• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2006.11a
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• pp.366-367
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• 2006

In general, HF chemistry lifts off the particles during scrubbing after polishing and effectively removes particles. It is sometimes impossible to apply HF chemistry on W plug due to the degradation of electrical characteristics of a device. In this paper, a post W CMP cleaning process is proposed to remove residue particles without applying HF chemistry. After W CMP, recessed plugs are created, therefore they easily trap slurry particles during CMP process. These particles in recessed plug are not easy to remove by brush scrubbing when $NH_4OH$ chemistry is used for the cleaning because the brush surface can not reach the recessed area of plugs. Buffing with oxide slurry was followed by W CMP due to its high selectivity to W. The buffing polishes only oxide slightly which creates higher plug profiles than surrounding oxide. Higher profiles make the brush contact much more effectively and result in a similar particle removal efficiency even in $NH_4OH$ cleaning to that in HF brush scrubbing.

• Journal of the Korean Institute of Telematics and Electronics
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• v.26 no.7
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• pp.13-20
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• 1989

An accurate design method for rectangular microstrip patch antenna that can be applied to wide range of frequencies (C-band to X-band) is proposed. With due regard the frequency dependent effective dielectric permittivity to design formula, the inaccuracy of previous design formulae can be overcome. The results predicted by new procedure are compared well experimental results that had varying operation frequencies between 7GHz and 15GHz. Antennas are fabricated over microwave substrates with the same dielectric permittivity and thickness. Radiation power patterns are also measured and they well with theoretical values.

• Journal of the Institute of Electronics and Information Engineers
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• v.50 no.1
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• pp.276-284
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• 2013

This paper considers the transfer alignment in the inertial navigation system and the observability analysis is performed for velocity matching. The state variable of the Kalman filter is modeled including the lever arm error and the measurement equation is obtained. The SOM(Stripped Observability Matrix) method is used for the observability analysis for various maneuvering conditions of the vehicle, which gives the full state observability condition as a specific maneuver sequence of the vehicle. While the observability analysis of a lever arm effect in the existing papers is mainly performed by simulations, we performed it analytically by the observability analysis method. The analysis result is verified using the computer simulations.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2003.07b
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• pp.1119-1122
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• 2003

In this paper, the electric field distribution in dielectric tube with one layer and spherical dielectric in water was simulated. The reactor was made up of the spherical dielectric that is diameter 2.5[mm], ${\epsilon}_r$ : 5, 100, 1000, 5000 respectively and one glass plate being 2[mm] thickness, ${\epsilon}_r$ : 5 as electrode. The discharge gap was 7[mm]. As a result of the simulation, in case of being about the same value between the dielectric constant of spherical dielectric and water, when the reactor was applied to high voltage dielectric polarization characteristic was trending toward disappearance. To get more strong electric field, the dielectric constant should be higher comparatively, Increasing the spherical dielectric constant, the location of equippotential line was shifting from the interior to the exterior.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2003.07b
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• pp.1143-1146
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• 2003

This paper was simulated the electric field distribution in dielectric tube with two layers and spherical dielectric in water. The reactor was made up of the spherical dielectric that is diameter : 2.5[mm], ${\epsilon}_r$ : 5, 25, 100, 1000, 5000 respectively and two glass plate being 2[mm] thickness, ${\epsilon}_r$ : 5 as electrode. The discharge gap was 9[mm]. As a result of the simulation, in case of being about the same value between the dielectric constant of spherical dielectric and water, when the reactor was applied to high voltage, dielectric polarization characteristic was trending toward disappearance. To get more strong electric field, the dielectric constant should be higher comparatively, Increasing the spherical dielectric constant, the location of equippotential line was shifting from the interior to the exterior.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2003.07b
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• pp.846-850
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• 2003

Thin film $SnO_2$ Gas Sensor was fabricated by using ion beam sputtering and ultra thin film Pt catalyst of $45{\AA}$ was deposited on $SnO_2$ thin film. The effects of annealing temperature on the structural properies of $SnO_2$ were investigated using the X-ray diffraction. Using SEM, microstructures of thin film were investigated. The good gas sensitivity is shown when annealing condition is $650^{\circ}C$, 5hr and ultra thin film Pt catalyst thickness is $45{\AA}$.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2004.11a
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• pp.640-643
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• 2004

유도결합형 플라즈마는 낮은 가스 압력에서도 고밀도의 플라즈마를 발생시키기 때문에 무전극 램프에 많이 적용되고 있다. 그리고 무전극 램프는 장 수명을 실현하고 고품질의 빛을 발생하기 때문에 앞으로 광범위하고 다양한 장소에 사용이 예상된다. 본 논문에서는 유도결합형 플라즈마를 이용한 아르곤 가스의 방전 특성 중에서 색 좌표 특성을 살펴보았다. 즉, 외부 안테나에 의해 발생된 13.56[MHz]의 RF Power를 방전관 내부로 전달하고, 아르곤 가스 압력과 RF Power 변화에 따른 아르곤 가스의 방전 특성을 측정하였다. 또한, 유도결합형 플라즈마를 방전시키기 위한 아르곤 가스의 압력은 1[mTorr]에서 100[mTorr], RF 전력은 10[W]에서 120[W]이며 이의 색 좌표 특성과 스펙트럼을 살펴보았다. 측정 결과 RF 출력이 증가하면 색 좌표의 x, y 값이 동시에 감소하였다. 아르곤 가스 압력이 증가하면 농도의 증가로 인해 발광이 어려웠으며, 색 좌표 특성은 압력이 증가하면서 y 값은 변화가 적었으나 x 값이 100[mTorr]일 크게 증가하는 현상이 나타났다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2010.06a
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• pp.230-230
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• 2010

본 연구에서는 개조된 MOCVD법을 이용하여 (100) GaAs 기판 위에 나노 구조 $Bi_2Te_3$ 열전 필름을 성장시켰다. 기존의 MOCVD법과 달리 서셉터의 모양을 변화시켜 기체상태에서 $Bi_2Te_3$ 나노파티클의 형성과 기판위에서 성장을 유도 하였다. 또한 서셉터의 노즐의 면적을 변화시켜 기체의 속도를 제어함에 따라 $Bi_2Te_3$ 필름을 형성시켰다. 서셉터의 모양의 변화에 따라 기체 상태에서 $Bi_2Te_3$ 나노파티클을 형성하고 이를 기판위에서 성장시켜 $Bi_2Te_3$ 열전 필름의 결정립계를 조절할 수 있었고, 또한 노즐의 면적의 변화에 따른 기체의 속도를 제어하여 $Bi_2Te_3$ 결정립계 및 결정 배향 방향을 조절 하였다. 본 연구결과에서는 MOCVD 반응관의 서셉터의 모양 및 노즐의 면적의 변화에 따라 결정립계 및 결정 성장방향이 조절될 수 있음을 확인하였고 이러한 변화에 따라 열전도도를 제어하여 열전성능지수의 향상을 기대 할 수 있다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2008.11a
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• pp.130-131
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• 2008

Chalcogenide glass has been known for many photo induced phenomena and superial electron / optical specific by structure flexibility, unique electronic configuration. It is become known to the greatest specific as photonic material medium that possible to perfect controlling by continuity and photo inducing direction of amorphous chalcogenide. In our experiment, we choose the amorphous As-Ge-Se-S and coming glass as a substrate. And then we have evaporated in the ${\sim}2{\times}10^{-6}$ Torr using a E-beam evaporator, completed thin film sample that have 1um thickness of As-Ge-Se-S 600 $\AA$, 10~5 $\AA$/s. At first, we let the change the angle between laser and sample by holography litho method and then, expect that satisfied conclusion which 2-dimension diffraction lattice manufacture and specifics by investing a He-Ne laser for 2000 seconds.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2008.11a
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• pp.334-345
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• 2008

컴퓨터의 발달과 더불어 현대사회는 기록하고 보존해야할 정보의 양이 점점 방대해 지고 있다. 그로 인해 자기기록매체처럼 정보를 사용자의 편의에 따라 반복적으로 기록하고 재생할 수 있는 광기록매체에 대한 관심이 증가되고 있다. $Ge_2Sb_2Te_5$(GST)는 기존의 CD-RW나 Floppy Disk(FD)를 대체할 차세대 기록매체로 주목받고 있다. 따라서 본 연구에서는 비정질상과 결정상으로 변하는 성질을 가지고 있는 GST롤 상변화 기록매체로서 이용하기 위해 굴절률을 평가하였다. 시료는 5N의 순도를 갖는 Ge, Sb, Te 물질을 준비하고 조성비에 맞추어서 석영관에 진공 봉입한 후 용융-냉각법으로 벌크를 제작하였고 열증착 방법으로 Si 및 유리 기판위에 1000nm 두께로 박막을 제작하였다. UV-Vis-IR spectrophotometer를 사용하여 반사도와 투과도를 측정하였고 측정한 스펙트럼을 이용하여 Swanepoel method로 굴절률을 계산하였다. 본 연구진이 자체 개발한 계산툴에 실험값을 대입하였고 실험에 의해 얻은 투과도와 계산툴에 의해 얻은 투과도 스펙트럼을 비교하였다.