72 research outputs found

    Interpretation and Regulation of Electronic Defects in IGZO TFTs Through Materials & Processes

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    The recent rise in the market for consumer electronics has fueled extensive research in the field of display. Thin-Film Transistors (TFTs) are used as active matrix switching devices for flat panel displays such as LCD and OLED. The following investigation involves an amorphous metal-oxide semiconductor that has the potential for improved performance over current technology, while maintaining high manufacturability. Indium-Gallium-Zinc-Oxide (IGZO) is a semiconductor material which is at the onset of commercialization. The low-temperature large-area deposition compatibility of IGZO makes it an attractive technology from a manufacturing standpoint, with an electron mobility that is 10 times higher than current amorphous silicon technology. The stability of IGZO TFTs continues to be a challenge due to the presence of defect states and problems associated with interface passivation. The goal of this dissertation is to further the understanding of the role of defect states in IGZO, and investigate materials and processes needed to regulate defects to the level at which the associated influence on device operation is controlled. The relationships between processes associated with IGZO TFT operation including IGZO sputter deposition, annealing conditions and back-channel passivation are established through process experimentation, materials analysis, electrical characterization, and modeling of electronic properties and transistor behavior. Each of these components has been essential in formulating and testing several hypotheses on the mechanisms involved, and directing efforts towards achieving the goal. Key accomplishments and quantified results are summarized as follows: โ€ข XPS analysis identified differences in oxygen vacancies in samples before and after oxidizing ambient annealing at 400 ยฐC, showing a drop in relative integrated area of the O 1s peak from 32% to 19%, which experimentally translates to over a thousand fold decrease in the channel free electron concentration. โ€ข Transport behavior at cryogenic temperatures identified variable range hopping as the electron transport mechanism at temperature below 130 K, whereas at temperature greater than 130 K, the current vs temperature response followed an Arrhenius relationship consistent with extended state transport. โ€ข Refinement of an IGZO material model for TCAD simulation, which consists of oxygen vacancy donors providing an integrated space charge concentration NVO = +5e15 cm-3, and acceptor-like band-tail states with a total integrated ionized concentration of NTA = -2e18 cm-3. An intrinsic electron mobility was established to be Un = 12.7 cm2/Vโˆ™s. โ€ข A SPICE-compatible 2D on-state operation model for IGZO TFTs has been developed which includes the integration of drain-impressed deionization of band-tail states and results in a 2D modification of free channel charge. The model provides an exceptional match to measured data and TCAD simulation, with model parameters for channel mobility (Uch = 12 cm2/Vโˆ™s) and threshold voltage (VT = 0.14 V) having a close match to TCAD analogs. โ€ข TCAD material and device models for bottom-gate and double-gate TFT configurations have been developed which depict the role of defect states on device operation, as well as provide insight and support of a presented hypothesis on DIBL like device behavior associated with back-channel interface trap inhomogeneity. This phenomenon has been named Trap Associated Barrier Lowering (TABL). โ€ข A process integration scheme has been developed that includes IGZO back-channel passivation with PECVD SiO2, furnace annealing in O2 at 400 ยฐC, and a thin capping layer of alumina deposited via atomic layer deposition. This process supports device stability when subjected to negative and positive bias stress conditions, and thermal stability up to 140 ยฐC. It also enables TFT operation at short channel lengths (Leff ~ 3 ยตm) with steep subthreshold characteristics (SS ~ 120 mV/dec). The details of these contributions in the interpretation and regulation of electronic defect states in IGZO TFTs is presented, along with the support of device characteristics that are among the best reported in the literature. Additional material on a complementary technology which utilizes flash-lamp annealing of amorphous silicon will also be described. Flash-Lamp Annealed Polycrystalline Silicon (FLAPS) has realized n-channel and p-channel TFTs with promising results, and may provide an option for future applications with the highest performance demands. IGZO is rapidly emerging as the candidate to replace a-Si:H and address the performance needs of display products produced by large panel manufacturing

    Oxide transistors produced by Combustion Synthesis: Influence of the PVP on the properties of the insulator

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    Solution processing of amorphous metal oxides has been used as an option to implement in flexible electronics, allowing to reduce the associated costs, when compared with vacuum processes. Recent research has been more focused on the semiconductor layer; however, the dielectric layer is equally important since its responsible for the stability and electric performance of the device. This work aims to evaluate hybrid dielectric thin films, using aluminium oxide and different types of polyvinylpyrrolidone (PVP), both obtained by solution process using solution combustion synthesis (SCS), to study the influence of the amount of organic material used in the insulator layer, as well as to study the influence of the hybrid insulator obtained in oxide thin film transistors (TFTs) using indium-gallium-zinc-oxide (IGZO) and zinc-tin-oxide (ZTO) as semiconductor layer. The insulator layer was obtained using aluminium nitrate nonahydrate and polyvinylpyrrolidone (PVP) with different molecular weights (10000 and 40000) and different percentages as precursor solutions, using urea as fuel and 2-methoxyethanol as solvent. The best hybrid dielectric was obtained with 0.8 % PVP 40000 (weight per volume), showing a breakdown voltage of 1.1 MV/cm, low density leakage current of 9.6 ร— 10-5 A/cm2, capacitance per area of 123 nF/cm2, thickness of 49.35 nm, annealed at 200 ยฐC for 30 minutes. Moreover, the roughness study obtained using atomic force microscopy showed highly smooth surface, resulting in improvement dielectric-semiconductor interface, while still maintaining an amorphous nature. These characteristics allowed this hybrid dielectric, lead to enhanced TFTs electrical properties. The best performing thin films were applied in IGZO TFTs as hybrid dielectrics. The optimized TFTs show good reproducibility with an average mobility of 40.24 ยฑ 1.1 cm2โˆ™V-1โˆ™s-1, subthreshold slope of 0.169 ยฑ 0.012 Vโˆ™dec-1, a turn-on voltage of 0.078 ยฑ 0.004 V and a low operating voltage (maximum 2 V)

    Ta2O5/SiO2 Multicomponent Dielectrics for Amorphous Oxide TFTs

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    Co-sputtering of SiO2 and high-ฮบ Ta2O5 was used to make multicomponent gate dielectric stacks for In-Ga-Zn-O thin-film transistors (IGZO TFTs) under an overall low thermal budget (T = 150 ยฐC). Characterization of the multicomponent layers and of the TFTs working characteristics (employing them) was performed in terms of static performance, reliability, and stability to understand the role of the incorporation of the high-ฮบ material in the gate dielectric stack. It is shown that inherent disadvantages of the high-ฮบ material, such as poorer interface properties and poor gate insulation, can be counterbalanced by inclusion of SiO2 both mixed with Ta2O5 and as thin interfacial layers. A stack comprising a (Ta2O5)x(SiO2)100 โˆ’ x film with x = 69 and a thin SiO2 film at the interface with IGZO resulted in the best performing TFTs, with field-effect mobility (ยตFE) โ‰ˆ 16 cm2ฮ‡Vโˆ’1ฮ‡sโˆ’1, subthreshold slope (SS) โ‰ˆ 0.15 V/dec and on/off ratio exceeding 107. Anomalous Vth shifts were observed during positive gate bias stress (PGBS), followed by very slow recoveries (time constant exceeding 8 ร— 105 s), and analysis of the stress and recovery processes for the different gate dielectric stacks showed that the relevant mechanism is not dominated by the interfaces but seems to be related to the migration of charged species in the dielectric. The incorporation of additional SiO2 layers into the gate dielectric stack is shown to effectively counterbalance this anomalous shift. This multilayered gate dielectric stack approach is in line with both the large area and the flexible electronics needs, yielding reliable devices with performance suitable for successful integration on new electronic applications.publishersversionpublishe

    Low-temperature amorphous oxide semiconductors for thin-film transistors and memristors: physical insights and applications

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    While amorphous oxides semiconductors (AOS), namely InGaZnO (IGZO), have found market application in the display industry, their disruptive properties permit to envisage for more advanced concepts such as System-on-Panel (SoP) in which AOS devices could be used for addressing (and readout) of sensors and displays, for communication, and even for memory as oxide memristors are candidates for the next-generation memories. This work concerns the application of AOS for these applications considering the low thermal budgets (< 180 ยฐC) required for flexible, low cost and alternative substrates. For maintaining low driving voltages, a sputtered multicomponent/multi-layered high-ฮบ dielectric (Ta2O5+SiO2) was developed for low temperature IGZO TFTs which permitted high performance without sacrificing reliability and stability. Devicesโ€™ performance under temperature was investigated and the bias and temperature dependent mobility was modelled and included in TCAD simulation. Even for IGZO compositions yielding very high thermal activation, circuit topologies for counteracting both this and the bias stress effect were suggested. Channel length scaling of the devices was investigated, showing that operation for radio frequency identification (RFID) can be achieved without significant performance deterioration from short channel effects, which are attenuated by the high-ฮบ dielectric, as is shown in TCAD simulation. The applicability of these devices in SoP is then exemplified by suggesting a large area flexible radiation sensing system with on-chip clock-generation, sensor matrix addressing and signal read-out, performed by the IGZO TFTs. Application for paper electronics was also shown, in which TCAD simulation was used to investigate on the unconventional floating gate structure. AOS memristors are also presented, with two distinct operation modes that could be envisaged for data storage or for synaptic applications. Employing typical TFT methodologies and materials, these are ease to integrate in oxide SoP architectures

    ํ”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

    Process Investigations on Sputter Deposited Indium Tungsten Oxide TFT

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    Indium-Tungsten Oxide (IWO) has been investigated as a potential semiconductor material for next-generation display devices. Several publications have reported on IWO thin-film transistors (TFTs) with a channel mobility ฮผch ~ 20cm2/Vs, approximately 2X higher than typically reported for Indium-Gallium-Zinc Oxide (IGZO). However, other attributes of the device characteristics have not performed as well as IGZO such as the subthreshold behavior. This work presents a study on the electronic properties of sputtered IWO, with the sputter ambient (i.e. percent O2 ) and O2 annealing conditions as the primary factors investigated. In the early stages of the study, a problem with the IWO target surface condition was found to be responsible for non-reproducible TFT properties. This initiated an extensive investigation on the details of target reconditioning, presputter conditions and reactive sputter ambient with oxygen. IWO sputter recipes and procedures were implemented which ensured consistent plasma characteristics and target surface condition. Reactive sputter conditions with low O2 content resulted in electrical behavior that was very different from argon-only sputtering (zero percent oxygen). IWO TFTs processed with 1.2% O2 sputter ambient, followed by O2 annealing at 300ยฐC for 8-10 hours demonstrated promising current-voltage characteristics, with a low-field channel mobility ฮผch ~ 18 cm2/Vs @ VDS = 0.1V. While higher oxygen content sputter conditions (10% O2) demonstrated a higher post-anneal resistivity, the device operation was inferior to the low oxygen treatment TFT. This was apparent in both on-state and off-state conditions, with the low oxygen treatment exhibiting higher current drive and steeper subthreshold. Increasing the O2 anneal temperature to 350ยฐC on TFTs with the low oxygen treatment showed encouraging gate-controlled channel modulation for a 2 hour anneal. Raising this temperature to 400ยฐC resulted in reduced gate control and current modulation, suggesting the onset of an additional defect mechanism. Degradation in device operation demonstrated by the high oxygen treatment as-sputtered material, or by aggressive O2 annealing at T \u3e 350ยฐC, may have a similar origin

    Interpretation and Physical Modeling of Electronic Transport and Defect States in IGZO Thin-Film Transistors

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    This work is a comprehensive study on the interpretation and modeling of electronic transport behavior and defect states in indium-gallium-zinc-oxide (IGZO) TFTs. Key studies have focused on advancing the state of IGZO TFTs by addressing several challenges in device stability, scaling, and device modeling. These studies have provided new insight on the associated mechanisms and have resulted in the realization of scaled thin-film transistors that exhibit excellent electrical performance and stability. This work has demonstrated the ability to scale the conventional inverted staggered IGZO TFT down to one micron channel length, with excellent on-state and off-state performance where the VT โ‰ˆ1 V, ยตeff =12 cm2/Vs, Ileak โ‰ค 10-12 A/ยตm and SS โ‰ˆ 160 mV/dec. The working source/drain electrodes are direct metal contact regions to the IGZO, which requires several microns of gate overlap to provide ohmic behavior with minimal series resistance and ensure tolerance to overlay error. New results utilizing ion implantation for self-aligned source/drain regions present a path towards submicron channel length. This strategy offers a reduction in channel length as well as parasitic capacitance, which translates to improvement in RC delay and associated voltage losses due to charge-sharing. The realization of self-aligned TFTs using boron ion implantation for selective activation was introduced in a first-time report of boron-doped IGZO. Cryogenic measurements made on long-channel devices has revealed temperature-dependent behavior that is not explained by existing TCAD models employed for defect states and carrier mobility. A completely new device model using Silvaco Atlas has been established which properly accounts for the role of donor-like oxygen vacancy defects, acceptor-like band-tail states, acceptor-like interface traps, and a temperature-dependent intrinsic channel mobility. The developed model demonstrates a remarkable match to transfer characteristics measured at T = 150 K to room temperature. A power-law fit for the ยตch = f(T) relationship, which resembles ใ€–ฮผ ~ Tใ€—^((+3)โ„2) behavior consistent with ionized defect scattering. The mobility model is expressly independent of carrier concentration, without dependence on the applied gate bias. The device model is consistent with a compact model developed for circuit simulation (SPICE) that has been recently refined to include on-state and off-state operation. While IGZO is the only AOS technology mature enough for commercialization, the effective electron channel mobility ยตeff ~ 10 cm2/Vs presents a performance limitation. Other candidate AOS materials which have higher reported channel mobility values have also been investigated; specifically, indium-tungsten-oxide (IWO) and indium-gallium-tin-oxide (ITGO). These investigations serve as preliminary studies; device characteristics support the claims of high channel mobility; however the influence of defect states clearly indicates the need for further process development. The advancements realized in IGZO TFTs in this work will serve as a foundation for these alternative AOS materials

    Solution-based IGZO nanoparticles memristor

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    This work aims to characterize Indium-Gallium-Zinc-Oxide nanoparticles (IGZOnp) as a resistive switching matrix in metal-insulator-metal (MIM) structures for memristor application. IGZOnp was produced by low cost solution-based process and deposited by spin-coating technique. Several top and bottom electrodes combinations, including IZO, Pt, Au, Ti, Ag were investigated to evaluate memory performance, yield and switching properties. The effect of ambient and annealing temperature using 350 ยบC and 200 ยบC was also analysed in order to get more insight into resistive switching mechanism. The Ag/IGZOnp/Ti memristor structure annealed at 200 ยบC exhibits the best results with a large yield. The device shows a self-compliant bipolar resistive switching behavior. The switching event is achieved by the set/reset voltages of -1 V/+1 V respectively with an operating window of 10, and it can be programmed for more than 100 endurance cycles. The retention time of on and off-states is up to 104 s. The obtained results suggest that Ag/IGZOnp/Ti structure could be applied in system on a panel (SoP) as a viable device
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