• Proceedings of the Korean Vacuum Society Conference
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• 2000.02a
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• pp.191-191
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• 2000

마이크로파 절연파괴(breakdown) 및 ECR 플라즈마를 발생시키기 위해 2.45 GHz 마그네트론을 사용하여 간편한 마이크로파 발생장치를 제작하였다. 이 장치는 KAIST-토카막에서 고온 플라즈마를 발생시킬 때 재현성이 좋은 플라즈마를 얻기 위해서 전 이온화하는데 이용된다. 장치에 사용한 마그네트론은 LG 전자의 2M213이고 출력 500W, 주파수 2.45GHz이며, 가정용 전자오븐에 사용된다. 기존의 가정용 마그네트론은 음극(cathode)과 양극(anode)사이에 걸리는 고전압이 60Hz의 주기를 갖기 때문에 약 16ms 마다 8ms동안만 주기적으로 초고주파를 발생한다. 이 마그네트론을 사용하여 연속적으로 발생되는 마이크로파를 얻기 위해서 음극과 양극사이에 개량된 회로로 리플전압이 작은 DC 고전압(5kV, 1A)을 인가하였다. 본 연구에서는 주기적으로 생성.소멸하는 ECR 프라즈마와 연속적인 ECR 플라즈마를 발생시켜 랑뮈어탐침과 광증배관(PMT)을 이용한 H$\alpha$ 방출(emission)을 측정하여 마이크로파 발생장치의 특성을 조사하였다.

• 전기의세계
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• v.28 no.2
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• pp.61-67
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• 1979

연속파 마그네트론을 구동하는 전원회로에 대하여 컴퓨터 시뮬레이션을 행함으로써, 컴퓨터를 이용한 회로설계 방법을 제시하였다. 철공진변압기는 잘 알려진 T-등가회로보다 비선형 특성을 해석하기에 용이한 .pi.-등가회로를 나타내었다. 변압기 철심의 자화특성은 i=a.phi.+b.phi.$^{7}$ 의 함수로 모델링하였으며, 마그네트론과 다이오드는 구분적직선 모델로 근사화하였다. 해석적 설계방정식으로부터 구한 커패시턴스, 변압기의 누설 인덕턴스 및 권수비의 값들을 사용하여 전원회로에 대한 컴퓨터 시뮬레이션을 행하여서 마그네트론의 전류파형및 평균양극전류의 값들을 얻었다. 이 시뮬레이션 결과를 해석적 계산치 및 실험측정 결과와 비교하였으며 특히 해석적 설계방법의 유효성을 검토하였다.

• Journal of the Korean Society for Precision Engineering
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• v.12 no.9
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• pp.126-136
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• 1995

Copper magnetron anode of a microsave-over consists of an cylindrical outer-tube and various inner-vanes. The magnetron anode is produced by the complex processes; vane blanking, pipe cutting and silver-alloy brazing of vanes. Recently, the backward extrusion process for forming vanes has been developed to avoid the complex procedures. The developed process is analyzed by using upper-bound elemental technique (UBET). In the UBET analysis, the upper-bound load, the configuration and the vane-height of final extruded product are determined by minimizing the roral power consumption with repect to chosen parameters. To verify theoretical analysis, experiments have been carried out with pure plasticine billets at room temperature, using different web-thickness and number of vanes. The theoretical predictions both for forming load and vane-height are in reasonable agreement with the experimental results.

• Proceedings of the Korean Society of Precision Engineering Conference
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• 1995.04b
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• pp.204-208
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• 1995

Copper magnetron anode of a microwave-oven consists of an cylindrical outer-tube and various inner-vanes. The magnetron anode is produced by the complex process ; vane blanking, pipe cutting and sliver-alloy brazing of vanes. Recently, the backward extrusion process for forming vanes has been developed to avoid the complex procedures. The developed process is analyzed by using upper-bound elemental technique(UBET). In the UBET analysis, the upper-bound load, the configuration and the vane-height of final extruded product are determined by minimizing the total power consumption with respect to chosen parameters. To verify theoretical analysis, experiments have been carried out with pure plasticine billets at room temperature, using different web-thickness and number of vanes. The theoretical predictions both for forming load and vane-height are in reasonable agreement with the experimental results.

• Journal of the Korean Vacuum Society
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• v.9 no.3
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• pp.290-295
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• 2000

In order to utilize as a pre-ionization means for reproducible ohmic plasma on KAIST-TOKAMAK, a simple, safe, economical and continuous microwave source has been developed using a home kitchen micro-wave oven. The magnetron used in the study can provide 500 W of power at 2.45 GHz. A conventional magnetron in a home kitchen microwave oven generates microwave for 8 ms at every 16 ms periodically due to the periodic (60 Hz) high voltage applied to the magnetron cathode. In order to generate continuous microwave which is suitable for tokamak pre-ionization, the magnetron operation circuit has been modified using a DC high voltage (5 kV, 1 A) power supply. It provides high-voltage with small ripple for magnetron cathode bias. Using the developed magnetron system, electron cyclotron resonace heated (ECH) plasmas were produced and the characteristics of the system were studied by diagnosing the ECH plasma using Langmuir probe and $H_{\alpha}$ emission diagnostics.

• Proceedings of the Korean Society Of Semiconductor Equipment Technology
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• 2003.12a
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• pp.105-108
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• 2003

본 논문은 파이렉스 #7740 유리박막을 이용한 MEMS용 MLCA와 Si기판의 양극접합 특성에 관한 것이다. 최적의 RF 마그네트론 스퍼터링 조건(Ar 100 %, input power $1W/\textrm{cm}^2$)하에서 MLCA 기판위에 파이렉스 #7740 유리의 특성을 갖는 박막을 증착한 후 600 V, $400^{\circ}C$에서 1시간동안 양극접합했다. 그 다음에 Si 다이어프램을 제조한 후, MLCA/Si 접합계면과 MLCA 구동을 통한 Si 다이어프램 변위특성을 분석 및 평가하였다. 다이어프램 형상에 따라 정밀한 변위 제어가 가능했으며 0.05-0.08 %FS의 우수한 선형성을 나타내었다. 또한, 측정동안 접합계면 균열이나 계면분리가 일어나지 않았다. 따라서, MLCA/Si기판 양극접합기술은 고성능 압전 MEMS 소자 제작공정에 유용하게 사용가능할 것이다.

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2007.11a
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• pp.149-150
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• 2007

플라즈마 코팅공정시 질소 인입량 조절에 따라 비대칭 마그네트론 스퍼터링법으로 CrN 박막을 합성하였으며 증착된 CrN 박막을 XRD, SEM, EDX, ESCA, 양극분극시험 등을 통하여 분석을 실시하였다. 플라즈마 공정시 챔버에 인입하는 질소량이 증가함에 따라 박막의 부식특성이 우수해짐을 확인하였다.

• Journal of the Korean Vacuum Society
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• v.19 no.1
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• pp.45-51
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• 2010

We measured the temperature of target surface inducing by various physical phenomenon on magnetron sputtering target and confirmed the possibilities if the temperature distribution could affect plasma and deposited thin film. The target of magnetron sputtering has two types: round type and rectangular type. In a rectangular target, the concentrated discharge area by corner effect by magnetic field and non-uniform erosion of target are generated. And we found the generation of non-uniform temperature distribution on the target surface from this. This area was $10{\sim}20^{\circ}C$ higher than non-sputtering area. And if particles are generated during sputtering process, they were $20^{\circ}C$ higher than the area where is higher than non-sputtering area. These effects result in non-uniformity of thin films, crack of ceramic target, and shortening target life by non-uniform erosion.

• Journal of the Korea Institute of Information and Communication Engineering
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• v.14 no.4
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• pp.923-928
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• 2010

Anodic aluminum oxide (AAO) nanotemplates for nano electronic device applications have been attracting increasing interest because of ease of fabrication, low cost process, and possible fabrication in large area. The size and density of the nanostructured materials can be controlled by changing the pore diameter and the pole density of AAO nanotemplate. In this paper, nano porous alumina films AAO nanotemplate was fabricated by second anodization method using sputterd Al films. In addition, effects of electrolyte temperature and anodization voltate on the microstructure of porous alumina films were investigated. As the electrolyte temperature was increased from $8^{\circ}C$ to $20^{\circ}C$, the growth rate of nanoporous alumina films was increased from 86.2 nm/min to 179.5 nm/min. The AAO nanotemplate fabricated with optimal condition had the mean pore diameter of 70 nm and the pore depth of $1\;{\mu}m$.

• Journal of the Korea Academia-Industrial cooperation Society
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• v.20 no.6
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• pp.80-85
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• 2019

Vanadium dioxide is a well-known metal-insulator phase transition material. Lots of researches of vanadium redox flow batteries have been researched as large scale energy storage system. In this study, vanadium oxide($VO_x$) thin films were applied to cathode for lithium ion battery. The $VO_x$ thin films were deposited on Si substrate($SiO_2$ layer of 300 nm thickness was formed on Si wafer via thermal oxidation process), quartz substrate by RF magnetron sputter system for 60 minutes at $500^{\circ}C$ with different RF powers. The surface morphology of as-deposited $VO_x$ thin films was characterized by field-emission scanning electron microscopy. The crystallographic property was confirmed by Raman spectroscopy. The optical properties were characterized by UV-visible spectrophotometer. The coin cell lithium-ion battery of CR2032 was fabricated with cathode material of $VO_x$ thin films on Cu foil. Electrochemical property of the coin cell was investigated by electrochemical analyzer. As the results, as increased of RF power, grain size of as-deposited $VO_x$ thin films was increased. As-deposited thin films exhibit $VO_2$ phase with RF power of 200 W above. The transmittance of as-deposited $VO_x$ films exhibits different values for different crystalline phase. The cyclic performance of $VO_x$ films exhibits higher values for large surface area and mixed crystalline phase.