133 research outputs found

    Ataxin-1 occupies the promoter region of E-cadherin in vivo and activates CtBP2-repressed promoter

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    AbstractAtaxin-1 is a polyglutamine protein of unknown function that is encoded by the ATXN1 gene in humans. To gain insight into the function of ataxin-1, we sought to identify proteins that interact with ataxin-1 through yeast two-hybrid screening. In this study, transcriptional corepressor CtBP2 was identified as a protein that interacted with ataxin-1. CtBP2 and ataxin-1 colocalized in the nucleus of mammalian cells. Since the E-cadherin promoter is a target of CtBP-mediated repression, the relationship between ataxin-1 and the E-cadherin promoter was investigated. Chromatin immunoprecipitation assays showed that CtBP2 and ataxin-1 were recruited to the E-cadherin promoter in mammalian cells. Luciferase assays using E-cadherin promoter reporter constructs revealed that the luciferase activity was enhanced as the level of ataxin-1 protein expression increased. CtBP2 overexpression decreased E-cadherin expression, but expression of ataxin-1 inversely increased the mRNA and protein levels of endogenous E-cadherin. Interestingly, siRNA experiments showed that the transcriptional activation of ataxin-1 was associated with the presence of CtBP2. This study demonstrates that ataxin-1 occupies the promoter region of E-cadherin in vivo and that ataxin-1 activates the promoter in a CtBP2-mediated transcriptional regulation manner

    A Unified Compression Framework for Efficient Speech-Driven Talking-Face Generation

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    Virtual humans have gained considerable attention in numerous industries, e.g., entertainment and e-commerce. As a core technology, synthesizing photorealistic face frames from target speech and facial identity has been actively studied with generative adversarial networks. Despite remarkable results of modern talking-face generation models, they often entail high computational burdens, which limit their efficient deployment. This study aims to develop a lightweight model for speech-driven talking-face synthesis. We build a compact generator by removing the residual blocks and reducing the channel width from Wav2Lip, a popular talking-face generator. We also present a knowledge distillation scheme to stably yet effectively train the small-capacity generator without adversarial learning. We reduce the number of parameters and MACs by 28ร—\times while retaining the performance of the original model. Moreover, to alleviate a severe performance drop when converting the whole generator to INT8 precision, we adopt a selective quantization method that uses FP16 for the quantization-sensitive layers and INT8 for the other layers. Using this mixed precision, we achieve up to a 19ร—\times speedup on edge GPUs without noticeably compromising the generation quality.Comment: MLSys Workshop on On-Device Intelligence, 2023; Demo: https://huggingface.co/spaces/nota-ai/compressed_wav2li

    ์‹ค์‹œ๊ฐ„ ๊ฐ€์—ด ๋ฐ ์•ก์ƒ ํˆฌ๊ณผ์ „์žํ˜„๋ฏธ๊ฒฝ ๊ธฐ๋ฒ•์„ ํ†ตํ•œ ์ด‰๋งค ๋‚˜๋…ธ์ž…์ž์˜ ๊ตฌ์กฐ ๋ณ€ํ™” ๋ฐ ํ™•์‚ฐ ๊ณผ์ •

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€, 2024. 2. ๋ฐ•์ •์›.์ตœ๊ทผ ์ˆ˜์‹ญ ๋…„ ๋™์•ˆ ๋‚˜๋…ธ ์ž…์ž๋Š” ๋‹ค์–‘ํ•œ ๊ณผํ•™ ๋ถ„์•ผ์™€ ์‘์šฉ ๋ถ„์•ผ์—์„œ ์ค‘์š”ํ•œ ๊ตฌ์„ฑ ์š”์†Œ๊ฐ€ ๋˜์—ˆ๋‹ค. ์ด๋Ÿฌํ•œ ์‘์šฉ ๋ถ„์•ผ ์ค‘ ์ด์ข… ์ด‰๋งค๋Š” ์ž‘์€ ํฌ๊ธฐ์˜ ๋…ํŠนํ•œ ํŠน์„ฑ๊ณผ ๊ธˆ์† ์ข…์˜ ๋ถ„์‚ฐ์„ ๊ทน๋Œ€ํ™”ํ•  ์ˆ˜ ์žˆ๋Š” ๋Šฅ๋ ฅ์œผ๋กœ ์ธํ•ด ๋‚˜๋…ธ ์ž…์ž๊ฐ€ ์‚ฌ์šฉ๋˜๋Š” ๊ฐ€์žฅ ์ค‘์š”ํ•œ ๋ถ„์•ผ ์ค‘ ํ•˜๋‚˜์ด๋‹ค. ์›ํ•˜๋Š” ๊ตฌ์กฐ์™€ ํŠน์„ฑ์„ ๊ฐ€์ง„ ์ด‰๋งค ๋‚˜๋…ธ์ž…์ž๋ฅผ ์„ค๊ณ„ํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ๋‚˜๋…ธ์ž…์ž์˜ ์›์ž ๊ตฌ์กฐ์™€ ์—ด์ฒ˜๋ฆฌ ๋ฐ ์•ก์ฒด์™€ ๊ฐ™์€ ๋ฐ˜์‘ ์กฐ๊ฑด์—์„œ์˜ ๊ตฌ์กฐ์  ๋ณ€ํ™”์— ๋Œ€ํ•œ ์ดํ•ด๊ฐ€ ํ•„์š”ํ•˜๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ์ด‰๋งค ๋‚˜๋…ธ์ž…์ž์˜ ๊ตฌ์กฐ์  ๋ณ€ํ™”๋Š” ์ด๋Ÿฌํ•œ ํ™”ํ•™์  ํ™˜๊ฒฝ์—์„œ ๊ฐœ๋ณ„ ๋‚˜๋…ธ์ž…์ž๋ฅผ ์›์ž ๋‹จ์œ„๋กœ ์ง์ ‘ ๊ด€์ฐฐํ•˜๋Š” ๊ฒƒ์ด ์–ด๋ ต๊ธฐ ๋•Œ๋ฌธ์— ์ดํ•ดํ•˜๊ธฐ ์–ด๋ ต๋‹ค. ์‹ค์‹œ๊ฐ„ ํˆฌ๊ณผ์ „์žํ˜„๋ฏธ๊ฒฝ(TEM)์€ ๋ฐ˜์‘ ์กฐ๊ฑด์—์„œ ๊ฐœ๋ณ„ ๋‚˜๋…ธ ์ž…์ž๋ฅผ ์›์ž ํ•ด์ƒ๋„๋กœ ๊ด€์ฐฐํ•  ์ˆ˜ ์žˆ๋Š” ์œ ๋งํ•œ ๋„๊ตฌ์ด๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š”, ์—ด์ฒ˜๋ฆฌ ์ค‘ ๋‹ด์ง€๋œ ์ด‰๋งค ๋‚˜๋…ธ์ž…์ž์˜ ๊ตฌ์กฐ ๋ณ€ํ™” ๊ณผ์ •๊ณผ ์•ก์ฒด ๋‚ด ์ด‰๋งค ๋‚˜๋…ธ์ž…์ž์˜ ํ™•์‚ฐ ๊ณผ์ •์„ ์ดํ•ดํ•˜๊ธฐ ์œ„ํ•ด ์ด‰๋งค์—์„œ ๊ธฐ์ดˆ์ ์ด๋ฉด์„œ๋„ ์‹ค์šฉ์ ์œผ๋กœ ์ค‘์š”ํ•œ ์„ธ ๊ฐ€์ง€ ๋‚˜๋…ธ์ž…์ž ์‹œ์Šคํ…œ์„ ์—ฐ๊ตฌํ–ˆ์œผ๋ฉฐ, ์ด๋ฅผ ์œ„ํ•ด ์‹ค์‹œ๊ฐ„ ํˆฌ๊ณผ์ „์žํ˜„๋ฏธ๊ฒฝ๋ฒ•์„ ์‚ฌ์šฉํ–ˆ๋‹ค. ์„ธ๋ฆฌ์•„์— ๋‹ด์ง€๋œ ๋ฐฑ๊ธˆ์˜ ์‘์ง‘ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ์ดํ•ดํ•˜๋Š” ๊ฒƒ์€ ๋‚ด๊ตฌ์„ฑ ์žˆ๋Š” ์ด‰๋งค๋ฅผ ๊ฐœ๋ฐœํ•˜๋Š” ๋ฐ ์žˆ์–ด ๊ทผ๋ณธ์ ์ด๊ณ  ์‹ค์งˆ์ ์ธ ์ค‘์š”์„ฑ์„ ๊ฐ–๋Š”๋‹ค. ์„ธ๋ฆฌ์•„์— ์ง€์ง€๋œ ๋ฐฑ๊ธˆ์˜ ์‘์ง‘์€ ๊ณ ์˜จ ํ™˜์› ์‹œ ๋‹ด์ง€์ฒด์ธ ์„ธ๋ฆฌ์•„ ๋‚˜๋…ธ์ž…์ž์˜ ์‘์ง‘๊ณผ ํ•จ๊ป˜ ๋ฐœ์ƒํ•˜๋Š” ๊ฒƒ์œผ๋กœ ์•Œ๋ ค์ ธ ์žˆ์ง€๋งŒ, ์›์ž ์ˆ˜์ค€ ๊ณผ์ •์— ๋Œ€ํ•œ ์‹ค์‹œ๊ฐ„ ์ง์ ‘ ๊ด€์ฐฐ์ด ๋ถ€์กฑํ•˜์—ฌ ๊ทธ ๋ฉ”์ปค๋‹ˆ์ฆ˜์— ๋Œ€ํ•ด ์•Œ๋ ค์ง„ ๋ฐ”๊ฐ€ ๊ฑฐ์˜ ์—†๋‹ค. ์ œ์–ด๋œ ๊ณต๊ฐ„ ๋ถ„ํฌ์™€ ๋‹ค์–‘ํ•œ ์ž…์ž ๊ฒฝ๊ณ„ ํ˜•ํƒœ๋ฅผ ๊ฐ€์ง„ ์„ธ๋ฆฌ์•„ ์ž…์ž์™€ ๋‹ด์ง€๋œ ๋ฐฑ๊ธˆ์œผ๋กœ ๊ตฌ์„ฑ๋œ ๋ชจ๋ธ ์ด‰๋งค์—์„œ ๋ฐฑ๊ธˆ์˜ ์—ด ๊ฑฐ๋™์„ ์กฐ์‚ฌํ•˜๊ธฐ ์œ„ํ•ด ์‹ค์‹œ๊ฐ„ ๋ฐ ์ผ๋ฐ˜ ํˆฌ๊ณผ์ „์žํ˜„๋ฏธ๊ฒฝ ๊ธฐ๋ฒ•์„ ์ด์šฉํ–ˆ์œผ๋ฉฐ, ๊ทธ ๊ฒฐ๊ณผ ๋ฐฑ๊ธˆ์˜ ์‘์ง‘์ด ๋ฐœ์ƒํ•˜๋Š” ์ •๋„๋Š” ๋‹ด์ง€์ฒด ์„ธ๋ฆฌ์•„ ์ž…์ž์˜ ์‘์ง‘๊ณผ ์ƒ๊ด€๊ด€๊ณ„๊ฐ€ ์žˆ๋Š” ๊ฒƒ์„ ๋ฐํ˜”๋‹ค. ์„ธ๋ฆฌ์•„ ์ž…์ž์˜ ์‘์ง‘์€ ์ž˜ ์ •๋ ฌ๋œ ๊ฒฐ์ •๋ฆฝ๊ณ„๋ฅผ ๊ฐ€์ง„ ์„ธ๋ฆฌ์•„ ์ž…์ž ๊ฐ„ ์ ‘์ด‰์—์„œ ๋ฐœ์ƒํ•  ๊ฐ€๋Šฅ์„ฑ์ด ๊ฐ€์žฅ ๋†’์Œ์„ ๋ฐํ˜€๋ƒˆ๋‹ค. ๋ณธ ๊ฒฐ๊ณผ๋Š” ์„ธ๋ฆฌ์•„ ์‘์ง‘ ์ค‘ ํ‘œ๋ฉด ์žฌ๊ตฌ์„ฑ์ด ๋ฐฑ๊ธˆ์˜ ์‘์ง‘์„ ์œ ๋„ํ•  ๊ฐ€๋Šฅ์„ฑ์ด ์žˆ์Œ์„ ์‹œ์‚ฌํ•ฉ๋‹ˆ๋‹ค. ๋ฃจํ…Œ๋Š„์€ ์•”๋ชจ๋‹ˆ์•„ ํƒˆ์ˆ˜์†Œํ™” ๋ฐ˜์‘์— ๊ฐ€์žฅ ํ™œ์„ฑ์ด ๋†’์€ ๊ธˆ์† ์›์†Œ์ด๋ฉฐ, ํŠนํžˆ Ru(0001) ํ‘œ๋ฉด์˜ ์›์ž ์ˆ˜์ค€ ๊ณ„๋‹จ ๊ตฌ์กฐ์ธ B5 ์ž๋ฆฌ๊ฐ€ ํ™œ์„ฑ์ด ๋†’์€ ๊ฒƒ์œผ๋กœ ์•Œ๋ ค์ ธ ์žˆ๋‹ค. ํ•˜์ง€๋งŒ ์ผ๋ฐ˜์ ์œผ๋กœ ์ œ์กฐ๋œ ์ด‰๋งค์—์„œ B5 ์ž๋ฆฌ์˜ ๋ฐ€๋„๋Š” ์ผ๋ฐ˜์ ์œผ๋กœ ๋‚ฎ๋‹ค. ์œก๋ฐฉ์ •๊ณ„ ์งˆํ™”๋ถ•์†Œ(h-BN)์™€ ๋ฃจํ…Œ๋Š„์˜ ๊ฒฐ์ •์„ฑ ๋Œ€์นญ์ด ์œ ์‚ฌํ•˜๋‹ค๋Š” ์ ์— ์ฐฉ์•ˆํ•˜์—ฌ B5 ๋ถ€์œ„๊ฐ€ ํ’๋ถ€ํ•œ ๋ฃจํ…Œ๋Š„ ๋‚˜๋…ธ์ž…์ž๋ฅผ ํ•ฉ์„ฑํ–ˆ์œผ๋ฉฐ, ๊ตฌ๋ฉด์ˆ˜์ฐจ๋ณด์ • ํˆฌ๊ณผ์ „์žํ˜„๋ฏธ๊ฒฝ์„ ์ด์šฉํ•˜์—ฌ ์œก๊ฐํ˜• ๋ชจ์–‘์˜ ๋ฃจํ…Œ๋Š„ ๋‚˜๋…ธ์ž…์ž๊ฐ€ h-BN ์‹œํŠธ์—์„œ ์—ํ”ผํƒ์‹œ์–ผํ•˜๊ฒŒ ํ•ฉ์„ฑ๋œ ๊ฒƒ์„ ํ™•์ธํ–ˆ๋‹ค. B5 ์ž๋ฆฌ๋Š” ๋ฃจํ…Œ๋Š„ ๋‚˜๋…ธ์ž…์ž์˜ ๊ฐ€์žฅ์ž๋ฆฌ๋ฅผ ๋”ฐ๋ผ ๋ฐœ๊ฒฌ๋˜์—ˆ์œผ๋ฉฐ, ๋ฐ˜์‘ ์กฐ๊ฑด์—์„œ ์ด‰๋งค๋ฅผ ํ™œ์„ฑํ™”ํ•˜๋ฉด Ru ๋‚˜๋…ธ์ž…์ž์˜ ๋ชจ์–‘์ด ๋” ์ž˜ ๋ฐœ๋‹ฌ๋œ ์œก๊ฐํ˜•์œผ๋กœ ๋ณ€ํ˜•๋˜์–ด B5 ๋ถ€์œ„์˜ ์ˆ˜๊ฐ€ ์ฆ๊ฐ€ํ•˜๋Š” ๊ฒƒ์„ ๋ฐํ˜€๋ƒˆ๋‹ค. ์ฝœ๋กœ์ด๋“œ ์ด‰๋งค ๋‚˜๋…ธ ์ž…์ž์˜ ์—ด ์šด๋™๊ณผ ๊ทธ ์ƒํ˜ธ์ž‘์šฉ์€ ๋‚˜๋…ธ ๊ณผํ•™์—์„œ ๊ทผ๋ณธ์ ์œผ๋กœ ์ค‘์š”ํ•˜์ง€๋งŒ, ๋‚˜๋…ธ ๊ทœ๋ชจ์—์„œ ๊ฐœ๋ณ„ ์ž…์ž์˜ ๋™์—ญํ•™์„ ์—ฐ๊ตฌํ•  ์ˆ˜ ์žˆ๋Š” ์ ์ ˆํ•œ ๋ถ„์„ ๋„๊ตฌ๊ฐ€ ์—†๊ธฐ ๋•Œ๋ฌธ์— ์ •๋Ÿ‰์ ์œผ๋กœ ์ ‘๊ทผํ•˜๊ธฐ ์–ด๋ ต๋‹ค. ์—ฌ๊ธฐ์„œ๋Š” ์•ก์ฒด ์†์— ๋ถ„์‚ฐ๋˜์–ด ์žˆ๋Š” 2 nm ํฌ๊ธฐ์˜ ๊ธˆ ๋‚˜๋…ธ์ž…์ž์˜ ์—ด์šด๋™๊ณผ ์‘์ง‘ ์—ญํ•™์„ ๊ทธ๋ž˜ํ•€ ์•ก์ƒ์…€ ํˆฌ๊ณผ์ „์žํ˜„๋ฏธ๊ฒฝ์„ ์‚ฌ์šฉํ•˜์—ฌ ์ง์ ‘ ๊ด€์ฐฐํ–ˆ๋‹ค. ์ž‘์€ ํฌ๊ธฐ์˜ ๋‚˜๋…ธ์ž…์ž๋Š” ๋ธŒ๋ผ์šด ์šด๋™์„ ๋ณด์ด์ง€๋งŒ ๊ฐ€์šฐ์‹œ์•ˆ ๋ณ€์œ„ ๋ถ„ํฌ๋ฅผ ๋”ฐ๋ฅด์ง€ ์•Š์•˜์œผ๋ฉฐ ์ด๋Š” ์•ก์ƒ ํ™˜๊ฒฝ์˜ ๋™์  ์ด์งˆ์„ฑ์œผ๋กœ ์ธํ•œ ๋‚˜๋…ธ์ž…์ž์˜ ํ™•์‚ฐ ๊ณ„์ˆ˜์˜ ๋ณ€๋™์œผ๋กœ ์ธํ•œ ๊ฒƒ์ž„์„ ๋ฐํ˜€๋ƒˆ๋‹ค. ๋˜ํ•œ, ๋‘ ๋‚˜๋…ธ์ž…์ž ๊ฐ„ ์œ ์ฐฉ ๊ณผ์ •์€ ํ™•์‚ฐ์— ์ œํ•œ๋œ ๋‚˜๋…ธ์ž…์ž ๋ณตํ•ฉ์ฒด์˜ ํ˜•์„ฑ๊ณผ ํ‘œ๋ฉด ๋ฆฌ๊ฐ„๋“œ๊ฐ€ ์ค‘์š”ํ•œ ์—ญํ• ์„ ํ•˜๋Š” ๋ฐฐํ–ฅ ๋ถ€์ฐฉ์ด๋ผ๋Š” ๋‘ ๊ฐ€์ง€ ๊ณผ์ •์— ์˜ํ•ด ๋ฐœ์ƒํ•˜๋Š” ๊ฒƒ์„ ๋ฐœ๊ฒฌํ•˜์—ฌ ์ œ์•ˆํ•˜์˜€๋‹ค. ์ฃผ์š”์–ด : ์‹ค์‹œ๊ฐ„ ํˆฌ๊ณผ์ „์žํ˜„๋ฏธ๊ฒฝ, ๋‚˜๋…ธ์ž…์ž, ์ด‰๋งค, ๊ตฌ์กฐ ๋ณ€ํ™”, ํ™•์‚ฐ ํ•™ ๋ฒˆ : 2018-21563 ์„ฑ ๋ช… : ๊ฐ•์„ฑ์ˆ˜In recent decades, nanoparticles have become important building blocks for a wide range of scientific fields and applications. Among these applications, heterogeneous catalysis is one of the most important areas where nanoparticles are used, due to their unique properties at small sizes and their ability to maximize the dispersion of metal species. The design of catalytic nanoparticles with desired structures and properties requires an understanding of the atomic structures of the nanoparticles and the structural evolution under reaction conditions, such as thermal treatments and in liquid. However, the structural evolution of catalytic nanoparticles is less understood due to the challenges of directly observing individual nanoparticles in such chemically active environments at the atomic scale. In situ transmission electron microscopy (TEM) is a promising tool that allows the observation of individual nanoparticles under reaction conditions at atomic resolution. Here, in situ and ex situ TEM are used to study three nanoparticle systems of fundamental and practical importance in catalysis to understand the structural annealing of supported catalytic nanoparticles during heat treatments and the diffusion of catalytic nanoparticles in liquid. Understanding the sintering mechanism of platinum (Pt) supported on ceria (CeO2) is of fundamental and practical importance for the development of durable catalysts. The sintering of Pt supported on CeO2 is known to occur along with the aggregation of CeO2 support nanoparticles during high temperature reduction, but little is known about its mechanism due to the lack of direct in situ observations of the atomic scale processes. In situ and ex situ TEM are used to investigate the thermal behavior of Pt on CeO2 in model catalysts consisting of Pt on CeO2 particles with controlled spatial distributions and different grain boundary conformations. The extent to which Pt sintering occurs is correlated with the aggregation of the supporting CeO2 particles. CeO2 particle aggregation is most likely to occur at particle contacts with well-aligned grain boundaries, which serve as sites for the most significant Pt sintering. The results suggest that surface reconstruction during CeO2 aggregation is likely to induce Pt sintering. Ruthenium (Ru) is the most active metal element for the ammonia dehydrogenation reaction. The B5 site, an atomic level on Ru(0001) of Ru, is known to exhibit the highest catalytic activity for ammonia dehydrogenation, but the populations of B5 sites in prepared catalysts are typically low. Here, Ru nanoparticles rich in B5 sites are synthesized based on the similarity in the crystal symmetries of hexagonal boron nitride (h-BN) and Ru. Aberration-corrected TEM shows that hexagonal Ru nanoparticles are epitaxially synthesized on h-BN sheets. The B5 sites are identified along the edges of the Ru nanoparticles. Activation of the catalyst under reaction conditions increases the population of B5 sites by transforming the shape of the Ru nanoparticles into better developed hexagons. The electron density of the Ru nanoparticles also increases during activation. The thermal motion of colloidal catalytic nanoparticles and their interactions are of fundamental importance in nanoscience, but are difficult to access quantitatively, mainly due to the lack of appropriate analytical tools to study the dynamics of individual particles at the nanoscale. Here, the stochastic thermal motion and coalescence dynamics of gold nanoparticles as small as 2 nm in liquid are directly observed using graphene liquid cell (GLC) TEM. The small nanoparticles show Brownian but non-Gaussian motion, indicating the fluctuation of the diffusion coefficient of the nanoparticles due to the dynamic heterogeneity of the liquid environment. Furthermore, the coalescence of two nanoparticles occurs by two processes: the diffusion-limited formation of a transient nanoparticle complex and subsequent coalescence by oriented attachment, in which surface-passivating ligands play a critical role. Keyword: In situ transmission electron microscopy (TEM), nanoparticle, catalyst, structural annealing, diffusion Student Number: 2018-21563Chapter 1 Introduction . 1 1.1. Structural dynamics of catalytic nanoparticles in reaction 1 1.2. In situ transmission electron microscopy for mechanistic understanding of single nanoparticle reactions 2 1.3. Purpose of research . 4 Chapter 2 Aggregation of CeO2 particles with aligned grains drives sintering of Pt single atoms in Pt/CeO2 catalysts 6 2.1. Introduction . 6 2.2. Methods . 7 2.2.1. Sample preparation . 7 2.2.2. H2-temperature programmed reduction (H2-TPR) 8 2.2.3. X-ray diffraction (XRD) 8 2.2.4. Raman spectroscopy 8 2.2.5. Surface area measurement 9 2.2.6. Transmission electron microscopy 9 2.3. Results and discussion. 11 2.3.1. Catalyst preparation and structural analysis . 11 2.3.2. Relationship between CeO2 aggregation and Pt sintering investigated by the control of interparticle distance 13 2.3.3. Effects of grain boundaries in aggregated CeO2 domains for Pt sintering . 14 2.3.4. Conclusion 17 Chapter 3 Heteroepitaxial growth of B5-site-rich Ru nanoparticles guided by h- BN for low-temperature NH3 dehydrogenation 38 3.1. Introduction 38 3.2. Methods 40 vi 3.2.1. Catalyst synthesis 40 3.2.2. Adsorption and desorption isotherms 42 3.2.3. Inductively coupled plasma-optical emission spectroscopy (ICP-OES) 43 3.2.4. X-ray photoelectron spectroscopy (XPS) 44 3.2.5. Transmission electron microscopy (TEM) 44 3.2.6. Catalytic activity test 45 3.2.7. Density functional theory (DFT) calculation 47 3.3. Results and discussion. 48 3.3.1. Epitaxial growth of B5-site-rich Ru nanoparticles on h-BN. 48 3.3.2. Activation of Ru/h-BN catalyst 53 3.3.3. Catalytic performances 56 3.3.4. Conclusion 60 Chapter 4 Real-space imaging of nanoparticle transport and interaction dynamics in graphene liquid cell TEM 95 4.1. Introduction 95 4.2. Methods 98 4.2.1. GLC preparation 98 4.2.2. Liquid-phase TEM 99 4.2.3. Single-particle tracking and drift correction . 100 4.2.4. Off-lattice random walk model in dynamically heterogeneous environment 103 4.2.5. Kinetics of two-step coalescence between ligand-passivated nanoparticles 120 4.2.6. Survival probability calculation 129 4.3. Results and discussion 131 4.3.1. GLC TEM of nanoparticles in liquid 131 4.3.2. Fickian diffusion of nanoparticles in a GLC . 132 4.3.3. Fluctuation in diffusion coefficient of nanoparticles in a GLC 134 4.3.4. Origin of diffusion coefficient fluctuations 137 vii 4.3.5. Precise prediction of displacement distribution of nanoparticles in a finite pixel size 139 4.3.6. Encounter complex formation and coalescence of nanoparticles 140 4.3.7. Conclusion . 144 Chapter 5 Summary and Conclusions 192 Bibliography 194 ๊ตญ ๋ฌธ ์ดˆ ๋ก . 206 List of Publications 209 viii๋ฐ•

    Machine Learning-Based Anomaly Detection on Seawater Temperature Data with Oversampling

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    This study deals with a method for anomaly detection in seawater temperature data using machine learning methods with oversampling techniques. Data were acquired from 2017 to 2023 using a Conductivityโ€“Temperatureโ€“Depth (CTD) system in the Pacific Ocean, Indian Ocean, and Sea of Korea. The seawater temperature data consist of 1414 profiles including 1218 normal and 196 abnormal profiles. This dataset has an imbalance problem in which the amount of abnormal data is insufficient compared to that of normal data. Therefore, we generated abnormal data with oversampling techniques using duplication, uniform random variable, Synthetic Minority Oversampling Technique (SMOTE), and autoencoder (AE) techniques for the balance of data class, and trained Interquartile Range (IQR)-based, one-class support vector machine (OCSVM), and Multi-Layer Perceptron (MLP) models with a balanced dataset for anomaly detection. In the experimental results, the F1 score of the MLP showed the best performance at 0.882 in the combination of learning data, consisting of 30% of the minor data generated by SMOTE. This result is a 71.4%-point improvement over the F1 score of the IQR-based model, which is the baseline of this study, and is 1.3%-point better than the best-performing model among the models without oversampling data
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