• 한국표면공학회지
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• 제42권6호
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• pp.267-271
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• 2009

Multicomponent transparent conducting oxide films were deposited on glass substrates at 150 by dual magnetron sputtering of AZO and ITO targets. In the case of mixing a limited amount of ITO (10W), resistivity of TCO films was significantly increased compared to the AZO film; from $3.5{\times}10^{-3}$ to $9.7{\times}10^{-3}{\Omega}{\cdot}cm$. Deterioration of the electrical conductivity is attributed to the decreases in carrier concentration and Hall mobility. Improvement of the conductivity could be obtained for the films prepared with ITO powers larger than 40 W. The lowest resistivity ($\rho$) of $7.3{\times}10^{-4}{\Omega}{\cdot}cm$ was achieved when ITO power was 100 W. Effects of $H_2$ incorporation on the electrical and optical properties of AZO-ITO films were investigated in this work. Addition of small amount of hydrogen resulted in the increase of carrier concentration and the improvement of electrical conductivity. It is apparent that the roughness of AZO-ITO films decreases dramatically after the transition of microstructure from polycrystalline to amorphous phase, which gives practical advantages such as an excellent uniformity of surface and a high etching rate. AZO-ITO films grown at sputtering ambient with hydrogen gas are expected to be applicable to optoelectronic devices such as organic light emitting diodes and flexible displays due to their sufficient electrical and structural properties.

• 한국전자통신학회논문지
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• 제18권6호
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• pp.1067-1072
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• 2023

본 연구에서는 본 연구에서는 펄스 레이저 증착법으로 기판온도에 따른 AZO(Al₂O₃ : 3 wt %)박막을 제작하여, 구조적 특성과 전기적 및 광학적 특성을 조사하였다. 기판온도 400℃ 에서 증착한 AZO박막에서 가장 우수한 (002) 배향성을 나타내었으며, 이때의 반가폭은 0.42° 였다. 전기적 특성을 조사한 결과, 기판온도가 상승함에 따라 캐리어 농도와 이동도는 증가하였고 비저항은 감소하였다. 가시광 영역에서의 평균 투과도는 기판온도에 상관없이 85% 이상의 높은 값을 나타내었고, 기판온도에 상승함에 따라 캐리어 농도가 증가하고 이로 인해 에너지 밴드갭이 넓어지는 Burstein-Moss효과도 관찰할 수 있었다. 기판온도 400℃ 에서 증착한 AZO박막의 비저항과 재료평가지수는 각각 6.77 × 10^-4 Ω·cm 과 1.02 × 10⁴ Ω^-1·cm^-1 로 가장 우수한 값을 나타내었다.

• 한국재료학회지
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• 제17권12호
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• pp.629-633
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• 2007

This study examined the effect of growth temperature on the electrical and optical properties of hydrogenated Al-doped zinc oxide (AZO:H) thin films deposited by rf magnetron sputtering using a ceramic target (98 wt.% ZnO, 2 wt.% $Al_2O_3$). Various AZO films on glass were prepared by changing the substrate temperature from room temperature to $200^{\circ}C$. It was shown that intentionally incorporated hydrogen plays an important role on the electrical properties of AZO : H films by increasing free carrier concentration. As a result, in the 2% $H_2$ addition at the growth temperature of $150^{\circ}C$, resistivity of $3.21{\times}10^{-4}{\Omega}{\cdot}cm$, mobility of $21.9cm^2/V-s$, electric charge carrier concentration of $9.35{\times}10^{20}cm^{-3}$ was obtained. The AZO : H films show a hexagonal wurtzite structure preferentially oriented in the (002) crystallographic direction.

• 한국전자통신학회논문지
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• 제19권1호
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• pp.47-52
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• 2024

본 연구에서는 유리 기판 위에 BZO박막을 제작한 후, 열처리 온도가 박막의 전기적 및 광학적 특성에 미치는 영향을 조사하였다. XRD 분석 결과, 열처리 온도에 무관하게 모든 박막이 c-축 배향성을 나타내었다. 열처리 온도가 400에서 600℃ 로 증가함에 따라 반가폭(FWHM)은 1.65에서 1.07° 로 감소하였다. 가시광 영역(400-800nm)에서의 평균 투과도는 열처리 온도에 큰 영향 없이 85% 이상의 높은 값을 나타내었다. Hall 측정결과, 열처리 온도에 따라 캐리어 농도와 이동도는 증가하였고 비저항은 감소하였다. 600℃ 에서 열처리한 BZO박막의 비저항과 캐리어 농도는 각각 9.75 × 10^-2 Ω·cm 과 4.21×10¹⁹ cm^-3 로 가장 우수한 값을 나타내었다. 향후 BZO박막의 공정 조건과 열처리 조건을 최적화시킨다면, 차세대 광전자 소자에 응용될 수 있는 매우 유망한 재료로 주목받을 것으로 기대된다.

• 한국결정성장학회지
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• 제7권2호
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• pp.271-275
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• 1997

HWE방법으로 GaAs 기관위에 Cl이 첨가된 ZnSe 박막을 성장하였다. 성장된 박막의 표면 상태는 경면이 있었으며 좋은 결정성과 낮은 비저항 n 형 전도성을 나타내었다. 성장된 박막의 운반자 농도는 $10^{16}Cm{-3}$ 정도였으며 비저항값은 10$\\Omega$\cdotcm였다. 실온에서 청색 발광을 하는 photoluminescence를 나타내었다. 나타내었다.

• 한국진공학회지
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• 제6권1호
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• pp.69-76
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• 1997

순간 증착법으로 $Bi_{0.5}Sb_{1.5}Te_3$(p형)와 $Bi_2Te_{2.4} Se_{0.6}$(n형) 박막을 제조하여 두께와 어닐 링 조건에 따른 Seebeck 계수, 전기전도도, carrier 농도 및 이동도, 열전도도, 성능지수의 변화 등 열-전기적 특성을 조사하였다. 473K에서, 1시간 진공 열처리한 결과 p형과 n형의 성능지구는 각각 $1.3{\times}10^{-3}K^{-1}$ 및 $0.3{\times}10^{-3}K^{-1}$으로 향상되었으며 두께에 크게 의존하지 않았 다. 이런 성질을 갖는 열전 박막을 소자화한 박막 온도 센서를 유리와 Teflon기판 위에 제 조하였으며, 이들의 온도 변화에 대한 열기전력, 민감도 및 시간 상수 등 센서 특성을 측정 하였다. p 및 n형의 leg 폭 1mm$\times$길이 16mm인 박막 온도 센서의 경우, Teflon 기판일 때 좋은 성능을 나타내었으며, 민감도는 2.91V/W, 시간 상수는 28.2초이었다.

• 한국재료학회지
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• 제21권9호
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• pp.491-496
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• 2011

Transparent conducting oxides (TCOs) used in the antireflection layer and current spreading layer of heterojunction solar cells should have excellent optical and electrical properties. Furthermore, TCOs need a high work function over 5.2 eV to prevent the effect of emitter band-bending caused by the difference in work function between emitter and TCOs. Sn-doped $In_2O_3$ (ITO) film is a highly promising material as a TCO due to its excellent optical and electrical properties. However, ITO films have a low work function of about 4.8 eV. This low work function of ITO films leads to deterioration of the conversion efficiency of solar cells. In this work, ITO films with various Zn contents of 0, 6.9, 12.7, 28.8, and 36.6 at.% were fabricated by a co-sputtering method using ITO and AZO targets at room temperature. The optical and electrical properties of Zn-doped ITO thin films were analyzed. Then, silicon heterojunction solar cells with these films were fabricated. The 12.7 at% Zn-doped ITO films show the highest hall mobility of 35.71 $cm^2$/Vsec. With increasing Zn content over 12.7, the hall mobility decreases. Although a small addition of Zn content increased the work function, further addition of Zn content over 12.7 at.% led to decreasing electrical properties because of the decrease in the carrier concentration and hall mobility. Silicon heterojunction solar cells with 12.7 at% Zn-doped ITO thin films showed the highest conversion efficiency of 15.8%.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.286-289
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• 2001

Single phase CuGaS$_2$ thin film with the highest diffraction peak of (112) at diffraction angle (2$\theta$) of 28.8$^{\circ}$ was made at substrate temperature of 7$0^{\circ}C$, annealing temperature of 35$0^{\circ}C$ and annealing time of 60 min. And second highest (204) peak was shown at diffraction angle (2$\theta$) of 49.1$^{\circ}$. Lattice constant of a and c of that CuGaS$_2$ thin film was 5.37 $\AA$ and 10.54 $\AA$ respectively. The greatest grain size of the thin film was about 1${\mu}{\textrm}{m}$. The (112) peak of single phase of CuGaS$_2$ thin film at annealing temperature of 35$0^{\circ}C$ with excess S supply was appeared with a little higher about 10 % than that of no exces S supply And the resistivity, mobility and hole density at room temperature of p-type CuGaS$_2$ thin film with best crystalline was 1.4 $\Omega$cm, 15 cm2/V . sec and 2.9$\times$10$^{17}$ cm$^{-3}$ respectively. It was known that carrier concentration had considerable effect than mobility on variety of resistivity of the fabricated CuGaS$_2$ thin film, and the polycrystalline CuGaS$_2$ thin films were made at these conditions were all p-type.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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• pp.497-497
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• 2013

Semiconducting amorphous InGaZnO (a-IGZO) has attracted significant research attention as improved deposition techniques have made it possible to make high-quality a-IGZO thin films. IGZO thin films have several advantages over thin film transistors (TFTs) based on other semiconducting channel layers.The electron mobility in IGZO devices is relatively high, exceeding amorphous Si (a-Si) by a factor of 10 and most organic devices by a factor of $10^2$. Moreover, in contrast to other amorphous semiconductors, highly conducting degenerate states can be obtained with IGZO through doping, yet such a state cannot be produced with a-Si. IGZO thin films are capable of mobilities greaterthan 10 $cm^2$/Vs (higher than a-Si:H), and are transparent at visible wavelengths. For oxide semiconductors, carrier concentrations can be controlled through oxygen vacancy concentration. Hence, adjusting the oxygen partial pressure during deposition and post-deposition processing provides an effective method of controlling oxygen concentration. In this study, we deposited IGZO thinfilms at optimized conditions and then analyzed the film's electrical properties, surface morphology, and crystal structure. Then, we explored how to generate IGZO thin films using DC magnetron sputtering. We also describe the construction and characteristics of a bottom-gate-type TFT, including the output and transfer curves and bias stress instability mechanism.

• JSTS:Journal of Semiconductor Technology and Science
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• 제13권4호
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• pp.342-354
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• 2013

The aim of this work is to investigate and study the quantum effects in the modeling of nanoscale symmetric double-gate InAlAs/InGaAs/InP HEMT (High Electron Mobility Transistor). In order to do so, the carrier concentration in InGaAs channel at gate lengths ($L_g$) 100 nm and 50 nm, are modelled by a density gradient model or quantum moments model. The simulated results obtained from the quantum moments model are compared with the available experimental results to show the accuracy and also with a semi-classical model to show the need for quantum modeling. Quantum modeling shows major variation in electron concentration profiles and affects the device characteristics. The two triangular quantum wells predicted by the semi-classical model seem to vanish in the quantum model as bulk inversion takes place. The quantum effects thus become essential to incorporate in nanoscale heterostructure device modeling.