core and a semiconducting shell. The veracity of this structure is demonstrated by comparing experimental results with the predictions of a resistor network model, and detailed finite element simulations. The next study focuses on electrical self-oscillation of an NbOx threshold switching device incorporated into a Pearson-Anson circuit configuration. Measurements confirm stable operation of the oscillator at source voltages as low as 1.06 V, and demonstrate frequency control in the range from 2.5 to 20.5 MHz with maximum frequency tuning range of 18 MHz/V. The oscillator exhibit three distinct oscillation regimes: sporadic spiking, stable oscillation and damped oscillation. The oscillation frequency, peak-to-peak amplitude and frequency are shown to be temperature and voltage dependent with stable oscillation achieved for temperatures up to โˆผ380 K. A physics-based threshold switching model with inclusion of device and circuit parameters is shown to explain the oscillation waveform and characteristic. The final study explores the oscillation dynamics of capacitively coupled Nb/Nb2O5 relaxation oscillators. The coupled system exhibits rich collective behaviour, from weak coupling to synchronisation, depending on the negative differential resistance response of the individual devices, the operating voltage and the coupling capacitance. These coupled oscillators are shown to exhibit stable frequency and phase locking states at source voltages as low as 2.2 V with MHz frequency tunable range. The numerical simulation of the coupled system highlights the role of source voltage, and circuit and device capacitance in controlling the coupling modes and dynamics
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