657 research outputs found

    On variability and reliability of poly-Si thin-film transistors

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    In contrast to conventional bulk-silicon technology, polysilicon (poly-Si) thin-film transistors (TFTs) can be implanted in flexible substrate and can have low process temperature. These attributes make poly-Si TFT technology more attractive for new applications, such as flexible displays, biosensors, and smart clothing. However, due to the random nature of grain boundaries (GBs) in poly-Si film and self-heating enhanced negative bias temperature instability (NBTI), the variability and reliability of poly-Si TFTs are the main obstacles that impede the application of poly-Si TFTs in high-performance circuits. The primary focus of this dissertation is to develop new design methodologies and modeling techniques for facilitating new applications of poly-Si TFT technology. In order to do that, a physical model is first presented to characterize the GB-induced transistor threshold voltage (V th)variations considering not only the number but also the position and orientation of each GB in 3-D space. The fast computation time of the proposed model makes it suitable for evaluation of GB-induced transistor Vthvariation in the early design phase. Furthermore, a self-consistent electro-thermal model that considers the effects of device geometry, substrate material, and stress conditions on NBTI is proposed. With the proposed modeling methodology, the significant impacts of device geometry, substrate, and supply voltage on NBTI in poly-Si TFTs are shown. From a circuit design perspective, a voltage programming pixel circuit is developed for active-matrix organic light emitting diode (AMOLED) displays for compensating the shift of Vth and mobility in driver TFTs as well as compensating the supply voltage degradation. In addition, a self-repair design methodology is proposed to compensate the GB-induced variations for liquid crystal displays (LCDs) and AMOLED displays. Based on the simulation results, the proposed circuit can decrease the required supply voltage by 20% without performance and yield degradation. In the final section of this dissertation, an optimization methodology for circuit-level reliability tests is explored. To effectively predict circuit lifetime, accelerated aging (i.e. elevated voltage and temperature) is commonly applied in circuit-level reliability tests, such as constant voltage stress (CVS) and ramp voltage stress (RVS) tests. However, due to the accelerated aging, shifting of dominant degradation mechanism might occur leading to the wrong lifetime prediction. To get around this issue, we proposed a technique to determine the proper stress range for accelerated aging tests

    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

    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

    ๊ธˆ์† ์‚ฐํ™”๋ฌผ ๋ฐ ์ด์ฐจ์› ๋‚˜๋…ธ ๋ฌผ์งˆ ๊ธฐ๋ฐ˜์˜ ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ: ์„ฑ๋Šฅ ์ตœ์ ํ™” ๋ฐ ์–‘์ž์  ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ์— ๋Œ€ํ•œ ์‘์šฉ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2021.8. ๊ณฝ์ •ํ›ˆ.๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ๋ฅผ ์ง‘์ ํ•œ ์ „์ž ๋””์Šคํ”Œ๋ ˆ์ด์˜ ๊ฐœ๋ฐœ์€ ๋›ฐ์–ด๋‚œ ์žฅ์ ์œผ๋กœ ์ธํ•ด ํฐ ๊ด€์‹ฌ์„ ๋ฐ›์•„์™”๋‹ค. ์ง€๋‚œ ์ˆ˜์‹ญ ๋…„ ๋™์•ˆ ๋Šฅ๋™ ๋งคํŠธ๋ฆญ์Šค ์•ก์ • ๋””์Šคํ”Œ๋ ˆ์ด ๋ฐ ์œ ๊ธฐ ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ์™€ ๊ฐ™์€ ํ‰ํŒ ๋””์Šคํ”Œ๋ ˆ์ด์— ๋Œ€ํ•œ ์—ฌ๋Ÿฌ ์—ฐ๊ตฌ๊ฐ€ ๋ณด๊ณ ๋˜์—ˆ์Šต๋‹ˆ๋‹ค. ์ด๋Ÿฌํ•œ ์šฐ์ˆ˜ํ•œ ์„ฑ๊ณผ์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ , pํ˜• ์‚ฐํ™”๋ฌผ/๋‚˜๋…ธ ๋ฐ˜๋„์ฒด์˜ ๊ฐœ๋ฐœ๊ณผ ๋ฐฑํ”Œ๋ ˆ์ธ ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ๋กœ ๊ตฌ๋™๋˜๋Š” ์–‘์ž์  ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ์˜ ๊ตฌ๋™์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋Š” ์ œํ•œ์ ์ž…๋‹ˆ๋‹ค. pํ˜• ๋ฐ˜๋„์ฒด์˜ ์ „๊ธฐ์  ํŠน์„ฑ์€ ์ด๋™๋„๊ฐ€ ๋‚ฎ๊ณ , ์˜คํ”„ ์ „๋ฅ˜๊ฐ€ ๋†’์œผ๋ฉฐ, ์†Œ์ž์˜ ๋ถˆ์•ˆ์ •์„ฑ์ด ์žˆ๊ธฐ ๋•Œ๋ฌธ์ž…๋‹ˆ๋‹ค. ์ด๋Ÿฌํ•œ ์˜๋ฏธ์—์„œ ์šฐ๋ฆฌ๋Š” ์•ž์„œ ์–ธ๊ธ‰ํ•œ ์‘์šฉ์„ ์œ„ํ•œ p-ํ˜• ์‚ฐํ™”๋ฌผ/๋‚˜๋…ธ ๋ฌผ์งˆ ๊ธฐ๋ฐ˜ ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ์™€ ์ฝœ๋กœ์ด๋“œ ์–‘์ž์  ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ๋ฅผ ์—ฐ๊ตฌํ–ˆ์Šต๋‹ˆ๋‹ค. ๋จผ์ €, ์šฐ๋ฆฌ๋Š” ์œ ์—ฐํ•œ ์ „์ž ์žฅ์น˜์— ์ž ์žฌ์ ์œผ๋กœ ๋งค๋ ฅ์ ์ธ ๋‚˜๋…ธ ์™€์ด์–ด ๊ตฌ์กฐ๋กœ ํ˜•์„ฑ๋œ ๋Œ€์ฒด ์ „๊ทน์œผ๋กœ ์ „๊ธฐ์  ํŠน์„ฑ์„ ์œ„ํ•ด ์Šคํ”„๋ ˆ์ด ์ฝ”ํŒ…๋œ ๋‹จ์ผ๋ฒฝ ํƒ„์†Œ๋‚˜๋…ธ ํŠœ๋ธŒ๋ฅผ ์†Œ์Šค ๋ฐ ๋“œ๋ ˆ์ธ ์ „๊ทน์œผ๋กœ ์‚ฌ์šฉํ•˜๋Š” p ํ˜• ์ฃผ์„ ์‚ฐํ™”๋ฌผ (SnO) ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ๋ฅผ ๊ตฌํ˜„ํ–ˆ์Šต๋‹ˆ๋‹ค. ํด๋ฆฌ๋จธ ์—์น˜ ์Šคํ† ํผ ์ธต์— SU-8์ด ์žˆ๋Š” SnO ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ์˜ ์†Œ์ž ๊ตฌ์กฐ๋Š” SnO ์ฑ„๋„ ์ธต์˜ ์—ดํ™” ์—†์ด ์›ํ•˜๋Š” ์˜์—ญ์—์„œ ๋‹จ์ผ๋ฒฝ ํƒ„์†Œ๋‚˜๋…ธํŠœ๋ธŒ์˜ ์„ ํƒ์  ์—์นญ์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•ฉ๋‹ˆ๋‹ค. ๋˜ํ•œ ๋‹จ์ผ๋ฒฝ ํƒ„์†Œ๋‚˜๋…ธํŠœ๋ธŒ ์ „๊ทน์œผ๋กœ ์‚ฌ์šฉํ•˜๋Š” SnO ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ๋Š” ์ ์ ˆํ•œ ์ฑ„๋„ํญ๊ณผ ์ •๊ทœํ™”๋œ ์ „๊ธฐ์  ์ปจํƒ ํŠน์„ฑ (~ 1 kฮฉ cm), ์ „๊ณ„ ํšจ๊ณผ ์ด๋™์„ฑ (~ 0.69 cm2/Vs), ๋ฌธํ„ฑ์ „์••์ดํ•˜ ์Šค์œ™ (~ 0.4 V/dec) ๋ฐ ์ „๋ฅ˜ ์˜จ-์˜คํ”„ ํŠน์„ฑ (Ion/Ioff ~ 3.5ร—103)์„ ์„ฑ๊ณต์ ์œผ๋กœ ๊ตฌํ˜„ํ•˜์˜€์Šต๋‹ˆ๋‹ค. ๋˜ํ•œ ์˜จ๋„์— ๋”ฐ๋ฅธ ์ „๊ธฐ์  ์ปจํƒ ๋ฐ ์ฑ„๋„ ํŠน์„ฑ์€ Ni ์ „๊ทน์— ํ•„์ ํ•˜๋Š” ์ ์ ˆํ•œ ์ ‘์ด‰ ์ €ํ•ญ๊ณผ ํ•จ๊ป˜ ๋ฌด์‹œํ•  ์ˆ˜ ์žˆ๋Š” ์ˆ˜์ค€์˜ ๊ฐ€์ „์ž๋  ํ…Œ์ผ ์Šคํ…Œ์ดํŠธ์˜ 3 x 10-3 eV ํ™œ์„ฑํ™” ์—๋„ˆ์ง€๋กœ SnO ์ฑ„๋„ ์ „์†ก์„ ์„ค๋ช…ํ•ฉ๋‹ˆ๋‹ค. ๋‘˜์งธ, ์šฐ๋ฆฌ๋Š” ๋จผ์ € ์ƒ๋ณดํ˜• ํŠธ๋žœ์ง€์Šคํ„ฐ๋ฅผ ๊ตฌํ˜„ํ•˜์—ฌ p (๋˜๋Š” n ํ˜•) MoTe2 ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ์— ์˜ํ•ด ์ œ์–ด๋˜๋Š” ์–‘์ž์  ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ ๊ตฌ๋™์„ ์‹œ์—ฐํ•ฉ๋‹ˆ๋‹ค. ์ด ์—ฐ๊ตฌ์—์„œ๋Š” MoTe2 ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ์˜ ์œ ํ˜• ๋ณ€ํ™˜์„ ์œ„ํ•ด Poly-L-lysine (PLL)์— ์˜ํ•œ ๋ถ„์ž ๋„ํ•‘์„ ๋„์ž…ํ•˜๊ณ , ์–‘์ž์  ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ ์„ฑ๋Šฅ ํ–ฅ์ƒ์„ ์œ„ํ•ด ํ‘œ๋ฉด ๋ฆฌ๊ฐ„๋“œ ๋ณ€ํ˜•์„ ํ™œ์šฉํ•ฉ๋‹ˆ๋‹ค. ์ด์™€ ๊ด€๋ จํ•˜์—ฌ PLL ์ฒ˜๋ฆฌ๋Š” ์ „๊ธฐ์  ํŠน์„ฑ์˜ ์ €ํ•˜์—†์ด MoTe2 ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ์˜ ๋›ฐ์–ด๋‚œ ์œ ํ˜• ๋ณ€ํ™˜์„ ๋‹ฌ์„ฑํ•˜์—ฌ, ์•ˆ์ •์ ์ธ p (๋˜๋Š” n ํ˜•) ์œ ํ˜• ์žฅ์น˜๋ฅผ ํ™•๋ณดํ•˜์—ฌ ๋ณด์™„ ํšŒ๋กœ์˜ ๊ฐ€์šฉ์„ฑ์„ ๋ณด์žฅํ•ฉ๋‹ˆ๋‹ค. ๋˜ํ•œ, ์˜ฅํ‹ธ ์•„๋ฏผ์œผ๋กœ ๋ฆฌ๊ฐ„๋“œ ์น˜ํ™˜๋œ ์–‘์ž์ ์€ ์–‘์ž์  ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ์—์„œ ๊ท ํ˜• ์žกํžŒ ์ „์ž/์ •๊ณต ์ฃผ์ž…์„ ์ƒ์„ฑํ•˜์—ฌ, ์ „๋ฅ˜ ํšจ์œจ (ฮทA = 13.9 cd/A)์ด ๊ฐœ์„ ๋˜๊ณ  ์ˆ˜๋ช…์ด ๋” ๊ธธ์–ด์ง‘๋‹ˆ๋‹ค (L0 = 3000 cd/m2์—์„œ T50 = 66 h). ๊ฒฐ๊ณผ์ ์œผ๋กœ MoTe2 ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ๋Š” ์ ์ ˆํ•œ ์Šค์œ„์นญ ํŠน์„ฑ์„ ๊ฐ€์ง„ ๋””์Šคํ”Œ๋ ˆ์ด ๋ฐฑํ”Œ๋ ˆ์ธ ํŠธ๋žœ์ง€์Šคํ„ฐ, ๊ด‘ ์ „๋ฅ˜ ์ƒ์„ฑ์— ๋Œ€ํ•œ ๋‚ด์„ฑ ๋ฐ ์ž‘๋™ ์•ˆ์ •์„ฑ์„ ํฌํ•จํ•˜์—ฌ ์–‘์ž์  ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ๋ฅผ ๊ตฌ๋™ํ•˜๋Š” ๋Šฅ๋ ฅ์„ ๋ณด์—ฌ์ค๋‹ˆ๋‹ค. ์ด ๋…ผ๋ฌธ์—์„œ ์šฐ๋ฆฌ๋Š” ์œ ๋งํ•œ ์‘์šฉ์„ ์œ„ํ•œ ์‚ฐํ™”๋ฌผ/๋‚˜๋…ธ ๋ฌผ์งˆ ๊ธฐ๋ฐ˜ ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šคํ„ฐ์™€ ๋ฆฌ๊ฐ„๋“œ ์น˜ํ™˜ ๊ธฐ์ˆ ์ด ์ ์šฉ๋œ ํ›„๋ฉด ๋ฐœ๊ด‘ ์ ์ƒ‰ ์–‘์ž์  ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ์— ๋Œ€ํ•ด ๋…ผ์˜ํ•ฉ๋‹ˆ๋‹ค. ๋ฐฑํ”Œ๋ ˆ์ธ ๋ฐ•๋ง‰ ํŠธ๋žœ์ง€์Šค๋กœ pํ˜• SnO์™€ MoTe2๋ฅผ ์‚ฌ์šฉํ•˜๊ณ , ์ƒˆ๋กœ์šด ๋””์Šคํ”Œ๋ ˆ์ด ์žฅ์น˜๋กœ CdSe ์–‘์ž์  ๋ฐœ๊ด‘ ๋‹ค์ด์˜ค๋“œ๋ฅผ ์‚ฌ์šฉํ•œ ์šฐ๋ฆฌ์˜ ์—ฐ๊ตฌ ์„ฑ๊ณผ๋Š” ์œตํ•ฉ ์—ฐ๊ตฌ๋ฅผ ์œ„ํ•œ ๊ตฌ์ƒ ๋ถ„์•ผ์—์„œ ์ž ์žฌ์ ์œผ๋กœ ์‚ฌ์šฉ๋  ์ˆ˜ ์žˆ์Šต๋‹ˆ๋‹ค.The development of electronic displays integrated with Thin Film Transistors (TFTs) has been great interests due to their superb merits. For the past decades, several studies have been reported for the flat-panel displays (FPDs) such as active-matrix liquid crystal display (LCD) and organic light-emitting diode (OLED). Despite of these excellent achievements, progress of p-type oxide/nano semiconductors and operation of quantum dot light-emitting diode (QLED) driven by backplane TFTs are limited. This is because the electrical characteristics of p-type semiconductor have low mobility, high off current, and device instability. In this sense, we investigated p-type oxide/nano material-based TFTs and colloidal quantum dot light-emitting diodes (QLEDs) for the afore-mentioned application. First, we implemented p-type tin oxide (SnO) TFTs with spray-coated single-wall carbon nanotube (SWNTs) as source and drain electrodes for their electrical characteristics as alternative electrodes formed of nanowire structures, which are potentially attractive for flexible electronics. The device architecture of SnO TFTs with a polymer etch stop layer (SU-8) enables the selective etching of SWNTs in a desired region without the detrimental effects of SnO channel layers. In addition, SnO TFTs with SWNT electrodes as substitutes successfully demonstrate decent width normalized electrical contact properties (~1 kฮฉ cm), field effect mobility (~0.69 cm2/Vs), sub-threshold slope (~0.4 V/dec), and current on-off ratio (Ion/Ioff ~ 3.5ร—103). Furthermore, temperature-dependent electrical contact and channel properties elucidate SnO channel transports with an activation energy of 3ร—10-3 eV, interpreted as a negligible level of valence-band tail states, together with decent contact resistance comparable to that of Ni electrodes. Second, we firstly demonstrated the QLEDs operation modulated by p (or n-type) MoTe2 TFTs with the realization of complementary type transistor. In this study, molecular doping by Poly-L-lysine (PLL) as an electron dopant is adopted for a type conversion of MoTe2 TFTs, and surface ligand modification is utilized for the improvement of QLED performance. In this regard, the PLL treatment achieves the outstanding type conversion of MoTe2 TFTs without any degradation of electrical properties, leading to securing reliable p (or n-type) devices, thus, availability of complementary circuits. Furthermore, ligand modified QDs capped with octylamine result in balanced electron/hole injection in QLEDs, yielding improved current efficiency (ฮทA =13.9 cd/A) and longer lifetimes (T50 = 66 h at L0 = 3000 cd/m2). As a result, MoTe2 TFTs demonstrate their capabilities to drive the QLEDs for the envisioned application including display backplane transistor with decent switching properties, immunity for generation of photocurrent, and operation stability. In this thesis, we discuss the oxide/nano material based TFTs and ligand modified bottom emitting red QLEDs for many promising applications. Our research achievements using p-type SnO and MoTe2 as backplane TFTs, and CdSe QLED as novel display device can be used in potentially envision fields for the convergence research.Chapter 1 1 1.1 An Overview of Thin Film Transistors 1 1.2 An Overview of Quantum Dot Light-Emitting Diodes 8 1.3 Outline of Thesis 13 Chapter 2 15 2.1 Materials 15 2.1.1 Synthesis of ZnO Nanoparticles 15 2.1.2 Synthesis of Red Light-Emitting CdSe/Cd1-xZnxS Quantumd Dots 15 2.2 Device Characterization of Thin Film Transistors 17 2.2.1 Characterization for Thin Film Transistor 17 2.2.2 Characterization of Light Response 18 2.3 Device Characterization of Quantum Dot Light-Emitting Diodes 18 2.3.1 Current-voltage-luminance Measurement of QLEDs 18 2.3.2 Efficiency Calculation Methods 21 2.3.3 Other Characterization Methods 22 Chapter 3 24 3.1 Devic Fabrication of SnO TFTs with Spray-Coated Single Walled Carbon Nanotubes as S/D Electrodes 26 3.2 Electrical Performance of SnO TFTs 30 3.3 Contact Resistance of Spray-coated SWNTs as S/D Electrodes 33 3.4 Summary 40 Chapter 4 41 4.1 Description of QLED display driven by MoTe2 TFTs 45 4.2 Ligand Modification of Red CdSe/Cd1-xZnxS Quantum Dots 49 4.3 Type Conversion of MoTe2 TFTs via Electron-Donated Charge Enhancer 54 4.4 Light-Insensitive Behaviors on Photocurrent Generation in MoTe2 TFTs 61 4.5 Operation of QLEDs Driven by Channel-type Controlled MoTe2 TFTs 66 4.6 Summary 70 Chapter 5 71 Bibilography 73 ํ•œ๊ธ€ ์ดˆ๋ก 81๋ฐ•

    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

    Wide Bandwidth - High Accuracy Control Loops in the presence of Slow Varying Signals and Applications in Active Matrix Organic Light Emitting Displays and Sensor Arrays

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    This dissertation deals with the problems of modern active matrix organic light-emitting diode AMOLED display back-plane drivers and sensor arrays. The research described here, aims to classify recently utilized compensation techniques into distinct groups and further pinpoint their advantages and shortcomings. Additionally, a way of describing the loops as mathematical constructs is utilized to derive new circuits from the analog design perspective. A novel principle on display driving is derived by observing those mathematical control loop models and it is analyzed and evaluated as a novel way of pixel driving. Specifically, a new feedback current programming architecture and method is described and validated through experiments, which is compatible with AMOLED displays having the two transistor one capacitor (2T1C) pixel structure. The new pixel programming approach is compatible with all TFT technologies and can compensate for non-uniformities in both threshold voltage and carrier mobility of the pixel OLED drive TFT. Data gathered show that a pixel drive current of 20 nA can be programmed in less than 10usec. This new approach can be implemented within an AMOLED external or integrated display data driver. The method to achieve robustness in the operation of the loop is also presented here, observed through a series of measurements. All the peripheral blocks implementing the design are presented and analyzed through simulations and verified experimentally. Sources of noise are identified and eliminated, while new techniques for better isolation from digital noise are described and tested on a newly fabricated driver. Multiple versions of the new proposed circuit are outlined, simulated, fabricated and measured to evaluate their performance.A novel active matrix array approach suitable for a compact multi-channel gas sensor platform is also described. The proposed active matrix sensor array utilizes an array of P-i-N diodes each connected in series with an Inter-Digitated Electrode (IDE). The functionality of 8x8 and 16x16 sensor arrays measured through external current feedback loops is also presented for the 8x8 arrays and the detection of ammonia (NH3) and chlorine (Cl2) vapor sources is demonstrated

    Thinโ€Film Transistors for Large Area Opto/Electronics

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    The present work addresses several issues in the field of organic and transparent electronics. One of them is the prevailing high power consumption in state-of-the-art organic field-effect transistors (OFETs). A possible solution could be the implementation of complementary, rather than unipolar logic, but this development is currently inhibited by a distinct lack of high performance electron transporting (n-channel) OFETs. Here, the issue is addressed by investigating a series of solution processable n-channel fullerene molecules in combination with optimized transistor architectures. Furthermore, the trend towards complementary circuit design could be facilitated by employing ambipolar organic semiconductors, such as squaraine molecules or polymer/fullerene blends. These materials can fill the role of p- or n-channel semiconductors and enable the facile implementation of power saving complementary-like logic, eliminating the cost-intensive patterned deposition of discrete p-and n-channel transistors. Alternatively, a patterning method for organic materials adapted from standard photolithography is discussed. Furthermore, ambipolar FETs are found to be capable of light sensing at wavelength of 400-1000 nm. Hence their use in low-cost, organic based optical sensor arrays can be envisioned. Another strategy to reduce the power consumption and operating voltages of OFETs is the use of ultra-thin, self-assembled molecular gate dielectrics, such as alkyl-phosphonic acid molecules. Based on this approach solution processed n- and p-channel OFETs and a complementary organic inverter circuit are demonstrated, which operate at less than 2 Volts. Finally, transparent oxide semiconductors are investigated for use in thin-film transistors. Titanium dioxide (TiO2) and zinc oxide (ZnO) films are deposited by means of a low-cost large area compatible spray pyrolysis technique. ZnO transistors exhibit high electron mobility of the order of 10 cm2/Vs and stable operation in air at less than 2 Volts. These results are considered significant steps towards the development of organic and transparent large-area optoelectronics
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