• Journal of the Korean Vacuum Society
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• v.16 no.3
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• pp.187-191
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• 2007

In this paper, the catalyst layer is deposited on silicon substrate using magnetron sputtering system and carbon nanotubes(CNTs) were grown in $NH_3\;and\; C_2H_2$ gas by hot-filament plasma enhanced chemical vapor deposition (HFPECVD) system. A growth temperature of carbon nanotubes was changed from $350^{\circ}C\;to\;650^{\circ}C\;by\;100^{\circ}C$. We observed the shape of CNTs by a field-emission scanning electron microscope(FE-SEM) measurement and analyzed the surface characteristic of CNTs layer by contact angle measurement. That is, the growth temperature of CNTs is the important factor leads to the variation of the properties.

• Journal of Korean Society of Environmental Engineers
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• v.22 no.2
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• pp.211-216
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• 2000

In this paper, experimental investigations were carried out to remove NOx, SOx simultaneously from a simulated combustion flue gas [$NO(0.02%)-SO_2(0.08%)-CO_2-Air-N_2$] by using a pulse corona induced plasma chemical processing. Discharge domain of wire-cylindrical plasma reactor was separated from a gas flow duct to avoid unstable discharge by aerosol particle deposited on discharge electrode and grounded electrode. The NOx, SOx removal was experimentally investigated by a reaction induced to ammonium nitrate, ammonium sulfate using a low price of aqueous NaOH solution and a small quantity of ammonia. Volume percentage of aqueous NaOH solution used was 20% and $N_2$ flow rate was $2.5{\ell}/min$ for bubbling aqueous NaOH solution. Ammonia gas(l4.82%) balanced by argon was diluted by air and was introduced to a main simulated flue gas duct through $NH_3$ injection system which was in downstream of reactor. The $NH_3$ molecular ratio(MR) was determined based on [$NH_3$] and [$NO+SO_2$]. MR is 1.5. The NOx removal rates increased in the order of DC, AC and pulse, but SOx removal rates was not significantly effected by source of electricity. The NOx removal rate slightly decreased with increasing initial concentration. but SOx removal rate was not significantly affected by initial concentration. The NOx, SOx removal rates decreased with increasing gas flow rate.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.02a
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• pp.183-184
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• 2013

Two main MBE growth techniques have been used: plasma-assisted MBE (PA-MBE), which utilizes a rf plasma to supply active nitrogen, and ammonia MBE, in which nitrogen is supplied by pyrolysis of NH3 on the sample surface during growth. PA-MBE is typically performed under metal-rich growth conditions, which results in the formation of gallium droplets on the sample surface and a narrow range of conditions for optimal growth. In contrast, high-quality GaN films can be grown by ammonia MBE under an excess nitrogen flux, which in principle should result in improved device uniformity due to the elimination of droplets and wider range of stable growth conditions. A drawback of ammonia MBE, on the other hand, is a serious memory effect of NH3 condensed on the cryo-panels and the vicinity of heaters, which ruins the control of critical growth stages, i.e. the native oxide desorption and the surface reconstruction, and the accurate control of V/III ratio, especially in the initial stage of seed layer growth. In this paper, we demonstrate that the reliable and reproducible growth of GaN on Si (110) substrates is successfully achieved by combining two MBE growth technologies using rf plasma and ammonia and setting a proper growth protocol. Samples were grown in a MBE system equipped with both a nitrogen rf plasma source (SVT) and an ammonia source. The ammonia gas purity was ＞99.9999% and further purified by using a getter filter. The custom-made injector designed to focus the ammonia flux onto the substrate was used for the gas delivery, while aluminum and gallium were provided via conventional effusion cells. The growth sequence to minimize the residual ammonia and subsequent memory effects is the following: (1) Native oxides are desorbed at $750^{\circ}C$ (Fig. (a) for [$1^-10$] and [001] azimuth) (2) 40 nm thick AlN is first grown using nitrogen rf plasma source at $900^{\circ}C$ nder the optimized condition to maintain the layer by layer growth of AlN buffer layer and slightly Al-rich condition. (Fig. (b)) (3) After switching to ammonia source, GaN growth is initiated with different V/III ratio and temperature conditions. A streaky RHEED pattern with an appearance of a weak ($2{\times}2$) reconstruction characteristic of Ga-polarity is observed all along the growth of subsequent GaN layer under optimized conditions. (Fig. (c)) The structural properties as well as dislocation densities as a function of growth conditions have been investigated using symmetrical and asymmetrical x-ray rocking curves. The electrical characteristics as a function of buffer and GaN layer growth conditions as well as the growth sequence will be also discussed. Figure: (a) RHEED pattern after oxide desorption (b) after 40 nm thick AlN growth using nitrogen rf plasma source and (c) after 600 nm thick GaN growth using ammonia source for (upper) [110] and (lower) [001] azimuth.

• Proceedings of the Korean Vacuum Society Conference
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• 2015.08a
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• pp.136.1-136.1
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• 2015

In the present study, UHF (320 MHz) in combination with RF (13.56 MHz) plasmas was used for the synthesis of hydrogenated silicon nitride (SiNx:H) films by PECVD process at low temperature. RF/UHF hybrid plasmas were maintained at a fixed pressure of 410 mTorr in the N2/SiH4 and N2/SiH4/NH3 atmospheres. To investigate the radical generation and plasma formation and their control for the growth of the film, plasma diagnostic tools like vacuum ultraviolet absorption spectroscopy (VUVAS), optical emission spectroscopy (OES), and RF compensated Langmuir probe (LP) were utilized. Utilization of RF/UHF hybrid plasmas enables very high plasma densities ~ 1011 cm-3 with low electron temperature. Measurements using VUVAS reveal the UHF source is quite effective in the dissociation of the N2 gas to generate more active atomic N. It results in the enhancement of the Si-N bond concentration in the film. Consequently, the deposition rate has been significantly improved up to 2nm/s for the high rate synthesis of highly transparent (up to 90 %) SiNx:H film. The films properties such as optical transmittance and chemical composition are investigated using different analysis tools.

• Proceedings of the KAIS Fall Conference
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• 2004.11a
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• pp.195-198
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• 2004

실리콘 산화막 위에 구리 확산 방지막으로서 W-N 박막을 $NH_3$ 펄스 플라즈마를 이용한 원자층 증착방법으로 형성하였다. 플라즈마 원자층 증착방법 (PPALD)은 일반적인 원자층 증착방법(ALD)의 성장 기구를 그대로 따라 간다. 그러나 일반적인 ALD 방법에 의해 증착한 W-N 박막에 비해 PPALD 방법으로 증착한 W-N 박막은 F 함유량과 비저항이 감소하였고 열적 안정성에 대한 특성도 향상되었다. 또한 $WF_6$ 가스는 실리콘 산화막과 반응을 하지 않기 때문에 $WF_6$ 가스와 $NH_3$ 가스를 사용해서 ALD 증착방법으로 실리콘 산화막 위에 W-N 박막을 증착하기 어려운 문제점(8,9)을 $NH_3$ 반응종으로 실리콘 산화막 표면을 먼저 변형시켜 $WF_6$ 가스가 산화막과 반응을 할 수 있게 함으로써 ALD 방법으로 W-N 박막을 실리콘 산화막 위에 증착 할 수 있었다.

• Proceedings of the Korean Vacuum Society Conference
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• 2010.02a
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• pp.305-305
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• 2010

태양전지의 개발이 본격화 되면서 태양전지 웨이퍼 표면에서의 재결합에 의한 손실을 줄이고 전면에서의 반사도를 감소시키기 위한 ARC (Anti-reflection Coating) layer에 대한 연구가 활발히 진행되고 있다. 이 중 대표적인 물질이 실리콘 질화막이 있다. 실리콘 질화막은 PECVD(plasma-enhanced chemical vapor deposition)법으로 저온에서 실리콘 기판 위에 증착 가능한 장점이 있다. 또한 실리콘 질화막의 광학적, 전기적인 특성은 $SiH_4:NH_3$의 화학적 조성비에 의해 결정되며 가스비 가변에 따라 균일도 및 굴절률 조절을 가능케 하여 태양전지의 효율을 향상시킬 수 있다. 본 연구에서는 태양전지의 표면 반사도 저감 및 효율 향상에 최적화된 실리콘 질화막을 형성하기 위해 PECVD를 이용하였고, 가스비 가변을 통해 굴절률을 조절하여 실리콘 질화막을 증착하고 이를 이용한 태양전지를 제작한 후 특성을 비교, 분석하였다. 실리콘 질화막 증착을 위해 압력, 온도, 파워를 1Torr, $450^{\circ}C$, 300W로 고정하고 가스비는 $SiH_4$를 45 sccm으로 고정한 후 $NH_3$의 양을 각각 30, 60, 90, 120 sccm으로 가변하였다. $SiH_4:NH_3$ 비율이 45:90일 때 박막의 passivation효과가 최대였으며 이 조건로 ARC를 형성한 태양전지는 77% 후반의 높은 FF(Fill Factor)와 17%의 광 변환 효율을 나타냈다.

• Proceedings of the KIEE Conference
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• 1993.07b
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• pp.1147-1149
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• 1993

ZnO/$SnO_2$:F bilayer films have been prepared by pyrosol deposition method to develop optimum transparent electrode for use in amorphous silicon solar cells. The solution for $SnO_2:F$ film was composed of $SnCl_4{\cdot}5H_2O,\;NH_4F,\;CH_3OH$ and HCl, and ZnO films have been deposited on the $SnO_2:F$ films by using the solution of $ZnO(CH_3COO){_2}{\cdot}2H_2O,\;H_2O\;and\;CH_3OH$. These films have been investigated the variation of electrical and optical properties under the hydrogen plasma exposure. The sheet resistance of the $SnO_2:F$ film was sharply increased and its transmittance was decreased with the blackish effect after plasma treatment. However, the ZnO/$SnO_2:F$ bilayer film was shown hydrogen plasma durability because the electrical and optical properties was almost unchanged more then 60 seconds exposure time.

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2001.06a
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• pp.73-73
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• 2001

Boron-containing materials have several excellent properties, such as superlnardness, insulation and non-Rinear optical property. Recently, oxynitride compounds, such as Si(ON), Ti(ON), became the promising materials applied in diffusion barrier layer and solar cell. With the expectation of obtaining the hybrid property, we have firstly grown the BON thin film by radio frequency (R.F.) plasma enhanced metalorganic chemical vapm deposition (PEMOCVD) with 100 kHz frequency and trimethyl borate precursor. The plasma source gases used in this study were Ar and $H_2$, and two kinds of nhmgen source gases, $N_2$ and <$NH_3$, were also employed. The as-grown films were characterized by XPS, IR, SEM and Knoop microlhardness tester. The relationship between the films hardness and the growth rate indicated that the hardness of the film was dependent on several factors such as nitrogen source gas, substrate temperature and film thickness due to the variation of the composition and the structure of the film. Both nitrogen and carbon content could raise the film hardness, on which nitrogen content did stronger effect than carbon. The smooth morphology and continuous structure was benefit of obtaining high hardness. The maximum hardness of BON film was about 10 GPa.

• Applied Science and Convergence Technology
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• v.23 no.3
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• pp.139-144
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• 2014

GaN deposition equipment and processes for the fabrication of white LEDs (Light Emitting Diode) using MOCVD (Metal Organic Chemical Vapor Deposition) were numerically modeled to analyze the effects of a reactive gas introduction strategy. The source gases, TMGa and $NH_3$, were injected from a shower head at the top of the chamber; the carrier gases, $H_2$ or $N_2$, were introduced using two types of injection structures: vertical and horizontal. Wafers sat on the holder at a radial distance between 100 mm and 150 mm. The non-uniformity of the deposition rates for vertical and horizontal injection were 4.3% and 3.1%, respectively. In the case of using $H_2$ as a carrier gas instead of $N_2$, the uniform deposition zone was increased by 20%.

• 한국정보디스플레이학회:학술대회논문집
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• 2008.10a
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• pp.218-221
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• 2008

Bottom-gate microcrystalline silicon thin film transistors (${\mu}c$-Si:H TFTs) were fabricated on glass and transparent polyimide substrates by conventional 13.56 MHz RF plasma enhanced chemical vapor deposition at $200^{\circ}C$. The deposition rate of the ${\mu}c$-Si:H film is 24 nm/min and the amorphous incubation layer near the ${\mu}c$-Si:H/silicon nitride interface is unobvious. The threshold voltage of ${\mu}c$-Si:H TFTs can be improved by $H_2$ or $NH_3$ plasma pretreatment silicon nitride film.