• 한국진공학회:학술대회논문집
• /
• 한국진공학회 2011년도 제40회 동계학술대회 초록집
• /
• pp.131-131
• /
• 2011

이종접합 태양전지 제작을 위해 기판의 buffer layer로 사용되는 기존의 a-Si 박막을 SiON 박막으로 대체하려는 연구가 진행 중이다. 기존의 a-Si 박막은 대면적에서 균일도를 담보하기 어렵고, 열적 안정성에 취약한 문제점이 있다. 이에 반해 SiON 박막은 일종의 화학 반응인 oxidation 방법으로 형성이 되기 때문에 막의 균일도를 담보 할 수 있고, $400^{\circ}C$이상의 온도에서 형성되기 때문에 열적 안정성이 우수한 장점이 있다. 이러한 장점에도 불구하고 기판위에 직접 형성이 되기 때문에 기판과 SiON 계면 사이의 pssivation이 무엇보다 중요하다. 본 연구에서는 비정질 실리콘 이종접합 태양전지에 적용키 위한 SiON 박막을 형성하고, 기판과 SiON 계면에서의 passivation 향상을 위한 계면 결함 감소에 대한 연구를 진행하였다. 실험을 위한 SiON 박막은 공정온도 $450^{\circ}C$, 공정압력 100 mTorr, 증착파워 120 mW/cm2에서 5분간 증착하였으며, 이때 50 sccm의 N2O 가스를 주입하였다. 증착된 박막은 2~4 nm의 두께로 증착이 되었으며, 1.46의 광학적 굴절률을 가지는 것으로 분석되었다. 계면의 결함을 줄이기 위해 PECVD를 이용한 NH3 plasma treatment를 실시하였다. 공정온도 $400^{\circ}C$, 공정압력 150mTorr~450 mTorr, 플라즈마 파워 60mW/cm2에서 30분간 진행하였으며, 50 sccm의 N2O 가스를 주입하였다. 계면의 결함이 줄었는지 확인하기 위해 C-V 측정을 위한 시료를 제작하여 분석을 하였다. 실험 결과 VFB가 NH3 plasma treatment 이후 positive 방향으로 shift 됨을 알 수 있었다. Dit 분석을 통해 공정 압력 450 mTorr에서 $4.66{\times}108$[cm2/eV]로 가장 낮은 계면 결함 밀도를 확인 할 수 있었다. 결과적으로 NH3 plasma 처리를 통해 positive charge를 갖는 N-content가 형성되었음을 예측해 볼 수 있으며, N-content가 증가하면, 조밀한 Si-N 결합을 형성하면서, boron 및 phosphorus diffusion을 막는데 효과적이다. 또한, plasma treatment 과정에서 H-content에 의한 passivation 효과를 기대할 수 있다.

• 한국진공학회:학술대회논문집
• /
• 한국진공학회 2011년도 제41회 하계 정기 학술대회 초록집
• /
• pp.277-277
• /
• 2011

디스플레이의 기술발전에 의해 대면적 고해상도의 LCD가 제작되어 왔다. 이에 따라 LCD 점등검사를 위한 Probe Unit의 기술 또한 급속도로 발전하고 있다. 고해상도에 따라 TFT LCD pad가 미세피치화 되어가고 있으며, panel의 검사를 위한 Probe 또한 30 um 이하의 초미세피치를 요구하고 있다. 따라서, 초미세 pitch의 LCD panel의 점등검사를 위한 Probe Unit의 개발이 시급하가. 본 연구에서는 30 um 이하의 미세피치의 Probe block을 위한 Slit wafer의 식각 공정 조건을 연구하였다. Si 공정에서 식각율과 식각깊이에 따른 profile angle의 목표를 설정하고, 식각조건에 따라 이 두 값의 변화를 관측하였다. 식각실험으로 Si DRIE 장비를 이용하여, chamber 압력, cycle time, gas flow, Oxygen의 조건에 따라 각각의 단면 및 표면을 SEM 관측을 통해 최적의 식각 조건을 찾고자 하였다. 식각율은 5um/min 이상, profile angle은 $90{\pm}1^{\circ}$의 값을 목표로 하였다. 이 때 최적의 식각조건은 Etching : SF6 400 sccm, 10.4 sec, passivation : C4F8 400 sccm, 4 sec의 조건이었으며, 식각공정의 Coil power는 2,600 W이었다. 이러한 조건의 공정으로 6 inch Si wafer에 공정한 결과 균일한 식각율 및 profile angle 값을 보였으며, oxygen gas를 미량 유입함으로써 식각율이 균일해짐을 알 수 있었다. 결론적으로 최적의 Slit wafer 식각 조건을 확립함으로써 Probe Unit을 위한 Pin 삽입공정 또한 수율 향상이 기대된다.

• 한국표면공학회지
• /
• 제47권3호
• /
• pp.109-115
• /
• 2014

High power impulse magnetron sputtering (HIPIMS), also known as the technology is called peak power density in a short period, you can get high, so high ionization sputtering rate can make. Higher ionization of sputtered species to a variety of coating materials conventional in the field of improving the characteristics and self-assisted ion thin film deposition process, which contributes to a superior being. HIPIMS at the same power, but the deposition speed is slow in comparison with DC disadvantages. Since recently as a replacement for HIPIMS modulated pulse power (MPP) has been developed. This ionization rate of the sputtered species can increase the deposition rate is lowered and at the same time to overcome the problems to be reported. The differences between the MPP and the HIPIMS is a simple single pulse with a HIPIMS whereas, MPP is 3 ms in pulse length is adjustable, with the full set of multi-pulses within the pulse period and the pulse is applied can be micro advantages. In this experiment, $In_2O_3$ : $SnO_2$ composition ratio of 9 : 1 wt% target was used, Ar : $O_2$ flow rate ratio is 4.8 to 13.0% of the rate of deposition was carried out at room temperature. Ar 40 sccm and the flow rate of $O_2$ and then fixed 2 ~ 6 sccm was compared against that. The thickness of the thin film deposition is fixed at 60 nm, when the partial pressure of oxygen at 9.1%, the specific resistance value of $4.565{\times}10^{-4}{\Omega}cm$, transmittance 86.6%, mobility $32.29cm^2/Vs$ to obtain the value.

• 대한전기학회:학술대회논문집
• /
• 대한전기학회 1998년도 하계학술대회 논문집 E
• /
• pp.1803-1805
• /
• 1998

Electron temperature, electron density and electron energy distribution function were measured in Radio-Frequency Inductively Coupled Plasma(RFICP) using a probe method. Measurements were conducted in argon discharge for pressure from 10 mTorr to 40 mTorr and input rf power from 100W to 600W and flow rate from 3 sccm to 12 sccm. Spatial distribution electron temperature and electron density and electron energy distribution function were measured for discharge with same aspect ratio(R/L=2). Electron temperature was found to depend on pressure, but only weakly on power. Electron density and electron energy distribution function strongly depended on both pressure and power. Electron density and electron energy distribution function increased with increasing flow rate. Radial distribution of the electron density and electron energy distribution function were peaked in the plasma center. Normal distribution of the electron density electron energy distribution function were peaked in the center between quartz plate and substrate. These results were compared to a simple model of ICP, then we found out the generation mechanism of Radio-Frequency Inductively Coupled Plasma.

• 반도체디스플레이기술학회지
• /
• 제11권4호
• /
• pp.25-30
• /
• 2012

In this study, we have investigated the effect of the substrate temperature and oxygen flow rate on the characteristics of IZO thin films for the organic light emitting diodes (OLED) devices. For this purpose, IZO thin films were deposited by RF magnetron sputtering at room temperature and $300^{\circ}C$ with various $O_2$ flow rate. In order to investigate the influences of the oxygen, the flow rate of oxygen in argon mixing gas has been changed from 0.1sccm to 0.5sccm. IZO thin films deposited at room temperature show amorphous structure, whereas IZO thin films deposited at $300^{\circ}C$ show crystalline structure having an (222) preferential orientation regardless of $O_2$ flow rate. The electrical resistivity of IZO film increased with increasing flow rate of $O_2$ under $Ar+O_2$. The change of electrical resistivity with increasing flow rate of $O_2$ was mainly interpreted in terms of the charge carrier concentration rather than the charge carrier mobility. The electrical resistivity of the amorphous-IZO films deposited at R.T. was lower than that of the crystalline-IZO thin films deposited at $300^{\circ}C$. The change of electrical resistivity with increasing substrate temperature was mainly interpreted in terms of the charge carrier mobility rather than the charge carrier concentration. All the films showed the average transmittance over 83% in the visible range.

• 한국진공학회:학술대회논문집
• /
• 한국진공학회 2011년도 제41회 하계 정기 학술대회 초록집
• /
• pp.269-269
• /
• 2011

티타늄-알루미늄(Titanium-Aluminum) 질화물(Nitride)은 고경도 난삭재의 고능률 절삭 분야에 사용되는 공구의 수명 향상을 위한 표면처리 소재로 각광을 받고 있다. 건식고속가공을 효과적으로 수행하기 위해서는 코팅막 재료가 가공 중 발생하는 고온에서도 견디는 우수한 내산화성을 지니면서 내마모, 내충격 특성등의 기계적 성질이 우수한 코팅을 필요로 하며 이러한 분야에 TiAlN을 적용하기 위한 많은 연구가 진행되고 있다. 본 연구에서는 아크(Cathodic Arc) 코팅을 시스템을 이용하여 N2 유량변화에 따라 TiAlN 박막을 제조하고 그 특성을 평가하였다. 아크 소스에 장착된 타겟은 120 $mm{\Phi}$, Ti : Al=50 : 50 at% 의 TiAl 타겟을 사용 하였고, 시편과 타겟 간의 거리는 약 30 cm이며, 시편은 SUS를 사용하였다. 시편을 진공용기에 장착하고 ~10-6 Torr까지 진공배기를 실시하고, Ar 가스를 진공용기 내로 공급하여 ~10-4 Torr에서 시편에 bias (Pulse : 400V)를 인가한 후 아크를 발생시켜 약 5분간 청정을 실시하였다. 플라즈마 청정이 끝나면 시편에 인가된 bias를 차단하고 N2 유량을 변화시키며 코팅을 실시하였다. 질소 유량이 증가함에 따라 색상은 회색에서 어두운 보라색으로 변화하였고 SEM 사진을 통해 Micro paticle 이 감소하는 것을 확인 할 수 있었으며 이는 질소유량이 증가 할수록 표면조도 또한 감소하는 분석결과와도 일치하였다. XRD 분석을 통해 질소 유량이 160 sccm 이상에서 TiAlN이 합성되는 것을 볼 수 있었고 질소 유량이 240 sccm일 때 가장 높은 경도를 보였다. 따라서 본 연구에서 얻어진 결과를 바탕으로 더욱 다양한 조건에서 TiAlN 코팅에 응용한다면 다양한 색상 구현과 내마모성 등에서 많은 장점을 얻을 수 있을 것으로 예상된다.

• 한국재료학회지
• /
• 제13권4호
• /
• pp.266-270
• /
• 2003

We studied BCl$_3$ dry etching of GaAs in a planar inductively coupled plasma system. The investigated process parameters were planar ICP source power, chamber pressure, RIE chuck power and gas flow rate. The ICP source power was varied from 0 to 500 W. Chamber pressure, RIE chuck power and gas flow rate were controlled from 5 to 15 mTorr, 0 to 150 W and 10 to 40 sccm, respectively. We found that a process condition at 20 sccm $BCl_3$ 300 W ICP, 100 W RIE and 7.5 mTorr chamber pressure gave an excellent etch result. The etched GaAs feature depicted extremely smooth surface (RMS roughness < 1 nm), vertical sidewall, relatively fast etch rate (> $3000\AA$/min) and good selectivity to a photoresist (> 3 : 1). XPS study indicated a very clean surface of the material after dry etching of GaAs. We also noticed that our planar ICP source was successfully ignited both with and without RIE chuck power, which was generally not the case with a typical cylindrical ICP source, where assistance of RIE chuck power was required for turning on a plasma and maintaining it. It demonstrated that the planar ICP source could be a very versatile tool for advanced dry etching of damage-sensitive compound semiconductors.

• 한국재료학회지
• /
• 제23권1호
• /
• pp.47-52
• /
• 2013

Graphene has been synthesized on 100- and 300-nm-thick Ni/$SiO_2$/Si substrates with $CH_4$ gas (1 SCCM) diluted in mixed gases of 10% $H_2$ and 90% Ar (99 SCCM) at $900^{\circ}C$ by using inductively-coupled plasma chemical vapor deposition (ICP-CVD). The film morphology of 100-nm-thick Ni changed to islands on $SiO_2$/Si substrate after heat treatment at $900^{\circ}C$ for 2 min because of grain growth, whereas 300-nm-thick Ni still maintained a film morphology. Interestingly, suspended graphene was formed among Ni islands on 100-nm-thick Ni/$SiO_2$/Si substrate for the very short growth of 1 sec. In addition, the size of the graphene domains was much larger than that of Ni grains of 300-nm-thick Ni/$SiO_2$/Si substrate. These results suggest that graphene growth is strongly governed by the direct formation of graphene on the Ni surface due to reactive carbon radicals highly activated by ICP, rather than to well-known carbon precipitation from carbon-containing Ni. The D peak intensity of the Raman spectrum of graphene on 300-nm-thick Ni/$SiO_2$/Si was negligible, suggesting that high-quality graphene was formed. The 2D to G peak intensity ratio and the full-width at half maximum of the 2D peak were approximately 2.6 and $47cm^{-1}$, respectively. The several-layer graphene showed a low sheet resistance value of $718{\Omega}/sq$ and a high light transmittance of 87% at 550 nm.

• 한국표면공학회:학술대회논문집
• /
• 한국표면공학회 2016년도 추계학술대회 논문집
• /
• pp.156-156
• /
• 2016

The effect of nitrogen doping on the mechanical and tribological performance of single-layer tetrahedral amorphous carbon (ta-C:N) coatings of up to $1{\mu}m$ in thickness was investigated using a custom-made filtered cathode vacuum arc (FCVA). The results obtained revealed that the hardness of the coatings decreased from $65{\pm}4.8GPa$ to $25{\pm}2.4GPa$ with increasing nitrogen gas ratio, which indicates that nitrogen doping occurs through substitution in the $sp^2$ phase. Subsequent AES analysis showed that the N/C ratio in the ta-C:N thick-film coatings ranged from 0.03 to 0.29 and increased with the nitrogen flow rate. Variation in the G-peak positions and I(D)/I(G) ratio exhibit a similar trend. It is concluded from these results that micron-thick ta-C:N films have the potential to be used in a wide range of functional coating applications in electronics. To achieve highly conductive and wear-resistant coatings in system components, the friction and wear performances of the coating were investigated. The tribological behavior of the coating was investigated by sliding an SUJ2 ball over the coating in a ball-on-disk tribo-meter. The experimental results revealed that doping using a high nitrogen gas flow rate improved the wear resistance of the coating, while a low flow rate of 0-10 sccm increased the coefficient of friction (CoF) and wear rate through the generation of hematite (${\alpha}-Fe_2O_3$) phases by tribo-chemical reaction. However, the CoF and wear rate dramatically decreased when the nitrogen flow rate was increased to 30-40 sccm, due to the nitrogen inducing phase transformation that produced a graphite-like structure in the coating. The widths of the wear track and wear scar were also observed to decrease with increasing nitrogen flow rate. Moreover, the G-peaks of the wear scar around the SUJ2 ball on the worn surface increased with increasing nitrogen doping.

• 한국전기전자재료학회논문지
• /
• 제21권2호
• /
• pp.111-117
• /
• 2008

We have studied surface roughness, contamination of impurity, bonding with some gas element, reflectance and zeta potential on masks to be generated or changed during photolithography/dry or wet etching process. Mask surface roughness was not changed after photolithography/dry etching process. But surface roughness was changed on some area under MoSi film of Cr/MoSi/Qz. There was not detected any impurity on mask surface after plasma dry etching process. Reflectance of mask was increased after variable plasma etching treatment, especially when mask was treated with plasma including $O_2$ gas. Blank mask was positively charged when the mask was treated with Cr plasma etching gas($Cl_2:250$ sccm/He:20 $sccm/O_2:29$ seem, source power:100 W/bias power:20 W, 300 sec). But this positive charge was changed to negative charge when the mask was treated with $CF_4$ gas for MoSi plasma etching, resulting better wet cleaning. There was appeared with negative charge on MoSi/Qz mask treated with Cr plasma etching process condition, and this mask was measured with more negative after SC-1 wet cleaning process, resulting better wet cleaning. This mask was charged with positive after treatment with $O_2$ plasma again, resulting bad wet cleaning condition.