• Title/Summary/Keyword: bulk deposition

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Study on diffusion barrier properties of Tantalum films deposited by substrate bias voltage (Ta 확산 방지막 특성에 미치는 기판 바이어스에 관한 연구)

  • ;;Minoru Isshiki
    • Journal of the Korean Vacuum Society
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    • v.12 no.3
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    • pp.174-181
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    • 2003
  • Ta diffusion barriers have been deposited on Si (100) substrate by applying a negative substrate bias voltage. The effect of the substrate bias voltage on the properties of the Ta films was investigated. In the case of the Ta films deposited without the substrate bias voltage, a columnar structure and small grains were observed distinctly, and the electrical resistivity of the deposited Ta films was very high (250 $\mu\Omega$cm). By applying the substrate bias voltage, no clear columnar structure and grain boundary were observed. The resistivity of the Ta films decreased remarkably and at a bias voltage of -125 V, reaching a minimum value of 40 $\mu\Omega$cm, which is close to that of Ta bulk (13 $\mu\Omega$cm). The thermal stability of Cu(100 mm)/Ta(50 mm)/Si structures was evaluated after annealing in H2 atmosphere for 60 min at various temperatures. The Ta films deposited by applying the substrate bias voltage were found to be stable up to $600^{\circ}C$, while the Ta films deposited without the substrate bias voltage degraded at $400^{\circ}C$.

Effect of Negative Oxygen Ions Accelerated by Self-bias on Amorphous InGaZnO Thin Film Transistors

  • Kim, Du-Hyeon;Yun, Su-Bok;Hong, Mun-Pyo
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.02a
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    • pp.466-468
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    • 2012
  • Amorphous InGaZnO (${\alpha}$-IGZO) thin-film transistors (TFTs) are are very promising due to their potential use in thin film electronics and display drivers [1]. However, the stability of AOS-TFTs under the various stresses has been issued for the practical AOSs applications [2]. Up to now, many researchers have studied to understand the sub-gap density of states (DOS) as the root cause of instability [3]. Nomura et al. reported that these deep defects are located in the surface layer of the ${\alpha}$-IGZO channel [4]. Also, Kim et al. reported that the interfacial traps can be affected by different RF-power during RF magnetron sputtering process [5]. It is well known that these trap states can influence on the performances and stabilities of ${\alpha}$-IGZO TFTs. Nevertheless, it has not been reported how these defect states are created during conventional RF magnetron sputtering. In general, during conventional RF magnetron sputtering process, negative oxygen ions (NOI) can be generated by electron attachment in oxygen atom near target surface and accelerated up to few hundreds eV by self-bias of RF magnetron sputter; the high energy bombardment of NOIs generates bulk defects in oxide thin films [6-10] and can change the defect states of ${\alpha}$-IGZO thin film. In this paper, we have confirmed that the NOIs accelerated by the self-bias were one of the dominant causes of instability in ${\alpha}$-IGZO TFTs when the channel layer was deposited by conventional RF magnetron sputtering system. Finally, we will introduce our novel technology named as Magnetic Field Shielded Sputtering (MFSS) process [9-10] to eliminate the NOI bombardment effects and present how much to be improved the instability of ${\alpha}$-IGZO TFTs by this new deposition method.

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Advanced Low-k Materials for Cu/Low-k Chips

  • Choi, Chi-Kyu
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.02a
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    • pp.71-71
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    • 2012
  • As the critical dimensions of integrated circuits are scaled down, the line width and spacing between the metal interconnects are made smaller. The dielectric film used as insulation between the metal lines contributes to the resistance-capacitance (RC) time constant that governs the device speed. If the RC time delay, cross talk and lowering the power dissipation are to be reduced, the intermetal dielectric (IMD) films should have a low dielectric constant. The introduction of Cu and low-k dielectrics has incrementally improved the situation as compared to the conventional $Al/SiO_2$ technology by reducing both the resistivity and the capacitance between interconnects. Some of the potential candidate materials to be used as an ILD are organic and inorganic precursors such as hydrogensilsequioxane (HSQ), silsesquioxane (SSQ), methylsilsisequioxane (MSQ) and carbon doped silicon oxide (SiOCH), It has been shown that organic functional groups can dramatically decrease dielectric constant by increasing the free volume of films. Recently, various inorganic precursors have been used to prepare the SiOCH films. The k value of the material depends on the number of $CH_3$ groups built into the structure since they lower both polarity and density of the material by steric hindrance, which the replacement of Si-O bonds with Si-$CH_3$ (methyl group) bonds causes bulk porosity due to the formation of nano-sized voids within the silicon oxide matrix. In this talk, we will be introduce some properties of SiOC(-H) thin films deposited with the dimethyldimethoxysilane (DMDMS: $C_4H_{12}O_2Si$) and oxygen as precursors by using plasma-enhanced chemical vapor deposition with and without ultraviolet (UV) irradiation.

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Cat-CVD법을 이용하여 다양한 제막압력 조건에서 증착된 PTFE(polytetrafluoroethylene) 박막의 소수성 평가에 관한 연구

  • Alghusun, Mohammad;Yeo, Seung-Jun;An, Jeong-Seon
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.02a
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    • pp.281-281
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    • 2012
  • 연꽃잎 효과(Lotus effect)라 불리는 자가 세정 효과(self cleaning effect)는 연꽃이 항상 깨끗한 상태를 유지하는 것이 관찰되면서 꾸준히 관심에 대상이 되어 왔었다. 자가 세정 효과는 접촉각 $150^{\circ}$ 이상의 초소수성 표면에서 구현이 가능하며 이런 표면을 일상생활부터 산업분야까지 응용하고자 하는 많은 노력들이 있었다. 물질의 친수성 또는 소수성은 표면의 거칠기(roughness)와 표면에너지(surface energy)의 두 가지 특성에 의해 결정된다. 하지만 낮은 표면에너지 물질을 사용해도 접촉각 $150^{\circ}$ 이상의 초소수성 표면을 얻긴 힘들며, 표면의 거칠기를 증가시켜야 한다. PTFE (polytetrafluoroethylene)는 낮은 표면에너지를 가진 소수성 물질로 bulk일 경우 접촉각이 약 $108^{\circ}$이지만 거친 표면을 가진 박막으로 만들 경우 접촉각이 $150^{\circ}$ 이상의 값을 가지는 초수수성 표면이 가능한 물질이다. 특히, 초소수성 표면 이외에 우수한 내열성 및 내화학성 특성을 가지고 있어 디스플레이 및 태양전지 등의 자가세정(self cleaning) 보호막으로써 응용이 기대되고 있다. 본 연구에서는 HFPO (hexafluoropropylene)를 원료 가스로 이용하여, Si(100)과 유리 기판위에 Cat-CVD (Catalytic Chemical Vapor Deposition)법으로 PTFE 박막을 증착하였다. 텅스텐(W)을 촉매로 사용하였으며, 촉매온도가 $850^{\circ}C$이상인 조건에서 접촉각이 $150^{\circ}$ 이상인 초소수성 PTFE 표면을 쉽게 얻을 수 있었다. 특히 본 연구에서는 제막압력을 300 mTorr에서 700 mTorr까지 변화시켜 가며 유리와 Si 기판위에 증착하였다. Cat-CVD 제막압력을 변화시켜가며 증착된 PTFE 박막의 접촉각을 측정한 결과, 제막압력이 300 mTorr일 때 glass와 Si 기판위에 증착된 PTFE박막 표면에서의 접촉각은 각각 133, $117^{\circ}$였지만, 제막압력이 400 mTorr이상일 땐 $150^{\circ}$ 이상의 높은 접촉각을 갖는 초소수성 표면을 얻을 수 있었다.

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고밀도 알루미늄 박막 코팅과 특성 분석

  • Yang, Ji-Hun;Jeong, Jae-In;Jang, Seung-Hyeon;Park, Hye-Seon
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.45-45
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    • 2011
  • 알루미늄과 그 합금은 내부식성(corrosion resistance)이 좋고, 밀도가 낮아 높은 연료소비 효율을 필요로 하는 항공기와 자동차 같은 운송수단의 내-외장 소재로 사용되고 있다. 또한 알루미늄의 높은 내부식성을 이용하여 철강소재의 부식을 방지하는 보호막으로도 폭 넓게 사용된다. 물리기상증착(physical vapor deposition)으로 알루미늄을 코팅하면 박막 성장 초기단계에서 핵(nucleus)을 형성하고, 형성된 핵을 중심으로 주상 구조(columnar structure)로 박막이 성장하는 것이 일반적으로 알려진 방식이다. 주상 구조의 알루미늄 박막은 주상정과 주상정 사이에 필연적으로 공극(pore)이 존재하게 되어 부식을 일으키는 물질이 박막으로 침투하게 되고, 부식 물질과 모재가 반응하여 공식(pitting corrosion)이 발생한다. 본 연구에서는 스퍼터링(magnetron sputtering)을 이용하여 치밀한 조직을 갖는 알루미늄 박막을 코팅할 수 있는 공정을 개발하고, 치밀한 알루미늄 조직이 내부식성에 어떠한 영향을 미치는지 평가하였다. 기판은 냉연강판(cold rolled steel sheet)이 사용되었으며, 알루미늄 타겟의 순도는 99.999%, 크기는 직경 4"이었다. 냉연강판은 진공용기(vacuum chamber)에 장착하기 전에 계면활성제를 이용하여 표면에 존재하는 기름성분을 제거하였으며, 진공용기에 장착한 후에는 아르곤 가스를 이용하여 발생시킨 글로우 방전으로 표면에 존재하는 산화물을 제거하였다. 알루미늄 박막의 조직에 영향을 미치는 공정변수를 확인하기 위해서 스퍼터링 파워, 공정 온도, 공정 압력, 외부 자기장 세기 등의 공정 조건을 변화시켜 코팅을 실시하였다. 실험을 통해서 얻어진 최적 조건으로 알루미늄을 코팅할 경우, 알루미늄 bulk의 밀도와 비교하여 약 94.7%의 밀도를 갖는 알루미늄 박막을 코팅할 수 있었다. 알루미늄 박막이 약 3 ${\mu}$m의 두께로 코팅된 냉연강판의 내부식성 평가(salt spray test, 5% NaCl) 결과, 평가를 시작한 후 72시간 후에도 적청이 발생하지 않았다.

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Electrochemical Properties of Buckminsterfullerene ($C_{60}$) in Acetonitrile Containing Quarternary Ammonium Electrolytes

  • Kim, Il Kwang;Kim, Hyun Jin;Oh, Gi Su;Jeon, Il Chol;Ahn, Byoung Joon
    • Analytical Science and Technology
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    • v.8 no.4
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    • pp.675-682
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    • 1995
  • Thin films of buckminsterfullerene($C_{60}$) formed by solution drop casting on Pt foil electrode surfaces were studied by cyclic voltammetry(CV) in acetonitrile(MeCN) containing quaternary ammonium or alkali-metal salts as supporting electrolyte. The electrochemical behaviors of $C_{60}$ films are found to be strongly dependent on the nature of the supporting electrolytes, especially with tetrabutyl ammonium perchlorate (TBAP, $NBu_4ClO_4$), and tetrabutyl ammonium tetrafluoroborate ($TBABF_4$, $NBu_4BF_4$). Reasonably stable films are formed into which electrons can be injected. The interaction of $C_{60}$ film with the quaternary ammonium cation may produce the fulleride salts $(TBA^+)(C{_{60}}^-)$ and $(TBA^+)_2(C{_{60}}^{2-})$. The bulk electroreduction with a controlled potential to generate the soluble $C{_{60}}^{3-}$ anions(dark red-brown color) is followed by electrooxidative deposition to produce a neutral $C_{60}$ film on the surface. The peak currents($I_{pc}$ and $I_{pa}$) of these thin film were dramatically decreased with repetitive potential scanning. These results could be explained by the adsorption-desorption phenomena and ion pairing interaction of reduced species($C{_{60}}^-$, and $C{_{60}}^{2-}$) onto the electrode surface. The peak current changes and peak potential shifts of the thin $C_{60}$ film in cyclic voltammograms formed from solution were observed by varying scan rates.

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A Study on the Mechanical Properties of Ag-X(X=Cu,Ni,C) Alloys Prepared by the Vacuum-deposition Technique (진공증착법으로 제작한 Ag-X(X=Cu,Ni,C) 합금의 기계적 성질에 관한 연구)

  • Oh, Chang-Sup;Han, Chang-Suk
    • Journal of the Korean Society for Heat Treatment
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    • v.24 no.5
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    • pp.243-250
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    • 2011
  • When alloys are vacuum-deposited on cooled substrates, super-rapidly cooled alloy films in the unequilibrium state can be obtained. As an application of this method, Ag-Cu, Ag-Ni and Ag-C alloys were successfully produced, and their mechanical properties with tempering temperature were investigated. The following results were obtained : (1) In case of Ag-Cu alloys, the solid solution was hardened by tempering at $150^{\circ}C$. The hardening is considered to occur when the solid solution begins to decompose into ${\alpha}$ and ${\beta}$ phases. The Knoop hardness number of a 40 at.%Ag-Cu alloy film deposited on a cooled glass substrate was 390 $kg/mm^2$. The as-deposited films were generally very hard but fractured under stresses below their elastic limits. (2) In case of Ag-Ni and Ag-C alloys, after the tempering of 4 at.%Ni-Ag alloy at $400^{\circ}C$ and of 1 and 2 at.%C-Ag alloys at $200^{\circ}C$, they were hardened by the precipitation of fine nickel and carbon particles. The linear relationship between proof stress vs. $(grain\;diameter)^{-l/2}$ for bulk silver polycrystals can be applied to vacuum-deposited films up to about 0.1 ${\mu}m$ grain diameter, but the proof stress of ultra-fine grained silver with grain diameters of less than 0.1 ${\mu}m$ was smaller than the value expected from the Petch's relation.

A Study on the Growth of CdTe Films by Close-Spaced Sublimation (근접승화법을 이용한 CdTe박막의 성장에 관한 연구)

  • Lee, Min-Suk;Huh, Joo-Youl;Kim, Dong-Hwan
    • Korean Journal of Materials Research
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    • v.8 no.5
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    • pp.383-393
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    • 1998
  • Cadmium telluride films were grown by close-spaced sublimation(CSS) technique. The effects of various deposition parameters such as ambient pressure, source- to-substrate spacings and temperatures on the growth rate and the microstructure were investigated. The growth mode of CdTe films showed a transition as the ambient pressure changed. This transition was interpreted in terms of the diffusion limited transport and the sublimation limited transport of Cd and $Te_2$ vapors. Experimental results indicated that the transition of growth mode was related with the mean free path of gas molecules. The growth rate and the microstructure of CdTe films were affected by the source type- bulk or powder. This change was due to the temperature difference at the source surface. XRD and SEM analysis showed that the growth rate was one of the main factors to determine CdTe microstructures.

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Nanotubular Structures of Oxides and Their Applications (산화물 나노튜브 구조체 제작 방법 및 그 응용)

  • Yoo, Hyun-Jun;Bae, Chang-Deuck;Kim, Hyun-Chul;Yoon, Young-Jin;Kim, Myung-Jun;Shin, Hyun-Jung
    • Journal of the Korean Vacuum Society
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    • v.19 no.2
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    • pp.105-113
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    • 2010
  • One-dimensional nanostructures have been researched widely because of its unique physical properties such as optical, electrical, mechanical, and chemical properties in comparison with bulk structures. Especially nanotubular structures are able to provide larger surface area, capability to load purposeful materials, and unique mechanical modulus. We reviewed the oxide nanotube technology with focusing on the method of template-directed fabrication. We can easily control of physical dimensions of nanotubes by control of nanotemplate and fabrication condition. and template-directed fabrication is ideal tool to fabricate the amount of monodisperse nanotubes. They have potentials for application in solar cell, drug-delivery, Li-ion batteries and photocatalyst. We discussed these potential applications and research trends.

Microstructure Control of Tungsten Film for Bragg Reflectors of Thin Film Bulk Acoustic Wave Resonators (체적탄성파 공진기 브라그 반사층 적용을 위한 텅스텐 박막의 미세구조 조절에 대한 연구)

  • 강성철;이시형;박종완;이전국
    • Journal of the Korean Ceramic Society
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    • v.40 no.3
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    • pp.268-272
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    • 2003
  • The microstructures of tungsten films were controlled by changing the sputtering pressure and substrate temperatures during D.C. sputter deposition. As the sputtering pressures were decreased, the sputtered models of the tungsten films were changed from the zone I model to zone T model. The tungsten film having zone T model microstructure shows a resistivity of 10${\times}$10$\^$-6/ $\Omega$-cm and (110) preferred orientation. FBAR with Bragg reflector composed of $SiO_2$and tungsten films having zone T model microstructure shows quality factor, Q$\_$s/, of 494 and K$\_$eff/$\^$2/ of 5.5% due to the high acoustic impedance and the smooth surface.