• 제목/요약/키워드: Physical Vapor Deposition

검색결과 325건 처리시간 0.025초

Al 박막의 underlayer로서의 Ionized Physical Vapor Deposition (I-PVD) Ti 또는 I-PVD Ti/Metal-Organic Chemical Vapor Deposition TiN (Ti Prepared by ionized physical vapor deposition (I-PVD) and TiN prepared by metal-organic chemical vapor deposition(MOCVD) as underlayers of aluminum TiN)

  • 이원준;나사균
    • 한국진공학회지
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    • 제9권4호
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    • pp.394-399
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    • 2000
  • Underlayer의 종류 및 두께가 Al 박막의 texture 및 면저항 변화에 미치는 영향을 연구하였다. Al의 underlayer로는 ionized physical vapor deposition(I-PVD)에 의해 제조된 Ti와 I-PVD Ti 위에 metalorganic chemical vapor deposition(MOCVD)에 의해 제조된 TiN을 적층한 구조가 사용되었으며, 각각에 대해 두께를 변화시키면서 Al 박막의 배향성, 면저항을 조사하고, $400^{\circ}C$, $N_2$분리기에서 열처리하면서 면저항의 변화를 조사하였다. I-PVD Ti만을 Al의 underlayer로 사용한 경우, Ti두께가 5 nm이어도 Al 박막이 우수한 <111> 배향성을 나타내었으나, Al-Ti반응 때문에 열처리 후 Al 배선의 면저항이 크게 상승하였다. I-PVD 와 Al 사이에 MOCVD TiN을 적용함에 의해 Al <111> 배향성의 큰 저하없이 Al-Ti 반응에 의한 면저항의 증가를 억제할 수 있었으며, MOCVD TiN의 두께가 4 nm 이하일 때 특히 우수한 Al <111> 배향성을 나타내었다.

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증기증착 공정 감시를 위한 반도체 레이저 흡수 분광학 (Semiconductor laser-based absorption spectroscopy for monitoring physical vapor deposition process)

  • 정의창;송규석;차형기
    • 한국진공학회지
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    • 제13권2호
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    • pp.59-64
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    • 2004
  • 반도체 레이저를 광원으로 사용하는 원자흡수분광 방법으로 금속증기의 증착 공정을 감시하는 연구를 수행하였다. 전자빔 가열 방식을 이용하여 gadolinium (Gd) 금속을 대량으로 증발시켰다. 파장 영역이 770-794 nm (중심파장 780 nm)인 반도체 레이저빔과 388-396 nm 영역의 제 2 고조파 빔을 진공용기에 입사시켜 증발되는 금속증기의 원자흡수 스펙트럼을 실시간으로 기록하였다. 흡수 스펙트럼을 분석하여 증기의 원자밀도를 구했다. 전자빔 출력을 변화시키면서 측정한 원자밀도를 수정 결정 모니터 장치를 사용하여 측정한 증착률과 비교하였다. 산업적으로 많이 사용되는 Ti 등의 증착 공정 감시에 이 실험에서 구현한 레이저 분광장치를 적용할 수 있다는 것을 제시하였다.

Influence of Mg Vapor Pressure on the $MgB_2$/Carbon Fiber Fabricated by Physical Vapor Deposition method

  • Li, Xiang;Ha, Hong-Soo;Kim, Cheol-Jin
    • 한국초전도ㆍ저온공학회논문지
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    • 제13권4호
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    • pp.5-9
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    • 2011
  • We have fabricated the superconducting $MgB_2$/carbon fiber by physical vapor deposition method. Mg (Magnesium) and B (Boron) were simultaneously deposited on the carbon fiber using the RF-sputtering and thermal evaporation, respectively. To ensure the relatively high vapor pressure of Mg at the growth region and the subsequent phase stability of $MgB_2$ at the deposition temperature, inverted funnel-like guide made of Mg-foil was employed while one side of the guide were open for the sputtered B flux. Mg vapor pressure should be controlled precisely to secure the complete reaction. The $MgB_2$/carbon fiber showed a uniformly deposited thin layer with dense and well-formed grains. The $MgB_2$/carbon fibers in this study showed $T_c$~37.5K, $J_c$ ~ $2{\times}10^4\;A/cm^2$ in the 20K, 0T.

Controllability of Structural, Optical and Electrical Properties of Ga doped ZnO Nanowires Synthesized by Physical Vapor Deposition

  • Lee, Sang Yeol
    • Transactions on Electrical and Electronic Materials
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    • 제14권3호
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    • pp.148-151
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    • 2013
  • The control of Ga doping in ZnO nanowires (NWs) by physical vapor deposition has been implemented and characterized. Various Ga-doped ZnO NWs were grown using the vapor-liquid-solid (VLS) method, with Au catalyst on c-plane sapphire substrate by hot-walled pulsed laser deposition (HW-PLD), one of the physical vapor deposition methods. The structural, optical and electrical properties of Ga-doped ZnO NWs have been systematically analyzed, by changing Ga concentration in ZnO NWs. We observed stacking faults and different crystalline directions caused by increasing Ga concentration in ZnO NWs, using SEM and HR-TEM. A $D^0X$ peak in the PL spectra of Ga doped ZnO NWs that is sharper than that of pure ZnO NWs has been clearly observed, which indicated the substitution of Ga for Zn. The electrical properties of controlled Ga-doped ZnO NWs have been measured, and show that the conductance of ZnO NWs increased up to 3 wt% Ga doping. However, the conductance of 5 wt% Ga doped ZnO NWs decreased, because the mean free path was decreased, according to the increase of carrier concentration. This control of the structural, optical and electrical properties of ZnO NWs by doping, could provide the possibility of the fabrication of various nanowire based electronic devices, such as nano-FETs, nano-inverters, nano-logic circuits and customized nano-sensors.

Vapor Deposition Techniques for Synthesis of Two-Dimensional Transition Metal Dichalcogenides

  • Song, Jeong-Gyu;Park, Kyunam;Park, Jusang;Kim, Hyungjun
    • Applied Microscopy
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    • 제45권3호
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    • pp.119-125
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    • 2015
  • Two-dimensional (2D) transition metal dichalcogenides (TMDCs) have attracted significant attention due to their unique and exotic properties attributed to their low dimensionality. In particular, semiconducting 2D TMDCs such as $MoS_2$, $WS_2$, $MoSe_2$, and $WSe_2$ have been demonstrated to be feasible for various advanced electronic and optical applications. In these regards, process to synthesize high quality 2D TMDCs layers with high reliability, wafer-scale uniformity, controllable layer number and excellent electronic properties is essential in order to use 2D TMDCs in practical applications. Vapor deposition techniques, such as physical vapor deposition, chemical vapor deposition and atomic layer deposition, could be promising processes to produce high quality 2D TMDCs due to high purity, thickness controllability and thickness uniformity. In this article, we briefly review recent research trend on vapor deposition techniques to synthesize 2D TMDCs.

진공증착법을 이용한 PVDF 유기박막의 분자배향 (The Molecular Orientation of PVDF Organic Thin Film by Vapor Deposition Method)

  • 박수홍;이선우;임응춘;최충석;이덕출
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 1997년도 춘계학술대회 논문집
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    • pp.297-300
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    • 1997
  • In this study, The PVDF thin film was fabricated on the one method of dry-process the physical vapor deposition method, applied electric field, and evaporation control in $\beta$-PVDF thin film preparation. A study on the electric-field-phase change of PVDF thin film in physical vapor deposition using the polymer deposition apparatus which are manufactured for oneself. In the analysis of Fourier-Transform Infrared spectra, according to increasing of electric field intensity, the 510$cm^{-1}$ / peak and 1273$cm^{-1}$ / peak which are showed in $\beta$-PVDF increase, on the contrary the 530$cm^{-1}$ / peak and 977$cm^{-1}$ / peak which are showed in $\alpha$-PVDF decrease.

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Development of Highly Conductive and Corrosion-Resistant Cr-Diamond-like Carbon Films

  • Ko, Minjung;Jun, Yee Sle;Lee, Na Rae;Kang, Suhee;Moon, Kyoung Il;Lee, Caroline Sunyong
    • 한국세라믹학회지
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    • 제56권3호
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    • pp.317-324
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    • 2019
  • Cr-diamond-like carbon (Cr-DLC) films were deposited using a hybrid method involving both physical vapor deposition and plasma-enhanced chemical vapor deposition. DLC sputtering was carried out using argon and acetylene gases. With an increase in the DC power, the Cr content increased from 14.7 to 29.7 at%. The Cr-C bond appeared when the Cr content was 17.6 at% or more. At a Cr content of 17.6 at%, the films showed an electrical conductivity of > 363 S/cm. The current density was 9.12 × 10-2 ㎂/㎠, and the corrosion potential was 0.240 V. Therefore, a Cr content of 17.6 at% was found to be optimum for the deposition of the Cr-DLC thin films. The Cr-DLC thin films developed in this study showed high conductivity and corrosion resistance, and hence, are suitable for applications in separators.

박막제조 기술의 동향과 전망 (Trend and Prospect of Thin Film Processing Technology)

  • 정재인;양지훈
    • 한국자기학회지
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    • 제21권5호
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    • pp.185-192
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    • 2011
  • 박막제조 기술은 과학 기술의 기초가 되는 분야로 양질의 박막을 제조하기 위한 다양한 노력이 경주되고 있다. 박막제조는 표면개질과 함께 표면처리 기술의 한 분야이며 이중 진공증착으로 알려진 물리증착법과 화학증착법은 현대의 과학기술 연구는 물론 산업적으로 폭넓게 이용되는 박막제조 기술 중의 하나이다. 진공증착을 이용한 박막제조 기술은 나노 기술의 등장과 함께 비약적인 발전을 이루었으며 자연모사와 완전화 박막의 제조, 융복합 공정을 이용한 기능성 코팅과 Engineered Structure 구현 그리고 초고속 증착과 원가 저감 기술의 실현이 주요 이슈로 등장하고 있다. 본 논문에서는 물리증착법과 화학증착법을 중심으로 박막제조 기술의 종류와 원리를 설명하고 박막제조 기술의 최신 동향과 기술적 이슈 및 향후 전망에 대해 기술한다.

진공증착법을 이용한 PVDF 유기박막의 제조와 전기전도현상 (The Fabrication of PVDF Organic Thin Films by Physical Vapor Deposition Method and Their Electrical Conductivity Phenomena)

  • 임응춘;이덕출
    • E2M - 전기 전자와 첨단 소재
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    • 제10권3호
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    • pp.217-225
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    • 1997
  • In this study, the PVDF organic thin film was fabricated by the physical vapor deposition method to be dry-process. The distance of heat source and substrate was 5[cm] and the temperature of substrate was 30[.deg. C], when the pressure had reached 2.0 x 10$^{-5}$ [Torr], the temperature of heat source was reached to 285[.deg. C] to heat at 6-8[.deg. C/min] rate, the shutter was opened and deposition was started. TG-DTA(Thermogravimetric-Differential Thermal Analysis) spectrum of PVDF pellets showed that endothermic peak arose at 170[.deg. C] and exothermic peak at 524[.deg. C], but that of thin PVDF film showed that endothermic peak arose at 145[.deg. C] and exothermic peak at 443[.deg C]. The current density was increased linearly with increasing voltage but increased nonlinearly with higher electric field than 250[kV/cm] and activation energy was about 0.667[eV] at the temperature of 30-90[.deg. C].

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