• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1992년도 춘계학술대회 논문집
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• pp.42-45
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• 1992

The poly silicon thin films were prepared by solid phase crystallization at 600$^{\circ}C$ of amorphous silicon films deposited on Corning 7059 glass and (100) silicon wafer with thermally grown SiO$_2$substrate by plasma enhanced chemical vapor deposition with varying rf power, deposition temperature, total flow rate. Crystallization time, microstructure, absorption coefficients were investigated by RAMAN, XRD analysis and UV transmittance measurement. Crystallization time of amorphous silicon films was increased with increasing rf power, decreasing deposition temperature and decreasing total flow rate.

• 한국세라믹학회지
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• 제42권2호
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• pp.104-109
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• 2005

PbO 완충층의 역할을 확인하기 위해, r.f. magnetron sputtering법을 이용하여 p-type (100) Si 기판 위에 $Pt/Pb_{1.1}Zr_{0.53}Ti_{0.47}O_{3}$와 PbO target으로 Pt/PZT/PbO/Si의 MFIS 구조를 제조하였다. MFIS 구조에 완충층으로 PbO를 삽입함으로써 PZT 박막의 결정성이 크게 향상되었고, 박막의 공정온도도 상당히 낮출 수 있었다. 그리고 XPS depth profile 분석 결과, PbO 증착시 기판온도가 PbO와 Si의 계면에서 Pb의 확산에 미치는 영향을 확인하였다. PbO 완충층을 삽입한 MFIS는 높은 메모리 윈도우와 낮은 누설전류 밀도를 가지는 추수한 전기적 특성을 나타내었다. 특히, 기판온도 $300^{\circ}C$에서 증착된 PbO를 삽입한 Pt/PZT(200nm, $400^{\circ}C)PbO(80nm)/Si$는 9V의 인가전압에서 2.OV의 가장 높은 메모리 윈도우 값을 나타내었다.

• 한국표면공학회지
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• 제38권4호
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• pp.144-149
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• 2005

ZnO박막을 R.F. sputtering방법으로 R.F Power와 기판온도를 공정변수로 하여 Si(100)과 $Al_2O_3(0001)$ 기판에 증착하였다. 공정변수에 따른 박막의 미세구조와 잔류응력 및 광학적 특성 등을 평가하였다. 전반적으로 R.F. Power증가에 따른 박막의 미세구조와 잔류응력 및 광학적 특성 등을 평가하였다. 전반적으로 R.F. Power증가에 따른 박막의 미세구조는 결정립이 커지면서 더 거칠어지는 것으로 나타났다. 기판온도 $800^{\cric}C$에서 증착된 박막의 경우, Si기판에 증착한 것보다 $Al_2O_3$기판에 증착된 박막의 막질이 우수한 것으로 나타났다. 박막의 잔류 응류변화는 R.F. Power 보다는 기판온도에 더 의존하는 것으로 나타났다. 대부분의 시편의 잔류응력이 공정변수인 기판온도가 증가할수록 작아지는 것으로 측정되었다. ZnO박막의 열안정성을 평가하기위해 열싸이클링을 실시하였다. 열싸이클링 결과 $Al_2O_3$(0001)기판에 증착된 박막이 Si(100)기판에 증착된 것보다 열안정성이 우수한 것으로 나타났다. PL측정의 경우, $Al_2O_3$기판에 증착된 ZnO박막이 Si기판에 증착된 것보다 UV영역의 발광이 크고 가시광선영역의 발광이 작은것으로 나타났다. 이것은 박막안의 결함이 작아서 낮은 잔류응력을 갖고 있기 때문인 것으로 생각된다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.378.1-378.1
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• 2014

In this study, we investigated that the resistance switching characteristics of Nb-doped HfO2 films with increasing Nb doping concentration. The Nb-doped HfO2 based ReRAM devices with a TiN/Nb-doped HfO2/Pt/Ti/SiO2 were fabricated on Si substrates. The Nb-doped HfO2 films were deposited by reactive dc magnetron co-sputtering at $300^{\circ}C$ and oxygen partial ratio of 60% (Ar: 16sccm, O2: 24sccm). Microstructure of Nb-doped HfO2 films and atomic concentration were investigated by XRD, TEM, and XPS, respectively. The Nb-doped HfO2 films showed set/reset resistance switching behavior at various Nb doping concentrations. The process voltage of forming/set is decreased and whereas the initial current level is increased in doped HfO2 films. However, the switching properties of Nb-doped HfO2 were changed above the specific doping concentration of Nb. The change of resistance switching behavior depending on doping concentration was discussed in terms of concentration of non-lattice oxygen and micro-structure of Nb-doped HfO2.

• 한국재료학회지
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• 제24권3호
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• pp.152-158
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• 2014

We report the effect of the fabric of the surface microstructure on the CO gas sensing properties of $SnO_2$ thin films deposited on self-assembled Au nanodots ($SnO_2$/Au) that were formed on $SiO_2/Si$ substrates. We characterized structural and morphological properties, comparing them to those of $SnO_2$ thin films deposited directly onto $SiO_2/Si$ substrates. We observed a significant enhancement of CO gas sensing properties in the $SnO_2$/Au gas sensors, specifically exhibiting a high maximum response at $200^{\circ}C$ and quite a low detection limit of 1 ppm level in dry air. In particular, the response of the $SnO_2/Au$ gas sensor was found to reach the maximum value of 32.5 at $200^{\circ}C$, which is roughly 27 times higher than the response (~1.2) of the $SnO_2$ gas sensor obtained at the same operating temperature of $200^{\circ}C$. Furthermore, the $SnO_2/Au$ gas sensors displayed very fast response and recovery behaviors. The observed enhancement in the CO gas sensing properties of the $SnO_2/Au$ sensors is mainly ascribed to the formation of a nanostructured morphology in the active $SnO_2$ layer having a high specific surface-reaction area by the insertion of a nanodot form of Au nucleation layer.

• 한국재료학회:학술대회논문집
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• 한국재료학회 2001년도 추계 학술발표강연 및 논문개요집
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• pp.29-29
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• 2001

• 한국세라믹학회지
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• 제29권10호
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• pp.757-764
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• 1992

The platelet reinforced mullite-zirconia composites were prepared by pressurelss sintering with addition of Al2O3 or SiC platelets. The sintered density of 10 vol% Al2O3 platelet reinforced mullite-zirconia composite was 98.3% at 1700$^{\circ}C$. The fracture strength (290 MPa) and fracture toughness (4.9 MPa$.${{{{ SQRT { m} }}) in the Al2O3 platelet reinforced mullite-zirconia composite were enhanced compared with those of mullite-zirconia due to the crack deflection and load transfer effect of platelets. Whereas, the SiC platelet reinforced mullite-zirconia composite sintered at 1650$^{\circ}C$ showed relatively lower density (95.7%), fracture strength (170 MPa), and fracture toughness (3.9 MPa$.${{{{ SQRT { m} }} than the Al2O3 platelet reinforced mullite-zirconia composite.

• 한국재료학회지
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• 제15권3호
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• pp.189-194
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• 2005

[ $SiO_2$ ] nanowires were synthesized using the catalyst evaporation method. Grown nanowires had different shapes by kind of used metal catalyst. Mean diameters of grown $SiO_2$ nanowire were about 30 nm. The kind of catalysts affected microstructure of grown $SiO_2$ nanowire because of its typical growth reactions through the liquid state metal catalysts. Optical property were measured by photoluminescence spectroscopy. Relatively broad peak was obtained and mean peak positioned at 450 nm.

• 한국재료학회지
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• 제24권12호
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• pp.671-676
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• 2014

It is known that bones get damaged by accidents and aging. Since the discovery of Bioglass, various kinds of ceramics have been also found to bond to living bone; some of these ceramics are already being clinically used as bone-repairing materials. In the present study, antibacterial calcium silicate gel ($Ag-30CaO{\cdot}70SiO_2$ gel) was prepared by sol-gel method in order to control the microstructure, which is related to the dissolution rate and induction period of apatite formation in body environment. In addition, biological $Ag-30CaO{\cdot}70SiO_2$ is tested. This was done to impart antimicrobial activity to the $30CaO{\cdot}70SiO_2$. Ag ion was added during sol-gel synthesis to replace the $H_2O$ added during the making of the $30CaO{\cdot}70SiO_2$ gel, which has silver solutions of various concentration. After the sol-gel process, 1N-$HNO_3$ solution was used to wash the gel when synthesizing the gel, in order to maintain the porous structure and remove PEG, water soluble polymers. Then, the apatite forming ability of the sol-gel derived CaO-$SiO_2$ gels was investigated using simulated body fluid (SBF), which had almost the same ion concentration as that of human blood plasma. The gels were analyzed by FT-IR spectroscopy, SEM observation, XRD, and fluorescent microscopy. The apatite was successfully created even after washing the gel; apatite is present in an amorphous state, and was found to affect the concentration of the Ag ion in cells in MC3T3 live & dead assay results. From these results, it is suggested that a good material that can be used to repair defects of nature bone is $Ag-30CaO{\cdot}70SiO_2$ gel.

• E2M - 전기 전자와 첨단 소재
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• 제10권2호
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• pp.126-133
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• 1997

In order to apply for the gas sensing layer and the piezoelectric thin film devices, we studied the effects of magnetron sputtering conditions and annealing temperature on the electrical and structual characteristics of the ZnO thin film. The optimal deposition conditions, in order to obtain a c axis of the ZnO (002) phase thin film which is perpendicular to SiO$_{2}$/Si substrate, were like these ; substrate temperature 150.deg. C, chamber pressure 2 mtorr, R.F. power 300 watts, gas flow ratio 0.4[O$_{2}$(Ar + $O_{2}$)]. When the ZnO thin film was annealed in 600.deg. C, $O_{2}$ gas ambient for 1 hr, the resistivity was 2.6 x 10$^{2}$.ohm.cm and the grain size of ZnO thin film was less than 1 .mu.m. So the ZnO thin film acquired from above conditions can apply for the gas sensing layer which require a c axis perpendicular to the substrate surface.