• 한국결정학회지
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• 제6권2호
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• pp.111-117
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• 1995

화학증착법에 의해 TiO2 박막을 Si-wafer(100)위에 제조하였다. Titanium tetraisopropoxide (TTIP)를 출발물질로 하여 200-500℃의 온도범위에서 증착을 행하였다. 증착된 박막의 두께는 Ellipsometry 및 SEM을 사용하여 측정하였으며, 산소의 함량에 따른 증착층의 성분분석은 ESCA를 사용하였다. TiO2 박막의 증착속도는 산소의 함량에 따라 증가하였고, 반응가스인 산소를 공급하지 않았을 때 증착층내에 불순물로 탄소가 존재하였으며, 증착층의 성분은 내부로 갈수록 TiO2에서 Ti로 변하였다. 산소를 600scm 공급하였을 때 증착층내에 소량의 탄소가 존재하였으며, 증착층의 성분은 내부로 갈수록 TiO2에서 TiO, Ti로 됨을 알 수 있었다. 산소를 1200scm공급하였을 때 증착층내에 탄소가 존재하지 않았으며, 증착층 성분은 표면에는 TiO2를 이루나 증착층 내부로 갈수록 Ti복합화합물을 이루고 있었다.

• 한국재료학회:학술대회논문집
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• 한국재료학회 2009년도 춘계학술발표대회
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• pp.39.1-39.1
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• 2009

본 실험은 연성과 광 투명도가 뛰어난 아크릴 (PMMA) 과 폴리카보네이트 (Polycabonate) 기판의 축전 결합형 플라즈마 (CCP) 건식 식각 연구에 관한 것이다. 특히 식각 반응기 내부의 압력 변화에 따른 두 기판의 건식 식각 특성 분석에 초점을 맞추었다. 실험에 사용된 기판은 두께 1mm의 아크릴 (PMMA) 과 폴리카보네이트 (Polycabonate)를 $1.5\times1.5\;cm^2$로 절단하여 Photo-lithography 공정을 통하여 감광제 (Photo-resist)로 패턴하였다. 식각 반응기 내부에 패턴 된 아크릴(PMMA) 과 폴리카보네이트 (Polycabonate)를 넣은 후 반응기 내부 진공 상태로 만들었다. 그 후 5 sccm $O_2$ 가스를 유량조절기 (Mass flow controller)를 통하여 식각 반응기 내부로 유입하여 실험을 하였다. 이때 식각 공정 변수는 식각 반응기 내부 압력과 샘플 척 파워이다. 특성평가 항목은 식각 후 기판 (Substrate)의 식각율 (Etch rate), 식각 선택비 (Selectivity) 그리고 기판 표면 거칠기 (RMS roughness)이다. 실험 결과는 표면 단차 분석기(Surface profiler)를 이용하여 기판 (Substrate)의 표면을 분석 하였다. 또한 OES (Optical Emission Spectroscopy) 를 이용하여 식각 중 내부 플라즈마의 상태를 분석하였다. 본 실험 결과에 따르면 5 sccm $O_2$ 가스와 100 W 척 파워를 고정한 후 반응기 내부의 압력을 25 mTorr에서 180 mTorr까지 변화시켜 실험한 결과 40 mTorr의 반응기 내부 압력에서 실험 자료 중 가장 높은 식각율로 아크릴 (PMMA)은 $0.46\;{\mu}m/min$, 폴리카보네이트 (Polycabonate)는 $0.28\;{\mu}m/min$의 결과를 얻었다. 또한 이 자료를 바탕으로 5 sccm $O_2$ 가스와 반응기 내부 압력을 40 mTorr로 고정시키고 RIE 척 파워를 25 W에서 150 W로 증가시켰을 때 아크릴 (PMMA)의 식각율은 $0.15\;{\mu}m/min$에서 $0.72\;{\mu}m/min$까지 증가하였고, 폴리카보네이트 (Polycabonate) 의 식각율은 $0.1\;{\mu}m/min$에서 $0.36\;{\mu}m/min$까지 증가하였다.

• 조명전기설비학회논문지
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• 제13권4호
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• pp.82-86
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• 1999

본 연구에서는 푸로브법과 교류중첩법을 이용하여 고주파 유도결합 플라즈마에서 전자에너지 분포함수를 측정하였다. 실험조건은 압력 10∼40[mTorr], 입력파워는 100∼600[W]이고, 가스유량은 3∼12[sccm]이며, 전자에너지 분포함수의 공간분포 측정에 있어서 아스펙트비(R/L)는 2로 하였다. 전자에너지 분포함수는 압력 및 입력파워에 대하여 강한 의존성을 나타내었고, 가스유량이 증가할수록 증가 하였다. 전자에너지 분포함수의 반경방향 분포는 플라즈마 중심에서 최대가 되었다. 전자에너지 분포함수의 축방향 분포는 석영창과 기판 사이의 중심에서 최대가 되었다. 이러한 결과는 고주파 유도결합 플라즈마의 생성 메커니즘 이해와 간단한 ICP(Inductively Coupled Plasma) 모델링 응용에 기여할 수 있을 것이다.

• Transactions on Electrical and Electronic Materials
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• 제13권3호
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• pp.157-161
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• 2012

In this study, we investigated the etching characteristics of ITO thin films and the effects of inert gases added to $Cl_2/BCl_3$ inductivity coupled plasma. The maximum etch rate of ITO thin film was 130.0 nm/min upon the addition of Ar (6 sccm) to the $Cl_2/BCl_3$ (4:16 sccm) plasma, which was higher than that with He or $N_2$ added to the plasma. The ion bombardment by $Ar^+$ sputtering was due to the relatively low volatility of the by-products formed in the $Cl_2/BCl_3$ (4:16 sccm) plasma. The surface of the etched ITO thin film was characterized by x-ray photoelectron spectroscopy (XPS) and atomic force microscopy (AFM). From the XPS results, it is concluded that the proper addition of Ar and He to the $Cl_2/BCl_3$ plasma removes carbon and by-products from the surface of the etched ITO thin film.

• 한국전기전자재료학회논문지
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• 제27권10호
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• pp.662-667
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• 2014

B-doped Si nanoparticles were synthesized by using inductive coupled plasma and specially designed double tube reactor, and their microstructures were investigated. 0~10 sccm of $B_2H_6$ gas was injected during the synthesis of Si nanoparticles from $SiH_4$ gas. Highly crystalline Si nanoparticles were synthesized, and their crystallinity did not change with increase of $B_2H_6$ flow rates. From SEM measurement, their particle sizes were approximately 30 nm regardless of $B_2H_6$ flow rates. From SIMS analysis, almost saturation of B in Si nanoparticles was detected only when 1 sccm of $B_2H_6$ was injected. When $B_2H_6$ flow rate exceeded 5 sccm, higher concentration of B than solubility limit was detected even if any secondary phase was not detected in XRD or HR-TEM results. Due to their high electronic conductivity, those heavily B-doped Si nanoparticles can be a potential candidate for an active material in Li-ion battery anode.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2009년도 제38회 동계학술대회 초록집
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• pp.149-149
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• 2010

The double-layer antireflection (DLAR) coatings have significant advantages over single-layer antireflection (SLAR) coatings. This is because they will be able to cover a broad range of the solar spectrum which would enhance the overall performance of solar cells. Moreover films deposited at high frequency are expected to show excellent and UV-stable passivation in the refractive index that we adopted. In this work, we present a novel DLAR coating using SiNx:H thin films with refractive indices 1.9 and 2.3 as the top and bottom layers. This approach is cost effective when compared to earlier DLAR coatings with two different materials. SiNx:H films were deposited by Plasma enhanced chemical vapor deposition (PECVD) technique using $SiH_4$, $NH_3$ and $N_2$ gases with flow rates 20~80sccm, 200sccm and 85 sccm respectively. The RF power, plasma frequency and substrate temperature for the deposition were 300W, 13.56 MHz and $450^{\circ}C$, respectively. The optimum thickness and refractive indices values for DLAR coatings were estimated theoretically using Macleod simulation software as 82.24 nm for 1.9 and 68.58 nm for 2.3 respectively. Solar cells were fabricated with SLAR and DLAR coatings of SiNx:H films and compared the cell efficacy. SiNx:H> films deposited at a substrate temperature of $450^{\circ}C$ and that at 300 W power showed best effective minority carrier lifetime around $50.8\;{\mu}s$. Average reflectance values of SLAR coatings with refractive indices 1.9, 2.05 and 2.3 were 10.1%, 9.66% and 9.33% respectively. In contrast, optimized DLAR coating showed a reflectance value as low as 8.98% in the wavelength range 300nm - 1100nm.

• 반도체디스플레이기술학회지
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• 제9권3호
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• pp.53-58
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• 2010

In this study, we have investigated the effect of the ambient gases on the characteristics of IZO thin films for the OLED (organic light emitting diodes) devices. For this purpose, IZO thin films were deposited by RF magnetron sputtering under various ambient gases (Ar, $Ar+O_2$ and $Ar+H_2$) at $150^{\circ}C$. In order to investigate the influences of the oxygen and hydrogen, the flow rate of oxygen and hydrogen in argon mixing gas has been changed from 0.1sccm to 0.5sccm, respectively. All the samples show amorphous structure regardless of ambient gases. The electrical resistivity of IZO film increased with increasing flow rate of $O_2$ under $Ar+O_2$ while under $Ar+H_2$ atmosphere the electrical resistivity showed minimum value near 0.5sccm of $H_2$. All the films showed the average transmittance over 85% in the visible range. The OLED device was fabricated with different IZO substrates made by configuration of IZO/${\alpha}$-NPD/DPVB/$Alq_3$/LiF/Al to elucidate the performance of IZO substrate. OLED devices with the amorphous-IZO (a-IZO) anode film show better current densityvoltage-luminance characteristics than that of OLED devices with the commercial crystalline-ITO (c-ITO) anode film. It can be explained that very flat surface roughness and high work function of a-IZO anode film lead to more efficient hole injection by reduction of interface barrier height between anode and organic layers. This suggests that a-IZO film is a promising anode materials substituting conventional c-ITO anode in OLED devices.

• 대한금속재료학회지
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• 제46권10호
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• pp.683-690
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• 2008

In order to develop transparent electrodes for high efficiency GaN-based light emitting diodes (LEDs), the electrical and optical properties of the electron beam evaporated ITO contacts have been investigated as a function of the deposition temperature and flow rate of oxygen during the deposition. As the deposition temperature increases from $140^{\circ}C$ to $220^{\circ}C$, the resistivity of the ITO films decreases slightly from $4.0{\times}10^{-4}{\Omega}cm$ to $3.3{\times}10^{-4}{\Omega}cm$, meanwhile the transmittance of the ITO films significantly increases from 67% to 88% at the wavelength of 470 nm. When the flow rate of oxygen during the deposition increases from 2 sccm to 4 sccm, the resistivity of the ITO films increases from $3.6{\times}10^{-4}{\Omega}cm$ to $7.4{\times}10^{-4}{\Omega}cm$, meanwhile the transmittance of the ITO films increases from 86% to 99% at 470 nm. Blue LEDs fabricated with the electron beam evaporated ITO electrode show that the ITO films deposited at $200^{\circ}C$ and 3 sccm of the oxygen flow rate give a low forward-bias voltage of 3.55 V at injection current of 20 mA with a highest output power.

• Journal of Ceramic Processing Research
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• 제13권spc2호
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• pp.260-264
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• 2012

We have investigated the effect of ambient gases on the structural, electrical, and optical characteristics of IZO thin films intended for use as anode contacts in the organic light emitting diodes (OLED) devices. These IZO thin films were deposited on the PES film by radio frequency (RF) magnetron sputtering under different ambient gases (Ar, Ar + O2, and Ar + H2) at room temperature. In order to investigate the influences of the ambient gases, the flow rate of oxygen and hydrogen in argon has been changed from 0.1 sccm to 0.5 sccm, respectively. All the IZO thin film has an (222) preferential orientation regardless of ambient gases. The electrical resistivity of the IZO film increased with increasing O2 flow rate, whereas the electrical resistivity decreased sharply under an Ar + H2 atmosphere and was nearly similar regardless of the H2 flow rate. The change of electrical resistivity with changes in the ambient gas composition was mainly interpreted in terms of the charge carrier concentration rather than the charge carrier mobility. All the films showed the average transmittance over 85% in the visible range. The OLED device was fabricated with different IZO substrates made with the configuration of IZO/α-NPD/DPVB/Alq3/LiF/Al in order to elucidate the performance of the IZO substrate. The current density and the luminance of OLED devices with IZO thin films deposited in 0.5 sccm H2 ambient gas are the highest amongst all other films.

• 한국진공학회지
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• 제18권2호
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• pp.141-146
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• 2009

rf magnetron sputtering 법을 이용하여 Pt/Ti/$SiO_2$/Si 기판 위에 buffer layer인 $TiO_2$ 층을 증착한 후 PLZT 강유전체 박막을 증착하였다. PLZT 박막 증착 시 가스 분압비가 박막의 특성에 미치는 영향을 알아보기 위해 Ar/$O_2$ 분압비를 각각 27/1.5 sccm, 23/5.5 sccm, 21/7.5 sccm, 19/9.5 sccm로 변화시키면서 박막을 증착하였다. 이들 박막의 구조적인 특성을 분석하기 위해 X-선 회절법을 사용하였으며 FE-SEM을 이용하여 입자상을 관찰하였다. 또한 박막의 유전특성을 분석하기 위해 Precision LC를 이용하여 이력곡선, 잔류분극, 누설전류를 측정하였다. 산소 분압이 높아질수록 박막의 결정성 및 치밀성이 저하되었으며, (110) 방향에서 (111) 방향으로 우선배향성이 변화하는 것을 확인하였다. 산소 분압비의 변화는 박막 표면 및 강유전 특성에 영향을 미치는 것으로 판단된다.