• Title/Summary/Keyword: SiC film

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The TDDB Characteristics of Thin $SiO_2$ with Stress Voltage Polarity (스트레스전압 극성에 따른 얇은 산화막의 TDDB 특성)

  • Kim, Cheon-Soo;Yi, Kyoung-Soo;Nam, Kee-Soo;Lee, Jin-Hyo
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.26 no.5
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    • pp.52-59
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    • 1989
  • The reliability of the thin thermal oxide was investigated by using constant current stress method. Polysilicon gate MOS capacitors with oxide thickness range of 20-25nm were used in this experiment. Automatic measurement and statistical data analysis which were essential in reliability evaluation of VLSI process preformed by HP 9000 computer. Based on TDDB results, defect density, breakdown charge (Qbd) and lifetime of oxide film were evaluated. According to the polarity of the stress, some different characteristics were shown. Defect density was 62/$cm^2$ at negative gate injection. The value of Qbd was about 30C/$cm^2$ at positive gate injection, and about 21C/$cm^2$ at negative. The current density acceleration factor was 1.43$cm^2$/A for negative gate injection, and 1.25$cm^2$/A for positive gate injection.

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Growth and photocurrent study on the splitting of the valence band for ZnIn2S4 single crystal thin film by hot wall epitaxy (Hot Wall Epitaxy (HWE)법에 의한 ZnIn2S4 단결정 박막 성장과 가전자대 갈라짐에 대한 광전류 연구)

  • Hong, Kwang-Joon
    • Journal of Sensor Science and Technology
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    • v.16 no.6
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    • pp.419-427
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    • 2007
  • Single crystal $ZnIn_{2}S_{4}$ layers were grown on a thoroughly etched semi-insulating GaAs(100) substrate at $450^{\circ}C$ with the hot wall epitaxy (HWE) system by evaporating the polycrystal source of $ZnIn_{2}S_{4}$ at $610^{\circ}C$ prepared from horizontal electric furnace. The crystalline structure of the single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of single crystal $ZnIn_{2}S_{4}$ thin films measured with Hall effect by van der Pauw method are $8.51{\times}10^{17}\;electron/cm^{-3}$, $291{\;}cm^{2}/v-s$ at 293 K, respectively. The photocurrent and the absorption spectra of $ZnIn_{2}S_{4}$/SI(Semi-Insulated) GaAs(100) are measured ranging from 293 K to 10 K. The temperature dependence of the energy band gap of the $ZnIn_{2}S_{4}$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)$=2.9514 eV. ($7.24{\times}10^{-4}\;eV/K$)$T^{2}$/(T+489 K). Using the photocurrent spectra and the Hopfield quasicubic model, the crystal field energy(${\Delta}cr$) and the spin-orbit splitting energy(${\Delta}so$) for the valence band of the $ZnIn_{2}S_{4}$ have been estimated to be 167.8 meV and 14.8 meV at 10 K, respectively. The three photocurrent peaks observed at 10 K are ascribed to the $A_{1}$-, $B_{1}$-, and $C_{41}$-exciton peaks.

Photocurrent properties for $CdGa_2Se_4$ single crystal thin film grown by using hot wall epitaxy(HWE) method (Hot Wall Epitaxy(HWE)법에 의한 $CdGa_2Se_4$ 단결정 박막의 광전류 연구)

  • You, Sang-Ha;Hong, Kwang-Joon
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.11a
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    • pp.124-125
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    • 2007
  • Single crystal $CdGa_2Se_4$ layers were grown on a thoroughly etched semi-insulating GaAs(100) substrate at $420^{\circ}C$ with the hot wall epitaxy (HWE) system by evaporating the polycrystal source of $CdGa_2Se_4$ at $630^{\circ}C$ prepared from horizontal electric furnace. The photocurrent and the absorption spectra of $CdGa_2Se_4$/SI(Semi-Insulated) GaAs(100) are measured ranging from 293K to 10K. The temperature dependence of the energy band gap of the $CdGa_2Se_4$, obtained from the absorption spectra was well described by the Varshni's relation, $E_g$(T) = 2.6400 eV - $(7.721{\times}10^{-4}\;eV/K)T^2$/(T + 399 K). Using the photocurrent spectra and the Hopfield quasicubic model, the crystal field energy$({\Delta}cr)$ and the spin-orbit splitting energy$({\Delta}so)$ for the valence band of the $CdGa_2Se_4$ have been estimated to be 106.5 meV and 418.9 meV at 10 K, respectively. The three photocurrent peaks observed at 10 K are ascribed to the $A_{1^-},\;B_{1^-},\;and\;C_{11^-}$ exciton peaks.

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Characteristics and Processing Effects Of $HfO_2$ Thin Films grown by Metal-Organic Molecular Beam Epitaxy (금속 유기 분자 빔 에피택시로 성장시킨 $HfO_2$ 박막의 특성과 공정변수가 박막의 성장 및 특성에 미치는 영향)

  • Kim, Myoung-Seok;Ko, Young-Don;Nam, Tae-Hyoung;Jeong, Min-Chang;Myoung, Jae-Min;Yun, Il-Gu
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2004.07a
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    • pp.74-77
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    • 2004
  • [ $HfO_2$ ] dielectric layers were grown on the p-type Si(100) substrate by metalorganic molecular beam epitaxy(MOMBE). Hafnium $t-butoxide[Hf(O{\cdot}t-C_4H_9)_4]$ was used as a Hf precursor and Argon gas was used as a carrier gas. The thickness of the layers was measured by scanning electron microscopy (SEM) and high-resolution transmission electron measurement(HR-TEM). The properties of the $HfO_2$ layers were evaluated by X-ray diffraction(XRD), high frequency capacitance-voltage measurement(HF C-V), current-voltage measurement(I-V), and atomic force measurement(AFM). HF C-V measurements have shown that $HfO_2$ layer grown by MOMBE has a high dielectric constant(k=19-21). The properties of $HfO_2$ films are affected by various process variables such as substrate temperature, bubbler temperature, Ar, and $O_2$ gas flows. In this paper, we examined the relationship between the $O_2/Ar$ gas ratio and the electrical properties of $HfO_2$.

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Template-Based Carbon Nanotubes Field Emitter

  • Jeong, Soo-Hwan;Lee, Ok-Joo;Hwang, Sun-Kyu;Lee, Kun-Hong
    • Journal of Information Display
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    • v.2 no.3
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    • pp.78-85
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    • 2001
  • The growth of carbon nanotubes(CNTs) in anodic aluminum oxide(AAO) template and their application to a field emitter are described. AAO templates were fabricated by anodizing bulk aluminum and sputtered thin Al film on Nb-coated Si wafers. After Co catalyst had been electrochemically deposited into the bottom of the pores in AAO template, CNTs were grown by pyrolyzing $C_2H_2$. Depending on the reaction conditions, CNTs grew up to or over the top of the pores in AAO template with different structures. The morphology and structure of CNTs were observed with a scanning electron microscope and a transmission electron microscope. The diameter of CNTs strongly depended on the size of the pores in AAO template and the growing conditions. The electron field emission measurement of the samples resulted in the turn-on field of 1.9-2.2 $V/{\mu}m$ and the field enhancement factor of 2450-5200. The observation of high field enhancement factors is explained in terms of low field screening effect.

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Silicon Nitride Cantilever Arrays Integrated with Si Heater and Piezoelectric Sensors for SPM Data Storage Applications

  • Nam, Hyo-Jin;Jang, Seong-Soo;Kim, Young-Sik;Lee, Caroline-Sunyong;Jin, Won-Hyeog;Cho, Il-Joo;Bu, Jong-Uk
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.5 no.1
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    • pp.24-29
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    • 2005
  • Silicon nitride cantilevers integrated with silicon heaters and piezoelectric sensors were developed for the scanning probe microscope (SPM) based data storage application. These nitride cantilevers are expected to have better mechanical stability and uniformity of initial bending than the previously developed silicon cantilevers. Data bits of 40 nm in diameter were recorded on PMMA film and the sensitivity of the piezoelectric sensor was 0.615 fC/nm, meaning that indentations less than 20 nm in depth can be detected. For high speed operation, $128{\times}128$ cantilever array was developed.

VLS growth of ZrO2 nanowhiskers using CVD method

  • Baek, Min-Gi;Park, Si-Jeong;Jeong, Jin-Hwan;Choe, Du-Jin
    • Proceedings of the Korean Vacuum Society Conference
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    • 2016.02a
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    • pp.149-149
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    • 2016
  • Ceramic is widely known material due to its outstanding mechanical property. Besides, Zirconia(ZrO2) has a low thermal conductivity so it is advantage in a heat insulation. Because of these superior properties, ZrO2 is attracted to many fields using ultra high temperature for example vehicle engines, aerospace industry, turbine, nuclear system and so on. However brittle fracture is a disadvantage of the ZrO2. In order to overcome this problem, we can make the ceramic materials to the forms of ceramic nanoparticles, ceramic nanowhiskers and these forms can be used to an agent of composite materials. In this work, we selected Au catalyzed Vapor-Liquid-Solid mechanism to synthesize ZrO2 nanowhiskers. The ZrO2 whiskers are grown through Hot-wall Chemical Vapor Deposition(Hot wall CVD) using ZrCl4 as a powder source and Au film as a catalyst. This Hot wall CVD method is known to comparatively cost effective. The synthesis condition is a temperature of $1100^{\circ}C$, a pressure of 760torr(1atm) and carrier gas(Ar) flow of 500sccm. To observe the morphology of ZrO2 scanning electron microscopy is used and to identify the crystal structure x-ray diffraction is used.

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Modeling of RF Sputtering Process for ZnO Thin film Deposition using Neural Network (신경회로망을 이용한 RF 스퍼터링 ZnO 박막 증착 프로세스 모델링)

  • Lim, Keun-Young;Lee, Sang-Keuk;Park, Choon-Bae
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.19 no.7
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    • pp.624-630
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    • 2006
  • ZnO deposition parameters are not independent and have a nonlinear and complex property. To propose a method that could verify and predict the relations of process variables, neural network was used. At first, ZnO thin films were deposited by using RF magnetron sputtering process with various conditions. Si, GaAs, and Glass were used as substrates. The temperature, work pressure, and RF power of the substrate were $50\sim500^{\circ}C$, 15 mTorr, and $180\sim210W$, respectively : the purity of the target was ZnO 4 N. Structural properties of ZnO thin films were estimated by using XRD (0002) peak intensity. The structure of neural network was a form of 4-7-1 that have one hidden layer. In training a network, learning rate and momentum were selected as 0.2, 0.6 respectively. A backpropagation neural network were performed with XRD (0002) peak data. After training a network, the temperature of substrate was evaluated as the most important parameter by sensitivity analysis and response surface. As a result, neural network could capture nonlinear and complex relationships between process parameters and predict structural properties of ZnO thin films with a limited set of experiments.

Effect of DC Bias on the Growth of Nanocrystalline Diamond Film over Poly-Silicon Substrate (DC Bias가 다결정 실리콘 기판 위 나노결정 다이아몬드 박막의 성장에 미치는 영향)

  • Kim, Seon-Tae;Gang, Chan-Hyeong
    • Proceedings of the Korean Institute of Surface Engineering Conference
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    • 2016.11a
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    • pp.180-180
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    • 2016
  • 보론이 도핑된 $3{\times}3cm$ 크기의 p 형 다결정 실리콘 기판의 표면을 경면연마한 후, 다이아몬드 입자의 seeding을 위해 슬러리 중 다이아몬드 분말의 입도를 5 nm로 고정하고 초음파 전처리 공정을 진행한 후, 다이아몬드 박막을 증착하였다. 다이아몬드 증착은 Microwave Plasma Chemical Vapor Deposition 장비를 이용하였으며, 공정 조건은 초기 진공 $10{\times}10^{-3}Torr$, 공정 가스 비율 $Ar:CH_4=200:2$, 가스 유량 202 sccm, 공정압력 90 Torr, 마이크로웨이브 파워 600 W, 기판 온도 $600^{\circ}C$이었다. 기판에 DC bias 전압을 인가하는 것을 공정 변수로 하여 0, -50, -100, -150, -200 V로 변화시켜가며, 0.5, 1, 2, 4 h 동안 증착을 진행하였다. 주사전자현미경과 XRD, AFM, 접촉각 측정 장비를 이용하여 증착된 다이아몬드 입자와 막의 특성을 분석하였다. 각 bias 조건에서 초기에는 다이아몬드 입자가 형성되어 성장되었다가 시간이 증가될수록 연속적인 다이아몬드 막이 형성되었다. Table 1은 각 bias 조건에서 증착 시간을 4 h까지 변화시키면서 얻은 다이아몬드 입자 또는 박막의 높이(두께)를 나타낸 것이다. 2 h까지의 공정 초기에는 bias 조건의 영향을 파악하기 어려운데, 이는 bias에 의한 과도한 이온포격으로 입자가 박막으로의 성장에 저해를 받는 것으로 사료된다. 증착시간이 4 h가 경과하면서 -150 V 조건에서 가장 두꺼운 막이 성장되었다. 이는 기판 표면을 덮은 다이아몬드 박막 위에서 이차 핵생성이 bias에 의해 촉진되기 때문으로 해석된다. -200 V의 조건에서는 오히려 막의 성장이 더 느렸는데, 이는 Fig. 1에 보이듯이 과도한 이온포격으로 Si/diamond 계면에서 기공이 형성된 것과 연관이 있는 것으로 보인다.

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Fabrication and Properties of MIS Inversion Layer Solar Cell using $Al_2O_3$ Thin Film ($Al_2O_3$ 박막을 이용한 MIS Inversion Layer Solar Cell의 제작 및 특성평가)

  • Kim, Hyun-Jun;Byun, Jung-Hyun;Kim, Ji-Hun;Jeong, Sang-Hyun;Kim, Kwang-Ho
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.06a
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    • pp.242-242
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    • 2010
  • 산화 알루미늄($Al_2O_3$) 박막을 p-type Czochralski(CZ) Si 위에 Remote Plasma Atomic Layer Deposition(RPALD)을 이용하여 저온 공정으로 증착하였다. Photolithography 공정으로 grid 패턴을 형성한 후 열 증착기로 알루미늄을 증착하여 MIS-IL (Metal-Insulator-Semiconductor Inversion Layer) solar cell을 제작하였다. 반응소스로는 Trimethylaluminum (TMA)과 $O_2$를 이용하였다. $Al_2O_3$ 박막의 전기적 특성 평가를 위해 MIS capacitor를 제작하여 Capacitance-voltage (C-V), Current-voltage (I-V), Interface state density ($D_{it}$)를 평가하였으며 Solar simulator를 이용하여 MIS-IL Solar cell의 Efficiency을 측정하였다.

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