• Title/Summary/Keyword: a-Si:H

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Growth characteristics of 4H-SiC homoepitaxial layers grown by thermal CVD (화학기상증착법으로 성장시킨 4H-SiC 동종박막의 성장 특성)

  • Jang, Seong-Joo;Jeong, Moon-Taeg;Seol, Woon-Hag;Park, Ju-Hoon
    • Proceedings of the Korea Association of Crystal Growth Conference
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    • 1999.06a
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    • pp.271-284
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    • 1999
  • As a semiconductor material for electronic devices operated under extreme environmental conditions, silicon carbides (SiCs) have been intensively studied because of their excellent electrical, thermal and other physical properties. The growth characteristics of single-crystalline 4H-SiC homoepitaxial layers grown by a thermal chemical vapor deposition (CVD) were investigated. Especially, the successful growth condition of 4H-SiC homoepitaxial layers using a SiC-uncoated graphite susceptor that utilized Mo-plates was obtained. The CVD growth was performed in an RF-induction heated atmospheric pressure chamber and carried out using off-oriented substrates prepared by a modified Lely method. In order to investigate the crystallinity of grown epilayers, Nomarski optical microscopy, Raman spectroscopy, photoluminescence(PL), scanning electron microscopy (SEM) and other techniques were utilized. The best quality of 4H-SiC homoepitaxial layers was observed in conditions of growth temperature 1500$^{\circ}C$ and C/Si flow ratio 2.0 of C3H3 0.2sccm & SiH4 0.3sccm. The growth rate of epilayers was about 1.0$\mu\textrm{m}$/h in the above growth condition.

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The Effect of RF Power and $SiH_4$/($N_2$O+$N_2$) Ratio in Properties of SiON Thick Film for Silica Optical Waveguide (실리카 광도파로용 SiON 후막 특성에서 RF Power와 $SiH_4$/($N_2$O+$N_2$) Ratio가 미치는 영향)

  • 김용탁;조성민;서용곤;임영민;윤대호
    • Journal of the Korean Ceramic Society
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    • v.38 no.12
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    • pp.1150-1154
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    • 2001
  • Silicon oxynitride (SiON) thick films using the core layer of silica optical waveguide have been deposited on Si wafer by PECVD at low temperature (32$0^{\circ}C$) were obtained by decomposition of appropriate mixture of (SiH$_4$+$N_2$O+$N_2$) gaseous mixtures under RF power and SiH$_4$/($N_2$O+$N_2$) ratio deposition condition. Prism coupler measurements show that the refractive indices of SiON layers range from 1.4663 to 1.5496. A high SiH$_4$/($N_2$O+$N_2$) of 0.33 and deposition power of 150 W leads to deposition rates of up to 8.67 ${\mu}{\textrm}{m}$/h. With decreasing SiH$_4$/($N_2$O+$N_2$) ratio, the SiON layer become smooth from 41$\AA$ to 6$\AA$.

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Hydrogenated a-Si TFT Using Ferroelectrics (비정질실리콘 박막 트랜지스터)

  • Hur Chang-Wu
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.9 no.3
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    • pp.576-581
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    • 2005
  • In this paper. the a-Si:H TFT using ferroelectric of $SrTiO_3$ as a gate insulator is fabricated on glass. High k gate dielectric is required for on-current, threshold voltage and breakdown characteristics of TFT Dielectric characteristics of ferroelectric are superior to $SiO_2$ and $Si_3N_4$. Ferroelectric increases on-current and decreases threshold voltage of TFT and also ran improve breakdown characteristics.$SrTiO_4$ thin film is deposited by e-beam evaporation. Deposited films are annealed for 1 hour in N2 ambient at $150^{\circ}C\~600^{\circ}C$. Dielectric constant of ferroelectric is about 60-100 and breakdown field is about IMV/cm. In this paper, the TFT using ferroelectric consisted of double layer gate insulator to minimize the leakage current. a-SiN:H, a-Si:H (n-type a-Si:H) are deposited onto $SrTiO_3$ film to make MFNS(Metal/ferroelectric/a-SiN:H/a-Si:H) by PECVD. In this paper, TFR using ferroelectric has channel length of$8~20{\mu}m$ and channel width of $80~200{\mu}m$. And it shows that drain current is $3.4{\mu}A$at 20 gate voltage, $I_{on}/I_{off}$ is a ratio of $10^5\~10^8,\;and\;V_{th}$ is$4\~5\;volts$, respectively. In the case of TFT without having ferroelectric, it indicates that the drain current is $1.5{\mu}A$ at 20gate voltage and $V_{th}$ is $5\~6$ volts. If properties of the ferroelectric thin film are improved, the performance of TFT using this ferroelectric thin film can be advanced.

Recrystallized poly-Si TFTs on metal substrate (금속기판에서 재결정화된 규소 박막 트랜지스터)

  • 이준신
    • Electrical & Electronic Materials
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    • v.9 no.1
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    • pp.30-37
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    • 1996
  • Previously, crystallization of a-Si:H films on glass substrates were limited to anneal temperature below 600.deg. C, over 10 hours to avoid glass shrinkage. Our study indicates that the crystallization is strongly influenced by anneal temperature and weakly affected by anneal duration time. Because of the high temperature process and nonconducting substrate requirements for poly-Si TFTs, the employed substrates were limited to quartz, sapphire, and oxidized Si wafer. We report on poly-Si TFT's using high temperature anneal on a Si:H/Mo structures. The metal Mo substrate was stable enough to allow 1000.deg. C anneal. A novel TFT fabrication was achieved by using part of the Mo substrate as drain and source ohmic contact electrode. The as-grown a-Si:H TFT was compared to anneal treated poly-Si TFT'S. Defect induced trap states of TFT's were examined using the thermally stimulated current (TSC) method. In some case, the poly-Si grain boundaries were passivated by hydrogen. A-SI:H and poly-Si TFT characteristics were investigated using an inverted staggered type TFT. The poly -Si films were achieved by various anneal techniques; isothermal, RTA, and excimer laser anneal. The TFT on as grown a-Si:H exhibited a low field effect mobility, transconductance, and high gate threshold voltage. Some films were annealed at temperatures from 200 to >$1000^{\circ}C$ The TFT on poly-Si showed an improved $I_on$$I_off$ ratio of $10_6$, reduced gate threshold voltage, and increased field effect mobility by three orders. Inverter operation was examined to verify logic circuit application using the poly Si TFTs.

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삼중접합 실리콘 박막 태양전지 고효율화를 위한 a-$SiO_x$ 상부전지 특성 연구

  • Lee, JiEun;Jo, Jun Sik;Park, Sang Hyun;Yoon, Kyung Hoon;Song, Jinsoo;Kim, Dong Hwan;Lee, Jeong Chul
    • 한국신재생에너지학회:학술대회논문집
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    • 2010.06a
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    • pp.63.2-63.2
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    • 2010
  • 삼중접합 태양전지에 상부전지로 이용되는 a-SiO:H 태양전지는 PECVD(Plasma Enhanced Chemical Vapour Deposition)을 이용하여 증착하였다. i a-SiO:H는 $CO_2/SiH_4$ 비율을 변화하여 밴드갭을 조절하였다. $CO_2/SiH_4$가 0에서 0.43으로 증가 할수록 밴드갭이 1.74 eV에서 1.94 eV로 증가하는 경향을 보였다. 이는 FTIR에서 나타난 결과인 Si-O-Si 결합의 증가 때문인 것으로 판단한다. 그에 반해서 광 전도도는 감소하는 경향을 보였다.그러나 암전도도와 광전도도의 비율인 광민감도는 $10^5$에서 $10^4$의 값으로 비정질 태양전지에 적용가능한 값을 보였다. 이러한 박막 특성을 가진 i a-SiO:H를 이용하여 비정질 실리콘 태양전지를 제작한 결과 $CO_2/SiH_4$의 비율이 증가함에 따라 태양전지의 $V_{oc}$가 0.8 V에서 0.5 V로 현저하게 감소하였고, $J_{sc}$와 FF 역시 11 $mA/cm^2$에서 4 $mA/cm^2$, 69%에서 50%로 감소하였다. 단위박막 결함을 측정하는 CPM(Constant Photocurrent Method)을 이용하여 i a-SiO:H 내부에 $10^{16}cm^{-3}$ 정도의 내부 결함을 관찰하였고 이는 태양전지의 특성 감소와 관련이 있는 것으로 판단한다.

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A Study on Improved Open-Circuit Voltage Characteristics Through Bi-Layer Structure in Heterojunction Solar Cells (이종접합 태양전지에서의 Bi-Layer 구조를 통한 향상된 개방전압특성에 대한 고찰)

  • Kim, Hongrae;Jeong, Sungjin;Cho, Jaewoong;Kim, Sungheon;Han, Seungyong;Dhungel, Suresh Kumar;Yi, Junsin
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.35 no.6
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    • pp.603-609
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    • 2022
  • Passivation quality is mainly governed by epitaxial growth of crystalline silicon wafer surface. Void-rich intrinsic a-Si:H interfacial layer could offer higher resistivity of the c-Si surface and hence a better device efficiency as well. To reduce the resistivity of the contact area, a modification of void-rich intrinsic layer of a-Si:H towards more ordered state with a higher density is adopted by adapting its thickness and reducing its series resistance significantly, but it slightly decreases passivation quality. Higher resistance is not dominated by asymmetric effects like different band offsets for electrons or holes. In this study, multilayer of intrinsic a-Si:H layers were used. The first one with a void-rich was a-Si:H(I1) and the next one a-SiOx:H(I2) were used, where a-SiOx:H(I2) had relatively larger band gap of ~2.07 eV than that of a-Si:H (I1). Using a-SiOx:H as I2 layer was expected to increase transparency, which could lead to an easy carrier transport. Also, higher implied voltage than the conventional structure was expected. This means that the a-SiOx:H could be a promising material for a high-quality passivation of c-Si. In addition, the i-a-SiOx:H microstructure can help the carrier transportation through tunneling and thermal emission.

Optimization of I layer bandgap for efficient triple junction solarcell by ASA simulation (삼중접합 태양전지에서 Intrinsic Layer 밴드갭 가변을 통한 태양전지 고효율화 시뮬레이션)

  • Kang, Minho;Jang, Juyeon;Baek, Seungsin;Yi, Junsin
    • 한국신재생에너지학회:학술대회논문집
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    • 2011.11a
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    • pp.64.1-64.1
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    • 2011
  • 다중접합 태양전지는 흡수대역이 다른 juntion으로 구성되어, 각각의 태양전지 간의 전류정합(current matching)이 효율 향상에 중요하다. 본 실험에서는 Top cell에 i-a-Si:H(Thinckness:100nm), Middle cell에는 i-a-SiGe:H(Thickness:800nm)을 적용하였고, bottom cell에는 i-${\mu}c$-Si:H(Thickness:1800nm), 수광부의 p-layer에 에 SiOx을 이용하여 triple juntion amorphous silicon solar cell(삼중접합태양전지)을 구현하였다. 이를 최적화 시키기 위해 ASA simulation을 이용하여 각 Cell의 intrinsic layer의 밴드갭을 가변하였다. 가변 결과 i-a-Si:H : 1.85 eV, i-a-SiGe:H: 1.6 eV, i-${\mu}c$-Si:H: 1.4 eV에서 태양전지 효율 14.5 %을 기록 하였다. 본 연구를 통해 Triple juntion cell에서의 intrinsic layer의 밴드갭 최적화를 구현해 볼 수 있었다.

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Effect of CH4 Concentration on the Dielectric Properties of SiOC(-H) Film Deposited by PECVD (CH4 농도 변화가 저유전 SiOC(-H) 박막의 유전특성에 미치는 효과)

  • Shin, Dong-Hee;Kim, Jong-Hoon;Lim, Dae-Soon;Kim, Chan-Bae
    • Korean Journal of Materials Research
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    • v.19 no.2
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    • pp.90-94
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    • 2009
  • The development of low-k materials is essential for modern semiconductor processes to reduce the cross-talk, signal delay and capacitance between multiple layers. The effect of the $CH_4$ concentration on the formation of SiOC(-H) films and their dielectric characteristics were investigated. SiOC(-H) thin films were deposited on Si(100)/$SiO_2$/Ti/Pt substrates by plasma-enhanced chemical vapor deposition (PECVD) with $SiH_4$, $CO_2$ and $CH_4$ gas mixtures. After the deposition, the SiOC(-H) thin films were annealed in an Ar atmosphere using rapid thermal annealing (RTA) for 30min. The electrical properties of the SiOC(-H) films were then measured using an impedance analyzer. The dielectric constant decreased as the $CH_4$ concentration of low-k SiOC(-H) thin film increased. The decrease in the dielectric constant was explained in terms of the decrease of the ionic polarization due to the increase of the relative carbon content. The spectrum via Fourier transform infrared (FT-IR) spectroscopy showed a variety of bonding configurations, including Si-O-Si, H-Si-O, Si-$(CH_3)_2$, Si-$CH_3$ and $CH_x$ in the absorbance mode over the range from 650 to $4000\;cm^{-1}$. The results showed that dielectric properties with different $CH_4$ concentrations are closely related to the (Si-$CH_3$)/[(Si-$CH_3$)+(Si-O)] ratio.

Electrical Characteristics of SiO2/4H-SiC Metal-oxide-semiconductor Capacitors with Low-temperature Atomic Layer Deposited SiO2

  • Jo, Yoo Jin;Moon, Jeong Hyun;Seok, Ogyun;Bahng, Wook;Park, Tae Joo;Ha, Min-Woo
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.17 no.2
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    • pp.265-270
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    • 2017
  • 4H-SiC has attracted attention for high-power and high-temperature metal-oxide-semiconductor field-effect transistors (MOSFETs) for industrial and automotive applications. The gate oxide in the 4H-SiC MOS system is important for switching operations. Above $1000^{\circ}C$, thermal oxidation initiates $SiO_2$ layer formation on SiC; this is one advantage of 4H-SiC compared with other wide band-gap materials. However, if post-deposition annealing is not applied, thermally grown $SiO_2$ on 4H-SiC is limited by high oxide charges due to carbon clusters at the $SiC/SiO_2$ interface and near-interface states in $SiO_2$; this can be resolved via low-temperature deposition. In this study, low-temperature $SiO_2$ deposition on a Si substrate was optimized for $SiO_2/4H-SiC$ MOS capacitor fabrication; oxide formation proceeded without the need for post-deposition annealing. The $SiO_2/4H-SiC$ MOS capacitor samples demonstrated stable capacitance-voltage (C-V) characteristics, low voltage hysteresis, and a high breakdown field. Optimization of the treatment process is expected to further decrease the effective oxide charge density.