4,487 research outputs found

    Dielectric breakdown II: Related projects at the University of Twente

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    In this paper an overview is given of the related activities in our group of the University of Twente. These are on thin film transistors with the inherent difficulty of making a gate dielectric at low temperature, on thin dielectrics for EEPROM devices with well-known requirements with respect to charge retention and endurance and, finally, on thin film diodes in displays with unexpected breakdown properties

    Flexible glass substrates with via holes for TFT backplanes

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    This paper looks at flexible glass substrates with via holes for TFT backplane

    Development of a Self Aligned CMOS Process for Flash Lamp Annealed Polycrystalline Silicon TFTs

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    The emerging active matrix liquid crystal (AMLCD) display market requires a high performing semiconductor material to meet rising standards of operation. Currently amorphous silicon (a-Si) dominates the market but it does not have the required mobility for it to be used in AMLCD manufacturing. Other materials have been developed including crystallizing a-Si into poly-silicon. A new approach to crystallization through the use of flash lamp annealing (FLA) decreases manufacturing time and greatly improves carrier mobility. Previous work on FLA silicon for the use in CMOS transistors revealed significant lateral dopant diffusion into the channel greatly increasing the minimum channel length required for a working device. This was further confounded by the gate overlap due to misalignment during lithography patterning steps. Through the use of furnace dopant activation instead of FLA dopant activation and a self aligned gate the minimum size transistor can be greatly reduced. A new lithography mask and process flow were developed for the furnace annealing and self aligned gate. Fabrication of the self aligned devices resulted in oxidation of the Molybdenum self aligned gate. Further development is needed to successfully manufacture these devices. Non-self aligned transistors were made simultaneously with self aligned devices and used the furnace activation. These devices showed an increase in sheet resistance from 250 ฮฉ to 800 ฮฉ and lower mobility from 380 to 40.2 V/cm2s. The lower mobility can be contributed to an increase in implanted trap density indicating furnace annealing is an inferior activation method over FLA. The minimum transistor size however was reduced from 20 to 5 ฮผm. With improvements in the self aligned process high performing small devices can be manufactured

    Electro-optical Simulation of a-Si Thin-Film-Transistor Liquid Crystal Display Pixels

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    An analysis of an amorphous silicon (a-Si) thin-film-transistor liquid-crystal display (TFT-LCD) pixel is presented. The electro-optical model combines the electrical properties of the switching element and the optical performance of a twisted nematic (TN) liquid-crystal cell.Publicad

    Flash Lamp Annealed LTPS TFTs with ITO Bottom-Gate Structures

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    As displays continue to increase in resolution and refresh rate, new materials for thin film transistors (TFTs) are required. Low temperature polycrystalline silicon (LTPS) formed by excimer laser annealing (ELA) has been very successful and has been implemented in small displays, but cost and scalability issues prevent it from entering larger display products. Currently LPTS TFTs are top-gate structures due to manufacturing challenges associated with crystallizing thin film silicon when a thermally conductive gate is under portions and insulating glass under others. Bottom-gate devices offer the benefit of higher breakdown voltage, better dielectric-semiconductor interface quality, and direct access to the back-channel region for interface trap passivation. The ability to fabricate bottom-gate devices would allow for different integration and design schemes and is a prerequisite for double gate structures. Flash lamp annealed (FLA) LTPS is an attractive method to expand the size of displays that use high mobility TFTs due to its scalability and parallel production nature. In this work bottom-gate LTPS TFTs were fabricated via FLA with indium tin oxide (ITO), a transparent conductive oxide, used as the gate electrode. A p-channel TFT with 4 ยตm channel length crystallized with a FLA energy of 4.4 J/cm2 for 250 ยตs demonstrated a low-field mobility of 190 cm2/(Vs), a subthreshold slope of 325 mV/dec, on/off state ratio of seven orders of magnitude, and a threshold voltage of -5.4 V. A dielectric failure mechanism was identified that compromised the transistor operation under high drain bias and an alternative dopant introduction techniques were proposed to mitigate this issue. An effect due to the transduction of optical energy from the field to thermal energy under the channel via the gate was observed. Details of the FLA crystallization process, device fabrication, and electrical characteristics will be presented

    ํ”Œ๋ผ์ฆˆ๋งˆ ํ™”ํ•™ ๊ธฐ์ƒ ์ฆ์ฐฉ๋ฒ•์„ ์ด์šฉํ•œ ๋ฒ ๋ฆฌ์–ด ํ•„๋ฆ„ ํ•ฉ์„ฑ๊ณผ ๋””์Šคํ”Œ๋ ˆ์ด ์‘์šฉ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์ž์—ฐ๊ณผํ•™๋Œ€ํ•™ ํ™”ํ•™๋ถ€, 2019. 2. ํ™๋ณ‘ํฌ.์ž๋ฐœ๊ด‘ํ˜• ๋””์Šคํ”Œ๋ ˆ์ด์ด๋ฉฐ, ์ €์ „์•• ๊ตฌ๋™์ด ๊ฐ€๋Šฅํ•˜๊ณ  ์–‡์€ ๋‘๊ป˜๋กœ ์ œ์ž‘์ด ๊ฐ€๋Šฅํ•˜๋ฉฐ ๋™์ž‘์†๋„๊ฐ€ ๋งค์šฐ ๋น ๋ฅผ ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ๋†’์€ ํ•ด์ƒ๋„ ๊ตฌํ˜„์ด ๊ฐ€๋Šฅํ•œ OLED๋Š” ๋””์Šคํ”Œ๋ ˆ์ด์—์„œ ๋น ๋ฅธ ์„ฑ์žฅ์„ธ๋ฅผ ๋ณด์ด๊ณ  ์žˆ๋‹ค. ์ตœ๊ทผ OLED์˜ ๊ฐ€์žฅ ํฐ ๊ด€์‹ฌ ๋ถ„์•ผ๋Š” ๋ชจ๋ฐ”์ผ์šฉ ๋””์Šคํ”Œ๋ ˆ์ด์™€ ๋Œ€๋ฉด์  TV, ๊ทธ๋ฆฌ๊ณ  ํ”Œ๋ ‰์‹œ๋ธ” ๋ฐ ํˆฌ๋ช… ๋””์Šคํ”Œ๋ ˆ์ด ๊ตฌํ˜„์ด๋‹ค. ๋””์Šคํ”Œ๋ ˆ์ด๋ฅผ ๊ตฌ๋™ํ•˜๊ธฐ ์œ„ํ•œ ๊ตฌ๋™์†Œ์ž๋Š” ์ˆ˜๋™ํ˜•(passive matrix)๊ณผ ๋Šฅ๋™ํ˜•(active matrix, AM)๋กœ ๋‚˜๋‰˜๋ฉฐ, ์ˆ˜๋™ํ˜•์— ๋น„ํ•˜์—ฌ ๊ณ ํ™”์งˆ, ๋‚ฎ์€ ์†Œ๋น„ ์ „๋ ฅ, ๋Œ€ํ˜•ํ™”์— ์œ ๋ฆฌํ•œ ๋Šฅ๋™ํ˜• ๋””์Šคํ”Œ๋ ˆ์ด๊ฐ€ ์„ ํ˜ธ๋œ๋‹ค. ํ‘œ์‹œ์†Œ์ž๋ฅผ ๋Šฅ๋™ ๊ตฌ๋™ํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ๊ฐ ํ™”์†Œ๋งˆ๋‹ค ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ(thin-film transistor, TFT)์™€ ๊ฐ™์€ ์Šค์œ„์นญ ์†Œ์ž๋ฅผ ๋ถ€์ฐฉ์‹œ์ผœ์•ผ ํ•œ๋‹ค. ๋Šฅ๋™ํ˜• ๊ตฌ๋™์†Œ์ž์˜ ๊ฒฝ์šฐ ํ˜„์žฌ์˜ TFT-LCD๋‚˜ AMOLED์šฉ ๋ฐฑํ”Œ๋ ˆ์ธ์— ์ฃผ๋กœ ์‚ฌ์šฉ๋˜๋Š” ๋น„์ •์งˆ ์‹ค๋ฆฌ์ฝ˜(a-Si), ์ €์˜จ ๋‹ค๊ฒฐ์ • ์‹ค๋ฆฌ์ฝ˜ (LTPS) ๊ธฐ์ˆ ์ด ์šฐ์„  ๊ฐœ๋ฐœ๋˜์–ด ์‘์šฉ๋˜๊ณ  ์žˆ๋‹ค. ์ตœ๊ทผ์—๋Š” ํฐ ๋ฐด๋“œ ๊ฐญ์„ ๊ฐ€์ง€๋Š” ๋น„์ •์งˆ ์‚ฐํ™”๋ฌผ ๋ฐ˜๋„์ฒด๋ฅผ ์ด์šฉํ•ด ํˆฌ๋ช…ํ•˜๋ฉด์„œ ๋น ๋ฅธ ์‘๋‹ต์†๋„์˜ ๋””์Šคํ”Œ๋ ˆ์ด ๊ตฌ๋™์†Œ์ž์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๊ฐ€ ํ™œ๋ฐœํžˆ ์ง„ํ–‰๋˜๊ณ  ์žˆ๋‹ค. ๋˜ํ•œ ๋ฐฐ์„ ์˜ RC Delay๋ฅผ ์ตœ์†Œํ™” ์‹œ์ผœ์•ผ ํ•˜๊ณ , ํŒŒ์›Œ์†Œ๋น„๋Ÿ‰์„ ์ค„์—ฌ์•ผ ํ•˜๋Š” ๊ธฐ์ˆ ์ ์ธ ๋ฌธ์ œ๊ฐ€ ์žˆ๋‹ค. ๋””์Šคํ”Œ๋ ˆ์ด์˜ ๊ณ ํ•ด์ƒ๋„์ธ UHD (Ultra High Definition)์˜ backplane์—์„œ ๊ณ ์† TFT ๊ตฌํ˜„์„ ์œ„ํ•˜์—ฌ SD(Source-Drain) ๋ฉ”ํƒˆ ๋ฐฐ์„  ๊ตฌํ˜„์€ ํ•„์ˆ˜์ ์ธ ์š”์†Œ์ด๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” SD ๋ฉ”ํƒˆ ๋ฐฐ์„ ์œผ๋กœ์จ ์ €์ €ํ•ญ ๋ฐฐ์„ ์ธ Copper ๋ฐฐ์„ ์˜ diffusion barrier ์—ญํ• ์„ ํ•˜๋Š” Graphite ์„ฑ์žฅ์„ ๋‹ค๋ฃจ๊ณ  ์žˆ๋‹ค. ๊ธฐ์กด์˜ Graphene ํ•ฉ์„ฑ์€ ๊ธฐ๊ณ„์  ๋ฐ ํ™”ํ•™์  ๋ฐ•๋ฆฌ ๋ฐฉ๋ฒ•์—๋Š” ๋Œ€๋ฉด์  ํŒจ๋„ ๊ตฌํ˜„์œผ๋กœ์จ ํ•œ๊ณ„๊ฐ€ ์žˆ๋‹ค. ํ˜„์žฌ๊นŒ์ง€ ๋Œ€ํ˜• Size scale Graphene ์‹œ๋„๋Š” ์ „๊ทน์œผ๋กœ์จ Graphene ํ™œ์šฉ์€ ์žˆ์ง€๋งŒ, ์ด ๊ตฌํ˜„์€ Thermal CVD (900~1000โ„ƒ)์—์„œ Graphene ์„ ํ•ฉ์„ฑํ•˜๊ณ , Glass์— transfer ํ•œ ๋…ผ๋ฌธ์œผ๋กœ์จ ์‹ค์ œ ๋Œ€๋ฉด์ ์œผ๋กœ ๋งŒ๋“œ๋Š” ๊ณต์ • ์ ์šฉ์—๋Š” ํ•œ๊ณ„๊ฐ€ ์žˆ๋‹ค. ์ด์— ํ˜„์žฌ ๋งŽ์ด ์—ฐ๊ตฌ๋Š” ์ง„ํ–‰ ์ค‘์ด๊ณ  ์žˆ์ง€๋งŒ, PECVD (Plasma Enhanced Chemical Vapor Deposition)๋ฅผ ์ด์šฉํ•œ graphite ๋ฐ•๋ง‰ ํ•ฉ์„ฑ์€ ๋Œ€ํ˜• size, mass production์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•˜๋ฉฐ, ์•„์ง mass production ์ ์šฉ์„ ์œ„ํ•ด ์—ฐ๊ตฌํ•ด์•ผ ํ•  ์ ์€ ๋งŽ์ง€๋งŒ, ์ €์˜จ ๊ณต์ • Graphite ํ•ฉ์„ฑ์ด ๊ฐ€๋Šฅํ•˜๋‹ค๋ฉด, large scale device ๊ตฌํ˜„์— ํ•œ์ธต ๋” ์ง„๋ณด๋œ ๊ธฐ์ˆ ์ด ๋  ๊ฒƒ์ž„์„ ํ™•์‹ ํ•œ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ Copper diffusion barrier ์œผ๋กœ์จ์˜ ์—ญํ• ์„ ๊ฒ€์ฆํ•˜๊ณ , ์ฆ์ฐฉ ์˜จ๋„๋ฅผ ์ €์˜จ์œผ๋กœ ํ•ฉ์„ฑํ•จ์œผ๋กœ์จ TEM ๋ฐ EDAX ๋ถ„์„์œผ๋กœ Graphite barrier ๋ฐ mass production์˜ ๊ฐ€๋Šฅ์„ฑ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋ณธ ์—ฐ๊ตฌ์˜ ์ง์ ‘์ ์ธ PECVD ํ•ฉ์„ฑ ๋ฐฉ๋ฒ•์„ ํ†ตํ•ด ๋Œ€๋ฉด์ ์ด ๊ฐ€๋Šฅํ•จ์„ ์ œ์‹œํ•จ์œผ๋กœ์จ ๊ธฐ์กด์˜ ๋Œ€๋ฉด์  ํ•ฉ์„ฑ ๋ฌธ์ œ์ ์„ ํ•ด๊ฒฐํ•ด ์ค„ ์ˆ˜ ์žˆ๋Š” ๋ฐฉ์•ˆ์ด ๋  ๊ฒƒ์ด๋‹ค. ๋˜ํ•œ ๋””์Šคํ”Œ๋ ˆ์ด์˜ TFT ํŠน์„ฑ๋„ ๊ธฐ์กด์˜ Active material ์ธ a-Si TFT๋ณด๋‹ค ํ›จ์”ฌ ๋” ๋†’์€ ๊ณ ์ด๋™๋„ ์†Œ์ž๋ฅผ ์š”๊ตฌํ•˜๋ฉฐ, ํŠนํžˆ ํˆฌ๋ช… ๋””์Šคํ”Œ๋ ˆ์ด์˜ ์ ์šฉ ๊ฐ€๋Šฅํ•˜๋ฉฐ, ๊ณ ์ด๋™๋„ ํŠน์„ฑ์„ ๊ท ์ผํ•˜๊ฒŒ ๊ฐ€์งˆ ์ˆ˜ ์žˆ๋Š” ์‹ ๊ทœ TFT๋ฅผ ์š”๊ตฌํ•˜๊ฒŒ ๋˜์—ˆ๋‹ค. ์ด์— ๋Œ€ํ•œ ๋ฐฉ์•ˆ์œผ๋กœ ์‚ฐํ™”๋ฌผ TFT๋กœ์จ ZnO (Zinc Oxide), IZO (Indium Zinc Oxide), a-IGZO (Amorphous Indium Gallium Zinc Oxide) ๋“ฑ์˜ ์žฌ๋ฃŒ๊ฐ€ ์—ฐ๊ตฌ๋˜๊ณ  ์žˆ๋‹ค. ๊ธฐ์กด์˜ a-Si์˜ ์ด๋™๋„ (<1cm2/VยทS) ๋ณด๋‹ค ๋†’์€ ์ด๋™๋„๋ฅผ ๊ฐ€์ง„ IGZO ์žฌ๋ฃŒ๋Š” ํˆฌ๋ช…ํ•œ ์†Œ์ž๋กœ์จ ํˆฌ๋ช…๋””์Šคํ”Œ๋ ˆ์ด์—์„œ๋„ ํ™œ์šฉ์ด ๊ฐ€๋Šฅํ•˜์—ฌ, ์‘์šฉ์„ฑ์„ ํ™•๋Œ€ํ•˜๊ณ  ์žˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ํˆฌ๋ช…๋””์Šคํ”Œ๋ ˆ์ด ์—์„œ๋„ ํ™œ์šฉ์ด ๊ฐ€๋Šฅํ•˜๋„๋ก a-IGZO๋ฅผ substrate๋กœ ํ•˜๋Š” Graphite ๋ฐ•๋ง‰์„ ํ•ฉ์„ฑ ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•˜๊ณ , ๋Œ€๋ฉด์  ๊ตฌํ˜„์œผ๋กœ์จ ๊ทธ ์‘์šฉ์„ฑ์„ ๊ธฐ๋Œ€ํ•˜๊ณ  ์žˆ๋‹ค. Graphite์˜ ์ €์˜จ ํ•ฉ์„ฑ ๊ธฐ์ˆ  ๊ฐœ๋ฐœ์€ ๊ธฐ์กด ๋ผ์ธ์˜ CVD ์žฅ๋น„ ๊ต์ฒด ์—†์ด ๋‹จ์ง€ Graphene Gas ์‚ฌ์šฉ๋งŒ์œผ๋กœ ๊ณต์ •์„ ๊ตฌํ˜„ํ•œ๋‹ค๋Š” ์ ์ด cost ๋ฐ ๊ณต์ • ๋‹จ์ˆœํ™”์˜ ๊ด€์ ์—์„œ ๋งŽ์€ ์žฅ์ ์ด ์žˆ๋‹ค. ๋˜ํ•œ ๊ณ ์† ๊ตฌ๋™์„ ์œ„ํ•˜์—ฌ SD ๋ฐฐ์„ ์œผ๋กœ metal๋ฟ ์•„๋‹ˆ๋ผ ์‚ฐํ™”๋ฌผ ๋ฐ˜๋„์ฒด๋กœ๋„ Graphite ํ•ฉ์„ฑ์˜ catalyst๋กœ์จ ์‚ฌ์šฉ๋˜์–ด, ํŒจ๋„ ๊ตฌํ˜„์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•ด์ค€๋‹ค๋Š” ๊ด€์ ์—์„œ ์˜๋ฏธ๊ฐ€ ์žˆ๋‹ค. ๋˜ํ•œ Graphite ํ•ฉ์„ฑ ๊ธฐ์ˆ ์„ thin film ๋ฐ•๋ง‰์„ ๋งŒ๋“ค์–ด ๋‹ค๋ฅธ application ์—์„œ๋„ ํ™œ์šฉ ๊ฐ€๋Šฅํ•จ์„ ๋ณด์—ฌ์คŒ์œผ๋กœ์จ ํŒŒ๊ธ‰ ํšจ๊ณผ๊ฐ€ ํฌ๋‹ค๊ณ  ํŒ๋‹จ๋œ๋‹ค. ๋‹ค์Œ ์—ฐ๊ตฌ์—์„œ๋Š” LCD ๋””์Šคํ”Œ๋ ˆ์ด์—์„œ Backlight ์‚ฌ์šฉ์ด ํ•„์ˆ˜์ ์ด๋‹ค. Back light๋Š” ๊ฐ€์‹œ๊ด‘์„  ์˜์—ญ ๋ฟ ์•„๋‹ˆ๋ผ UV ํŒŒ์žฅ์˜์—ญ๋„ ํฌํ•จํ•˜๊ณ  ์žˆ์œผ๋ฉฐ, Active ์žฌ๋ฃŒ์ธ a-IGZO ์†Œ์ž์—์„œ TFT ํŠน์„ฑ์˜ ๋ถˆ์•ˆ์ •์„ฑ์˜ ๋ฌธ์ œ๋ฅผ ๊ฐ€์ง€๊ณ  ์žˆ๋‹ค. IGZO์˜ ํŠน์„ฑ์ƒ UV ํŒŒ์žฅ๋Œ€์—์„œ์˜ ๋น›๊ณผ์˜ ๋ฐ˜์‘์œผ๋กœ TFT ์†Œ์ž์˜ ์‹ ๋ขฐ์„ฑ ํŠน์„ฑ์ด ์•…ํ™”๋˜๋Š” ๋ฌธ์ œ์ ์„ ํ•ด๊ฒฐํ•˜๊ณ ์ž Barrier ๋ฐ•๋ง‰์„ ์‚ฌ์šฉ์ด ํ•„์ˆ˜์ ์ธ ์š”์†Œ์ด๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” TFT์˜ ์‹ ๋ขฐ์„ฑ ๋ฐ ์•ˆ์ •์„ฑ์„ ์œ ์ง€ํ•˜๊ธฐ ์œ„ํ•ด์„œ Photo blocking barrier๋กœ์จ SiGe (Silicon Germanium) ๋ฐ•๋ง‰ ์žฌ๋ฃŒ ํ•ฉ์„ฑ์„ ํ†ตํ•˜์—ฌ TFT ์‹ ๋ขฐ์„ฑ์˜ ํŠน์„ฑ ๋ณ€ํ™” ์—†๋Š” ๊ฒƒ์„ ์—ฐ๊ตฌํ•˜์˜€๋‹ค. ์ด์ „ SiGe ์—ฐ๊ตฌ๋˜์–ด์ง„ ๋ฐ”๋กœ๋Š” ํƒœ์–‘์ „์ง€์—์„œ P-I(intrinsic layer)-Nํ˜• ๊ตฌ์กฐ์—์„œ ์ค‘๊ฐ„ ์‚ฝ์ž…์ธต์—์„œ ๋ถˆ์ˆœ๋ฌผ์ด ์ฒจ๊ฐ€๋˜์ง€ ์•Š์€ ๋ฌด์ฒจ๊ฐ€์ธต (Intrinsic layer)์—์„œ SiGe ์ด ๊ด‘ํก์ˆ˜์ธต์œผ๋กœ ์‚ฌ์šฉ๋˜์–ด์ง„ ์—ฐ๊ตฌ๊ฐ€ ์žˆ์—ˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” TFT ์†Œ์ž์—์„œ a-IGZO ๊ฐ€ ๊ด‘๋ฐ˜์‘์œผ๋กœ ์ธํ•ด ์‚ฐ์†Œ ๊ฒฐํ• (Oxygen Vacancy)์„ ๋ง‰์•„ TFT ํŠน์„ฑ์˜ ์ €ํ•˜ ํšจ๊ณผ๋ฅผ ๋ง‰๊ณ ์ž SiGe์˜ ๊ด‘ ์ฐจ๋‹จ ๋ฐ•๋ง‰ ํ˜•์„ฑ์„ ํ†ตํ•ด ๊ด‘๋ฐ˜์‘์œผ๋กœ ์ธํ•œa-IGZOํŠน์„ฑ ๋ณ€ํ™”๊ฐ€ ๋˜์ง€ ์•Š๋„๋ก ํ•˜์˜€๋‹ค. ๋˜ํ•œ ๋ฐ•๋ง‰ ํ˜•์„ฑ ๋ฐ ์ ์ธต ๊ตฌ์กฐ์—์„œ SiGe ์™€ IGZO์˜ ๋ฐ•๋ง‰ ์‚ฌ์ด์— Capacitance ํ˜•์„ฑ์œผ๋กœ ์ „์ž์˜ charge๊ฐ€ IGZO ๋ฐ•๋ง‰ ๊ณ„๋ฉด์— ๋ˆ„์ ๋˜์–ด, ํŠธ๋žœ์ง€์Šคํ„ฐ ํŠน์„ฑ์ด ๋‹จ๋ฝ(short) ํ˜„์ƒ์ด ๋ฐœ์ƒ ํ•˜์˜€์œผ๋ฉฐ, ์ด๋ฅผ ๋ฐฉ์ง€ํ•˜๊ธฐ ์œ„ํ•ด Buffer layer ์˜ ๋‘๊ป˜ ์กฐ์ ˆ์ด ์ค‘์š”ํ•˜์˜€๋‹ค. ์ด์— Buffer layer์˜ ๋‘๊ป˜ ์ตœ์ ํ™”๋ฅผ ํ†ตํ•ด ํ•˜๋ถ€์—์„œ ๋“ค์–ด์˜ค๋Š” ๋น›์—๋„ ์ฐจ๋‹จ์„ ํ•  ์ˆ˜ ์žˆ๋Š” Barrier ์ ์ธต ๊ตฌ์กฐ๋ฅผ ๋งŒ๋“ค์–ด TFT ์†Œ์ž์˜ ์‹ ๋ขฐ์„ฑ ๊ฐœ์„ ๋จ์„ ๋ณด์—ฌ์ฃผ๊ณ ์ž ํ•˜์˜€๋‹ค. ์Šค๋งˆํŠธ Window ๋ฐ ๋ƒ‰์žฅ๊ณ ์—์„œ ๋ฌธ์„ ์—ด์ง€ ์•Š๊ณ  ๋‚ด์šฉ๋ฌผ์„ ํ™•์ธํ•  ์ˆ˜ ์žˆ๋Š” ํˆฌ๋ช… ๋””์Šคํ”Œ๋ ˆ์ด ๋ฐ ํ”Œ๋ ‰์‹œ๋ธ” ๋””์Šคํ”Œ๋ ˆ์ด ๊ตฌํ˜„์„ ์œ„ํ•ด ์—ฌ๋Ÿฌ ์š”์†Œ์˜ ๊ธฐ์ˆ  ์—ฐ๊ตฌ๊ฐ€ ์ง„ํ–‰๋˜๊ณ  ์žˆ์œผ๋ฉฐ, ์ด ๊ตฌํ˜„์„ ์œ„ํ•ด ๋ณธ ์—ฐ๊ตฌ์˜ Barrier ๋ฐ•๋ง‰ ๊ตฌํ˜„์€ ํ•„์ˆ˜์ ์ธ ์š”์†Œ๋กœ ์‘์šฉ์„ฑ์ด ํ™•๋Œ€๋˜์–ด ํ™œ์šฉ๋จ์„ ๊ธฐ๋Œ€ํ•ด ๋ณธ๋‹ค.OLED is a self-emissive display can be driven at low voltage and manufactured in a thin layer. In addition, this display operates at a very high speed and emit a color that can be rapidly implemented. Recently, OLEDs main interest is mobile screen, large screen TV, flexible and transparent display. The driving device for display is classified to the passive matrix and active matrix. Active matrix is preferred because of higher resolution, lower energy consumption, and large size screen. To apply active matrix on display device, a switching device such as thin-film transistor (TFT) is attached to each pixel. For active driving devices, amorphous silicon (a-Si) and low-temperature polycrystalline silicon (LTPS) technologies are applied in current TFT โ€“LCD or AMOLED back frame. Recently, there is an ongoing research on using amorphous oxide semiconductors with large bandgaps to research transparent and fast responsive display driving devices. Moreover, RC delay has a technical problem that must be minimized and reduce power consumption. Implementation of Source Drain (SD) is a metal wiring essential element for high-speed TFT execution in high-resolution UHD (Ultra High Definition) displays backplane. In this study, the graphite growth plays the role of diffusion barrier of copper wiring that has low resistance wiring with SD metal wiring. The chemical and mechanical stripping methods of conventional graphene synthesis application on large area panels is limited. Up to now, the large size graphene has been used as an electrode, but this implementation is limited to making the large-scale process by synthesizing graphene at thermal CVD (900~1000ยฐC) and transferring it to the glass. Despite the fact, a lot of ongoing studies, graphites thin film synthesis using Plasma Enhanced Chemical Vapor Deposition (PECVD) enables large size and mass production. Furthermore, this area still requires more research on mass production. If low-temperature process for graphite synthesis is possible, this will become a more advanced technology for device implementation. In this study, the role of copper diffusion barrier was verified, and the possibility of graphite barrier and mass production was verified by TEM and EDAX analysis by synthesizing the deposition temperature at low temperature. In addition, this study suggests the large size display can be obtained through direct PECVD synthesis that will solve the existing problems of large size synthesis. The displays TFT characteristics also require a high mobility device that is much higher than the conventional active material a-Si TFT. In particular, a new TFT capable of applying a transparent display and uniformly having high mobility characteristics is required. Materials such as ZnO (Zinc Oxide), IZO (Indium Zinc Oxide) and IGZO (Indium Gallium Zinc Oxide) have been studied as oxide TFTs. IGZO materials with higher mobility than conventional a-Si mobility (<1 cm2 / V ยท s) are transparent devices and can be used in transparent displays, thus extending applicability. In this study, we propose a graphite synthesis based on IGZO to be applicable to transparent display and expect the application on large size displays. The low-temperature Graphite synthesis has many advantages in terms of cost and process simplification because it implements the process only by using Graphene gas without replacing existing CVD equipment. In addition, it can be used as a graphite synthesis catalyst not only for metal but also for the oxide semiconductor, to raise activation. Moreover, the graphite synthesis to make a thin film can be applied to other fields. In the next study, it is essential to use backlight in LCD display. The backlight not only includes the visible light but also the UV region, and has instability of TFT characteristics in the active material IGZO device. Due to IGZOs reaction to light in UV region, it is essential to use a barrier film in order to solve the reliability characteristics of the TFT device deterioration. To maintain the reliability and stability of the TFT, this study on reliability of the TFT was not changed by SiGe (Silicon Germanium) synthesis thin film as a photo blocking barrier. Based on previous research on SiGe has been used as the light absorbing layer in the intrinsic layer in which a P-I (intrinsic layer)-N type structure in a solar cell that is not doped with an impurity in an intermediate insertion layer. In this study, in order to prevent oxygen vacancy during a-IGZO photoreaction on TFT device, the formation of a light-shielding film of Si-Ge prevents oxygen deficiency. Capacitance formation between SiGe and IGZO thin film in the thin film formation and lamination structure accumulates electrons charge on the IGZO thin film interface. The characteristics of the transistor were short, and to prevent this shortness, it is important to control the thickness of the buffer layer. Therefore, this shows that the reliability of the TFT device is improved by making the barrier laminate structure that can block the light from the bottom through the optimization of the thickness of the buffer layer. There are various ongoing technological studies on transparent and flexible displays that to observe the contents without opening the door through the smart window and refrigerator. For this application, the thin film barrier is an essential element and expect to be implemented.Table of Contents Abstract.........................................................................1 Contents........................................................................6 List of Figures.................................................................9 List of Tables................................................................15 Chapter 1. Introduction................................................16 1.1. Graphene characteristics 1.2. Amorphous Si:H and LTPS TFT backplane technology in display 1.3. High performance amorphous In-Ga-Zn-O TFTs 1.4. Overview of PECVD system 1.5. References Chapter 2. Growth of thin graphite films for solid diffusion barriers .......................................................60 2.1. Large-scale transfer-free growth of thin graphite films at low temperature for solid diffusion barriers 2.1.1. Introduction 2.1.2. Experimental 2.1.3. Results and discussion 2.1.4. Conclusion 2.1.5. References Chapter 3. Growth of silicon germanium films for photo-blocking layers in industrial display.................99 3.1. Silicon germanium photo-blocking layers for a-IGZO based industrial display 3.1.1. Introduction 3.1.2. Experimental 3.1.3. Results and Discussion 3.1.4. Conclusion 3.1.5. References Abstract in Koreanโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆ130 Appendixโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆโ€ฆ135Docto

    On the Reversible Effects of Bias-Stress Applied to Amorphous Indium-Gallium-Zinc-Oxide Thin Film Transistors

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    The role of amorphous IGZO (Indium Gallium Zinc Oxide) in Thin Film Transistors (TFT) has found its application in emerging display technologies such as active matrix liquid crystal display (LCD) and active matrix organic light-emitting diode (AMOLED) due to factors such as high mobility 10-20 cm2/(V.s), low subthreshold swing (~120mV/dec), overall material stability and ease of fabrication. However, prolonged application of gate bias on the TFT results in deterioration of I-V characteristics such as sub-threshold distortion and a distinct shift in threshold voltage. Both positive-bias and negative-bias affects have been investigated. In most cases positive-stress was found to have negligible influence on device characteristics, however a stress induced trap state was evident in certain cases. Negative stress demonstrated a pronounced influence by donor like interface traps, with significant transfer characteristics shift that was reversible over a period of time at room temperature. It was also found that the reversible mechanism to pre-stress conditions was accelerated when samples were subjected to cryogenic temperature (77 K). To improve device performance BG devices were subjected to extended anneals and encapsulated with ALD alumina. These devices were found to have excellent resistance to bias stress. Double gate devices that were subjected to extended anneals and alumina capping revealed similar results with better electrostatics compared to BG devices. The cause and effect of bias stress and its reversible mechanisms on IGZO TFTs has been studied and explained with supporting models

    An amorphous oxide semiconductor thin-film transistor route to oxide electronics

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    Amorphous oxide semiconductor (AOS) thin-film transistors (TFTs) invented only one decade ago are now being commercialized for active-matrix liquid crystal display (AMLCD) backplane applications. They also appear to be well positioned for other flat-panel display applications such as active-matrix organic light-emitting diode (AMOLED) applications, electrophoretic displays, and transparent displays. The objectives of this contribution are to overview AOS materials design; assess indium gallium zinc oxide (IGZO) TFTs for AMLCD and AMOLED applications; identify several technical topics meriting future scrutiny before they can be confidently relied upon as providing a solid scientific foundation for underpinning AOS TFT technology; and briefly speculate on the future of AOS TFTs for display and non-display applications
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