• Journal of the Optical Society of Korea
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• 제16권2호
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• pp.181-184
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• 2012

We report, for the first time, operation frequency dependence of current density-voltage ($J_{OLED}-V_{OLED}$) shift for multi-layer organic light-emitting diodes (OLEDs). When the OLEDs were electrically stressed for 21 hours with 50% duty voltage pulses at 60, 120, 240, and 360 Hz, the JOLED-VOLED shifts were suppressed by half for 360 Hz operation compared with 60 Hz operation, but with little change in emission efficiencies. This frequency dependent $J_{OLED}-V_{OLED}$ shift is believed to be commonly observed for typical multi-layer OLEDs and can be used to further improve lifetime of digitally-driven active-matrix OLED displays.

• 전자공학회논문지
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• 제53권5호
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• pp.87-97
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• 2016

본 논문에서는 시분할 기법을 적용하여 AMOLED 컬럼 구동회로용 DAC의 유효 채널 면적을 최소화한 2단 저항 열 기반의 10비트 DAC를 제안한다. 제안하는 DAC는 시분할 기법 기반의 DEMUX, 6비트 및 4비트의 2단 저항 열 구조를 기반으로 하는 롬 구조의 디코더를 2단계로 사용하여 기존의 디스플레이용 DAC보다 빠른 변환속도를 가지는 동시에 하나의 패널 컬럼 구동을 위한 DAC의 유효 면적을 최소화하였다. 두 번째 단 4비트 저항 열에서는 DAC 채널의 면적과 부하 영향을 줄이는 동시에 버퍼 증폭기로 인한 채널 간 오프셋 부정합을 제거하기 위해 기존의 단위-이득 버퍼 대신 간단한 구조의 전류원으로 대체하였다. 제안하는 1:24 DEMUX는 하나의 클록과 5비트 2진 카운터만을 사용하여, 하나의 DAC 채널이 24개의 컬럼을 순차적으로 구동할 수 있도록 하였다. 각 디스플레이 컬럼을 구동하는 출력 버퍼 입력 단에는 0.9pF의 샘플링 커패시터와 작은 크기의 source follower를 추가하여 top-plate 샘플링 구조를 사용하면서 채널 전하 주입에 의한 영향을 최소화하는 동시에 출력 버퍼의 신호정착 정확도를 향상시켰다. 제안하는 DAC는 $0.18{\mu}m$ CMOS 공정으로 제작하였으며, DAC 출력의 정착 시간은 입력을 '$000_{16}$'에서 '$3FF_{16}$'으로 인가했을 때 62.5ns의 수준을 보인다. 제안하는 DAC 단위 채널의 면적 및 유효 채널 면적은 각각 $0.058mm^2$ 및 $0.002mm^2$이며, 3.3V의 아날로그 및 1.8V의 디지털 전원 전압에서 6.08mW의 전력을 소모한다.

• 한국정보디스플레이학회:학술대회논문집
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• 한국정보디스플레이학회 2008년도 International Meeting on Information Display
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• pp.107-108
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• 2008

The spectacular development of AMLCDs, been made possible by a-Si:H technology, still faces two major drawbacks due to the intrinsic structure of a-Si:H, namely a low mobility and most important a shift of the transfer characteristics of the TFTs when submitted to bias stress. This has lead to strong research in the crystallization of a-Si:H films by laser and furnace annealing to produce polycrystalline silicon TFTs. While these devices show improved mobility and stability, they suffer from uniformity over large areas and increased cost. In the last decade we have focused on microcrystalline silicon (${\mu}c$-Si:H) for bottom gate TFTs, which can hopefully meet all the requirements for mass production of large area AMOLED displays [1,2]. In this presentation we will focus on the transfer of a deposition process based on the use of $SiF_4$-Ar-$H_2$ mixtures from a small area research laboratory reactor into an industrial gen 1 AKT reactor. We will first discuss on the optimization of the process conditions leading to fully crystallized films without any amorphous incubation layer, suitable for bottom gate TFTS, as well as on the use of plasma diagnostics to increase the deposition rate up to 0.5 nm/s [3]. The use of silicon nanocrystals appears as an elegant way to circumvent the opposite requirements of a high deposition rate and a fully crystallized interface [4]. The optimized process conditions are transferred to large area substrates in an industrial environment, on which some process adjustment was required to reproduce the material properties achieved in the laboratory scale reactor. For optimized process conditions, the homogeneity of the optical and electronic properties of the ${\mu}c$-Si:H films deposited on $300{\times}400\;mm$ substrates was checked by a set of complementary techniques. Spectroscopic ellipsometry, Raman spectroscopy, dark conductivity, time resolved microwave conductivity and hydrogen evolution measurements allowed demonstrating an excellent homogeneity in the structure and transport properties of the films. On the basis of these results, optimized process conditions were applied to TFTs, for which both bottom gate and top gate structures were studied aiming to achieve characteristics suitable for driving AMOLED displays. Results on the homogeneity of the TFT characteristics over the large area substrates and stability will be presented, as well as their application as a backplane for an AMOLED display.

• 대한전자공학회논문지SD
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• 제42권12호
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• pp.13-18
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• 2005

본 논문에서는 Poly-ethylene-terephthalate (PET) 기판 위에 Organic Thin Film Transistor (OTFT)와 Organic Light Emitting Diode (OLED)를 직렬 연결시킨 픽셀과 64 x 64 픽셀로 구성된 어레이를 제작하여 동작을 시연하였다. OTFT는 PET 기판과의 호환성을 고려하여 Poly 4-vinylphenol을 게이트 절연체로, 펜타센을 활성층으로 사용하여 제작되었다. 개별 소자 수준에서는 이동도가 $1.0\;cm^2/V{\cdot}sec$로 나타났으나, 어레이에서는 $0.1\~0.2\;cm^2/V{\cdot}sec$로 약 10배 정도 감소하였다. 어레이의 동작을 분석하였고 OTFT의 OLED에 대한 전류구동능력을 확인하였다.

• JSTS:Journal of Semiconductor Technology and Science
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• 제15권5호
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• pp.519-525
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• 2015

Positive bias stress-induced instability in amorphous indium-gallium-zinc-oxide (a-IGZO) bottom-gate thin-film transistors (TFTs) was investigated under high $V_{GS}$/low $V_{DS}$ and low $V_{GS}$/high $V_{DS}$ stress conditions through incorporating a forward/reverse $V_{GS}$ sweep and a low/high $V_{DS}$ read-out conditions. Our results showed that the electron trapping into the gate insulator dominantly occurs when high $V_{GS}$/low $V_{DS}$ stress is applied. On the other hand, when low $V_{GS}$/high $V_{DS}$ stress is applied, it was found that holes are uniformly trapped into the etch stopper and electrons are locally trapped into the gate insulator simultaneously. During a recovery after the high $V_{GS}$/low $V_{DS}$ stress, the trapped electrons were detrapped from the gate insulator. In the case of recovery after the low $V_{GS}$/high $V_{DS}$ stress, it was observed that the electrons in the gate insulator diffuse to a direction toward the source electrode and the holes were detrapped to out of the etch stopper. Also, we found that the potential profile in the a-IGZO bottom-gate TFT becomes complicatedly modulated during the positive $V_{GS}/V_{DS}$ stress and the recovery causing various threshold voltages and subthreshold swings under various read-out conditions, and this modulation needs to be fully considered in the design of oxide TFT-based active matrix organic light emitting diode display backplane.

• 한국전기전자재료학회논문지
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• 제16권4호
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• pp.292-297
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• 2003

We fabricated a single crystal silicon thin film transistor for active matrix organic light emitting displays(AMOLEDs) using silicon on insulator wafer (SOI wafer). Poly crystal silicon thin film transistor(poly-Si TFT) Is actively researched and developed nowsdays for a pixel switching devices of AMOLEDs. However, poly-Si TFT has some disadvantages such as high off-state leakage currents and low field-effect mobility due to a trap of grain boundary in active channel. While single crystal silicon TFT has many advantages such as high field effect mobility, low off-state leakage currents, low power consumption because of the low threshold voltage and simultaneous integration of driving ICs on a substrate. In our experiment, we compared the property of poly-Si TFT with that of SOI TFT. Poly-Si TFT exhibited a field effect mobility of 34 $\textrm{cm}^2$/Vs, an off-state leakage current of about l${\times}$10$\^$-9/ A at the gate voltage of 10 V, a subthreshold slope of 0.5 V/dec and on/off ratio of 10$\^$-4/, a threshold voltage of 7.8 V. Otherwise, single crystal silicon TFT on SOI wafer exhibited a field effect mobility of 750 $\textrm{cm}^2$/Vs, an off-state leakage current of about 1${\times}$10$\^$-10/ A at the gate voltage of 10 V, a subthreshold slope of 0.59 V/dec and on/off ratio of 10$\^$7/, a threshold voltage of 6.75 V. So, we observed that the properties of single crystal silicon TFT using SOI wafer are better than those of Poly Si TFT. For the pixel driver in AMOLEDs, the best suitable pixel driver is single crystal silicon TFT using SOI wafer.