• Title/Summary/Keyword: Passivation layer

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Study on Electro-Optic Characteristics Dependent on Passivation Layer Thickness in the FFS mode using a Liquid Crystal with Positive Dielectric Anisotropy (유전율 이방성이 양인 액정을 이용한 FFS모드의 절연층 두께에 따른 전기 광학 특성 연구)

  • Lee, Ji-Youn;Park, Sang-Hyun;Oh, Sang-Min;Lee, Seung-Hee
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2005.07a
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    • pp.485-486
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    • 2005
  • Fringe-field switching mode which has a horizontal and vertical electric field exhibits high transmittance and wide viewing angle characteristics. In the FFS mode, a passivation layer between common and pixel electrodes exists, which functions as preventing current leakage of fringe-field. In this paper, we have studied LC behavior, transmittance and operating voltage characteristics with applied voltage as a function of the passivation layer thickness and defined optimal value of the layer to be about $0.5{\mu}m$.

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Electro-Optic Characteristics of the Fringe Field Switching (FFS) Mode Depending on Thickness of Passivation Layer between Pixel and Common Electrodes (FFS 모드의 공통전극과 화소전극 사이의 절연층 두께에 따른 전기광학 특성)

  • Jung, Jun-Ho;Ha, Kyung-Su;Lim, Young-Jin;Yoo, Il-Sou;Jeong, Yeon-Hak;Lyu, Jae-Jin;Kim, Kyeong-Hyeon;Lee, Seung-Hee
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.22 no.7
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    • pp.589-594
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    • 2009
  • We have studied electro-optic characteristics as a function of passivation thickness existing between common electrode and pixel electrodes in the fringe-field switching (FFS) mode using the LC with positive dielectric anisotropy. A steep increase in the transmission is observed with increase in the passivation layer from $0.29{\mu}m$ to $1.09{\mu}m$ and thereafter it almost saturates over the $1.09{\mu}m$ of passivation layer. This saturation is mainly associated with correlation between transmittance at the center region of pixel electrode and at the center region between pixel electrodes. From the results, optimal thickness of passivation layer can be defined.

InGaN/GaN Blue LED device 제조시 ALD (Atomic Layer Deposition) 방법으로 증착된 Al2O3 Film의 Passivation 효과

  • Lee, Seong-Gil;Bang, Jin-Bae;Yang, Chung-Mo;Kim, Dong-Seok;Lee, Jeong-Hui
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.08a
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    • pp.211-212
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    • 2010
  • GaN 기반의 상부발광형 LED는 동작되는 동안 생기는 전기적 단락, 그리고 칩 위의 p-형 전극과 n-형 전극 사이에 생기는 누설전류 및 신뢰성 확보를 위하여 칩 표면에 passivation 층을 형성하게 된다. SiO2, Si3N4와 같은 passivation layers는 일반적으로 PECVD (Plasma Enhanced Chemical Vapor Deposition)공정을 이용한다, 하지만 이는 공정 특성상 plasma로 인한 damage가 유발되기 때문에 표면 누설 전류가 증가 한다. 이로 인해 forward voltage와 reverse leakage current의 특성이 저하된다. 본 실험에서는 원자층 단위의 박막 증착으로 인해 PECVD보다 단차 피복성이 매우 우수한 PEALD(Plasma Enhanced Atomic Layer Deposition)공정을 이용하여 Al2O3 passivation layer를 증착한 후, 표면 누설전류와 빛의 출력 특성에 대해서 조사해 보았다. PSS (patterned sapphire substrate) 위에 성장된 LED 에피구조를 사용하였고, TCP(Trancformer Copled Plasma)장비를 사용하여 에칭 공정을 진행하였다. 이때 투명전극을 증착하기 위해 e-beam evaporator를 사용하여 Ni/Au를 각각 $50\;{\AA}$씩 증착한 후 오믹 특성을 향상시키기 위하여 $500^{\circ}C$에서 열처리를 해주었다. 그리고 Ti/Au($300/4000{\AA}$) 메탈을 사용하여 p-전극과 n-전극을 형성하였다. Passivation을 하지 않은 경우에는 reverse leakage current가 -5V 에서 $-1.9{\times}10-8$ A 로 측정되었고, SiO2와 Si3N4을 passivation으로 이용한 경우에는 각각 $8.7{\times}10-9$$-2.2{\times}10-9$로 측정되었다. Fig. 1 에서 보면 알 수 있듯이 5 nm의 Al2O3 film을 passivation layer로 이용할 경우 passivation을 하지 않은 경우를 제외한 다른 passivation 경우보다 reverse leakage current가 약 2 order ($-3.46{\times}10-11$ A) 정도 낮게 측정되었다. 그 이유는 CVD 공정보다 짧은 ALD의 공정시간과 더 낮은 RF Power로 인해 plasma damage를 덜 입게 되어 나타난 것으로 생각된다. Fig. 2 에서는 Al2O3로 passivation을 한 소자의 forward voltage가 SiO2와 Si3N4로 passivation을 한 소자보다 각각 0.07 V와 0.25 V씩 낮아지는 것을 확인할 수 있었다. 또한 Fig. 3 에서는 Al2O3로 passivation을 한 소자의 output power가 SiO2와 Si3N4로 passivation을 한 소자보다 각각 2.7%와 24.6%씩 증가한 것을 볼 수 있다. Output power가 증가된 원인으로는 향상된 forward voltage 및 reverse에서의 leakage 특성과 공기보다 높은 Al2O3의 굴절률이 광출력 효율을 증가시켰기 때문인 것으로 판단된다.

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Pt-AlGaN/GaN HEMT-based hydrogen gas sensors with and without SiNx post-passivation

  • Vuong, Tuan Anh;Kim, Hyungtak
    • Journal of IKEEE
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    • v.23 no.3
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    • pp.1033-1037
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    • 2019
  • GaN-based sensors have been widely investigated thanks to its potential in detecting the presence of hydrogen. In this study, we fabricated hydrogen gas sensors with AlGaN/GaN heterojunction and investigated how the sensing performance to be affected by SiN surface passivation. The gas sensor employed a high electron mobility transistors (HEMTs) with 30 nm platinum catalyst as a gate to detect the hydrogen presence. SiN layer was deposited by inductively-coupled chemical vapor deposition as post-passivation. The sensors with SiN passivation exhibited hydrogen sensing characteristics with various gas flow rates and concentrations of hydrogen in inert background gas at $200^{\circ}C$ similar to the ones without passivation. Aside from quick response time for both sensors, there are differences in sensitivity and recovery time because of the existence of the passivation layer. The results also confirmed the dependence of sensing performance on gas flow rate and gas concentration.

Passivation effect on large volume CdZnTe crystals

  • B. Park;Y. Kim;J. Seo;J. Byun;K. Kim
    • Nuclear Engineering and Technology
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    • v.54 no.12
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    • pp.4620-4624
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    • 2022
  • Several cadmium zinc telluride (CZT) crystals were fabricated into radiation detectors using methods that included slicing, dicing, lapping, polishing, and chemical etching. A wet passivation with sodium hypochlorite (NaOCl) was then carried out on the Br-etched detectors. The Te-rich layer on the CZT surface was successfully compensated to the Te oxide layer, which was analyzed with X-ray photoelectron spectroscopy data of both a Br-etched crystal and a passivated CZT crystals. We confirmed that passivation with NaOCl improved the transport property by analyzing the mobility-lifetime product and surface recombination velocity. The electrical and spectroscopic properties of large volume detectors were compared before and after passivation, and then the detectors were observed for a month. Both bar and quasi-hemispherical detectors show an enhancement in performance after passivation. Thus, we could identify the effect of NaOCl passivation on large volume CZT detectors.

Thin Film Passivation Characteristics in OLED Using In-situ Passivation

  • Kim, Kwan-Do;Shin, Hoon-Kyu;Chang, Sang-Mok
    • Transactions on Electrical and Electronic Materials
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    • v.13 no.2
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    • pp.93-97
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    • 2012
  • In this study, the fabrication and the characteristic analyses of OLED using in-situ passivation are investigated. OLEDs represent a disadvantage in decreasing its life due to the degradation caused by the penetration of moisture and oxygen. After the fabrication of OLED, an in-situ passivation method for inorganic thin films is developed. A process that uses PECVD method which can apply a vapor deposition process at room temperature is also developed. Changes in the degradation and electric characteristics of OLEDs are also analyzed by applying $SiO_2$ and SiNx thin films to OLED as a passivation layer. By applying the fabricated thin film to OLEDs as a passivation layer, the moisture penetration in a single layer film is ensured below $1{\times}10^{-2}\;g/m^2.day$. This leads to the improvement of such degradation characteristics in the application of multilayer films.

Passivation Quality of ALD $Al_2O_3$ Thin Film via Silicon Oxide Interfacial Layer for Crystalline Silicon Solar Cells (실리콘 산화막의 두께에 따른 ALD $Al_2O_3$ 박막의 passivation 효과)

  • Kim, Young-Do;Park, Sung-Eun;Tark, Sung-Ju;Kang, Min-Gu;Kwon, Soon-Woo;Yoon, Se-Wang;Kim, Dong-Hwan
    • 한국신재생에너지학회:학술대회논문집
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    • 2009.06a
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    • pp.93-93
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    • 2009
  • 실리콘 태양전지의 효율 향상을 위한 노력의 일환으로 결정질 실리콘 웨이퍼 표면passivation 물질 중 Atomic Layer Deposition (ALD)을 이용하여 증착한 $Al_2O_3$ 박막에 대한 관심이 증가하고 있다. 본 연구에서는 $Al_2O_3$ 박막의 증착 전 실리콘 웨이퍼의 산화막 두께에 따른 passivation 효과에 대해서 연구하였다. 실리콘 산화막은 $HNO_3$ 용액을 사용하여 화학적으로 생성시켰으며 $HNO_3$ 용액과의 반응 시간을 조절하여 실리콘 산화막의 두께를 조절하였다. 실리콘 산화막 생성 후 ALD로 $Al_2O_3$ 박막을 증착하였으며 증착 후 $N_2$ 분위기에서 annealing 하였다. Annealing 후 passivation 효과는 Quasi-Steady-State Photo Conductance를 사용하여 minority carrier의 lifetime을 측정하였다. Capacitance-Voltage measurement, Transmission Electron Microscopy, Ellipsometry를 사용하여 실리콘 산화막의 두께에 따른 $Al_2O_3$ 박막의 passivation 효과를 분석하였다.

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The formation of the passivation layer by the flourine layer by the fluorine treatment after Al(Cu 1%) plasma etching (Al(Cu 1%) 플라트마 식각후 fluorine 처리에 의한 passivation 막 형성)

  • 김창일;최광호;김상기;백규하;윤용선;남기수;장의구
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.35D no.1
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    • pp.27-33
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    • 1998
  • In this study, chlorine(Cl)-based gas chemistry is generally used to etching for AlCu films metallization.The corrosion phenomena of AlCu films were examined with XPS (X-ray photoelectron spectroscopy), SEM 9Scanning electron microscopy), and TEM (Transmission electron microscopy). SF$_{6}$ plasma treatment sulbsequent to the etching process preventas the corrosion effectively in the pressure of 300 mTorr. It is found that the cholrine atoms on the etched surface are not substituted for fluorine atoms during SF$_{6}$ treatment, but a passivation layer on the surface by fluorine-related compounds would be formed. The passivation layer prevents the moisture penetration on the SF$_{6}$ treated surface and suppresses the corrsion sucessfully.fully.

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InGaAs/InP HPT's with ITO Transparent Emitter Contacts (ITO 에미터 투명전극을 갖는 InGaAs/InP HPT의 연구)

  • Han, Kyo-Yong
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.20 no.3
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    • pp.268-272
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    • 2007
  • A fully integrable InP/InGaAs HPT with an ITO emitter contact was first fabricated by employing a $SiO_2$ passivation layer. The electrical and the optical characteristics of the HPT with a passivation layer were measured and compared with those of the HPT without a passivation layer. The only noticeable difference was the increased emitter series resistance of the HPT with a passivation layer. AES analysis was performed to explain the reason of the increased emitter series resistance. Results show that PECVD $SiO_2$ deposition and annealing processes cause the diffusion of oxygen to the interface and the depletion of tin at the interface, which may be responsible for the increase of the series resistance.

The Effect of Passivation Film with Inorganic/Epoxy Layers on Life Time Characteristics of OLED Device (OLED 내구성에 미치는 무기/에폭시층 보호막의 영향)

  • Lim, Jung-A;Ju, Sung-Hoo;Yang, Jae-Woong
    • Journal of the Korean institute of surface engineering
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    • v.42 no.6
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    • pp.287-293
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    • 2009
  • The passivation films with epoxy layer on LiF, $SiN_x$ and LiF/$SiN_x$ inorganic layer were fabricated on OLED to protect device from the direct damage of $O_2$ and $H_2O$ and to apply for a buffer layer between OLED device and passivation multi-layer with organic/inorganic hybrid structure as to diminish the thermal stress and expansion. Red OLED doped with 1 vol.% Rubrene in $Alq_3$ was used as a basic device. The device structure was multi-layer of ITO(150 nm) / ELM200_HIL(50 nm) / ELM002_HTL(30 nm) / $Alq_3$: 1 vol.% Rubrene(30 nm) / $Alq_3$(30 nm) / LiF(0.7 nm) / Al(100 nm). LiF/epoxy applied as a protective layer didn't contribute to the improvement of life time. While in case of $SiN_x$/epoxy, damage was done in the passivation process because of difference in heat expansion between films which could occur during the formation of epoxy film. Using LiF/$SiN_x$/epoxy improved lifetime significantly without suffering damage in the process of forming films, therefore, the best structure of passivation film with inorganic/epoxy layers was LiF/$SiN_x$/E1.