• Journal of Surface Science and Engineering
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• v.43 no.1
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• pp.36-40
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• 2010

The SiO vapor that was generated from a mixture of Si and $SiO_2$ was reacted at $1350^{\circ}C$ for 2 h under vacuum with carbon nanofibers to produce SiC nanofibers having an average diameter of 100~200 nm. In order to understand the gas corrosion behavior, SiC nanofibers were exposed to air up to $1000^{\circ}C$. SiC oxidized to amorphous $SiO_2$, but its oxidation resistance was inferior unlike bulk SiC, because of high surface area of nanofibers. When SiC nanofibers were exposed to Ar-1% $SO_2$ atmosphere, SiC oxidized to amorphous $SiO_2$, without forming $SiS_2$, owing to the thermodynamic stability of $SiO_2$.

• Korean Journal of Materials Research
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• v.9 no.12
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• pp.1155-1159
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• 1999

Thin film solar cells on a glass/$SnO_2$ substrate with p-SiC/i-Si/n-Si heterojunction structures were fabricated using a plasma-enhanced chemical-vapor deposition system. The photovoltaic properties of the solar cells were examined with varying the gas phase composition, x=$CH_4/\;(SiH_4+CH_4)$, during the deposition of the p-SiC layer. In the range of x=0~0.4, the efficiency of solar cell increased because of the increased band gap of the p-SiC window layer. Further increase in the gas phase composition, however, led to a decrease in the cell efficiency probably due to in the increased composition mismatch at the p-SiC/i-Si layers. As a result, the efficiency of a glass/$SnO_2$/p-SiC/i-SiC/i-Si/n-Si/Ag thin film solar cell with $1cm^2$ area was 8.6% ($V_{oc}$=0.85V, $J_{sc}$=16.42mA/$cm^2$, FF=0.615) under 100mW/$cm^2$ light intensity.

• Proceedings of the Korean Vacuum Society Conference
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• 1999.07a
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• pp.66-66
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• 1999

최근 들어 다결정 SiGe은 MOS(Metal-Oxide-Semiconductor)에서 기존에 사용되던 다결정 Si 공정과의 호환성 및 여러 장점으로 인하여 다결정 Si 대안으로 많은 연구가 진행되고 있다. 고농도로 도핑된 P type의 다결정 SiGe은 Ge의 함량에 따른 일함수의 조절과 낮은 비저항으로 submicrometer CMOS 공정에서 게이트 전극으로 이용하려는 연구가 진행되고 있으며, 55$0^{\circ}C$ 이하의 낮은 온도에서도 증착이 가능하고, 도펀트의 활성화도가 높아서 TFT(Thin Film Transistor)에서도 유용한 재료로 검토되고 있다. 현재까지 다결정 SiGe의 증착은 MBE, APCVD, RECVD. HV/LPCVD 등 다양한 방법으로 이루어지고 있다. 이중 HV/LPCVD 방법을 이용한 증착은 반도체 공정에서 게이트 전극, 유전체, 금속화 공정 등 다양한 공정에서 사용되고 있는 방법으로 현재 사용되고 있는 반도체 공정과의 호환성의 장점으로 다결정 SiGe 게이트 전극의 증착 공정에 적합하다고 할 수 있다. 본 연구에서는 HV/LPCVD 방법을 이용하여 게이트 전극으로의 활용을 위한 다결정 SiGe의 증착 메카니즘을 분석하고 Ex-situ implantation 후 열처리에 따라 나타나는 활성화 정도를 분석하였다. 도펀트를 첨가하지 않은 다결정 SiGe을 주성엔지니어링의 EUREKA 2000 장비를 이용하여, 1000$\AA$의 열산화막이 덮혀있는 8 in 웨이퍼에 증착하였다. 증착 온도는 55$0^{\circ}C$에서 6$25^{\circ}C$까지 변화를 주었으며, 증착압력은 1mtorr-4mtorr로 유지하였다. 낮은 증착압력으로 인한 증착속도의 감소를 방지하기 위하여 Si source로서 Si2H6를 사용하였으며, Ge의 Source는 수소로 희석된 10% GeH4와 100% GeH4를 사용하였다. 증착된 다결정 SiGe의 Ge 함량은 RBS, XPS로 분석하였으며, 증착된 박막의 두께는 Nanospec과 SEM으로 관찰하였다. 또한 Ge 함량 변화에 따른 morphology 관찰과 변화 관찰을 위하여 AFM, SEM, XRD를 이용하였으며, 이온주입후 열처리 온도에 따른 활성화 정도의 관찰을 위하여 4-point probe와 Hall measurement를 이용하였다. 증착된 다결정 SiGe의 두게를 nanospec과 SEM으로 분석한 결과 Gem이 함량이 적을 때는 높은 온도에서의 증착이 더 빠른 증착속도를 나타내었지만, Ge의 함량이 30% 되었을 때는 온도에 관계없이 일정한 것으로 나타났다. XRD 분석을 한 결과 Peak의 위치가 순수한 Si과 순수한 Ge 사이에 존재하는 것으로 나타났으며, ge 함량이 많아짐에 따라 순수한 Ge쪽으로 옮겨가는 경향을 보였다. SEM, ASFM으로 증착한 다결정 SiGe의 morphology 관찰결과 Ge 함량이 높은 박막의 입계가 다결정 Si의 입계에 비해 훨씬 큰 것으로 나타났으며 근 값도 증가하는 것으로 나타났다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2009.06a
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• pp.25-26
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• 2009

Pulsed-PECVD를 이용하여 상온에서 실리콘 나이트라이드(SiN) 박막을 증착하였다. 본 연구에서는, 60-100%의 duty ratio 변화에 따른 굴절률을 살펴보고, 굴절률에 대한 이온에너지의 영향을 분석했다. RF 소스파워는 900W로 고정하였고 $SiH_4-N_2$를 이용하였다. 이온에너지에 대한 정보는 non-invasive 이온 분석기를 이용하여 수집하였다. 측정된 이온에너지 변수는 high ion energy, low ion energy, high ion energy flux, low ion energy flux이며, 이를 이용해 또 다른 변수인 ion energy flux ratio를 계산하였다. Duty ratio의 감소에 따라 굴절률은 일반적으로 감소하였다. 또한 duty ratio의 감소에 따라 high ion energy는 증가하였다. 한편, 60-80%에서 굴절률은 이온에너지 flux의 비에 강한 의존성을 보였으며, 60%를 제외한 모든 duty ratio 구간에서 굴절률은 Nl에 강하게 영향을 알고 있는 것으로 유추되었다. 굴절률은 1.508와 1.714 사이에서 변화하였다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2008.06a
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• pp.37-37
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• 2008

Hydrogenated nanocrystalline Si (nc-Si:H) thin films were prepared by plasma enhanced chemical vapor deposition (PECVD). The films were deposited with a radio frequency power of 100 W, while substrates were exposed to direct current (DC) biases in the range from 0 to -400 V. The effects of the DC bias on the formation of nanoscale Si crystallites in the films and on their optical characteristics were investigated. The size of the Si crystallites in the films ranges from ~ 1.9 to ~ 4.1 nm. The relative fraction of the crystallites in the films reached up ~ 56.5 % when the DC bias of -400 V was applied. Based on the variation in the structural, chemical, and optical features of the films with DC bias voltages, a model for the formation of nanostructures of the nc-Si:H films prepared by PECVD was suggested. This model can be utilized to understand the evolution in the size and relative fraction of the nanocrystallites as well as the amorphous matrix in the nc-Si:H films.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2009.11a
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• pp.45-45
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• 2009

This paper describes the formation of porous 3C-SiC by anodization. 3C-SiC thin films were deposited on p-type Si(100) substrates by APCVD using HMDS (Hexamethyildisilane: $Si_2(CH_3)_6$). UV-LED(380 nm) was used as a light source. The surface morphology was observed by SEM and the pore size was increased with increase of current density. Pore diameter of 70 ~ 90 nm was achieved at 7.1 $mA/cm^2$ current density and 90 sec anodization time. FT-IR was conducted for chemical bonding of thin film and porous 3C-SiC. The Si-H bonding was observed in porous 3C-SiC around wavenumber 2100 $cm^{-1}$. PL shows the band gap enegry of thin film (2.5 eV) and porous 3C-SiC (2.7 eV).

• Journal of the Korean Vacuum Society
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• v.16 no.4
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• pp.279-285
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• 2007

We have demonstrated structural evolution and optical properties of the Si-NWs on Si (111) substrates with synthesized nanoscale Au-Si islands by rapid thermal chemical vapor deposition(RTCVD). Au nano-islands (10-50nm in diameter) were employed as a liquid-droplet catalysis to grow Si-NWs via vapor-liquid-solid mechanism. Si-NWs were grown by a mixture gas of $SiH_4\;and\;H_2$ at pressures of $0.1{\sim}1.0$Torr and temperatures of $450{\sim}650^{\circ}C$. SEM measurements showed the formation of Si-NWs well-aligned vertically for Si (111) surfaces. The resulting NWs are 30-100nm in diameter and $0.4{\sim}12um$ in length depending on growth conditions. HR-TEM measurements indicated that Si-NWs are single crystals convered with about 3nm thick layers of amorphous oxide. In addition, optical properties of NWs were investigated by micro-Raman spectroscopy. The downshift and asymmetric broadening of the Si optical phonon peak with a shoulder at $480cm^{-1}$ were observed in Raman spectra of Si-NWs.

• Journal of the Korean Vacuum Society
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• v.13 no.3
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• pp.114-119
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• 2004

Silicon Nitride thin films were deposited on p-type Si (100) substrates by atomic layer deposition (ALD) method at $550^{\circ}C$ using alternating exposures of $SiH_2Cl_2$ and $NH_3$, and the physical and electrical propeties of the deposited films were characterized. The thickness of the films was linearly increased with the number of deposition cycles, and the growth rate of the films was 0.13 nm/cycle with the reactant exposures of $3.0\times10^{9}$ L. The silicon nitride thin films deposited by Alf exhibited similar physical properties with the silicon nitride thin films deposited by low-pressure chemical vapor deposition (LPCVD) method in terms of refractive index and wet etch rate, lowering deposition temperature by more than 200 $^{\circ}C$. The ALD films showed the leakage current density of 0.79 nA/$\textrm{cm}^2$ at 3 MV/cm, which is lower than 6.95 nA/$\textrm{cm}^2$ of the LPCVD films under the same condition.

• Journal of the Semiconductor & Display Technology
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• v.13 no.3
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• pp.27-33
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• 2014

To develop high efficiency crystalline solar cells, the $SiN_x$ film for surface passivation and anti-reflection coating is very important and it is generally deposited by PECVD. In this paper, the $SiN_x$ film deposited by Hot-Wire chemical vapor deposition(HWCVD) that has no plasma damage was studied. First, to optimize the $SiN_x$ film deposition process, $SiH_4$ gas rate and substrate temperature were varied and then refractive index and thickness were measured. When $SiH_4$ gas rate was 22sccm and substrate temperature was $100^{\circ}C$, refractive index was 1.94 and higher than that of other process conditions. Second, the lifetime was measured by varying the annealing temperature and time. The annealing process was made from 5 to 30 minutes at $300{\sim}500^{\circ}C$. When the annealing temperature was $100^{\circ}C$ and time was 10minute, the lifetime was the highest. The lifetime of annealed samples was also measured after the firing process at $975^{\circ}C$. Although the lifetime of all samples was decreased by firing process, the lifetime of annealed samples before the firing process was higher than that of fired samples only. Finally, the characteristics of solar cells with HWCVD $SiN_x$ film were measured.

• The Bulletin of The Korean Astronomical Society
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• v.38 no.2
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• pp.77.2-77.2
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• 2013

We present the interim results of simultaneous time monitoring observations of $^{28}SiO$ v = 1, 2, J = 1-0, $^{29}SiO$ v = 0, J = 1-0 and $H_2O$ $6_{16}-5_{23}$ maser lines toward 10 known water fountain sources at a post-AGB stage. The observations have been carried out from 2009 June to 2013 September using the 21m single dish radio telescopes of the Korean VLBI Network. From six sources, we detected well separated red- and blue-shifted $H_2O$ maser features with large velocity ranges more than 100 km $s^{-1}$. From four sources, we detected red- and/or blue-shifted $H_2O$ maser features depended on observational epochs. However, we could not detected SiO maser emission from any sources and any epochs. For a representative water fountain source W43A, we obtained $H_2O$ maser spectra at 17 epochs which show a clear bipolar and discontinuous mass ejections. They also showed a periodic change between red-shifted and blue-shifted peaks. However, we need a more regular and short-time interval monitoring observations in order to fix the period and peak intensity variation interval.