• Journal of the Korean Ceramic Society
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• v.46 no.1
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• pp.86-93
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• 2009

The crack formation and the resistance of ITO film on PET substrate with a thickness of 20 nm were investigated as a function of strain. The onset strain for the increase of resistance increased with increasing strain rate, suggesting the crack initiation is dependent on the strain rate. Electrical resistance increased at the strain of 1.6% at the strain rates below $10^{-4}/sec$ while it increased at ${\sim}2%$ at the strain rates above $10^{-3}/sec$. The critical strain at which the cracks were formed is close to the proportional limit. Upon loading, the initial cracks perpendicular to the tensile axis were observed and propagated the whole sample width with increasing strain. The spacing between horizontal cracks is thought to be determined by the fracture strength and the interfacial strength between ITO and PET. The crack density increased with increasing strain. However, the effect of the strain rate on the crack density was less pronounced in ITO/PET with 20 nm ITO thickness than ITO/PET with 125 nm ITO thickness, the strength of ITO film is thought to increase as the thickness on ITO film decreases. The absence of cracks on ITO film at a strain as close as 1.5% can be attributed to the compressive residual stress of ITO film which was developed during cooling after the coating process. The higher critical strain for the onset of the resistance increase and the crack initiation of ITO/PET with a thinner ITO film (20 nm) can be linked with the higher strength of the thinner ITO film.

• Transactions on Electrical and Electronic Materials
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• v.14 no.5
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• pp.242-245
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• 2013

Sn-doped $In_2O_3$ (ITO) thin films were prepared by radio frequency magnetron sputtering without intentional substrate heating on bare glass and $TiO_2$-deposited glass substrates to investigate the effect of a $TiO_2$ buffer layer on the electrical and optical properties of ITO films. The thicknesses of $TiO_2$ and ITO films were kept constant at 5 and 100 nm, respectively. As-deposited ITO single layer films show an optical transmittance of 75.9%, while $ITO/TiO_2$ bi-layered films show a lower transmittance of 76.1%. However, as-deposited $ITO/TiO_2$ films show a lower resistivity ($9.87{\times}10^{-4}{\Omega}cm$) than that of ITO single layer films. In addition, the work function of the ITO film is affected by the $TiO_2$ buffer layer, with the $ITO/TiO_2$ films having a higher work-function (5.0 eV) than that of the ITO single layer films. The experimental results indicate that a 5-nm-thick $TiO_2$ buffer layer on the $ITO/TiO_2$ films results in better performance than conventional ITO single layer films.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.30 no.11
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• pp.740-744
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• 2017

Herein we studied the electrical and optical properties of indium tin oxide ITO/Ag/ITO multilayer thin films for application in transparent conducting electrodes. The ITO and Ag thin films were deposited onto soda lime glass (SLG) using radiofrequency and DC-sputtering methods, respectively. The as-synthesized ITO/Ag/ITO multilayer thin films were analyzed using 4-point probe, UV-Visible spectroscopy, and Hall measurement. We observed a rapid increase in electron concentration with increasing Ag thickness. However, electron mobility decreased with increasing Ag thickness. Finally, ITO/Ag/ITO multilayer thin films showed a characteristic low sheet resistance of $18{\Omega}/sq$ and high optical transmittance value (80%) with variation of Ag thickness (5~10 nm).

• Journal of the Korean institute of surface engineering
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• v.44 no.6
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• pp.260-263
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• 2011

GZO/ITO double layered films were deposited on unheated non-alkali glass substrates by RF magnetron sputtering using an ITO ($SnO_2$: 10 wt%) and GZO($Ga_2O_3$: 5.57 wt%) ceramic targets, respectively. The electrical resistivity of GZO/ITO films depends on the thickness ratio between the GZO film and ITO film. With increasing ITO film thickness, the resistivity of GZO/ITO films decreased which due to large increase in the Hall mobility. Also, the crystallinity of GZO/ITO film was improved with an increase in ITO thickness which was evaluated by X-ray diffraction. The average transmittance of the films was more than 85% in the visible region, which is slightly higher than ITO single layer films.

• Journal of the Korean institute of surface engineering
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• v.45 no.6
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• pp.242-247
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• 2012

Yb-doped ITO (ITO:Yb) films were deposited on unheated non-alkali glass substrates by magnetron cosputtering using two cathodes (DC, RF) equipped with the ITO and $Yb_2O_3$ target, respectively. The composition of the ITO:Yb films was controlled by adjusting the RF powers from 0 W to 480 W in 120 W steps with the DC power fixed at 70 W. The ITO:Yb films had a higher crystallization temperature ($200^{\circ}C$) than that of the ITO films ($170^{\circ}C$), which was attributed to both larger ionic radius of $Yb^{3+}$ and higher bond enthalpy of $Yb_2O_3$, compared to ITO. This amorphous ITO:Yb film post-annealed at $170^{\circ}C$ showed a resistivity of $5.52{\times}10^{-4}{\Omega}cm$, indicating that a introduction of Yb increased resistivity of the ITO film. However, these amorphous ITO:Yb films showed a high etching rate, fine pattering property, and a very smooth surface morphology above the crystallization temperature of the amorphous ITO films (about $170^{\circ}C$). The transmittance of all films was >80% in the visible region.

• Clean Technology
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• v.13 no.3
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• pp.180-187
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• 2007

The indium tin oxide(ITO) film on PET was prepared by a wet coating method to obtain the transparent film with a high conductance. ITO nano-particles was synthesized by a SAS method at 15 MPa and $50^{\circ}C$, where optimized rate of In/Sn was 65. Average diameter and resistivity of ITO obtained from SAS are $15{\pm}2\;nm$ and $4{\times}10^4\;{\Omega}{\cdot}cm$. Coating solution was prepared at pH 10. The ITO film was obtained by solution including 0.1 0.5, 1, and 2 ITO wt% on PET. Roughness(Ra) of ITO film with 0.1, 0.5, 1. and 2 ITO wt% is 4, 10, 12, and 16 nm. Resistivity with an increasing ITO concentration is $3.7{\times}10^6,\;2.4{\times}10^6,\;8{\times}10^5,\;and\;2{\times}10^5\;{\Omega}{\cdot}cm$. Transmissivity of ITO film decreased as 89, 88, 86, and 82% with an increasing ITO concentration as 0.1, 0.5, 1, and 2 wt%.

• Proceedings of the Materials Research Society of Korea Conference
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• 2009.05a
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• pp.19.2-19.2
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• 2009

ITO는 n형 반도체 특성을 가지며 이와 동시에 높은 가시광투과율과 낮은 전기전도도를 가짐으로써 다양한 투명전극소재와 가스 검출센서로 많이 활용되고 있다. 본 연구에서는 RF magnetron sputtering 법을 이용하여 상온에서 glass 기판 위에 두께 100nm로 ITO 그리고 하층 ITO 박막 (두께 50 nm) 위에 층간 금속 (두께 5 nm)을 증착하고 다시 상부 ITO 박막 (두께 45 nm)을 증착하여 3층의 적층형 박막센서를 제작하였다. 층간 금속으로는 Au와 Cu를 각각 사용하였다. 박막 증착 후엔 진공분위기에서 $150^{\circ}C$, $300^{\circ}C$로 열처리 과정을 거쳐 열처리 전후의 물성 및 감지특성을 비교해보았다. 분석방법으로는 XRD, SEM, AFM, Hall effect 장치 등을 이용하였다. 분석 결과 $300^{\circ}C$에서 진공 열처리한 ITO/Au/ITO(IAI) 박막센서가 높은 결정화도 와 전기적 특성이 나타났으며, 0 에서 1000ppm 까지의 메탄가스의 민감도 측정에서도 열처리된 IAI 박막센서가 기존의 ITO 박막센서보다도 약 70% 정도 향상된 민감도를 나타내었다.

• Journal of the Korean Ceramic Society
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• v.39 no.3
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• pp.233-239
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• 2002

Reflection properties of $SiO_2$/ITO (Indium Tin Oxide) thin films coated for electromagnetic shielding, anti-static and anti-reflection on the front surface in CRT were studied. The behavior of reflectance as a function of thickness of $SiO_2$/ITO was investigated and applied to theoretical anti0reflection model of double layers and three layers. As the thickness of ITO layer increased, the deviation from theoretical value increased because uniformity of film deteriorated by pore. Because of the effect of mixed layer of $SiO_2$ and ITO, experimental reflectance showed better acceptance to the three layer antireflection model of $SiO_2$/$SiO_2$+ITO/ITO than the two layer model. Based on the theoretical antireflection design, the double layer whose thickness of $SiO_2$ and ITO were 90, 65 nm, respectively appear 2.5% in reflectance at standard wavelength, 550 nm. This phenomenon was similar to theoretical reflectance in visual range.

• Proceedings of the Korean Vacuum Society Conference
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• 2014.02a
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• pp.336.1-336.1
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• 2014

대표적인 TCO 물질인 ITO는 디스플레이 패널이나 태양 전지 등과 같은 소자에 널리 사용되고 있다. 최근에는 대량생산 및 대면적화, 그리고 유연 디스플레이 응용을 위해 롤투롤 스퍼터링(roll to roll sputtering) 공정을 이용하여 플라스틱 기판에 ITO박막을 증착하여 ITO 필름을 제작하고 있다. 롤투롤 방식으로 ITO 필름의 제작 시 공정 변수에 따라 ITO 박막의 전기적 광학적 물성 변화가 매우 크기 때문에, 공정 변수에 따른 ITO 박막의 전기적, 광학적 특성 변화에 대한 연구의 필요성이 매우 높아지고 있다. 따라서 본 연구에서는 롤투롤 스퍼터링 방법으로 PET 기판 위에 다양한 조건으로 ITO 박막을 증착하여 공정변수에 따른 ITO 박막의 물성을 조사 하였다. 이를 위해 ITO (In/Sn=95/5 wt.%) 타겟을 사용하여 DC 파워와 산소 분압비, 열처리 온도 등을 변화시켜 낮은 면저항과 높은 광투과도를 가지는 최적의 ITO 증착 조건을 찾은 후 ITO 박막을 PET 기판 위에 두께 별로 증착 하였다. ITO 박막의 두께와 열처리 온도에 따른 전기적 특성은 면저항 측정기와 홀 측정 장치를 이용하여 분석하였고, 분광광도계와 탁도 측정기를 이용하여 광학적 특성을 관찰하였다. 또한, GIXD를 이용하여 이들 박막의 구조와 결정성에 대한 조사를 수행하였다. 이 결과들로부터 산소 분압비에 따른 ITO/PET 박막의 저항 특성 변화와 ITO 박막의 두께와 열처리 온도에 따른 구조적, 전기적, 광학적 특성을 조사하여, 롤투롤 스퍼터링법에서 공정 조건에 따른 ITO/PET 필름의 물성변화를 보고하고자 한다.

• Proceedings of the Korean Vacuum Society Conference
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• 2012.02a
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• pp.350-350
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• 2012

TCO 물질로 널리 사용되는 ITO 박막은 우수한 특성에도 불구하고 투과도와 전기적 특성 사이에 trade-off 현상이 존재하여 상온에서 증착시 두 가지 특성을 향상시키는데 큰 어려움이 있다 [1]. 본 실험에서는 ITO와 Ag embedded ITO (ITO-Ag) 샘플의 Ag의 증착 시간과 열처리에 따른 전기적 및 광학적 특성 변화를 연구하였다. 열처리 전에는 ITO-Ag 샘플들의 비저항이 ITO 보다 향상 되는 것을 확인 하였다. 하지만 ITO-Ag 샘플의 Ag 증착 시간이 증가 할수록 투과도는 예상한 바와 같이 계속 저하됨을 확인하였다. 열처리 이후에는 Figure 1에서와 같이 ITO와 ITO-Ag 샘플 모두 비저항과 투과도가 향상 되는 것을 알 수 있는데, 비저항의 경우 ITO-Ag 샘플 보다 ITO 샘플이 더욱 큰 향상을 나타내었다. 이러한 결과는 열처리 과정에서 일어나는 ITO의 결정화, 산소공공의 형성 등을 Ag가 방해하기 때문으로 사료된다. 하지만 투과도의 경우 Ag가 금속임에도 불구하고 박막을 형성하지 않을 정도로 매우 얇게 증착 되었기 때문에 열처리 이후 투과도가 향상되어 ITO와 ITO-Ag 샘플 모두 비슷한 향상을 나타내었다고 사료된다. 즉, embedded된 Ag는 열처리에 의해 전기적으로는 나쁜 영향을 주지만, as-deposit 상태에서는 순수 ITO 보다 좋은 전기적 특성을 나타냄을 알 수 있었으며, 이러한 결과는 유기물 반도체 소자에 적용 가능 할 것으로 사료된다.