• Title/Summary/Keyword: DC/RF magnetron sputter

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A Comparison of the Properties of DC and RF Sputter - deposited Cr films (DC 및 RF 스퍼터링법으로 증착한 Cr 박막의 특성 비교)

  • Park, Min-Woo;Lee, Chong-Mu
    • Korean Journal of Materials Research
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    • v.16 no.8
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    • pp.461-465
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    • 2006
  • Chromium (Cr) films were deposited on plain carbon steel sheets by DC and RF magnetron sputtering as well as by electroplating. Effects of DC or RF sputtering power on the deposition rate and properties such as, hardness, surface roughness and corrosion-resistance of the Cr films were investigated. X-ray diffraction (XRD), atomic force microscopy (AFM), scanning electron microcopy (SEM) analyses were performed to investigate the crystal structure, surface roughness, thickness of the Cr films. Salt fog tests were used to evaluate the corrosion resistance of the samples. The deposition rate, hardness, and surface roughness of the Cr film deposited by either DC or RF sputtering increase with the increase of sputtering power but the adhesion strength is nearly independent of the sputtering power. The deposition rate, hardness, and adhesion strength of the Cr film deposited by DC sputtering are higher than those of the Cr film deposited by RF sputtering, but RF sputtering offers smoother surface and higher corrosion-resistance. The sputter-deposited Cr film is harder and has a smoother surface than the electroplated one. The sputter-deposited Cr film also has higher corrosion-resistance than the electroplated one, which may be attributed to the smoother surface of the sputter-deposited film.

Preparation and PTC properties of thin films $BaTiO_3$ ceramic system using RF/DC magnetron sputtering method (RF/DC 마그네트론 스퍼터법을 이용한 $BaTiO_3$계 세라믹 박막의 제조와 PTC특성)

  • 박춘배;송민종;김태완;강도열
    • Electrical & Electronic Materials
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    • v.8 no.1
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    • pp.77-82
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    • 1995
  • PTCR(Positive Temperature Coefficient of Resistivity) thermistor in thin film BaTiO$_{3}$ system was prepared by using radio frequency(13.56 MHz) and DC magnetron sputter equipment. Polycrystalline, surface structure, and R-T(Resistivity-Temperature) characteristics of the specimens were measured by X-ray diffraction(D-Max3, Rigaku, Japan), SEM(Scanning Electron Microscopy: M.JSM84 01, Japan), and insulation resistance measuring system (Keithley 719), respectively. Thin films characteristics of the thermistor showed different properties depending on the substrate even with the same sputtering condition. The thin film formed on the A1$_{2}$O$_{3}$ substrate showed a good crystalline and a low resistivity at below curie point. However, the thin films prepared on slide glass and Si wafer were amorphous. The thicknesses of the three samples prepared under the same process conditions were 700[.angs.], 637.75[.angs.], and 715[.angs.], respectively.

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DC/RF Magnetron Co-Sputter를 이용하여 성막한 유기 태양 전지용 Si-Doped $In_2O_3$ (ISO) 박막의 특성 연구

  • Lee, Hye-Min;Gang, Sin-Bi;Jeong, Gwon-Beom;Kim, Han-Gi
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.02a
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    • pp.327-327
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    • 2013
  • 본 연구에서는 $SiO_2$ Target과 $In_2O_3$ Target으로 co-sputtering방법을 이용해 증착한 Si-doped $In_2O_3$ (ISO) 박막의 Si 도핑 농도에 따른 전기적, 광학적, 구조적 특성에 대해 연구하였고, 이를 유기태양 전지(OPVs) 에 적용함으로써 그 가능성을 타진하였다. $In_2O_3$ target의 DC power를 100 W로 고정시킨 채 $SiO_2$ target의 RF power 크기를 20~60 W 변화시키면서 상온에서 실험을 진행한 결과 최적 조건은 박막의 두께가 200 nm일 때 Working pressure는 3 mTorr이고, RF power는 50 W이었다. 이 조건으로 제작된 ISO 박막은 550 nm에서 81.51%의 광투과율과 51.91 Ohm/sq.의 비교적 낮은 면저항이 나타남을 Hall measurement 및 UV/Vis spectroscopy 분석을 통해 알 수 있었다. 또한 X-ray diffraction 분석법과 Transmission Electron Microscope 분석법을 통해 $SiO_2$ 도핑 power가 50 W 이상으로 증가할 경우 ISO 박막의 결정성이 감소하여 완벽한 비정질상의 ISO 투명박막이 형성됨을 확인할 수 있었다. 비정질 특성을 갖는 ISO 투명 전극을 이용하여 유기 박막형 태양전지를 제작한 결과 Voc (0.576 V), Jsc (7.671 mA/$cm^2$), FF (62.96%), PCE (2.78%)의 특성을 나타냄으로서 co-sputtering 공정을 통해 최적화된 ISO 박막을 유기 박막형 태양전지에 적용함으로써 광전소자로의 적용 가능성을 확인할 수 있었다.

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A thin film condition of material for AR and HR coating by the DC/RF Magnetron Sputter (DC/RF Magnetron Sputter를 이용한 무반사 및 고반사 박막증착)

  • Yang, Jin-Seok;Jo, Woon-Jo;Lee, Cheon;Kim, Dong-Woo;Shinn, Chun-Kyo
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2003.04a
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    • pp.206-209
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    • 2003
  • The purpose of AR and HR coating is acquire the very low reflection rate and the high reflection rate through the deposition of a thin film using the refraction ofmaterial. Basically if the high refractive material and the low refractive material are chosen and the condition for the experiment is determined, then we solve theproject with the optical design and multi thin film coating. First of all, we choose $SiO_2$for the low refractive material and $TiO_2$ for the high refractive material and apply Sputtering System easy to control the refraction rate and excellent in reconstruction to the equipment of thin film multiplication. For the control of the refraction rate and growth rate we modify RF Power and the ratio of Gas(Ar:O2), And we use Ellipsometer for estimation and analysis of the refraction rate and growth rate and AFM&SEM for the analysis of surface and component.

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A Study on the Annealed Properties of ITO Thin Film Deposited by RF-superimposed DC Reactive Magnetron Sputtering (RF/DC 동시인가 마그네트론 스퍼터링 방법으로 증착된 ITO 박막의 열처리 특성 연구)

  • Moon, Jin-Wook;Kim, Dong-Won
    • Journal of the Korean institute of surface engineering
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    • v.40 no.3
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    • pp.117-124
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    • 2007
  • The ITO films were deposited on glass substrates by RF-superimposed dc reactive magnetron sputtering and were annealed in $N_2$ vacuum furnace with temperatures in the range of $403K{\sim}573K$ for 30 minutes. Electrical, optical and structural properties of ITO films were examined with varying annealing temperatures from 403 K to 573 K. The resistivity of as-deposited ITO films was $5.4{\times}10^{-4}{\Omega}cm$ at the sputter conditions of applied RF/DC power of 200/200 W, $O_{2}$ flow of 0.2 seem and Ar flow of 0.2 seem. As a result of annealing in the temperature range of $403K{\sim}573K$, the crystallization occurred at 423 K that is lower than the crystallization temperature caused by a conventional sputtering method. And the resistivity decreased from $5.4{\times}10^{-4}{\Omega}cm\;to\;2.3{\times}10^{-4}{\Omega}cm$, the carrier concentration and mobility of ITO films increased from $4.9{\times}10^{20}/cm^3\;to\;6.4{\times}10^{20}/cm^3$, from $20.4cm^2/Vsec\;to\;41.0cm^2/Vsec$, respectively. The transmittance of ITO films in visible became higher than 90% when annealed in the temperature range of $423K{\sim}573K$. High quality ITO thin films made by RF-superimposed dc reactive magnetron sputtering and annealing in $N_2$ vacuum furnace will be applied to transparent conductive oxides of the advanced flat panel display.

PTCR Characteristics of BaTiO$_3$Thin Films made by rf/dc Magnetron Sputter Technique

  • Song, Min-Jong;So, Byung-Moom;Kim, Tae-Wan
    • Transactions on Electrical and Electronic Materials
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    • v.1 no.2
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    • pp.28-31
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    • 2000
  • BaTiO$_3$cerameic thin films doped with Mn were manufactured by rf/dc magnetron sputter technique. We have investigated crystal structure, surface morphology and PRCR(positive-temperature coefficient of resistance) characteristics of the specimen depending on second heat-treatment temperature. Second heat treatment of the specimen were performed in the temperature range of 400 to 1350$\^{C}$ X-ray diffraction patterns of BaTiO$_3$ thin films show that the specimen heat treated below 600$\^{C}$ is an amorphous phase and the one heat treated above 1100$\^{C}$ forms a poly-crystallization . In this specimen heat-treated at 1300$\^{C}$, a lattice constant ratio(c/a) was 1.188. Scanning electron microscope(SEM) image of BaTiO$_3$ thin films of the specimen heat treated in between 900 and 1100$\^{C}$ shows a grain growth. At 1100$\^{C}$, the specimen stops grain-growing and becomes a poly-crystallization . A resistivity-temperature characteristics of the specimen depends on the doping concentrations of Mn. A resistivity ratio between the value at room temperature and the one above Curie temperature was 10$^4$ for pure BaTiO$_3$ thin films and 10$\^$5/ fo BaTiO$_3$ : additive 0.127mol% MnO

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Magnetron Sputter내 Plasma 분포 및 Target Erosion Profile 해석

  • 김성구;오재준;신재광;이규상;허재석;이형인;이윤석
    • Proceedings of the Korean Vacuum Society Conference
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    • 1999.07a
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    • pp.209-209
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    • 1999
  • 현재 magnetron sputter는 반도체, LCD 등을 포함하는 microelectronics 산업에서 박막형성을 위한 주요 장비로 널리 쓰이고 있으며, 소자의 고집적화 및 대형화 추세에 따라 그 이용가치는 더욱 증대되고 있다. 본 연구엣는 TFT-LCD용 Color Filter 제조시 ITO박막형성을 위해 사용하는 magnetron sputter 내부의 플라즈마 분포 및 ion kinetic energy에 대한 해석을 실시하였으며, ITO target의 erosion 형상의 원인을 실험결과와 비교하였다. Magnetron sputtering은 target에 가해지는 bias 전압(DC 혹은 RF)에 의해 target과 shield 혹은 target과 substrate 사이에서 생성될 수 잇는 플라즈마를 target 및 부분에 붙어있는 영구자석을 이용하여 target 근처에 집중시키고, target 표면과 플라즈마 사이의 전위차에 의해 가속된 이온들이 target 표면과 충돌하여 이차 전자방출을 일으킴과 동시에 target 표면에서 sputtering을 일으키고, 이들 sputtered 된 중성의 atom 들이 substrate로 날아가 박막을 형성하는 원리로 작동된다. 이때 target에서 방출되는 이차전자들은 영구자석에 의한 자기장 효과에 의해 target 근처에 갇히게 되어 중성 기체분자들과 이온화반응을 통해 플라즈마를 유지하고 그 밀도를 높혀주는 역할을 담당하게 된다. 즉 낮은 압력 및 bias 전압에서도 플라즈마 밀도를 높일수 있고 sputtering 공정이 가능한 장점을 가지고 있다. Magnetron sputtering 현상에 대한 시뮬레이션은 크게 magnetron discharge와 sputtering에 대한 해석 두가지로 나누어 볼 수 있는데, sputtering 현상 자체를 수치묘사할 수 있는 정량적인 모델은 아직까지 명확하게 정립되어 있지 않다. 따라서 본 연구에서는 magnetron plasma 자체에 대한 수치해석에 주안점을 두고 아울러 bulk plasma 영역에서 target으로 입사하는 이온들의 입사에너지 및 입사각도 등을 Monte Carlo 방법으로 추적하여 sputtering 현상을 유추해보았다. Sputtering 현상을 살펴보기 위해 magnetron sputter 내 플라즈마 밀도, 전자온도, 특히 target 및 substrate를 충돌하는 이온의 입사에너지 및 입사각 분포등을 계산하는데 hybrid 방법으로 시뮬레이션을 하였다. 즉 ion과 bulk electron에 대해서는 fluid 방식으로 접근하고, 이차전자 운동과 그로 인한 반응관계 및 target으로 입사하는 이온의 에너지와 입사각 분포는 Monte-Carlo 방법으로 처리하였다. 정지기장해석의 경우 상용 S/W인 Vector Fields를 사용하였다. 이를 통해 sputter 내 플라즈마 특성, target으로 입사하는 이온에너지 및 각 분포, 이들이 target erosion 형상에 미치는 영향을 살펴보았다. 또한 이들 결과로부터 간단한 sputtering 모델을 사용하여 target으로부터 sputter된 입자들이 substrate에 부착되는 현상을 Monte-Carlo 방법으로 추적하여 성막특성도 살펴보았다.

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Structural evolution and electrical property of RF sputter-deposited ZnO:Al film by rapid thermal annealing process (RF sputter로 증착된 ZnO:Al 박막의 Rapid Thermal Annealing 처리에 따른 구조개선 및 전기적 특성)

  • Park, Kyeong-Seok;Lee, Kyu-Seok;Lee, Sung-Wook;Park, Min-Woo;Kwak, Dong-Joo;Lim, Dong-Gun
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2005.07a
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    • pp.466-467
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    • 2005
  • Al doped zinc oxide films (ZnO:Al) were deposited on glass substrate by RF magnetron sputtering from a ZnO target mixed with 2 wt% $Al_2O_3$. The as-deposited ZnO:Al films were rapid-thermal annealed. Electrical properties and structural evolution of the films, as annealed by rapid thermal process (RTP), were studied and compared with the films annealed by conventional annealing process. RTP, the (002) peak intensity increases and the electrical resistivity decreases by 20%, after RT annealing. The effects of RT annealing on the structural evolution and electrical properties of RF sputtered films were further discussed and compared also with the films deposited by DC magnetron sputtering.

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Development of Thermal Sensor Devices in the $BaTiO_3$ Systems ($BaTiO_3$계 박막형 열전센서소자 개발)

  • Song, Min-Jong
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2003.05d
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    • pp.100-104
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    • 2003
  • $BaTiO_3$ ceramic thin films were manufactured by rf/dc magnetron sputter technique. We have investigated crystal structure, surface morphology and PTCR(positive-temperature coefficient of resistance) characteristics of the specimen depending on second heat-treatment temperatures. Second heat treatments of the specimen were performed in the temperature range of 400 to $1350^{\circ}C$. X-ray diffraction patterns of $BaTiO_3$ thin films show that the specimen heat treated below $600^{\circ}C$ is an amorphous phase and the one heat treated above $1100^{\circ}C$ forms a poly-crystallization. In the specimen heat-treated at $1300^{\circ}C$, a lattice constant ratio (c/a) was 1.188. Scanning electron microscope(SEM) image of $BaTiO_3$ thin films of the specimen heat treated in between 900 and $1100^{\circ}C$ shows a grain growth. At $1100^{\circ}C$, the specimen stops grain-growing and becomes a poly-crystallization.

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Thermal Stability of Self-formed Barrier Stability Using Cu-V Thin Films

  • Han, Dong-Seok;Mun, Dae-Yong;Kim, Ung-Seon;Park, Jong-Wan
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.188-188
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    • 2011
  • Recently, scaling down of ULSI (Ultra Large Scale Integration) circuit of CMOS (Complementary Meta Oxide Semiconductor) based electronic devices, the electronic devices, become much faster and smaller size that are promising property of semiconductor market. However, very narrow interconnect line width has some disadvantages. Deposition of conformal and thin barrier is not easy. And metallization process needs deposition of diffusion barrier and glue layer for EP/ELP deposition. Thus, there is not enough space for copper filling process. In order to get over these negative effects, simple process of copper metallization is important. In this study, Cu-V alloy layer was deposited using of DC/RF magnetron sputter deposition system. Cu-V alloy film was deposited on the plane SiO2/Si bi-layer substrate with smooth surface. Cu-V film's thickness was about 50 nm. Cu-V alloy film deposited at $150^{\circ}C$. XRD, AFM, Hall measurement system, and AES were used to analyze this work. For the barrier formation, annealing temperature was 300, 400, $500^{\circ}C$ (1 hour). Barrier thermal stability was tested by I-V(leakage current) and XRD analysis after 300, 500, $700^{\circ}C$ (12 hour) annealing. With this research, over $500^{\circ}C$ annealed barrier has large leakage current. However vanadium-based diffusion barrier annealed at $400^{\circ}C$ has good thermal stability. Therefore thermal stability of vanadium-based diffusion barrier is desirable for copper interconnection.

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