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    Pโ€102: Amorphous Silicon Thinโ€Film Transistorsโ€based Activeโ€Matrix Organic Lightโ€Emitting Displays

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    In this paper, we describe hydrogenated amorphous silicon (aโ€Si:H) thinโ€film transistor (TFT)โ€based activeโ€matrix arrays for activeโ€matrix organic lightโ€emitting displays (AMโ€OLEDs). The proposed pixel electrode circuits based on three aโ€Si:H TFTs can supply a continuous output current for AMโ€OLEDs. Each pixel circuit has compensation circuits that can adjust for the OLED and aโ€Si:H TFTs electrical characteristics shifts.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/92089/1/1.1830416.pd

    Progress and challenges in commercialization of organic electronics

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    ๊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•

    Vertical Thin Film Transistors for Large Area Electronics

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    The prospect of producing nanometer channel-length thin film transistors (TFTs) for active matrix addressed pixelated arrays opens up new high-performance applications in which the most amenable device topology is the vertical thin film transistor (VTFT) in view of its small area. The previous attempts at fabricating VTFTs have yielded devices with a high drain leakage current, a low ON/OFF current ratio, and no saturation behaviour in the output current at high drain voltages, all induced by short channel effects. To overcome these adversities, particularly dominant as the channel length approaches the nano-scale regime, the reduction of the gate dielectric thickness is essential. However, the problems with scaling the gate dielectric thickness are the high gate leakage current and early dielectric breakdown of the insulator, deteriorating the device performance and reliability. A novel ultra-thin SiNx film suitable for the application as the gate dielectric of short channel TFTs and VTFTs is developed. The deposition is performed in a standard 13.56MHz PECVD system with silane and ammonia precursor gasses diluted in nitrogen. The deposited 50nm SiNx films demonstrate excellent electrical characteristics in terms of a leakage current of 0.1 nA/cmยฒ and a breakdown electric field of 5.6MV/cm. Subsequently, the state of the art performances of 0.5ยตm channel length VTFTs with 50 and 30nm thick SiNx gate dielectrics are presented in this thesis. The transistors exhibit ON/OFF current ratios over 10^9, the subthreshold slopes as sharp as 0.23 V/dec, and leakage currents in the fA range. More significantly, a high associated yield is obtained for the fabrication of these devices on 3-inch rigid substrates. Finally, to illustrate the tremendous potential of the VTFT for the large area electronics, a 2.2-inch QVGA AMOLD display with in-pixel VTFT-based driver circuits is designed and fabricated. An outstanding value of 56% compared to the 30% produced by conventional technology is achieved as the aperture ratio of the display. Moreover, the initial measurement results reveal an excellent uniformity of the circuit elements.1 yea

    Thin-Film Transistor Integration for Biomedical Imaging and AMOLED Displays

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    Thin film transistor (TFT) backplanes are being continuously researched for new applications such as active-matrix organic light emitting diode (AMOLED) displays, sensors, and x-ray imagers. However, the circuits implemented in presently available fabrication technologies including poly silicon (poly-Si), hydrogenated amorphous silicon (a-Si:H), and organic semiconductor, are prone to spatial and/or temporal non-uniformities. While current-programmed active matrix (AM) can tolerate mismatches and non-uniformity caused by aging, the long settling time is a significant limitation. Consequently, acceleration schemes are needed and are proposed to reduce the settling time to 20 ยตs. This technique is used in the development of a pixel circuit and system for biomedical imager and sensor. Here, a metal-insulator-semiconductor (MIS) capacitor is adopted for adjustment and boost of the circuit gain. Thus, the new pixel architecture supports multi-modality imaging for a wide range of applications with various input signal intensities. Also, for applications with lower current levels, a fast current-mode line driver is developed based on positive feedback which controls the effect of the parasitic capacitance. The measured settling time of a conventional current source is around 2 ms for a 100-nA input current and 200-pF parasitic capacitance whereas it is less than 4 ฮผs for the driver presented here. For displays needed in mobile devices such as cell phones and DVD players, another new driving scheme is devised that provides for a high temporal stability, low-power consumption, high tolerance of temperature variations, and high resolution. The performance of the new driving scheme is demonstrated in a 9-inch fabricated display intended for DVD players. Also, a multi-modal imager pixel circuit is developed using this technique to provide for gain-adjustment capability. Here, the readout operation is not destructive, enabling the use of low-cost readout circuitry and noise reduction techniques. In addition, a highly stable and reliable driving scheme, based on step calibration is introduced for high precision displays and imagers. This scheme takes advantage of the slow aging of the electronics in the backplane to simplify the drive electronics. The other attractive features of this newly developed driving scheme are its simplicity, low-power consumption, and fast programming critical for implementation of large-area and high-resolution active matrix arrays for high precision

    Organic Photodiodes and Their Optoelectronic Applications

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    Recently, organic photodiodes (OPDs) have been acknowledged as a next-generation device for photovoltaic and image sensor applications due to their advantages of large area process, light weight, mechanical flexibility, and excellent photoresponse. This dissertation targets for the development and understanding of high performance organic photodiodes for their medical and industrial applications for the next-generation. As the first research focus, A dielectric / metal / dielectric (DMD) transparent electrode is proposed for the top-illumination OPDs. The fabricated DMD transparent electrode showed the maximum optical transmittance of 85.7 % with sheet resistance of 6.2 ohm/sq. In the second part of the thesis, a development of novel transfer process which enables the dark current suppression for the inverted OPD devices will be discussed. Through the effort, we demonstrated OPD with high D* of 4.82 x 10^12 Jones at reverse bias of 1.5 V with dark current density (Jdark) of 7.7 nA/cm2 and external quantum efficiency (EQE) of 60 %. Additionally in the third part, we investigate a high performance low-bandgap polymer OPD with broadband spectrum. By utilizing the novel transfer process to introduce charge blocking layers, significant suppression of the dark current is achieved while high EQE of the device is preserved. A low Jdark of 5 nA/cm2 at reverse bias of 0.5 V was achieved resulting in the highest D* of 1.5 x 10^13 Jones. To investigate the benefit for the various OPD applications, we developed a novel 3D printing technique to fabricate OPD on hemispherical concave substrate. The techniques allowed the direct patterning of the OPD devices on hemispherical substrates without excessive strain or deformation. Lastly, a simulation of the OPD stacked a-ITZO TFT active pixel sensor (APS) pixel with external transimpedance amplifier (TIA) readout circuit was performed.PHDElectrical & Computer Eng PhDUniversity of Michigan, Horace H. Rackham School of Graduate Studieshttps://deepblue.lib.umich.edu/bitstream/2027.42/137168/1/hyunskim_1.pd
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