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    ์‚ฐํ™”์ฒ  ๋‚˜๋…ธ์ž…์ž์˜ ๊ธˆ์†-์ ˆ์—ฐ์ฒด ์ „์ด ํ˜„์ƒ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€, 2019. 2. ํ˜„ํƒํ™˜.๋‚˜๋…ธ์ž…์ž๋Š” ์ ์–ด๋„ ํ•œ์ชฝ ๋ฐฉํ–ฅ์˜ ๋„ˆ๋น„๊ฐ€ 100 nm, ๋‹ค์‹œ ๋งํ•ด ์ฒœ๋งŒ ๋ถ„์˜ 1๋ฏธํ„ฐ ์ดํ•˜์˜ ํฌ๊ธฐ๋ฅผ ๊ฐ€์ง„ ์ž…์ž์ด๋‹ค. ๋‚˜๋…ธ์ž…์ž๋Š” ๊ธฐ์กด์˜ ๋ฒŒํฌ ๋ฌผ์งˆ๊ณผ๋Š” ๋‹ฌ๋ฆฌ, ํ•˜๋‚˜์˜ ์ž…์ž๋ฅผ ๊ตฌ์„ฑํ•˜๋Š” ์›์ž ๊ฐœ์ˆ˜๊ฐ€ ๋งค์šฐ ์ ๋‹ค. ์ด๋กœ ์ธํ•ด์„œ ๊ธฐ์กด๊ณผ๋Š” ๋งค์šฐ ๋‹ค๋ฅธ ๋ฌผ๋ฆฌ์ , ํ™”ํ•™์  ์„ฑ์งˆ์„ ์ง€๋‹ ์ˆ˜ ์žˆ๋‹ค. ์ง€๋‚œ ์ˆ˜์‹ญ ๋…„์— ๊ฑธ์ณ์„œ ์ด๋Ÿฌํ•œ ์ฐจ์ด๋ฅผ ํ™•์ธํ•˜๋Š” ์—ฐ๊ตฌ ๋ฐ ๊ณตํ•™์ ์œผ๋กœ ์ด์šฉํ•˜๋ ค๋Š” ์—ฐ๊ตฌ๊ฐ€ ๋งŽ์ด ์ง„ํ–‰๋˜๊ณ  ์žˆ๋‹ค. ํ•œํŽธ, ์›ํ•˜๋Š” ์„ฑ์งˆ์˜ ๋‚˜๋…ธ์ž…์ž๋ฅผ ์‹ค์งˆ์ ์œผ๋กœ ํ™œ์šฉํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ๋‚˜๋…ธ์ž…์ž๋ฅผ ๊ท ์ผํ•˜๋ฉด์„œ๋„ ์›ํ•˜๋Š” ๋ชจ์–‘์œผ๋กœ ๋งŒ๋“ค ์ˆ˜ ์žˆ์–ด์•ผ ํ•œ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์˜ ์ฒซ ๋ฒˆ์งธ ์žฅ์—์„œ๋Š” ์–ด๋–ป๊ฒŒ ๋‚˜๋…ธ์ž…์ž๋ฅผ ํ•ฉ์„ฑํ•ด์•ผ ๊ท ์ผํ•˜๋ฉด์„œ๋„ ์›ํ•˜๋Š” ๋ชจ์–‘์œผ๋กœ ๋งŒ๋“ค ์ˆ˜ ์žˆ๋Š”์ง€ ์•Œ์•„๋ณด์•˜๋‹ค. ์ด๋ ‡๊ฒŒ ํ•ฉ์„ฑ๋œ ๋‚˜๋…ธ์ž…์ž๋ฅผ ๊ฐ€์ง€๊ณ  ๋‚˜๋…ธ์ž…์ž๋งŒ์ด ๊ฐ€์ง€๋Š” ํŠน์ดํ•œ ์„ฑ์งˆ์„ ์—ฐ๊ตฌํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋‘ ๋ฒˆ์งธ ์žฅ์—์„œ๋Š” ๋‹ค์–‘ํ•œ ํฌ๊ธฐ๋กœ ํ•ฉ์„ฑ๋œ ์‚ฐํ™”์ฒ  ๋‚˜๋…ธ์ž…์ž๋ฅผ ๊ฐ€์ง€๊ณ  ๊ธˆ์†-์ ˆ์—ฐ์ฒด ์ „์ด ํ˜„์ƒ์„ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ๋‚˜๋…ธ์ž…์ž์˜ ํฌ๊ธฐ๊ฐ€ ์ž‘์•„์งˆ์ˆ˜๋ก ๊ธˆ์†-์ ˆ์—ฐ์ฒด ์ „์ด ํ˜„์ƒ์— ํฐ ๋ณ€ํ™”๊ฐ€ ์ƒ๊ธฐ๋Š” ๊ฒƒ์„ ์•Œ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์„ธ ๋ฒˆ์งธ ์žฅ์—์„œ๋Š” ์‚ฐํ™”์ฒ  ๋‚˜๋…ธ์ž…์ž์— ๊ป์งˆ๊ตฌ์กฐ๋ฅผ ๋งŒ๋“ค์–ด์„œ ๊ธˆ์†-์ ˆ์—ฐ์ฒด ์ „์ด ํ˜„์ƒ์˜ ๋ณ€ํ™”๋ฅผ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ๊ป์งˆ ๋ฌผ์งˆ์˜ ์ข…๋ฅ˜ ๋ฐ ๋‘๊ป˜๊ฐ€ ๋‹ฌ๋ผ์ง์— ๋”ฐ๋ผ์„œ ๊ธˆ์†-์ ˆ์—ฐ์ฒด ์ „์ด ํ˜„์ƒ์—๋„ ๋ณ€ํ™”๊ฐ€ ์ƒ๊ธฐ๋Š” ๊ฒƒ์„ ์•Œ ์ˆ˜ ์žˆ์—ˆ๋‹ค.Nanocrystals are particles that are at least 100 nm wide in one direction. Nanocrystals, unlike their bulk counterparts, contain very few atoms that make up a single particle, leading to very different physical and chemical properties. In order to utilize the desired nanocrystals, nanocrystals must be able to be synthesized in a uniform and desired shape. In the first chapter of this thesis, I will discuss how nanocrystals can be synthesized in a uniform and desired shape. These synthesized nanocrystals allow us to study their unusual properties. In the second chapter, I studied size-dependent metal-insulator transition phenomena on uniform-sized iron oxide (magnetite) nanocrystals with various sizes. The smaller the nanocrystals, the greater the change in metal-insulator transition phenomena. In the third chapter, I synthesized core/shell Fe3O4/ferrite nanocrystals and investigated their metal-insulator transition phenomena. As the types and thickness of the shell materials are varied, changes in the metal-insulator transition phenomena were observed.Chapter 1. Introduction: Nucleation and growth of inorganic nanoparticles 1 1.1 Introduction 1 1.2 Molecule-to-solid transition 5 1.2.1 Structure of molecular clusters 5 1.3 Prenucleation and nucleation periods 9 1.3.1 Nucleation models 9 1.3.2 Stepwise phase transitions 12 1.3.3 Aggregation of nuclei 18 1.4 Growth by assembly and merging 21 1.4.1 Oriented attachment 22 1.4.2 Mesocrystals formation 34 1.5 Heterogeneous nucleation 36 1.5.1 Heterogeneous nucleation process 36 1.5.2 Interface energy minimization and property tuning by lattice strain 42 1.6 Conclusions 50 1.7 References 54 Chapter 2. Size Dependence of Metalโ€“Insulator Transition in Stoichiometric Fe3O4 Nanocrystals 71 2.1 Introduction 71 2.2 Experimental section 73 2.3 Synthesis of uniform sized Fe3O4 nanocrystals 81 2.4 Metal-insulator transition of Fe3O4 nanocrystals 98 2.5 Conclusions 108 2.6 References 110 โ€ƒ Chapter 3. Metalโ€“Insulator Transition of Fe3O4 Nanocrystals by Shell Formation 117 3.1 Introduction 117 3.2 Experimental section 121 3.3 Fe3O4-Fe3O4 core-shell nanocrystals 128 3.4 Fe3O4-MFe2O4 (M= Mn, Co, Ni, CU, Zn) core-shell nanocrystals 131 3.5 Conclusions 144 3.6 References 145 Bibliography 151 ๊ตญ๋ฌธ ์ดˆ๋ก (Abstract in Korean) 154Docto

    DC์™€ RF ๋งˆ๊ทธ๋„คํŠธ๋ก  ์Šคํผํ„ฐ๋ง ์‹œ ํ•˜์ „๋œ ํ”Œ๋Ÿญ์Šค๋ฅผ ๊ณ ๋ คํ•œ ์••๋ ฅ๊ณผ ๊ธฐํŒ ๋ฐ”์ด์–ด์Šค๊ฐ€ ๋ฐ•๋ง‰ ์ฆ์ฐฉ ๊ฑฐ๋™์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์žฌ๋ฃŒ๊ณตํ•™๋ถ€, 2023. 2. ํ™ฉ๋†๋ฌธ.์ตœ๊ทผ DC ๋ฐ RF ๋งˆ๊ทธ๋„คํŠธ๋ก  ์Šคํผํ„ฐ๋ง ๊ณต์ •์—์„œ ํ•˜์ „๋œ ํ”Œ๋Ÿญ์Šค์˜ ์ƒ์„ฑ๊ณผ ํ•„๋ฆ„ ์ฆ์ฐฉ์— ๋Œ€ํ•œ ํ•˜์ „๋œ ํ”Œ๋Ÿญ์Šค์˜ ์˜ํ–ฅ์ด ์—ฐ๊ตฌ๋˜์—ˆ๋‹ค. ๋”ฐ๋ผ์„œ ํ•˜์ „๋œ ํ”Œ๋Ÿญ์Šค ์ƒ์„ฑ์— ์˜ํ–ฅ์„ ๋ฏธ์น˜๋Š” ์ฆ์ฐฉ ํŒŒ๋ผ๋ฏธํ„ฐ๋ฅผ DC ๋ฐ RF ์Šคํผํ„ฐ๋ง ์‹œ์Šคํ…œ์—์„œ ์—ฐ๊ตฌํ•˜์˜€๋‹ค. ํŠนํžˆ, ํ”Œ๋ผ์ฆˆ๋งˆ๋ฅผ ์ƒ์„ฑํ•˜๊ธฐ ์œ„ํ•ด ์‚ฌ์šฉ๋˜๋Š” ์•„๋ฅด๊ณค(Ar) ์••๋ ฅ๊ณผ ๊ธฐํŒ ๋ฐ”์ด์–ด์Šค ํ•˜์—์„œ์˜ ํ•˜์ „ ๊ฑฐ๋™์„ ์—ฐ๊ตฌํ•˜์˜€๋‹ค. ๋จผ์ €, DC ๋งˆ๊ทธ๋„คํŠธ๋ก  ์Šคํผํ„ฐ๋ง์— ์˜ํ•ด ์ฆ์ฐฉ๋œ ์€(Ag) ๋ฐ•๋ง‰์˜ ์„ฑ์žฅ ์†๋„, ๊ฒฐ์ •๋„ ๋ฐ ๋น„์ €ํ•ญ์— ๋Œ€ํ•œ ์Šคํผํ„ฐ๋ง ํŒŒ์›Œ, ์ž‘๋™ ์••๋ ฅ ๋ฐ ๋ฐ”์ด์–ด์Šค์˜ ์˜ํ–ฅ์„ ์—ฐ๊ตฌํ•˜์˜€๋‹ค. ๋ฐ•๋ง‰์€ 20, 50, 100, 200 W์˜ ์Šคํผํ„ฐ๋ง ํŒŒ์›Œ, 2.5, 5, 10, 20 mTorr์˜ ๊ณต์ • ์••๋ ฅ๊ณผ -300, 0, +300 V์˜ ๊ธฐํŒ ๋ฐ”์ด์–ด์Šค ๊ณต์ • ์กฐ๊ฑด ํ•˜์—์„œ 30๋ถ„ ๋™์•ˆ ์ฆ์ฐฉ๋˜์—ˆ๋‹ค. ๋ชจ๋“  ์Šคํผํ„ฐ๋ง ํŒŒ์›Œ์—์„œ ๋ฐ•๋ง‰์˜ ์„ฑ์žฅ๋ฅ ์€ ์–‘์˜ ๋ฐ”์ด์–ด์Šค์— ์˜ํ•ด ์ฆ๊ฐ€ํ•œ ๋ฐ˜๋ฉด, ์Œ์˜ ๋ฐ”์ด์–ด์Šค์— ์˜ํ•ด ๊ฐ์†Œํ•˜์˜€๋‹ค. ์˜ˆ๋ฅผ ๋“ค์–ด, ์Šคํผํ„ฐ๋ง ํŒŒ์›Œ 100W์™€ ๊ณต์ • ์••๋ ฅ 2.5mTorr์—์„œ, ๋ฐ•๋ง‰์˜ ๋‘๊ป˜๋Š” ๊ฐ๊ฐ -300, 0, +300V์—์„œ 346, 378, 416nm์˜€๋‹ค. ๊ธฐํŒ ๋ฐ”์ด์–ด์Šค ํšจ๊ณผ๋Š” ๊ณต์ • ์••๋ ฅ์ด ๊ฐ์†Œํ•จ์— ๋”ฐ๋ผ ๋‘๋“œ๋Ÿฌ์กŒ๋‹ค. ๋ฐ”์ด์–ด์Šค์— ๋”ฐ๋ฅธ ๋ฐ•๋ง‰์„ฑ์žฅ์†๋„์˜ ๋ณ€ํ™”๋ฅผ ๊ณ ๋ คํ•˜๋ฉด ์Œ์œผ๋กœ ํ•˜์ „๋œ ํ”Œ๋Ÿญ์Šค์˜ ์–‘์€ ๋Œ€๋žต 10%๋กœ ์ถ”์ •๋œ๋‹ค. ๊ณต์ • ์••๋ ฅ์ด ๊ฐ์†Œํ•จ์— ๋”ฐ๋ผ ์ฆ์ฐฉ๋œ ๋ง‰์˜ ๊ฒฐ์ •ํ™”๋„๋Š” ์–‘์˜ ๋ฐ”์ด์–ด์Šค์— ์˜ํ•ด ์ฆ๊ฐ€ํ•œ ๋ฐ˜๋ฉด, ๋„ค๊ฑฐํ‹ฐ๋ธŒ ๋ฐ”์ด์–ด์Šค์— ์˜ํ•ด ๊ฐ์†Œํ•˜์˜€๋‹ค. ๋ฐ•๋ง‰์˜ ์ €ํ•ญ๊ฐ’๋„ ๊ฐ™์€ ๊ฒฝํ–ฅ์„ ๋ณด์˜€๋‹ค. ์€ ํ•„๋ฆ„์˜ ์ฆ์ฐฉ ๊ฑฐ๋™์˜ ์ด๋Ÿฌํ•œ ๋ณ€ํ™”๋Š” ํ•˜์ „๋œ ํ”Œ๋Ÿญ์Šค์˜ ํšจ๊ณผ๋กœ ์ดํ•ดํ•  ์ˆ˜ ์žˆ๋‹ค. ๋˜ํ•œ, RF ๋งˆ๊ทธ๋„คํŠธ๋ก  ์Šคํผํ„ฐ๋ง์— ์˜ํ•ด ์ฆ์ฐฉ๋œ ํ……์Šคํ…(W) ๋ง‰์— ์•„๋ฅด๊ณค ๊ฐ€์Šค ์••๋ ฅ๊ณผ ๊ธฐํŒ ๋ฐ”์ด์–ด์Šค๊ฐ€ ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์„ ์กฐ์‚ฌํ•˜์˜€๋‹ค. ํ……์Šคํ…์€ ์ผ๋ฐ˜์ ์œผ๋กœ ๋ฐ˜๋„์ฒด์šฉ ๊ตฌ๋ฆฌ ๋ฐฐ์„ ์„ ๋Œ€์ฒดํ•˜๋Š” ์žฌ๋ฃŒ๋กœ ์‚ฌ์šฉ๋˜๊ณ  ์žˆ๋‹ค. ์‹ค์˜จ์—์„œ ์Šคํผํ„ฐ๋ง์— ์˜ํ•ด ์ฆ์ฐฉ๋œ ํ……์Šคํ… ๋ฐ•๋ง‰์€ ์ƒ๋Œ€์ ์œผ๋กœ ์ €ํ•ญ์ด ๋†’์€ ์ค€์•ˆ์ • ฮฒ์ƒ์„ ๊ฐ–๊ณ , ํŠน์ • ์กฐ๊ฑด ํ•˜์—์„œ ์ƒ๋Œ€์ ์œผ๋กœ ์ €ํ•ญ์ด ๋‚ฎ์€ ์•ˆ์ •ํ•œ ฮฑ์ƒ์œผ๋กœ ๋ณ€ํ™˜๋˜๋Š” ๊ฒƒ์ด ์ผ๋ฐ˜์ ์œผ๋กœ ๊ด€์ฐฐ๋˜์–ด ์™”๋‹ค. 20 mTorr ๋ฐ -100 V์˜ ๊ธฐํŒ ๋ฐ”์ด์–ด์Šค ํ•˜์—์„œ 1์ดˆ๊ฐ„์˜ ์งง์€ ์ฆ์ฐฉ ์ดˆ๊ธฐ ๋‹จ๊ณ„์—์„œ, ํˆฌ๊ณผ ์ „์ž ํ˜„๋ฏธ๊ฒฝ(TEM)์„ ์‚ฌ์šฉํ•˜์—ฌ ฮฒ์ƒ ํ……์Šคํ…์˜ ๋‚˜๋…ธ ํฌ๊ธฐ์˜ ์ž…์ž๋ฅผ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ๋™์ผํ•œ ์••๋ ฅ ๋ฐ ๋ฐ”์ด์–ด์Šค ์กฐ๊ฑด์—์„œ ์ฆ์ฐฉ ์‹œ๊ฐ„์ด 10๋ถ„์œผ๋กœ ์ฆ๊ฐ€ํ•จ์— ๋”ฐ๋ผ ํ……์Šคํ… ํ•„๋ฆ„์€ ฮฑ์ƒ๊ณผ ฮฒ์ƒ์ด ๊ณต์กดํ•˜์˜€๋‹ค. ฮฑ์ƒ ํ……์Šคํ…์˜ ๋น„์œจ์€ ์Œ์˜ ๋ฐ”์ด์–ด์Šค๊ฐ€ -100์—์„œ -200V๋กœ ์ฆ๊ฐ€ํ•จ์— ๋”ฐ๋ผ ๋” ์ฆ๊ฐ€ํ•˜์˜€๋‹ค. ๋˜ํ•œ ๋ฐ”์ด์–ด์Šค๊ฐ€ +100์—์„œ -100V๋กœ ๋ณ€๊ฒฝ๋จ์— ๋”ฐ๋ผ ํ•„๋ฆ„ ๋ฐ€๋„๊ฐ€ ์ฆ๊ฐ€ํ•˜๊ณ  ํ‘œ๋ฉด ๊ฑฐ์น ๊ธฐ๊ฐ€ ๊ฐ์†Œํ–ˆ๋‹ค. ์ด๋Ÿฌํ•œ ๊ฒฐ๊ณผ๋Š” ์Œ์˜ ๋ฐ”์ด์–ด์Šค๊ฐ€ ฮฒ์ƒ์—์„œ ฮฑ์ƒ์œผ๋กœ ํ……์Šคํ…์˜ ์ƒ์„ ๋ณ€ํ™”์‹œํ‚จ ๊ฒƒ์„ ๋‚˜ํƒ€๋‚ธ๋‹ค. ฮฑ์ƒ ํ……์Šคํ…์˜ ํ˜•์„ฑ๊ณผ ํ•„๋ฆ„์˜ ์ €ํ•ญ๊ฐ’์— ๋Œ€ํ•œ ๋ฐ”์ด์–ด์Šค ํšจ๊ณผ๋Š” ์••๋ ฅ์ด ์ฆ๊ฐ€ํ•จ์— ๋”ฐ๋ผ ๋”์šฑ ๋‘๋“œ๋Ÿฌ์กŒ๋‹ค. ๋˜ํ•œ, DC ์Šคํผํ„ฐ๋ง ์‹œ ์ด์˜จํ™”์œจ์„ ๋†’์ด๊ธฐ ์œ„ํ•ด์„œ DC ๋งˆ๊ทธ๋„คํŠธ๋ก  ์Šคํผํ„ฐ๋ง ์‹œ์Šคํ…œ์— ์œ ๋„ ๊ฒฐํ•ฉ ํ”Œ๋ผ์ฆˆ๋งˆ(ICP)๋ฅผ ์„ค์น˜ํ•˜์˜€๋‹ค. ํ……์Šคํ… ๋ฐ•๋ง‰์€ -200, 0, +200V์˜ ๊ธฐํŒ ๋ฐ”์ด์–ด์Šค ์กฐ๊ฑด์—์„œ ICP ํŒŒ์›Œ๋ฅผ 0์—์„œ 200W๋กœ ์ฆ๊ฐ€์‹œํ‚ค๋ฉด์„œ ์ฆ์ฐฉ๋˜์—ˆ๋‹ค. ICP ํŒŒ์›Œ๊ฐ€ ์ฆ๊ฐ€ํ•˜๊ณ  ๊ธฐํŒ์— ์Œ์˜ ๋ฐ”์ด์–ด์Šค๊ฐ€ ๊ฐ€ํ•ด์งˆ ๋•Œ ฮฑ์ƒ ํ……์Šคํ…์˜ ์„ฑ์žฅ์ด ํ–ฅ์ƒ๋˜๊ณ  ํ……์Šคํ… ๋ง‰์˜ ์ €ํ•ญ์ด ๊ฐ์†Œํ•˜์˜€๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ XRD(X-ray diffraction) ๋ฐ์ดํ„ฐ์™€ ๋น„์ €ํ•ญ ์ธก์ • ๊ฒฐ๊ณผ๋กœ๋ถ€ํ„ฐ ฮฑ์ƒ ํ……์Šคํ…์˜ ์„ฑ์žฅ์„ ์œ„ํ•œ ์ตœ์ ํ™”๋œ ๊ณต์ • ์กฐ๊ฑด์ด ์žˆ์Œ์„ ์•Œ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์ด ์—ฐ๊ตฌ์—์„œ ๊ฐ€์žฅ ๋‚ฎ์€ ์ €ํ•ญ์„ ๊ฐ€์ง€๋Š” ํ……์Šคํ… ๋ฐ•๋ง‰์€ ICP ํŒŒ์›Œ๊ฐ€ 100W์ด๊ณ  ๊ธฐํŒ ๋ฐ”์ด์–ด์Šค๊ฐ€ -200V์ผ ๋•Œ ์–ป์–ด์กŒ๋‹ค.In recent years, the generation of charged flux during direct current (DC) and radio frequency (RF) magnetron sputtering and its effects on film deposition were studied. Thus, the deposition parameter that affects the generation of charged flux was examined in both DC and RF sputtering system. In particular, the charging behavior under the argon (Ar) pressure which is utilizing to generate plasma and the substrate bias were studied. First of all, effects of sputtering power, working pressure, and bias on the growth rate, crystallinity, and resistivity of Ag thin films deposited by DC magnetron sputtering were investigated. Thin films were deposited on the substrate under the electric biases of โˆ’ 300, 0, and + 300 V for 30 minutes with sputtering powers of 20, 50, 100, and 200 W and working pressures of 2.5, 5, 10, and 20 mTorr. Under all sputtering powers, the growth rate of the thin film was increased by the positive bias, whereas it was decreased by the negative bias. For example, the film thicknesses were 345.7, 377.9, and 416.0 nm at โˆ’ 300, 0, and + 300 V, respectively, at a sputtering power of 100 W and a working pressure of 2.5 mTorr. The bias effect was enhanced as the working pressure decreased. Considering the change of the film growth rate according to the bias, the amount of negatively charged flux was estimated to be roughly 10 %. As the working pressure decreased, the crystallinity of the deposited films increased by the positive bias whereas it decreased by the negative bias, which is indicated by the full width at half maximum (FWHM) determined by X-ray diffraction of the Ag (111) peak. The film resistivity had the same tendency. This change in the deposition behavior of the Ag film can be understood as the effect of the charged flux. In addition, effects of Ar pressure and substrate bias on tungsten (W) films deposited by RF magnetron sputtering were investigated. W is generally used as a material to replace copper interconnects for semiconductors. It is commonly observed that tungsten thin films deposited by sputtering at room temperature have a metastable ฮฒ-phase with relatively high resistivity and transform into a stable ฮฑ-phase with relatively low resistivity under certain conditions. In this study, to obtain W films with low resistivity suitable for interconnect materials for semiconductors, we tried to identify deposition parameters for the formation of ฮฑ-phase W by varying the substrate bias and argon (Ar) pressure in an RF magnetron sputtering system. In the initial stage for 1 s of deposition under 20 mTorr and a substrate bias of โ€“100 V, ฮฒ-phase W nanoparticles were observed using transmission electron microscopy (TEM). However, as the deposition time increased to 10 min under the same pressure and bias condition, the W film became a mixture of ฮฑ- and ฮฒ-phases. The fraction of ฮฑ-phase W increased further as the negative bias increased from โ€“100 to โ€“200 V. In addition, the film density increased and the surface roughness decreased as the bias changed from +100 to โ€“100 V. These results indicate that the negative bias triggered the phase transformation of W from ฮฒ to ฮฑ. The bias effect on the formation of ฮฑ-phase W and film resistivity became more pronounced as pressure increased. Furthermore, inductively coupled plasma (ICP) was installed in the DC magnetron sputtering system to increase the ionization rate during DC sputtering. W thin films were deposited at substrate biases of -200, 0, and +200 V with increasing the ICP power from 0 to 200 W. The growth of ฮฑ-phase W was enhanced and the resistivity of W film decreased when the ICP power was increased and a negative bias was applied to the substrate. However, from the X-ray diffraction (XRD) data and resistivity measurement results, it is shown that there are optimized process conditions for growing ฮฑ-phase W. The W thin film with the lowest resistivity in this study was obtained when the ICP power was 100 W and the substrate bias was -200 V.Chapter 1. Introduction 1 1.1. Non-classical crystallization 1 1.1.1. Theory of charged nanoparticles 2 1.1.2. Charge enhanced kinetics 3 1.2. Physical vapor deposition (PVD) 11 1.2.1. Sputter deposition 11 1.2.2. Direct current (DC) sputtering 14 1.2.3. Radio frequency (RF) sputtering 15 1.3. Purpose of this study 18 Chapter 2. Effects of Sputtering Power, Working Pressure, and Electric Bias on the Deposition Behavior of Ag Films during DC Magnetron Sputtering Considering the Generation of Charged Flux 19 2.1. Introduction 19 2.2. Experimental 22 2.3. Result and Discussion 25 2.4. Conclusion 33 Chapter 3. Effects of substrate bias and Ar pressure on growth of ฮฑ-phase in W thin films deposited by RF magnetron sputtering 44 3.1. Introduction 44 3.2. Experimental 46 3.3. Results 48 3.4. Discussion 56 3.5. Conclusion 62 Chapter 4. Effects of ICP power on growth of low-resistivity W thin films deposited by DC magnetron sputtering assisted by ICP 75 4.1. Introduction 75 4.2. Experimental 76 4.3. Result and Discussion 78 4.4. Conclusion 81 Bibliography 88 Abstract in Korean 102๋ฐ•

    Competition of van der Waals and chemical forces on gold-sulfur surfaces and nanoparticles

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    ยฉ 2017 Macmillan Publishers Limited. Chemists generally believe that covalent and ionic bonds form much stronger links between atoms than the van der Waals force does. However, this is not always so. We present cases in which van der Waals dispersive forces introduce new competitive bonding possibilities rather than just modulating traditional bonding scenarios. Although the new possibilities could arise from any soft-soft chemical interaction, we focus on bonding between gold atoms and alkyl or arylsulfur ligands, RS. Consideration of all the interactions at play in sulfur-protected gold surfaces and gold nanoparticles is necessary to understand their structural, chemical and spectroscopic properties. In turn, such knowledge opens pathways to new chemical entities and innovative nanotechnological devices. Such experimentation is complemented by modern theory, and presented here is a broad overview of computational methods appropriate to fields ranging from gas-phase chemistry to device physics and biochemistry

    Kinetic Features of Synthesis of Epoxy Nanocomposites

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    Kinetic features of the formation of epoxy nanocomposites with carbon (nanotubes, graphene, and graphite), metal-containing, and aluminosilicate (montmorillonite and halloysite) fillers are considered. In contrast to linear polymers, epoxy nanocomposites are obtained only via the curing of epoxy oligomers in the presence of filler or the corresponding precursor. These additives may affect the kinetics of the process and the properties of the resulting matrix. A high reactivity of epoxy groups and a thermodynamic miscibility of epoxy oligomers with many substances make it possible to use diverse curing agents and to accomplish curing reactions under various technological conditions. The mutual effect of both a matrix and nanoparticles on the kinetics of the composite formation is discussed

    In-situ TEM์„ ์ด์šฉํ•œ ๊ธฐํŒ์˜ ์ „๋„์„ฑ์— ๋”ฐ๋ฅธ ๊ธˆ์† ์ž… ๊ฑฐ๋™์˜ ๋™์—ญํ•™์  ๋ถ„์„ : ํ•˜์ „ ํšจ๊ณผ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์žฌ๋ฃŒ๊ณตํ•™๋ถ€, 2018. 2. ๊น€๋ฏธ์˜.๋‚˜๋…ธ ๊ตฌ์กฐ์ฒด์˜ ํ˜•์„ฑ์€ ๊ณ ์ „์ ์œผ๋กœ ์›์ž๋‚˜ ์ด์˜จ, ๋ถ„์ž์— ์˜ํ•œ ์†Œ๋ฆฝ์ž์˜ ์ ์ธต์œผ๋กœ ์„ฑ์žฅํ•œ๋‹ค๋Š” ๊ฒƒ์ด ์ผ๋ฐ˜์ ์ธ ๋ฉ”์ปค๋‹ˆ์ฆ˜์œผ๋กœ ๋ฐ›์•„๋“ค์—ฌ์ ธ ์™”๋‹ค. ๋‹ค์–‘ํ•œ ๋ถ„์•ผ์˜ ๋‚˜๋…ธ ๊ตฌ์กฐ์ฒด์˜ ์‘์šฉ์ด ๊ฐ€๋Šฅํ•˜๊ฒŒ ๋œ ์˜ค๋Š˜๋‚  ๋‹ค์–‘ํ•œ ์—ฐ๊ตฌ์—์„œ ๊ณ ์ „์ ์ธ ์„ฑ์žฅ ๋ฉ”์ปค๋‹ˆ์ฆ˜์œผ๋กœ ์„ค๋ช…ํ•  ์ˆ˜ ์—†๋Š” ๊ธฐํ•˜ํ•™์ ์ธ ๊ตฌ์กฐ๋“ค์ด ์ƒ์„ฑ ๋˜๋Š” ํ•ฉ์„ฑ์ด ๋˜๊ณ  ์žˆ๋‹ค. ์ด๋Š” ๋น„ ๊ณ ์ „์  ๊ฒฐ์ • ์„ฑ์žฅ (Non-classical Crystallization)๋กœ ๋ช…๋ช… ๋˜๋Š” ์ƒˆ๋กœ์šด ํ•™๋ฌธ ๋ถ„์•ผ๋กœ์„œ ๋‚˜๋…ธ ๊ตฌ์กฐ์ฒด์˜ ์กฐํ•ฉ์ด ๋‚˜๋…ธ ์ž…์ž ๋‹จ์œ„๋กœ ์ƒ์„ฑ๋œ๋‹ค๋Š” ์ƒˆ๋กœ์šด ์ ‘๊ทผ ๋ฐฉ๋ฒ•์„ ์ œ๊ณตํ•œ๋‹ค. ์ด ์ƒˆ๋กœ์šด ํ•™๋ฌธ ๋ถ„์•ผ์˜ ์ •๋ฆฝ์€ ๋Œ€๋ถ€๋ถ„ ์•ก์ƒ์—์„œ ํ•ฉ์„ฑ๋œ ๋ฌผ์งˆ์„ ๊ด€์ฐฐ ๋ฐ ๋ณด๊ณ ๋ฅผ ํ†ตํ•˜์—ฌ ๋˜๊ณ  ์žˆ์œผ๋‚˜, ์ผ์ฐ์ด ๋ณธ ์‹คํ—˜์‹ค์—์„œ๋Š” ์•ก์ƒ ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ๊ธฐ์ƒ์—์„œ ๋˜ํ•œ ์ด ํ˜„์ƒ์ด ์ผ์–ด๋‚จ์„ ๊ฐ„์ ‘์ ์œผ๋กœ ์ฆ๋ช…ํ•ด์™”๋‹ค. ๋‹ค๋งŒ, ์ด๋ฅผ ํ•ด์„ํ•˜๋Š”๋ฐ ์žˆ์–ด์„œ ๋…์ฐฝ์ ์œผ๋กœ ์ ์šฉ๋˜๋Š” ๊ฒƒ์ด ํ•˜์ „์— ๋Œ€ํ•œ ํšจ๊ณผ๋กœ, ๊ธฐ์ƒ์—์„œ ์ƒ์„ฑ๋˜๋Š” ๋‚˜๋…ธ ์ž…์ž๊ฐ€ ํ•˜์ „์„ ๊ฐ€์งˆ ๋•Œ Liquid-likeํ•œ ์„ฑ์งˆ์„ ๊ฐ€์ ธ ์ด๊ฒƒ์ด ๋‚˜๋…ธ ๊ตฌ์กฐ์ฒด๋ฅผ ํ˜•์„ฑํ•˜๋Š” ๊ธฐ๋ณธ ๋‹จ์œ„๊ฐ€ ๋œ๋‹ค๋Š” ๊ฒƒ์ด ํ•ต์‹ฌ์ด๊ณ , ์ด๊ฒƒ์„ ํ•˜์ „๋œ ๋‚˜๋…ธ ์ž…์ž ์ด๋ก (Theory of Charged Nanoparticle) ๋กœ ๋ช…๋ช…ํ•ด์™”๋‹ค. ์•ž์„  ๋น„ ๊ณ ์ „์  ๊ฒฐ์ • ์„ฑ์žฅ๋ฐฉ๋ฒ•์— ๋Œ€ํ•œ ๋ฉ”์ปค๋‹ˆ์ฆ˜์€ ์•„์ง ๋ช…ํ™•ํ•˜๊ฒŒ ์ •๋ฆฝ๋˜์ง€ ์•Š๋Š” ์˜์—ญ์œผ๋กœ, ๋‹ค๋งŒ, ์ค‘๊ฐ„ ๋‹จ๊ณ„๋Š” Oriented attachment๊ฐ€ ์ผ์–ด๋‚˜๋Š” ๊ฒƒ์€ ์ž˜ ์•Œ๋ ค์ ธ ์žˆ๋‹ค. ์ด๋Ÿฐ ๋‚˜๋…ธ์ž…์ž์— ์˜ํ•œ ์„ฑ์žฅ์˜ ์ฃผ๋„๋‹ˆ ์›๋™๋ ฅ์€ ํ‘œ๋ฉด ์—๋„ˆ์ง€์˜ ๊ฐ์†Œ๋ฅผ ์œ„ํ•œ ๊ฒƒ์œผ๋กœ ์ด๋ฅผ ์˜ˆ์ธกํ•˜๊ธฐ ์œ„ํ•œ ๋‹ค์–‘ํ•œ ๋ชจ๋ธ๋“ค์ด ์ œ์‹œ๋˜๊ณ  ์žˆ๋‹ค. ์ด์— ๋งž์ถฐ ์ œ๊ณต๋˜๋Š” ํ•ต์‹ฌ ์ฆ๊ฑฐ๋Š” ์ง์ ‘์ ์ธ ์œก์•ˆ ๊ด€์ฐฐ์ด ๊ฐ€๋Šฅํ•œ ํˆฌ๊ณผ์ „์žํ˜„๋ฏธ๊ฒฝ(TEM)์„ ์ด์šฉํ•œ ์‹ค์‹œ๊ฐ„ ๊ด€์ฐฐ์„ ํ†ตํ•˜์—ฌ ๋‹ค์–‘ํ•œ ์ฃผ์žฅ๋“ค์ด ์ œ๊ธฐ๋˜๊ณ  ์žˆ๋‹ค. ๋…ผ์˜ ๋˜๊ณ  ์žˆ๋Š” ๋‹ค์–‘ํ•œ ๋ฉ”์ปค๋‹ˆ์ฆ˜ ์†์—์„œ ํˆฌ๊ณผ์ „์žํ˜„๋ฏธ๊ฒฝ์„ ์‚ฌ์šฉํ–ˆ์„ ๋•Œ์— ๋†’์€ ์—๋„ˆ์ง€๋ฅผ ๊ฐ€์ง€๋Š” ๊ฐ€์†๋œ ์ „์ž์— ์˜ํ•œ ํƒ€์ผ“ ๋ฌผ์งˆ๊ณผ์˜ ์ƒํ˜ธ ์ž‘์šฉ์—์„œ ๋ฐœ์ƒํ•  ์ˆ˜ ์žˆ๋Š” ํ•˜์ „์˜ ์˜ํ–ฅ์„ ๊ฐ„๊ณผํ•˜๊ณ  ์žˆ๋Š”๋ฐ”, ๋ณธ ํ•™์œ„๋…ผ๋ฌธ์—์„œ๋Š” ํ•˜์ „์— ์ดˆ์ ์„ ๋‘๊ณ  ์ด๊ฒƒ์ด ์‹œ์Šคํ…œ ๋‚ด์— ์กด์žฌํ–ˆ์„ ๋•Œ ๋‚˜๋…ธ ๊ตฌ์กฐ์ฒด์— ์–ด๋– ํ•œ ์˜ํ–ฅ์„ ๋ฏธ์น˜๋Š”์ง€์— ๋Œ€ํ•ด์„œ ์ฒด๊ณ„์ ์ธ ์‹คํ—˜์„ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ์ผ์ฐจ์ ์œผ๋กœ ํƒ€์ผ“์œผ๋กœ ์‚ผ์€ ๊ธˆ ์ž…์ž๋ฅผ ๊ธฐํŒ์˜ ์ „๋„์„ฑ์— ๋”ฐ๋ผ ์ž…์ž์˜ ๊ฑฐ๋™ ์ฐจ์ด๋ฅผ ํ™•์ธํ•˜์˜€๋‹ค. ์ธ์œ„์ ์œผ๋กœ ํ•˜์ „์„ ๋ ๊ณ  ์žˆ๋Š” ๋น„ ์ „๋„์„ฑ ๊ธฐํŒ ์œ„์—์„œ์˜ ๊ธˆ ์ž…์ž๋Š” ๋งค์šฐ ๋ถˆ์•ˆ์ •ํ•œ ๊ฑฐ๋™์„ ๋ ๊ณ  ์žˆ์Œ์„ ํ™•์ธํ•˜์˜€์œผ๋‚˜ ๋Œ€์กฐ๊ตฐ์ธ ์ „๋„์„ฑ ๊ธฐํŒ์—์„œ๋Š” ๊ธด ์‹œ๊ฐ„๋™์•ˆ์—๋„ ์•ˆ์ •์ ์ธ ํ˜•ํƒœ๋ฅผ ๋ฐ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ด์— ๋”ํ•ด, ๋น„ ์ „๋„์„ฑ ๊ธฐํŒ ์œ„์˜ ๊ธˆ ์ž…์ž๊ฐ€ ๊ธฐํŒ์—์„œ ํƒˆ๋ฝ๋จ์„ ํ†ตํ•˜์—ฌ ์ฒ™๋ ฅ, ์ฆ‰ ์ •์ „๊ธฐ์  ๋ฐ˜๋ฐœ๋ ฅ์ด ์ž…์ž์™€ ๊ธฐํŒ ์‚ฌ์ด์— ์ž‘์šฉํ•˜๋Š” ๊ฒƒ์ด ๊ด€์ฐฐ๋จ์— ๋”ฐ๋ผ ์‹œ์Šคํ…œ ๋‚ด ์ž…์ž์— ํ•˜์ „์„ ์ธ์œ„์ ์œผ๋กœ ๊ตฌํ˜„ํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์ด์— ๋” ๋‚˜์•„๊ฐ€ ํ•˜์ „ ์œ ๋ฌด์— ๋”ฐ๋ฅธ ๋‚˜๋…ธ ์ž…์ž๋“ค๊ฐ„์˜ ์ƒ๊ด€๊ด€๊ณ„๋ฅผ 2๊ฐœ ์ด์ƒ์˜ ์ž…์ž๊ฐ€ ์กด์žฌํ•˜์˜€์„ ๋•Œ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ๋‚˜๋…ธ ์ž…์ž์˜ ํ‘œ๋ฉด ์—๋„ˆ์ง€๋ฅผ ์ค„์ด๊ธฐ ์œ„ํ•œ ๋ฐฉ๋ฒ• ์ค‘ ํ•˜๋‚˜์ธ coalescence๊ฐ€ ์ผ์–ด๋‚˜๋Š” ์‹œ์Šคํ…œ ๋‚ด์—์„œ, ํ•˜์ „์ด ์กด์žฌํ•  ๋•Œ ์•ฝ 15๋ฐฐ ์ •๋„์˜ ์‹œ๊ฐ„์ ์ธ ๋น ๋ฅด๊ธฐ๋ฅผ ๊ฐ€์ง€๊ณ  ์ด ๋ฉ”์ปค๋‹ˆ์ฆ˜์ด ์ž‘์šฉํ•จ์„ ํ™•์ธํ•จ์— ๋”ฐ๋ผ ๋‚˜๋…ธ ๊ตฌ์กฐ์ฒด๋ฅผ ํ˜•์„ฑํ•˜๋Š”๋ฐ ์žˆ์–ด์„œ ํ•˜์ „์€ ๋‚˜๋…ธ ์ž…์ž์˜ ๋ถˆ์•ˆ์ •์„ฑ์„ ์•ผ๊ธฐ ์‹œํ‚ด๊ณผ ๋™์‹œ์— ๋™์—ญํ•™์ ์ธ ์žฅ๋ฒฝ์„ ๋‚ฎ์ถ”๋Š” ํšจ๊ณผ๊นŒ์ง€ ๊ฐ€์ง์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ ์ด๋Ÿฌํ•œ ๊ด€์ฐฐ์„ TEM์„ ์ด์šฉํ•˜์—ฌ ์ง„ํ–‰ํ•  ๋•Œ์— ์ œ๊ธฐ๋  ์ˆ˜ ์žˆ๋Š” ์˜จ๋„ ์ƒ์Šน, Hydrocarbon ์˜ค์—ผ, ๋‹ค์–‘ํ•œ ๊ธฐํŒ์„ ์‚ฌ์šฉํ•จ์— ๋”ฐ๋ฅธ ํƒ€์ผ“ ๋ฌผ์งˆ์ด ์ฒ˜ํ•œ ํ™˜๊ฒฝ์  ์ฐจ์ด์— ๋”ฐ๋ฅธ ๋…ผ๋ž€์„ ํ•ด๊ฒฐํ•˜๋Š”๋ฐ ์ค‘์ ์„ ๋‘์—ˆ๋‹ค. ์˜จ๋„ ์ƒ์Šน์€ ๊ด€์ฐฐํ•˜๋Š” ํ™˜๊ฒฝ์˜ ์ „์ฒด์ ์ธ ์˜จ๋„๋ฅผ ์•ก์ฒด ์งˆ์†Œ ์˜จ๋„ ๊นŒ์ง€ ๋‚ด๋ฆผ์œผ๋กœ์„œ ํ™œ์„ฑ ์žฅ๋ฒฝ์„ ๋†’์˜€์Œ์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ  coalescence๊ฐ€ ์ผ์–ด๋‚˜ ์ด ๊ฒƒ์— ๋Œ€ํ•œ ์˜จ๋„ ์˜ํ–ฅ์„ ๋ฐฐ์ œํ•˜๋ ค๊ณ  ํ•˜์˜€๊ณ , ์ „๋„์„ฑ๊ณผ ๋น„์ „๋„์„ฑ ๋ฌผ์งˆ์˜ ๊ด€์ฐฐ๊ฐ„ ๋ฐœ์ƒํ•˜๋Š” ์‹œ๊ฐ„์ ์ธ ๊ฐ„๊ทน์— ๋”ฐ๋ฅธ TEM์˜ ํ™˜๊ฒฝ๊ณผ ์ƒ˜ํ”Œ์˜ ๋ณ€ํ™”๋ฅผ ๋ฐฐ์ œ ํ•˜๊ธฐ ์œ„ํ•˜์—ฌ ์ด๋ฅผ ํ•˜๋‚˜์˜ TEM Grid ์œ„์— ํ•˜์ „์ด ์กด์žฌํ•  ์ˆ˜ ์žˆ๋Š” ํ™˜๊ฒฝ๊ณผ ์กด์žฌํ•  ์ˆ˜ ์—†๋Š” ํ™˜๊ฒฝ์„ ํ•œ ๋ฒˆ์— ๊ตฌํ˜„ํ•จ์œผ๋กœ์„œ ํ•ด๊ฒฐํ•˜๊ณ ์ž ํ•˜์˜€๋‹ค. ๋™์ผํ•œ ๋ฌผ์งˆ์„ ์‚ฌ์šฉํ•œ Floating & Ground ์‹œ์Šคํ…œ์€ ๋ช…ํ™•ํ•˜๊ฒŒ ํ•˜์ „๋งŒ ๋ณ€์ˆ˜๋กœ ์‚ผ์„ ์ˆ˜ ์žˆ๋Š” ํ™˜๊ฒฝ์„ ์ œ๊ณตํ•˜์˜€์œผ๋ฉฐ, ๊ด€์ฐฐ ์ „ ํ›„์˜ ๋ช…ํ™•ํ•œ ์ฐจ์ด๋ฅผ ํ†ตํ•˜์—ฌ ๋‚˜๋…ธ ๊ตฌ์กฐ์ฒด๋ฅผ ํ˜•์„ฑํ•˜๋Š” ํ™˜๊ฒฝ ๋‚ด์—์„œ ํ•˜์ „์ด ์ค‘์š”๋ณ€์ˆ˜๋กœ ์ž‘์šฉํ•  ์ˆ˜ ์žˆ์Œ์„ ๋ณด์˜€๋‹ค. ๋˜ํ•œ, ์ด๋ฅผ ์€ ์ž…์ž์— ์ ์šฉํ•จ์œผ๋กœ์„œ ๊ธˆ ์ž…์ž๋กœ ๊ตฌ์„ฑ๋œ ์•ž์˜ ์‹คํ—˜์„ ๋„˜์–ด ํ•˜์ „ ํšจ๊ณผ๋ฅผ ๋‹ค๋ฅธ ๋ฌผ์งˆ๋กœ ์ ์šฉํ•˜์—ฌ ์ผ๋ฐ˜ํ™” ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ์ž‘์€ ๋‹จ์„œ๋ฅผ ๊ฐ™์ด ์ œ๊ณตํ•˜์˜€๋‹ค.Non-classical crystallization is a remarkable phenomenon in the nanostructure fabrication, which suggests that nanoparticle is the smallest unit as building block in crystal growth. In-situ transmission electron microscopy (in-situ TEM) provides crucial clues in understanding its mechanism. However, many mechanisms still remain unclear, especially the lack of understanding the charge effect caused by inelastic collision of the electron beam with sample in TEM. Here, we report that the structural instability and coalescence are promoted by charging through real-time observation of Au particles on substrates with difference conductivity. From a kinetic point view, this difference implies that the charge enhanced diffusion. This investigation broadens current knowledge of non-classical crystallization that grows by nanoparticles, sheds light on a potential factor to control the nanostructure fabrication. In this thesis, I carefully pay attention to the charge effect caused by the interaction between injected electron beam with high energy and sample during real-time TEM observation. In order to clarify the effect of charging in TEM, first, we clearly reproduced the difference in structure stability of a nanoparticle according to the substrate conductivity. Furthermore, the coalescence of multi-particles according to the degree of activation by charge was confirmed from the viewpoint of dynamics. Finally, we attempted to exclude various interpretations occurring within in-situ TEM by constructing a well-established artificial charging systemCh. 1 Introduction 1 1.1 Non-classical Crystallization 2 1.2 In-situ TEM Observation of Non-classical crystallization 9 1.3 Theory of Charged Nanoparticle 12 1.4 Charged Particle in Transmission Electron Microscope (TEM) 19 Ch. 2 An isolated Nanoparticle Observation 25 2.1 Structure instability of Nanoparticle 25 2.2 Experiment 27 2.3 Result & Discussion 31 2.4 Conclusion 41 Ch. 3 Two or more Nanoparticles Observation 43 3.1 Aggregation and Coalescence of Nanoparticles 44 3.2 Experiment 48 3.3 Result & Discussion 52 3.4 Conclusion 60 Ch. 4 Artificial current path systems : Floating & Ground environment formed simultaneously in a TEM grid 61 4.1 Controversy over the observation of charged nanoparticles using in-situ TEM 62 4.2 Experiment 65 4.3 Result & discussion 69 4.4 Behavior of Ag Nanoparticles in Floating & Ground systems 79 4.5 Conclusion 81 Ch.5 Summary 82 Reference 85 ๊ตญ๋ฌธ ์ดˆ๋ก 91Docto

    Proceedings of the Flat-Plate Solar Array Project Research Forum on Photovoltaic Metallization Systems

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    A photovoltaic Metallization Research forum, under the sponsorship of the Flat-Plate Solar Array Project consisted of five sessions, covering: (1) the current status of metallization systems, (2) system design, (3) thick-film metallization, (4) advanced techniques, and (5) future metallization challenges

    Non-classical crystallization of Al2O3 films by positively charged nanoparticles during aerosol deposition

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์žฌ๋ฃŒ๊ณตํ•™๋ถ€(ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์žฌ๋ฃŒ), 2022. 8. ํ™ฉ๋†๋ฌธ.Thin film growth through non-classical crystallization with a building block of charged nanoparticles (CNPs) has been studied in several fields, including chemical vapor deposition (CVD) and physical vapor deposition (PVD). To determine whether the same mechanism can be applied for aerosol deposition (AD) at room temperature, the generation and deposition behavior of CNPs were studied in the AD process for the first time. By measuring the current and examining the bias effect on the deposition behavior, it was confirmed that the fragmentation of Al2O3 particles generated numerous positively charged secondary nanoparticles as well as electrons by fracto-emission. In this work, the secondary particles passing between the two parallel biased and grounded electrodes were captured by the TEM grid membrane on each electrode, and it was revealed that they were mainly positively charged. Neutral secondary nanoparticles, not deflected by the electric field, produced a porous film on the silicon substrate, whereas charged secondary nanoparticles produced a dense film. The excess positive charging effects on the stacking fault energies of main slip systems were examined by density functional theory (DFT) calculations. When the electrons were removed, the activation barriers to create the stacking fault were decreased. The hypothesis that positive charges induce plastic deformation of secondary particles was supported by experiments and ab initio calculations. These results suggest that the positively charged secondary particles may be a major flux for film growth in the AD process. Combining the results, an aerosol deposition mechanism considering the charging effect was proposed.ํ•˜์ „ ๋œ ๋‚˜๋…ธ ์ž…์ž (CNPs)๋ฅผ ๋นŒ๋”ฉ ๋ธ”๋ก์œผ๋กœ ๋ฐ•๋ง‰์ด ์„ฑ์žฅํ•œ๋‹ค๋Š” ๋น„๊ณ ์ „์  ๊ฒฐ์ •ํ™” ์ด๋ก ์€ ํ™”ํ•™ ๊ธฐ์ƒ ์ฆ์ฐฉ๋ฒ• (CVD) ์™€ ๋ฌผ๋ฆฌ ๊ธฐ์ƒ ์ฆ์ฐฉ๋ฒ• (PVD)์„ ๋น„๋กฏํ•œ ๋‹ค์–‘ํ•œ ๋ถ„์•ผ์—์„œ ์—ฐ๊ตฌ๋˜๊ณ  ์žˆ๋‹ค. ์ƒ์˜จ์—์„œ ์น˜๋ฐ€ํ•œ ์„ธ๋ผ๋ฏน ๋ฐ•๋ง‰์„ ํ˜•์„ฑํ•˜๋Š” ์—์–ด๋กœ์กธ ์ฆ์ฐฉ (AD) ๊ณต์ •์€ ์•„์ง ๊ทธ ๋ฉ”์ปค๋‹ˆ์ฆ˜์ด ๋ช…ํ™•ํ•˜๊ฒŒ ์ดํ•ด๋˜์ง€ ์•Š์•˜์œผ๋ฉฐ, ์—์–ด๋กœ์กธ ์ฆ์ฐฉ ๊ณต์ •์„ ๋น„๊ณ ์ „์  ๊ฒฐ์ •ํ™” ์ด๋ก ์œผ๋กœ ์„ค๋ช…ํ•˜๊ธฐ ์œ„ํ•ด ํ•˜์ „ ๋œ ๋‚˜๋…ธ ์ž…์ž์˜ ์ƒ์„ฑ๊ณผ ์ฆ์ฐฉ ๊ฑฐ๋™์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋ฅผ ํ•˜์˜€๋‹ค. ์ „๋ฅ˜์ธก์ •๊ณผ ๋ฐ”์ด์–ด์Šค์— ์˜ํ•œ ์ฆ์ฐฉ ๊ฑฐ๋™ ๋น„๊ต๋ฅผ ํ†ตํ•ด ์—์–ด๋กœ์กธ ์ฆ์ฐฉ ๊ณต์ •์—์„œ ์‚ฐํ™”์•Œ๋ฃจ๋ฏธ๋Š„ ์ž…์ž์˜ ํŒŒ๋‹จ์ด ๋งŽ์€ ์–‘์˜ ์ „์ž๋ฅผ ๋ฐฉ์ถœํ•˜๋ฉฐ ์–‘์œผ๋กœ ํ•˜์ „ ๋œ ์ด์ฐจ ๋‚˜๋…ธ ์ž…์ž ๋“ค์„ ์ƒ์„ฑํ•˜๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์ „๊ธฐ์žฅ ์˜์—ญ์„ ํ†ต๊ณผํ•˜๋Š” ์ด์ฐจ ๋‚˜๋…ธ ์ž…์ž๋“ค์„ ๊ฐ ์ „๊ทน์—์„œ ์ „์žํ˜„๋ฏธ๊ฒฝ (TEM) ๊ทธ๋ฆฌ๋“œ์˜ ๋ฉค๋ธŒ๋ ˆ์ธ์— ํฌ์ง‘ํ•˜์—ฌ ์ด์ฐจ ๋‚˜๋…ธ ์ž…์ž๋“ค์ด ์ฃผ๋กœ ์–‘์œผ๋กœ ํ•˜์ „ ๋˜์–ด ์žˆ์Œ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ „๊ธฐ์žฅ์„ ์ด์šฉํ•ด ํ•˜์ „ ์ž…์ž์˜ ์–‘์„ ์ œ์–ดํ–ˆ์„ ๊ฒฝ์šฐ, ์–‘์œผ๋กœ ํ•˜์ „ ๋œ ์ด์ฐจ ๋‚˜๋…ธ ์ž…์ž๋“ค์€ ์‹ค๋ฆฌ์ฝ˜ ๊ธฐํŒ์— ์น˜๋ฐ€ํ•œ ๋ง‰์„ ํ˜•์„ฑํ•œ ๋ฐ˜๋ฉด ์ค‘์„ฑ ์ด์ฐจ ๋‚˜๋…ธ ์ž…์ž๋“ค์€ ๋‹ค๊ณต์„ฑ ๋ง‰์„ ํ˜•์„ฑํ•˜์˜€๋‹ค. ๋ฐ€๋„๋ฒ”ํ•จ์ˆ˜ ์ด๋ก ์œผ๋กœ ์‚ฐํ™”์•Œ๋ฃจ๋ฏธ๋Š„์˜ ์ฃผ์š” ์Šฌ๋ฆฝ ์‹œ์Šคํ…œ์— ๋Œ€ํ•œ ์–‘์ „ํ•˜์˜ ํšจ๊ณผ๋ฅผ ๊ณ„์‚ฐํ•œ ๊ฒฐ๊ณผ ์–‘์ „ํ•˜ ์ฆ๊ฐ€์— ๋”ฐ๋ผ ์ ์ธต ๊ฒฐํ•จ ํ˜•์„ฑ์˜ ์—๋„ˆ์ง€ ์žฅ๋ฒฝ์ด ๊ฐ์†Œํ•˜๋Š” ๊ฒฝํ–ฅ์ด ์žˆ์—ˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์‹คํ—˜๊ณผ ๊ณ„์‚ฐ์„ ํ†ตํ•ด ์—์–ด๋กœ์กธ ์ฆ์ฐฉ ๊ณต์ •์—์„œ ์–‘์ „ํ•˜๊ฐ€ ์ด์ฐจ์ž…์ž์˜ ์†Œ์„ฑ๋ณ€ํ˜•์„ ์œ ๋„ํ•œ๋‹ค๋Š” ๊ฐ€์„ค์„ ๋’ท๋ฐ›์นจํ•˜๊ณ  ๋น„๊ณ ์ „์  ๊ฒฐ์ •ํ™” ์ด๋ก ์„ ํ†ตํ•ด ์—์–ด๋กœ์กธ ์ฆ์ฐฉ ๊ณต์ •์˜ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ์ œ์‹œํ•˜์˜€๋‹ค.Chapter 1. Introduction 1 1.1 Non-classical crystallization 2 1.2 Aerosol deposition 7 Chapter 2. Generation of electrons and positively charged secondary nanoparticles by fracto-emission 10 2.1 Introduction 11 2.2 Experimental method 13 2.3 Results and discussion 17 2.4 Conclusion 36 Chapter 3. Deposition behavior of secondary nanoparticles with and without positive charge 37 3.1 Introduction 38 3.2 Experimental method 40 3.3 Results and discussion 43 3.4 Conclusion 53 Chapter 4. Positive charge effect on plastic deformation of Al2O3 (ab-initio calculation) 54 4.1 Introduction 55 4.2 Computational method 56 4.3 Results and discussion 59 4.4 Conclusion 66 Chapter 5. Effect of discharge on optical and mechanical properties of Al2O3 films 67 5.1 Introduction 68 5.2 Experimental method 70 5.3 Results and discussion 72 5.4 Conclusion 84 Chapter 6. Aerosol deposition mechanism of Al2O3 films 85 Referernces 92 Abstract in Korean 103๋ฐ•

    High humidity fabrication of rGO incorporated perovskite absorber and MoS2 electrode for prospective inverted PSC

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    Methylammonium lead triiodide (MAPbI3) is a perovskite material that is widely used in perovskite solar cells due to its potential for high power conversion efficiency. However, it is sensitive to humid environments, heat, oxygen and UV radiation, which can cause it to degrade and negatively affect crystal growth and the morphology of the material. This can ultimately affect the efficiency of the solar cell. Therefore, MAPbI3 is typically produced at a low humidity, which requires expensive equipment. The aim of this research study is to propose a facile fabrication process for fully solution-processable inverted perovskite solar cells employing reduced graphene oxide (rGO)-based material under high humidity conditions suitable for the weather in Malaysia. Overall, the research design was divided into three phases. The aim of phase 1 is to study the influence of incorporating sulfonated rGO (srGO) into the MAPbI3 absorber layer for the deposition of a high-quality thin film under open-air conditions with high relative humidity. Three different samples were prepared with different weight percentage (wt%) of srGO: 0% (T), 50% (TS B) and 15% (TS D). The morphology of the srGO-MAPbI3 films was improved by the addition of srGO, resulting in fewer defects and larger perovskite grain sizes approaching micron size. In phase 2, the study aimed to determine the optimal process parameter of molybdenum disulfide (MoS2) composite with rGO as a viable solution-processed top electrode for an effective electron-collecting electrode by taking advantage of Taguchi analysis. The results of the Taguchi analysis showed that a ratio of rGO:MoS2 (1:1), a heating temperature of 75ยฐC, and a heating period of 15 minutes were the optimal parameters for the electrode manufacturing process. The discovered optimal parameters were deployed to fabricate rGO:MoS2 composite electrode that showed a promising electrical conductivity of 9.36 ฮฉ/sq. In phase 3, the device performance of the inverted perovskite solar cells with the designated configuration of ITO/CuSCN/srGO-MAPbI3/PCBM/BCP/rGO-MoS2 was analyzed by numerical simulation with SCAPS-1D. The results proved that the device performance for the samples was affected by the addition of srGO to the absorber layer. The 15% srGO sample exhibited the highest PCE of 10.37% with Ag as the top electrode. However, when the conventional electrode was replaced with a rGO-MoS2 composite electrode, the PCE of the same sample was improved to 13.23%, with a significant increase in FF. In summary, the findings of this research study indicate that incorporation of srGO into the MAPbI3 absorber layer can improve the morphology of the srGO-MAPbI3 films, resulting in fewer defects and larger perovskite grain sizes. The study also provides insight into the use of rGOMoS2 composite material as a workable solution-processed top electrode for an effective electron-collecting electrode, particularly in inverted configuration of perovskite solar cells. The numerical simulation results showed that the device performance of the samples could be improved by replacing Ag with rGO-MoS2. The findings of this study could have significant implications for the growth of cost-effective, solution-processed perovskite solar cells under high relative humidity

    Biomolecule Mediating Synthesis Of Inorganic Nanoparticles And Their Applications

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    Project 1. The conventional phage display technique focuses on screening peptide sequences that can bind on target substrates, however the selected peptides are not necessary to nucleate and mediate the growth of the target inorganic crystals, and in many cases they only show moderate affinity to the targets. Here we report a novel phage display approach that can directly screen peptides catalytically growing inorganic nanoparticles in aqueous solution at room temperature. In this study, the phage library is incubated with zinc precursor at room temperature. Among random peptide sequences displayed on phages, those phages that can grow zinc oxide (ZnO) nanoparticles are selected with centrifugation. After several rounds of selection, the peptide sequences displayed on the phage viruses are analyzed by DNA sequencing. Our screening protocol provide a simple and convenient route for the discovery of catalytic peptides that can grow inorganic nanoparticles at room temperature. This novel screening protocol can extend the method on finding a wide range of new catalysts. Project 2. Genetically engineered collagen peptides are assembled into freestanding films when quantum dots (QDs) are co-assembled as joints between collagen domains. These peptide-based films show excellent mechanical properties with Young\u27s modulus of ~20 GPa, much larger than most of the multi-composite polymer films and previously reported freestanding nanoparticle-assembled sheets, and it is even close to that reported for the bone tissue in nature. These films show little permanent deformation under small indentation while the mechanical hysteresis becomes remarkable when the load approaches near and beyond the rupture point, which is also characteristic of the bone tissue. Project 3. The shape-controlled synthesis of nanoparticles have been established in single-phase solutions by controlling growth directions of crystalline facets on seed nanocrystals kinetically; however, it is difficult to rationally predict and design nanoparticle shapes. Here we introduce a methodology to fabricate nanoparticles in smaller sizes by evolving shapes thermodynamically. This strategy enables a more rational approach to fabricate shaped nanoparticles by etching specific positions of atoms on facets of seed nanocrystals in reverse micelle reactors where the surface energy gradient induces desorption of atoms on specific locations on the seed surfaces. From seeds of 12 nm palladium nanocubes, the shape is evolved to concave nanocubes and finally hollow nanocages in the size ~10 nm by etching the center of {200} facets. The high surface area-to-volume ratio and the exposure of a large number of palladium atoms on ledge and kink sites of hollow nanocages are advantageous to enhance catalytic activity and recyclability

    In situ XAFS Study of Palladium Electrodeposition at the Liquid/Liquid Interface

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    We report the use of XAFS (X-ray absorption fine structure) as an in situ method to follow the electrochemically driven deposition of palladium nanoparticles at a liquid/liquid interface. A novel glass/plastic hybrid electrochemical cell was used to enable control of the potential applied to the liquid/liquid interface. In situ measurements indicate that the nucleation of metallic nanoparticles can be triggered through chronoamperometry or cyclic voltammetry. In contrast to spontaneous nucleation at the liquid/liquid interface, whereby fluctuations in Pd oxidation state and concentration are observed, under a fixed interfacial potential the growth process occurs at a steady rate leading to a build-up of palladium at the interface. Raman spectroscopy of the deposit suggests that the organic electrolyte binds directly to the surface of the deposited nanoparticles. It was found that the introduction of citric acid results in the formation of spherical nanoparticles at the interface
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