• 대한기계학회논문집B
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• 제24권11호
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• pp.1464-1469
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• 2000

The effects of SiCl$_4$addition on flame structures have been studied in flame hydrolysis deposition (FHD) processes using Coherent anti-Stokes Raman spectroscopy (CARS) and planar laser induced fluorescence (PLIF) to measure temperatures and OH concentrations, respectively. The results demonstrate that even a small amount of SiCl$_4$ addition can change thermal and chemical structures of H$_2$/O$_2$ diffusion flames. When SiCl$_4$ is added to a flame temperature decreases in non-reacting zone due to the increases in both specific heat and density of the gas mixture, while flame temperature increase in particle formation zone due to the heat release through hydrolysis and oxidation reactions of SiCl$_4$. It is also found that OH concentration decreases dramatically in particle formation zone where temperatures increase. This can be attributed to consumption of oxidative species and generation of HCl during silica formation.

• 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.

• 대한기계학회논문집B
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• 제23권9호
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• pp.1139-1150
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• 1999

The evolution of silica aggregate particles in coflow diffusion flames has been studied experimentally using light scattering and thermophoretic sampling techniques. The measurements of scattering cross section from $90^{\circ}$ light scattering have been utilized to calculate the aggregate number density and volume fraction using with combination of measuring the particle size and morphology through the localized sampling and a TEM image analysis. Aggregate or particle number densities and volume fractions were calculated using Rayleigh-Debye-Gans and Mie theory for fractal aggregates and spherical particles, respectively. Of particular interests are the effects of flame temperature on the evolution of silica aggregate particles. As the flow rate of $H_2$ increases, the primary particle diameters of silica aggregates have been first decreased, but, further increase of $H_2$ flow rate causes the diameter of primary particles to increase and for sufficiently larger flow rates, the fractal aggregates finally become spherical particles. The variation of primary particle size along the upward jet centerline and the effect of burner configuration have also been studied.

• 한국세라믹학회지
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• 제39권3호
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• pp.278-285
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• 2002

화염가수분해증착(FHD : Flame Hydrolysis Deposition)공정으로 평면형 광수동소자를 구현하기 위한 1050$^{\circ}C$의 저온에서 실리카(silica)막을 형성하였다. 본 연구는 실리카 막을 저온에서 형성하기 위하여 B, P 의 함량을 증가시키면서 고밀화 온도 변화 및 고밀화 분위기에 따른 미세구조의 변화 등 고밀화 영향과 광학적 특성을 관찰하였다. He 분위기에서 고밀화한 경우 적정 고밀화 온도를 1050$^{\circ}C$까지 낮출 수 있었고, 그 결과 표면조도(Surface Roughness)가 5.6nm인 균질한 실리카 막을 저온에서 형성할 수 있었다.

• 대한기계학회논문집B
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• 제23권9호
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• pp.1151-1162
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• 1999

The effects of radial heat and $H_2O$ diffusion on the evolution of silica particles in coflow diffusion flames have been studied experimentally. The evolution of silica aggregate particles in coflow diffusion flames has been measured experimentally using light scattering and thermophoretic sampling techniques. The measurements of scattering cross section from $90^{\circ}$ light scattering have been utilized to calculate the aggregate number density and volume fraction using with combination of measuring the particle size and morphology through the localized sampling and a TEM image analysis. Aggregate or particle number densities and volume fractions were calculated using Rayleigh-Debye-Gans and Mie theory for fractal aggregates and spherical particles, respectively. Flame temperatures and volumetric differential scattering cross sections have been measured for different flame conditions such as inert gas species, $H_2$ flow rates, and burner injection configurations to examine the relation between the formation of particles and radial $H_2O$ diffusion. The comparisons of oxidation and flame hydrolysis have also been made for various $H_2$ flow rates using $N_2$ or $O_2$ as a carrier gas. Results indicate that the role of oxidation becomes dominant as both carrier gas($O_2$) and $H_2$ flow rates increases since the radial heat diffusion precedes $H_2O$ diffusion in coflow flames used in this study. The effect of carrier gas flow rates on the evolution of silica particles have also been studied. When using $N_2$ as a carrier gas, the particle volume fraction has a maximum at a certain carrier gas flow rate and as the flow rate is further increased, the hydrolysis reaction Is delayed and the spherical particles finally evolves into fractal aggregates due to decreased flame temperature and residence time.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2000년도 춘계학술대회논문집B
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• pp.428-433
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• 2000

The consolidation behavior of multicomponent particles prepared by the flame hydrolysis deposition process is examined to identify the effects of Si substrate temperature. To fabricate multi-component particles, a vapor-phase ternary mixture of $SiCl_4(100 cc/min),\;BCl_3(30cc/min)\;and\;POCl_3,(5cc/min)$ was fed into a coflow diffusion oxy-hydrogen flame burner. The doped silica soot bodies were deposited on silicon substrates under various deposition conditions. The surface temperature of the substrate was measured by an infrared thermometer. Changes in the chemical states of the doped silica soot bodies were examined by FT-IR(Fourier-transformed infrared spectroscopy). The deposited particles on the substrate were heated at $1300^{\circ}C$ for 3h in a furnace at a heating rate of 10K/min. Si-O-B bending peak has been found when surface temperature exceeds $720^{\circ}C$. Correspondingly, the case with substrate temperatures above loot produced good consolidation result.

• 한국세라믹학회지
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• 제34권8호
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• pp.811-816
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• 1997

SiO2-P2O5-B2O3 glass soot was fabricated by flame hydrolysis deposition and their properties by SEM, XRD, TGA-DSC were investigated., The mechanism of consolidation process of a glass soot as a function of consolidation temperature was analyzed by SEM observations. In the XRD patterns, the crystalline peaks which seem to be generated from B2O3 and BPO4 were observed. When the temperature of heat treatment exceeded 105$0^{\circ}C$, the non-crystalline state of SiO2-P2O5-B2O3 glass was observed. In the TGA-DSC curves, the evaporation of water molecule by a sudden endothermic reaction was observed at 128$^{\circ}C$ and a broad endothermic peak was seen in the temperature range of 40$0^{\circ}C$-95$0^{\circ}C$, without any weight loss. Finally, this peak was began to recover its baseline at 953$^{\circ}C$. This point is equal to the temperature at which the densification begins. Furthermore, we observed that the addition of dopants such as P2O5 and B2O3 decrease the onset of consolidation temperature till 95$0^{\circ}C$.

• 한국재료학회지
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• 제11권5호
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• pp.385-392
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• 2001

집적형 광증폭기는 대량생산이 용이하고. 단일 칩에 다기능의 광소자를 집적할 수 있다는 장점 때문에 활히 연구되어져 왔다. 본 연구에서는 수동형 집적광소자의 제작에 사용되는 화염가수분해증착법 (FHD)을 이용하여 실리콘 (Si) /실리카 ($SiO_2$) 광도파막을 제작하고, 이 박막에 Solution Doping 법을 이용하여 $Er^{3+}$ 를 첨가하여 광증폭 매질을 제작하는 연구를 수행하였다.

• 한국세라믹학회지
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• 제38권12호
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• pp.1144-1149
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• 2001

본 연구에서는 화염가수분해증착법(Flame Hydrolysis Deposition : FHD)을 이용하여 실리콘(Si)/실리카(SiO$_2$) 광도파막을 제조하고, 이 박막에 Solution Doping 법을 이용해 Er/Al을 복합 첨가하여 광증폭 매질을 제작하는 연구를 수행하였다. 형광 측정을 통해 Al의 복합첨가에 의한 형광효율의 감소 방지 및 형광 스펙트럼의 반치폭 증가를 확인할 수 있었다. 즉, Al가 0.48wt%가 첨가된 경우, Er가 0.14wt% 첨가되는 경우에도 형광세기가 감소하지 않음을 확인하였으며, $1.5mu extrm{m}$ 대역의 형광스펙트럼의 대역폭이 약 5nm 정도 증가됨을 관찰하였다.

• 한국재료학회지
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• 제8권4호
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• pp.337-344
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• 1998

화염가수분해증착법에 의해 형성된 $0.1\mu\textrm{m}$크기의 soot를 실리콘 기판위에 형성하여 $1325^{\circ}C$에서 2시간 동안 고밀화과정후 투명한 후막을 얻을 수 있었다. 고밀화 열처리는 탈수과정, 재배열 과정, 그리고 고밀화 과정으로 구성되었다. 고밀화 공정후의 두께 수축률은 초기 soot의 96%정도였으며, 급속한 두께의 감소는 $950^{\circ}C$부터 시작되었으며, 본격적인 고밀화가 시작되는 온도는 $1250^{\circ}C$임을 알 수 있었다. soot의 TGA와 DTA를 이용한 열분석 결과 탈수과정에 의하여 9/wt%의 질량감소와 $1250^{\circ}C$이상에서 인(P)의 증발에 의한 2wt%의 질량감소를 관찰하였다. DTA곡선에서는 $500^{\circ}C$, $570^{\circ}C$. $1258^{\circ}C$에서 흡열반응 피크를 나타내는데, 이는 $B_{2}$$O_{3}$, $P_{2}$$O_{5}$ 등의 도펀트들의 melting과 실리카 입자사이의 기공이 소멸되면서 입자간의 열전도도의 증가에 의해 나타난 것으로 판단된다.