• 한국세라믹학회지
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• 제40권6호
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• pp.589-593
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• 2003

실리카 평판광회로는 다양한 광수동소자에 응용이 되고 있으며, 이를 구성하는 SiO$_2$와 GeO$_2$-SiO$_2$ 막은 화염가수분해증착에 의해 증착되었다. SiO$_2$ 막은 산-수소 토치에 SiCl$_4$, POC1$_3$와 BCl$_3$를 주입하여 화염가수반응에 의해 생성되었으며, POC1$_3$/BC1$_3$ 유량비가 증가함에 따라 P 농도는 2.0-2.8 at%까지 증가하였고, 굴절률은 1.4584-1.4605로 증가하였다. GeO$_2$-SiO$_2$ 막의 굴절률은 GeCl$_4$ 유량에 의해 제어되었으며 30-120 sccm으로 증가함에 따라 1.4615-1.4809로 증가하였다.

• 한국세라믹학회지
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• 제44권10호
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• pp.589-595
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• 2007

Physical properties of sputtered YSZ thin film electrolytes on anode thin film by spray pyrolisis has been investigated to realize the porous electrode and dense electrolyte multilayer structure for micro solid oxide fuel cells. It is shown that for better crystallinity and density, YSZ need to be deposited at an elevated temperature. However, if pure NiO anode was used for high temperature deposition, massive defects such as spalling and delamination were induced due to high thermal expansion mismatch. By changing anode to NiOCGO composite, defects were significantly reduced even at high deposition temperature. Further research on realization of full cells by processing hybridization and cell performance characterization will be performed in near future.

• 한국세라믹학회지
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• 제41권3호
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• pp.183-189
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• 2004

음극전착법을 이용하여 전도성유리(ITO-glass)위에 Cu$_2$O 막을 제조하였다. Cu$_2$O 막의 특성을 향상시키기 위하여 전착방법, 시간, 전압, 전착 후 열처리 조건을 변화시켰다. 전착 후 열처리를 통해 얻어진 전극에 100mW/$ extrm{cm}^2$의 백색광을 조사하여 광전류밀도를 측정하고 XRD, SEM, UV-visible spectrophotometer를 통해 제조 조건변화에 따른 특성변화를 관찰하였다. 그리고 100mW/$\textrm{cm}^2$의 백색광하에서 bias 전압이 0V인 조건에서 전극의 안정성을 측정하였다 인가전압 -0.7V, 인가시간 300초 전착 조건에서 얻어진 막을 30$0^{\circ}C$에서 1시간 열처리하여 순수한 Cu$_2$O 막을 제조하였으며, 이 전극을 이용 광전류밀도를 측정한 결과 1048 $\mu$A/$\textrm{cm}^2$가 측정되었다. 또한 chemical deposition을 이용 TiO$_2$ 박막을 Cu$_2$O 막 위에 코팅하여 전극의 안정성을 향상시켰다.

• 한국세라믹학회지
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• 제40권12호
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• pp.1165-1169
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• 2003

이중 이온빔 스퍼터링(Dual ion-beam sputtering)을 사용하여 보조이온건의 Ar/O$_2$가스유량 변화에 따라 Si-(III) 기판과 glass에 Ta$_2$O$_{5}$ 박막을 증착시켰다. 보조 이온총의 산소 가스량의 비가 감소함에 따라서 증착되는 Ta$_2$O$_{5}$ 박막의 성장속도는 감소하였으며, 굴절률은 $O_2$ 가스의 양이 0∼12sccm인 범위에서 2.09(at 1550nm)로 일정한 값을 나타내었다. Ar:O$_2$가 3: 12인 조건에서 화학양론 조성인 Ta$_2$O$_{5}$를 형성하였으며, 표면 거칠기도 가장 작은 값을 나타내었다.나타내었다.

• 한국세라믹학회지
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• 제43권6호
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• pp.362-368
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• 2006

Epitaxial $Ba_{0.5}Sr_{0.5}TiO_3$ (BSTO) thin films have been grown on TiN buffered Si (001) substrates by Pulsed Laser Deposition (PLD) method and the effects of substrate temperature and oxygen partial pressure during the deposition on their dielectric properties and crystallinity were investigated. The crystal orientation, epitaxy nature, and microstructure of oxide thin films were investigated using X-Ray Diffraction (XRD) and Transmission Electron Microscopy (TEM). Thin films were prepared with laser fluence of $4.2\;J/cm^2\;and\;3\;J/cm^2$, repetition rate of 8 Hz and 10 Hz, substrate temperatures of $700^{\circ}C$ and ranging from $350^{\circ}C\;to\;700^{\circ}C$ for TiN and oxide respectively. BSTO thin-films were grown on TiN-buffered Si substrates at various oxygen partial pressure ranging from $1{\times}10^{-4}$ torr to $1{\times}10^{-5}$ torr. The TiN buffer layer and BSTO thin films were grown with cube-on-cube epitaxial orientation relationship of $[110](001)_{BSTO}{\parallel}[110](001)_{TiN}{\parallel}[110](001)_{Si}$. The crystallinity of BSTO thin films was improved with increasing substrate temperature. C-axis lattice parameters of BSTO thin films, calculated from XRD ${\theta}-2{\theta}$ scans, decreased from 0.408 m to 0.404 nm and the dielectric constants of BSTO epitaxial thin films increased from 440 to 938 with increasing processing oxygen partial pressure.

• 한국세라믹학회지
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• 제48권6호
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• pp.487-492
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• 2011

The effect of the application of lanthanum strontrium manganite and yttria-stabilized zirconia (LSM-YSZ) nano-composite fabricated by pulsed laser deposition (PLD) as a cathode of solid oxide fuel cell (SOFC) is studied. A gradient-structure thin-film cathode composed of 1 micron-thick LSM-YSZ deposited at an ambient pressure ($P_{amb}$) of 200 mTorr; 2 micron-thick LSM-YSZ deposited at a $P_{amb}$ of 300 mTorr; and 2 micron-thick lanthanum strontium cobaltite (LSC) current collecting layer was fabricated on an anode-supported SOFC with an ~8 micron-thick YSZ electrolyte. In comparison with a 1 micron-thick nano-structure single-phase LSM cathode fabricated by PLD, it was obviously effective to increase triple phase boundaries (TPB) over the whole thickness of the cathode layer by employing the composite and increasing the physical thickness of the cathode. Both polarization and ohmic resistances of the cell were significantly reduced and the power output of the cell was improved by a factor of 1.6.

• 분석과학
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• 제6권2호
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• pp.239-246
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• 1993

ITO coated glass, bare glass, 그리고 (100)Si 기판 위에 증착된 $(BaSr)TiO_3$ 박막의 구조는 기판의 종류에 관계없이 변하지 않았으나 결정성은 다결정 ITO층과 (100)Si 기판에 있어서 증대되었다. ITO coated glass 기판 위에 증착된 $(BaSr)TiO_3$ 박막의 조성은 거의 화학양론적으로 일치하였으며 ((Ba+Sr)/Ti=1.08~1.09) 증착 중 상당히 치밀하고 균질하였다. 그러나 증착온도가 증가함에 따라 성장한 박막과 ITO층 사이에, 그리고 ITO층과 base glass 사이에 확산이 보다 심화되었다. ITO coated glass 기판 위에 증착된 $(BaSr)TiO_3$ 박막은 상당히 투명하였으며(투과율 약 80%) 굴절률($n_f$)은 기판온도의 증가에 따라 2.138~2.286이었다.

• 한국세라믹학회지
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• 제34권6호
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• pp.636-644
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• 1997

The effect of various processing parameters, in particular the substrate and filament temperature, on the nucleation of diamond has been studied for the hot filament CVD process with a negative bias on the substrate. As far as the substrate temperature was maintained around the critical temperature of 73$0^{\circ}C$, the nucleation of diamond increased with increasing filament temperature. The maximum nucleation density of ~ 2$\times$109/$\textrm{cm}^2$ was obtained under the condition of filament temperature of 230$0^{\circ}C$, substrate temperature of 75$0^{\circ}C$, bias voltage of 300V, methane concentration of 20%, and deposition time of 2 hours. This nucleation density is about the same as those obtained in previous investigations. For fixed substrate temperatures, the nucleation density varies up to about 103 times depending on experimental conditions. This result is different from that of Reinke, et al. When the substrate temperature was above 80$0^{\circ}C$, a silkworm~shaped carbon phase was co-deposited with hemispherical microcrystalline diamond, and its amount increased with increasing substrate temperature. The Raman spectrum of the silkworm-shaped carbon was the same as that of graphitic soot. The silkworm-shaped carbon was etched and disappeared under the same as that of graphitic soot. The silkworm-shaped carbon was etched and disappeared under the deposition condition of diamond, implying that it did not affect the nucleation of diamond.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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• pp.552-552
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• 2013

In our study we consider Al2O3 ceramic substrates for Plasma Surface Treatments in order to improve deposited diamond surface and increase diamond deposition rate by applying DBD (Dielectric Barrier Dischrge) system. Because Plasma Surface Treatments was used as a modification method of material surface properties like surface free energy, wettability, and adhesion. By applying Plasma Surface Treatments diamond films are deposited on the Al2O3 ceramic substrates. DC Arc Plasmatron with mathane and hydrogen gases is used. Deposited diamond films are investigated by SEM (Scanning Electron Microscopy), AFM (Atomic Force Microscopy) and XRD (X-ray Diffractometer). Then the C-H stretching of synthetic diamond films by FTIR (Fourier Transform Infrared Spectroscopy) is studied. As a result, nanocrystalline diamond films were identified by using SEM and diamond properties in XRD peaks at (111, $43.8{\Box}$, (220, $75.3{\Box}$ and (311, $90.4{\Box}$ were shown. Absorption peaks in FTIR spectrum, caused by CHx sp3 bond stretching of CVD diamond films, were identified as well. Finally, we improved such parameters as depostion rate ($2.3{\mu}m$/h), diamond surface uniformity, and impurities level by applying Plasma Surface Treatments. These experimental results show the importance of Plasma Surface Treatments for diamond deposition by a plasma source.

• 대한금속재료학회지
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• 제50권8호
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• pp.569-573
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• 2012

In order to understand the difference in SiC deposition between the $CH_3SiCl_3-H_2$ and $C_3H_8-SiCl_4-H_2$ systems, we calculate the phase stability among ${\beta}$-SiC, graphite and silicon. We constructed the phase-diagram of ${\beta}$-SiC over graphite and silicon via computational thermodynamic calculation considering pressure (P), temperature (T) and gas composition (C) as variables. Both P-T-C diagrams showed a very steep phase boundary between the SiC+C and SiC region perpendicular to the H/Si axis, and also showed an SiC+Si region with a H/Si value of up to 6700 in the $C_3H_8-SiCl_4-H_2$, and 5000 in the $CH_3SiCl_3-H_2$ system. This difference in phase boundaries is explained by the ratio of Cl to Si, which is 4 for the $C_3H_8-SiCl_4-H_2$ system and 3 for the $C_3H_8-SiCl_4-H_2$ system. Because the C/Si ratio is fixed at 1 in the $CH_3SiCl_3-H_2$ system while it can be variable in the $C_3H_8-SiCl_4-H_2$ system, the functionally graded material is applicable for better mechanical bonding during SiC coating on graphite substrate in the $C_3H_8-SiCl_4-H_2$ system.