• 마이크로전자및패키징학회지
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• 제19권4호
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• pp.19-23
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• 2012

최근 발광다이오드(LED)의 출력 성능을 높이고, 전력 소비를 줄이기 위해 LED 패키지 분야에서 실리콘 기판 연구가 집중되고 있다. 본 연구에서는 공정 비용이 낮고 생산성이 높은 습식 식각을 이용하여 실리콘 기판의 실리콘 관통 비아 식각 공정을 살펴보았다. KOH를 이용한 양면 습식 식각 공정과 습식 식각과 건식 식각을 병행한 두 가지 공정 방법으로 실리콘 관통 비아를 제작하였고, 식각된 실리콘 관통 비아에 Cu 전극과 배선은 전기도금으로 증착하였다. Cu 전극을 연결하는 배선의 전기저항은 약 $5.5{\Omega}$ 정도로 낮게 나타났고, 실리콘 기판의 열 저항은 4 K/W으로 AlN 세라믹 기판과 비슷한 결과를 보였다.

• 한국세라믹학회지
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• 제39권5호
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• pp.517-522
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• 2002

본 연구에서는 PVD 공정으로 Si 양자점 형성시 증착조건의 변화가 증착된 양자점 크기와 분포에 미치는 영향을 Monte Carlo법을 응용한 전산모사를 통하여 정량적으로 분석하였다. 전산모사시 PVD 공정에서 일반적으로 제어가 가능한 기판온도, 증착시간, 가스압력과 타겟-기판거리를 공정변수로 선택하였다. 계산 겨로가 증착속도가 0.05 nm/sec이고 기판온도 490${\circ}$, 증착시간 7 sec, 가스압력 3 mTorr, 타겟-기판거리가 8 cm일때 증착 밀도가 $1{\times}10^{12}cm^{-2}$인 Si 양자점 형성이 가능할 것으로 예측되었다.

• 센서학회지
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• 제9권2호
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• pp.90-95
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• 2000

$Si_3N_4/SiO_2/Si_3N_4$/Si 판위에 MgO 박막을 성장하여 MgO 단결정과 결정배향성이 유사한 초전형 적외선 센서용 기판을 제작하였다. RF 마그네트론 스퍼터링법으로 MgO 박막을 성장하였고, 그 위에 Pt 하부전극과 PLT 박막을 성장시킨 후 c축 배향성을 조사하였다. $500^{\circ}C$의 기판온도와 30 mTorr의 분위기 압력 및 160 W의 RF power에서 성장된 MgO 박막이 단결정 MgO가 가지는 배향성 정도의 우수한 a축 배향성을 보였고, 그 위에 성장된 PLT 박막은 MgO 단결정 기판위에 성장된 것과 거의 회절강도 변화가 유사한 c축 배향성을 보였다.

• 센서학회지
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• 제4권2호
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• pp.58-63
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• 1995

$SiH_{4}$와 $NH_{3}$의 RF 글로우방전 분해에 의한 PECVD법으로 a-SiNx:H박막을 제조하고 기판온도, RF 전력, 그리고 $NH_{3}/SiH_{4}$ 유량비 등의 변화에 따른 a-SiNx:H 박막의 유전상수와 광학적 밴드갭 등을 조사하였다. a-SiNx:H막의 유전상수와 광학적 밴드갭은 기판온도, RF 전력 및 $NH_{3}/SiH_{4}$ 유량비 등의 증착변수에 따라 크게 변화하였다. 기판온도가 증가할수록 a-SiNx:H막의 유전상수는 증가하였으며 광학적 밴드갭은 감소하였다. 기판온도, RF 전력, 가스압력, $NH_{3}/SiH_{4}$ 유량비 및 두께를 각각 $250^{\circ}C$, 20 W, 500 mTorr, 10 및 $1500\;{\AA}$로 하였을 때 a-SiNx:H막의 유전상수, 절연파괴전장 및 광학적 밴드갭은 각각 4.3, 1 MV/cm 및 2.9 eV로 나타났다.

• 한국표면공학회지
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• 제46권4호
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• pp.145-152
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• 2013

The growth behavior of nanocrystalline diamond (NCD) film has been studied for three different substrates, i.e. bare Si wafer, 1 ${\mu}m$ thick W and Ti films deposited on Si wafer by DC sputter. The surface roughness values of the substrates measured by AFM were Si < W < Ti. After ultrasonic seeding treatment using nanometer sized diamond powder, surface roughness remained as Si < W < Ti. The contact angles of the substrates were Si ($56^{\circ}$) > W ($31^{\circ}$) > Ti ($0^{\circ}$). During deposition in the microwave plasma CVD system, NCD particles were formed and evolved to film. For the first 0.5h, the values of NCD particle density were measured as Si < W < Ti. Since the energy barrier for heterogeneous nucleation is proportional to the contact angle of the substrate, the initial nucleus or particle densities are believed to be Si < W < Ti. Meanwhile, the NCD growth rate up to 2 h was W > Si > Ti. In the case of W substrate, NCD particles were coalesced and evolved to the film in the short time of 0.5 h, which could be attributed to the fact that the diffusion of carbon species on W substrate was fast. The slower diffusion of carbon on Si substrate is believed to be the reason for slower film growth than on W substrate. The surface of Ti substrate was observed as a vertically aligned needle shape. The NCD particle formed on the top of a Ti needle should be coalesced with the particle on the nearby needle by carbon diffusion. In this case, the diffusion length is longer than that of Si or W substrate which shows a relatively flat surface. This results in a slow growth rate of NCD on Ti substrate. As deposition time is prolonged, NCD particles grow with carbon species attached from the plasma and coalesce with nearby particles, leaving many voids in NCD/Ti interface. The low adhesion of NCD films on Ti substrate is related to the void structure of NCD/Ti interface.

• 한국전기전자재료학회논문지
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• 제21권1호
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• pp.5-11
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• 2008

To study the effects of $H_2$ gas on AIN insulation thin film, we prepared AIN thin film on Si and GaAs substrate by means of reactive sputtering method using $H_2$ gas as an additives, With treatment conditions of $H_2$ gas AIN thin film shows variable electrical properties such as its crystallization and hysterisis affected to electrical property, As a results, AIN thin film fabricated on Si substrate post-treated with $H_2$ gas for 20 minutes shows much better an insulation property than that of pre-treated, And AIN film treated with $H_2$ gas comparing to non-treated AIN film shows a flat band voltage decreasment. But In GaAs substrate $H_2$ gas does not effect on the flat band voltage.

• 한국정보디스플레이학회:학술대회논문집
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• 한국정보디스플레이학회 2003년도 International Meeting on Information Display
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• pp.690-693
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• 2003

An Si substrate (100) was oxidized at $400^{\circ}C$ in inductively coupled oxygen plasma. Interstitial oxygen was found in the Si substrate at the initial stage of oxidation by IR measurements. An x-ray rocking curve of Si substrates showed a lower peak intensity due to lattice distortion by the interstitial oxygen. The refractive index of thin oxides, below which interstitial oxygen existed in the Si substrate, was smaller than the refractive index of thick oxides, below which no interstitial oxygen existed. The interstitial oxygen was found by plasma oxidation using $O_{2}$ gas and $N_{2}O$ gas. The inductively coupled plasma oxidation using $N_{2}O$ gas was performed by atomic oxygen, not by molecular oxygen, indicating that atomic oxygen in plasma is responsible for the incorporation of interstitial oxygen.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2007년도 춘계학술대회A
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• pp.215-219
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• 2007

In this work, the indium zinc oxide (IZO) films had been deposited on the glass substrate coated with the SiO film. Based on a comparative investigation of the IZO monolayer and IZO/SiO multilayer, it is shown that the thickness of SiO film has a great effect on the mechanical properties of the thin films. The AFM images of the IZO thin film included the SiO film were shown smoother surfaces than monolayer. Resistivity was in inverse proportion to Mobility. If it deposited the SiO film on the substrate, the layer of change was generated between two layer(SiO and substrate). The layer of change influenced resistance because of oxygen content was more than the IZO monolayer.

• 한국재료학회지
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• 제16권1호
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• pp.30-36
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• 2006

A novel method was proposed to grow an epitaxial $CoSi_2$ on (100)Si substrate. A $CoN_x$ interlayer was deposited by reactive sputtering of Co in an Ar+$N_2$ flow. From the Ti/Co/$CoN_x$/Si structure, a uniform and thin $CoSi_2$ layer was epitaxially grown on (100)Si by annealing above $700^{\circ}C$. Two amorphous layers were found at the $CoN_x$/Si interface, where the top layer has a silicon nitride (Si-N) bonding state with some Co content and the bottom layer has a Co-Si intermixing state. The SiNx amorphous layer seems to play a critical role of suppressing the diffusion of Co into Si substrate for the direct formation of epitaxial $CoSi_2$.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 추계학술대회 논문집
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• pp.77-80
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• 2001

Crystallographic and magnetic characteristics of CoCr-based magnetic thin film for perpendicular magnetic recording media were influenced on preparing conditions. In these, there is that substrate temperature was parameter that increases perpendicular coercivity of CoCrTa magnetic layer using recording layer. While preparation of CoCr-based doublelayer, by optimizing substrate temperature, we expect to increase perpendicular anisotropy of CoCr magnetic layer and prepare ferromagnetic recording layer with a good quality by epitaxial growth. CoCrTa/Si doublelayer showed a good dispersion angle of c-axis orientation $\Delta$$\theta$$_{50}$ caused by inserting amorphous Si underlayer which prepared at underlayer substrate temperature 250C. Perpendicular coercivity was constant, in-plane coercivity was controlled a low value about 2000e. This result implied that Si underlayer could restrain growth of initial layer of CoCrTa thin film, which showed bad magnetic properties effectively without participating magnetization patterns of magnetic layer. In case of CoCrTa/Si that prepared with ultra thin underlayer, crystalline orientation of CoCrTa was improved rather underlayer thickness 1nm, it was expected that amorphous Si layer played a important role in not only underlayer but also seed layer.t also seed layer.r.