• Title/Summary/Keyword: RF마그네트론 스퍼터링

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Influences of Target-to-Substrate Distance and Deposition Temperature on a-SiOx/Indium Doped Tin Oxide Substrate as a Liquid Crystal Alignment Layer (RF 마그네트론 스퍼터링에서 증착거리와 증착온도가 무기 액정 배향막의 물리적 성질에 미치는 영향에 대한 연구)

  • Park, Jeung-Hun;Son, Phil-Kook;Kim, Ki-Pom;Pak, Hyuk-Kyu
    • Korean Journal of Materials Research
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    • v.18 no.10
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    • pp.521-528
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    • 2008
  • We present the structural, optical, and electrical properties of amorphous silicon suboxide (a-$SiO_x$) films grown on indium tin oxide glass substrates with a radio frequency magnetron technique from a polycrystalline silicon oxide target using ambient Ar. For different substrate-target distances (d = 8 cm and 10 cm), the deposition temperature effects were systematically studied. For d = 8cm, oxygen content in a-$SiO_x$ decreased with dissociation of oxygen onto the silicon oxide matrix; temperature increased due to enlargement of kinetic energy. For d = 10 cm, however, the oxygen content had a minimum between $150^{\circ}\;and\;200^{\circ}$. Using simple optical measurements, we can predict a preferred orientation of liquid crystal molecules on a-$SiO_x$ thin film. At higher oxygen content (x > 1.6), liquid crystal molecules on an inorganic liquid crystal alignment layer of a-$SiO_x$ showed homogeneous alignment; however, in the lower case (x < 1.6), liquid crystals showed homeotropic alignment.

Annealing Temperature Properties of SBT Thin Film for Semiconductor Device (반도체 소자용 SBT 박막의 후속 열처리 특성)

  • Oh, Yong-Cheul;Kim, Ki-Joon;Jeon, Dong-Keun;Hong, Sun-Pyo;Kim, Sang-Jin;Song, Ja-Yoon;Lee, Joon-Ung
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2004.07b
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    • pp.697-700
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    • 2004
  • The SBT$(Sr_{0.8}Bi_{2.4}Ta_2O_9)$ thin films for semiconductor device were deposited on Pt-coated $Pt/TiO_2/SiO_2Si$ wafer by RF magnetron sputtering method at $400[^{\circ}C]$ and annealed at the temperature range from $600[^{\circ}C]$ to $850[^{\circ}C]$. The top electrodes(Pt) were deposited on SBT thin film by DC sputtering method. The crystallinity of SBT thin films were increased with increase of annealing temperature in the temperature range of $600[{\circ}C]\sim850[^{\circ}C]$. The annealing temperature properties were to be most excellent in the case of annealed SBT thin film at $750^{\circ}C]$. And, the maximum remanent polarization$(2P_r)$ and the coercive electric field$(E_c)$ at annealing temperature of $750[^{\circ}C]$ obtained about $11.60[{\mu}C/cm^2]$ and 48[kV/cm], respectively. Specially, it was seen that fatigue properties does not change in $10^{10}$ switching cycle.

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Post-annealing Effect of N-incorporated $WO_3$ Films for Photoelectrochemical Cells (광전기화학 전지를 위한 질소 도핑된 $WO_3$ 박막의 후열처리 효과)

  • Ahn, Kwang-Soon
    • Clean Technology
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    • v.15 no.3
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    • pp.202-209
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    • 2009
  • N-incorporated $WO_3$ ($WO_3$:N) films were synthesized using a reactive RF magnetron sputtering on unheated substrate and then post-annealed at different temperatures from 300 to $500^{\circ}C$ in air. The N anion narrowed optical band gap, due to its mixing effect with the O 2p valence states. Furthermore, it was found that the crystallinity of the $WO_3$:N films was significantly improved by the post-annealing at $350^{\circ}C$ and higher. As a result, the $WO_3$:N films exhibited much better photoelectrochemical performance, compared with pure $WO_3$ films post-annealed at the same temperature.

Electrical and Optical Properties of BZO Thin Films Deposited by RF Magnetron Sputtering with Various Annealing Temperatures (열처리 온도에 따른 BZO 박막의 전기적 및 광학적 특성)

  • Seong-Jun Kang;Yang-Hee Joung
    • The Journal of the Korea institute of electronic communication sciences
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    • v.19 no.1
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    • pp.47-52
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    • 2024
  • The effects of annealing temperature on the optical and electrical properties of BZO thin films, grown on glass substrate, have been investigated. Analysis of the XRD shows that regardless of the annealing temperature, all BZO thin films indicate the c-axis orientation. The full width of half maximum (FWHM) decreases from 1.65 to 1.07° as the annealing temperature increases from 400 to 600℃. The average transmittance in the visible light region showed a high value of 85% without significantly affecting the annealing temperature. The results of Hall effect measurements indicate that the carrier concentration and mobility increased and the resistivity decreased as the annealing temperature increased. The resistivity and the carrier concentration of the BZO thin films annealed 600℃ were 9.75×10-2 Ω·cm and 4.21×1019 cm-3 respectively, showing the best value. The optimization of deposition and annealing conditions will certainly make the BZO thin films promising materials for the application to the next generation of optoelectronic devices.

Preparation of Bismuth Telluride Thin Films using RF magnetron sputtering and Study on Their Thermoelectric Properties (RF 마그네트론 스퍼터링을 이용한 Bismuth Telluride 박막의 제조와 그 열전 특성 연구)

  • Kim, Dong-Ho;Lee, Gun-Hwan
    • Journal of the Korean Vacuum Society
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    • v.14 no.4
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    • pp.215-221
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    • 2005
  • Thermoelectric bismuth telluride thin films were prepared on $SiO_{2}$/Si substrate with co-sputtering of bismuth and tellurium targets. The effects of deposition temperature on surface morphology, crystallinity and electrical transport properties were investigated. Hexagonal crystallites were clearly visible at the surface of films deposited above $290 ^{\circ}C$. Change of dominant phase from rhombohedral $Bi_2Te_3$ to hexagonal BiTe was confirmed with X-ray diffraction analysis. The deviation from stoichiometric composition at high deposition temperature resulted in the change of structural and electrical characteristics. Seebeck coefficients of all samples have negative value, indicating the prepared $Bi_XTe_Y$ films are n-type thermoelectric. Optimum of Seebeck coefficient and power factor were obtained at the deposition temperature of $225 \^{circ}$C (about -55 $\mu$V/K and $3\times10^{-4}$ W/$k^{2}$m, respectively). Deterioration of thermoelectric properties at higher temperature.

투명 면상 발열체 응용을 위한 하이브리드 스퍼터 GZO/Ag/GZO 박막의 물성평가

  • Kim, Jae-Yeon;Song, Pung-Geun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2015.08a
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    • pp.182.2-182.2
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    • 2015
  • 최근 학계나 산업계에서 투명 전자 소자에 대하여 활발한 연구가 진행되면서, 투명 전 도성 산화물(TCO: transparent conductive oxide)에 대한 관심이 높아지고 있다. 대표적인 TCO 물질인 Indium Tin Oxide (ITO)는 가시 광 영역에서의 높은 투과 및 높은 도전성을 가져 전압을 인가하면 발열이 가능하므로 이를 투명 면상 발열체에 적용시키는 연구가 활발히 진행되고 있다. 하지만, ITO는 발열 테스트 결과 온도가 상승함에 따라 발열이 일부분에 집중되는 현상이 있으며, 전도성을 높이기 위하여 추가공정이 필요하다. 또한, 글라스의 곡면 부분에서 ITO를 사용하면 유연성이 부족하므로 크랙이 발생한다는 단점이 있다. 따라서, 최근 Silver nanowire (AgNW), Single-walled Carbon nanotube (SWCNT), ITO를 기반으로 한 AgNW에 ITO를 증착 하거나 SWCNT를 코팅하여 우수한 전기적, 광학적 특성을 지닌 하이브리드 전극이 투명 면상 발열체 재료로서 사용되고 있다. 하지만 대체된 재료들도 다양한 문제점을 가지고 있다. 예를 들어 고온에서 발열을 유지하지 못하고 끊어지거나 가시광영역의 투과율이 낮은 점 등이 있다. 이런 다양한 문제점들을 보완 할 수 있는 새로운 투명 면상 발열체에 적용한 연구가 요구되고 있다. 본 연구에서는 GZO/Ag/GZO 하이브리드 구조의 투명 면상 발열체를 제작하여 전기적, 광학적 특성을 비교하고 발열량, 온도 균일 성, 발열 유지 안정도를 확인하였다. 본 연구에서는 $50{\times}50mm$ 크기의 Non-alkali glass (삼성코닝 E2000) 기판 상에 DC마그네트론 스퍼터링 공정을 이용하여 상온에서 GZO, Ag, GZO 박막을 연속적으로 증착 하여 다층구조의 하이브리드형 투명 면상 발열체를 제조하였다. 박막 증착 파워는 DC (Ag) power 50 W, RF (GZO) power 200 W로 하였으며 GZO박막두께는 45 nm로 고정 시키고 Ag박막 두께는 5~20 nm로 변화를 주었다. 증착원은 3인치 GZO 세라믹 타깃 (2.27 wt. % Ga2O3) 과 Ag 금속 타깃 (순도 99.99%)을 사용하였으며, Ar을 40 sccm 주입 후 Working pressure는 고 순도 Ar을 사용하여 1.0 Pa로 고정하며 10분간 Pre-sputtering을하고 증착을 진행하였다. 앞선 실험을 통해 증착한 박막의 전기적, 광학적 특성은 각각 Hall-effect measurements system (ECOPIA, HMS3000), UV-Vis spectrophotometer (UV-1800, Shimadzu)를 사용해 측정 되었으며, 하이브리드 표면의 구조 및 형상은 FESEM으로 관찰하였다. 또한 표면온도 측정기infrared camera (IR camera)를 이용하여 4~12 V/cm의 전압을 인가 시 시간에 따른 투명 면상 발열체의 표면 온도변화를 관찰하였다.

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Effects of composition of preannealed Y-Ba-Cu-0 thin films deposited by sputtering on the superconducting properties and microstructure of post-annealed thin films (스퍼터링 증착된 Y-Ba-Cu-O계 박막의 열처리 전 조성이 열처리 후 박막의 초전도특성 및 미세구조에 미치는 영향)

  • Cho, Hae-Seok;Kim, Hyeong-Jun
    • Korean Journal of Materials Research
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    • v.1 no.1
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    • pp.54-61
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    • 1991
  • YBCO films deposited on MgO(100) and Si(100) by rf-magnetron sputtering using stoichiometric single target were annealed under oxygen atmosphere at $880^{\circ}C$ for 1 hr. The microstructure and superconducting properties of YBCO thin films depended on the composition of pre-annealed thin films. Basal planesuperconducting particles grown on MgO(100) substrate had small and rod-like shade due to preferred orientation, while superconducting film grown on the basal plane-superconducting particles showed round-shape particles. If pre-annealed thin film had nonstoichiometric composition, liquid phase was formed during the heat treatment, which made it easy for particles to grow in the preferred orientation and thus to form textured structure. But the thin films with the textured structure did not show good superconducting properties, especially $T_c$, since the liquid phase transformed into second phase in the grain boundary during the cooling. The effect of the second phase on $T_{c, \;zero}$ was greater than that on $T_{c, \;on}$.

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Influence of the RF Power on the Optical and Electrical Properties of ITZO Thin Films Deposited on SiO2/PES Substrate (RF파워가 SiO2/PES 기판위에 증착한 ITZO 박막의 광학적 및 전기적 특성에 미치는 효과)

  • Choi, Byeong-Kyun;Joung, Yang-Hee;Kang, Seong-Jun
    • The Journal of the Korea institute of electronic communication sciences
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    • v.16 no.3
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    • pp.443-450
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    • 2021
  • After selecting a PES substrate with excellent thermal stability and optical properties among plastic substrates, a SiO2 thin film was deposited as a buffer layer to a thickness of 20nm by plasma-enhanced chemical vapor deposition to compensate for the high moisture absorption. Then, the ITZO thin film was deposited by a RF magnetron sputtering method to investigate electrical and optical properties according to RF power. The ITZO thin film deposited at 50W showed the best electrical properties such as a resistivity of 8.02×10-4 Ω-cm and a sheet resistance of 50.13Ω/sq.. The average transmittance of the ITZO thin film in the visible light region(400-800nm) was relatively high as 80% or more when the RF power was 40 and 50W. Figure of Merits (ΦTC and FOM) showed the largest values of 23.90×10-4-1 and 5883 Ω-1cm-1, respectively, in the ITZO thin film deposited at 50W.

A Study on the Effect of O$_2$ annealing on Structural, Optical, and Electrical Characteristics of Undoped ZnO Thin Films Deposited by Magnetron Sputtering (산소 어닐링이 마그네 트론 스퍼터링으로 증착된 undoped ZnO박막의 구조적, 광학적, 전기적 특성에 미치는 영향에 대한 연구)

  • Yun, Eui-Jung;Park, Hyeong-Sik
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.46 no.7
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    • pp.7-14
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    • 2009
  • In this paper, the effects of annealing conditions on the structural ((002) intensity, FWHM, d-spacing, grain size, (002) peak position), optical (UV peak, UV peak position) and electrical properties (carrier concentrations, resistivity, mobility) of ZnO films were investigated. ZnO films were deposited onto SiO$_2$/si substrates by RF magnetron sputtering from a ZnO target. The substrate was not heated during deposition. ZnO films were annealed in temperature ranges of $500\sim650^{\circ}C$ in the O$_2$ flow for 5$\sim$20 min. The film average thicknesses were in the range of 291 nm. The surface morphologies and structures of the samples were characterize by SEM and XRD, respectively. The optical properties were evaluated by photoluminescence (PL) measurement at room temperature (RT) using a He-Cd 325 nm laser. As the annealing temperature and time vary, the following relations were also observed: (1) proportional relationships among UV intensity (002) intensity, and grain size exist, (2) UV intensity is inversely proportional to FWHM, (3) there is no special relationship between UV intensity and electron carrier concentrations, (4) d-spacing is inversely proportional to (002) peak position, (5) UV peak position in the range of 3.20$\sim$3.24 eV means that ZnO films have a n-type conductivity which was consistent with that obtained from the electrical property, (6) the optimal conditions for the best optical and structural characteristics were found to be oxygen fraction, (O$_2$/(O$_2$+Ar)) of 0.2, RF power of 240W, substrate temperature of RT, annealing condition of 600$^{\circ}C$ for 20 min, and sputtering pressure of 20 mTorr.

Deposition of ZnO Thin Films by RF Magnetron Sputtering and Cu-doping Effects (RF 마그네트론 스퍼터링에 의한 ZnO박막의 증착 및 구리 도우핑 효과)

  • Lee, Jin-Bok;Lee, Hye-Jeong;Seo, Su-Hyeong;Park, Jin-Seok
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.49 no.12
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    • pp.654-664
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    • 2000
  • Thin films of ZnO are deposited by using an RF magnetron sputtering with varying the substrate temperature(RT~39$0^{\circ}C$) and RF power(50~250W). Cu-doped ZnO(denoted by ZnO:Cu) films have also been prepared by co-spputtering of a ZnO target on which some Cu-chips are attached. Different substrate materials, such as Si, $SiO_{2}/Si$, sapphire, DLC/Si, and poly-diamond/Si, are employed to compare the c-axial growth features of deposited ZnO films. Texture coefficient(TC) values for the (002)-preferential growth are estimated from the XRD spectra of deposited films. Optimal ranges of RF powers and substrate temperatures for obtaining high TC values are determined. Effects of Cu-doping conditions, such as relative Cu-chip sputtering areas, $O_{2}/(Ar+O_{2})$ mixing ratios, and reactor pressures, on TC values, electrical resistivities, and relative Cu-compositions of deposited ZnO:Cu films have been systematically investigated. XPS study shows that the relative densities of metallic $Cu(Cu^{0})$ atoms and $CuO(Cu^{2+})$-phases within deposited films may play an important role of determining their electrical resistivities. It should be noted from the experimental results that highly resistive(> $10^{10}{\Omega}cm$ ZnO films with high TC values(> 80%) can be achieved by Cu-doping. SAW devices with ZnO(or Zn):Cu)/IDT/$SiO_{2}$/Si configuration are also fabricated to estimate the effective electric-mechanical coupling coefficient($k_{eff}^{2}$) and the insertion loss. It is observed that the devices using the Cu-doped ZnO films have a higher $k_{eff}^{2}$ and a lower insertion loss, compared with those using the undoped films.

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