• Bulletin of the Korean Chemical Society
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• v.31 no.12
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• pp.3593-3599
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• 2010

In an original effort, this lab attempted to employ polystyrene nanoparticles as a template for the synthesis of ordered and highly porous macroporous $SiO_2$ thin films, utilizing their high combustion temperature and narrow size distribution. However, polystyrene nanoparticle thin films were not obtained due to the low interaction between individual particles and between the particle and silicon substrate. However, polystyrene-polyacrylic acid (PS-AA) colloidal particles of a core-shell structure were synthesized by a one-pot miniemulsion polymerization approach, with hydrophilic polyacrylic acid tails on the particle surface that improved interaction between individual particles and between the particle and silicon substrate. The PS-AA thin films were spin-coated in the thickness ranges from monolayer to approximately $1.0\;{\mu}m$. Using the PS-AA thin films as sacrificial templates, macroporous $SiO_2$ thin films were successfully synthesized by vapor deposition or conventional solution sol-gel infiltration methods. Inspection with field emission scanning electron microscopy (FE-SEM) showed that the macroporous $SiO_2$ thin films consist of interconnected air balls (~100 nm). Typical macroporous $SiO_2$ thin films showed ultralow refractive indices ranging from 1.098 to 1.138 at 633 nm, according to the infiltration conditions, which were confirmed by spectroscopy ellipsometry (SE) measurements. This research shows how the synthetic control of the macromolecule such as hydrophilic polystyrene nanopaticles and silicate sol precursors innovates the optical properties and processabilities for actual applications.

• Bulletin of the Korean Chemical Society
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• v.28 no.6
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• pp.965-969
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• 2007

The spectral properties, namely the circular dichroism, electric absorption and luminescence properties, of Λ- and Δ-[Ru(II)(1,10-phenanthroline)2benzodipyrido[b:3,2-h:2',3'-j]phenazine]2+ ([Ru(phen)2BDPPZ]2+) in the presence and absence of single stranded poly(dA) and poly(dT) were compared in this work. In the presence of single stranded DNAs, hypochromism in the absorption spectrum and significant changes in the circular dichroism spectrum in the ligand absorption band were apparent, indicating the strong interaction of the [Ru(phen)2BDPPZ]2+ complex with the single stranded DNAs. The luminescence intensity of the Ru(II) complex decreased stoichiometrically with increasing concentrations of the single stranded DNAs. All of these spectral changes were independent of the configuration of the Ru(II) complex and the nature of the DNA bases. Therefore, it is conceivable that both enantiomers of the [Ru(phen)2BDPPZ]2+ complex interact electrostatically with the negatively charged phosphate groups of DNA. However, the spectral properties of [Ru(II)(1,10-phenanthroline)3]2+ were not altered even in the presence of single stranded DNAs. Therefore, the size of the ligand involved in the interaction of the metal complex with the phosphate group of DNA may play an important role, even when the nature of the interaction is electrostatic.

• The Journal of Advanced Prosthodontics
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• v.7 no.2
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• pp.85-92
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• 2015

PURPOSE. This study aimed to investigate the efficacy of cleaning solutions on saliva-contaminated zirconia in comparison to air-abrasion in terms of resin bonding. MATERIALS AND METHODS. For saliva-contaminated air-abraded zirconia, seven cleaning methods)-no contamination (NC), water-spray rinsing (WS), additional air-abrasion (AA), and cleaning with four solutions (Ivoclean [IC]; 1.0 wt% sodium dodecyl sulfate [SDS], 1.0 wt% hydrogen peroxide [HP], and 1.0 wt% sodium hypochlorite [SHC])-were tested. The zirconia surfaces for each group were characterized using various analytical techniques. Three bonded resin (Panavia F 2.0) cylinders (bonding area: $4.5mm^2$) were made on one zirconia disk specimen using the Ultradent jig method [four disks (12 cylinders)/group; a total of 28 disks]. After 5,000 thermocycling, all specimens were subjected to a shear bond strength test with a crosshead speed of 1.0 mm/minute. The fractured surfaces were observed using an optical and scanning electron microscope (SEM). RESULTS. Contact angle measurements showed that groups NC, AA, IC, and SHC had hydrophilic surfaces. The X-ray photoelectron spectroscopy (XPS) analysis showed similar elemental distributions between group AA and groups IC and SHC. Groups IC and SHC showed statistically similar bond strengths to groups NC and AA (P>.05), but not groups SDS and HP (P<.05). For groups WS, SDS, and HP, blister-like bubble formations were observed on the surfaces under SEM. CONCLUSION. Within the limitations of this in vitro study, some of the cleaning solutions (IC or SHC) were effective in removing saliva contamination and enhancing the resin bond strength.

• Korean Journal of Materials Research
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• v.21 no.6
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• pp.341-346
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• 2011

In this study, we inserted a Zn buffer layer into a AZO/p-type a-si:H layer interface in order to lower the contact resistance of the interface. For the Zn layer, the deposition was conducted at 5 nm, 7 nm and 10 nm using the rf-magnetron sputtering method. The results were compared to that of the AZO film to discuss the possibility of the Zn layer being used as a transparent conductive oxide thin film for application in the silicon heterojunction solar cell. We used the rf-magnetron sputtering method to fabricate Al 2 wt.% of Al-doped ZnO (AZO) film as a transparent conductive oxide (TCO). We analyzed the electro-optical properties of the ZnO as well as the interface properties of the AZO/p-type a-Si:H layer. After inserting a buffer layer into the AZO/p-type a-Si:H layers to enhance the interface properties, we measured the contact resistance of the layers using a CTLM (circular transmission line model) pattern, the depth profile of the layers using AES (auger electron spectroscopy), and the changes in the properties of the AZO thin film through heat treatment. We investigated the effects of the interface properties of the AZO/p-type a-Si:H layer on the characteristics of silicon heterojunction solar cells and the way to improve the interface properties. When depositing AZO thin film on a-Si layer, oxygen atoms are diffused from the AZO thin film towards the a-Si layer. Thus, the characteristics of the solar cells deteriorate due to the created oxide film. While a diffusion of Zn occurs toward the a-Si in the case of AZO used as TCO, the diffusion of In occurs toward a-Si in the case of ITO used as TCO.

• Proceedings of the Materials Research Society of Korea Conference
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• 2009.05a
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• pp.26.2-26.2
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• 2009

이 논문은 반응성 $BCl_3$ 플라즈마로 GaAs의 건식 식각을 진행한 후 그 결과에 대하여 연구 분석 한 것이다. 이 때 사용한 식각 공정 변수는 $BCl_3$ 플라즈마에서의 가스유량, 공정 압력과 RIE 척 파워의 변화이다. 먼저 공정 압력을 75 mTorr 고정시킨 후 $BCl_3$ 유량을 변화 (2.5~10 sccm)해서 실험하였다. 또한 BCl3의 유량을 5 sccm으로 고정시킨 후 공정압력을 변화(47~180 mTorr)해서 식각 실험을 실시하였다. 마지막으로 47 mTorr와 100 mTorr 의 각각의 공정압력에서 RF 척 파워를 변화시켜 (50~200 W) 실험하였다. GaAs 플라즈마 식각이 끝난 후 표면단차 측정기 (Surface profiler)를 사용하여 표면의 단차와 거칠기를 분석하였다. 그 후 그 결과를 이용하여 식각율 (Etch rate), 식각 표면 거칠기 (RMS roughness), 식각 선택비 (Selectivity) 등의 식각 특성평가를 하였다. 또한 식각 공정 중에 샘플 척에 발생하는 자기 바이어스와 $BCl_3$ 플라즈마 가스를 광학 발광 분석기 (Optical Emission Spectroscopy)를 이용하여 플라즈마의 상태를 실시간으로 분석하였다. 이 실험 결과에 따르면 공정 압력의 증가는 샘플 척의 자기 바이어스의 값을 감소시켰다. $BCl_3$ 압력 변화에 의한 GaAs의 식각 결과를 정리하면 5 sccm의 $BCl_3$ 가스유량과 RF 척 파워를 100 W로 고정시켰을 때 식각율은 47 mTorr에서 가장 높았으며, 그 값은 $0.42{\mu}m/min$ 이었다. GaAs의 식각 속도는 공정압력이 증가할수록 감소하였으며 180 mTorr에서는 식각율이 $0.03{\mu}m/min$로 거의 식각되지 않았다. 또한 공정압력을 75 mTorr, RF 척 파워를 100 W로 고정시키고, $BCl_3$ 가스유량을 2.5 sccm에서 10 sccm까지 변화시켰을 때, 10 sccm 의 $BCl_3$ 가스유량에서 가장 높은 식각율인 $0.87{\mu}m/min$이 측정되었다. 압력에 따른 GaAs의 식각 후 표면 거칠기는 최대 2 nm 정도로 비교적 매끈하였으며, 거의 식각되지 않은 180mTorr의 조건에서는 약 1 nm로 낮아졌다. 본 실험 조건에서 GaAs의 감광제에 대한 식각 선택비는 최대 약 3:1 이내였다.

• Proceedings of the Materials Research Society of Korea Conference
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• 2009.05a
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• pp.39.1-39.1
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• 2009

본 실험은 연성과 광 투명도가 뛰어난 아크릴 (PMMA) 과 폴리카보네이트 (Polycabonate) 기판의 축전 결합형 플라즈마 (CCP) 건식 식각 연구에 관한 것이다. 특히 식각 반응기 내부의 압력 변화에 따른 두 기판의 건식 식각 특성 분석에 초점을 맞추었다. 실험에 사용된 기판은 두께 1mm의 아크릴 (PMMA) 과 폴리카보네이트 (Polycabonate)를 $1.5\times1.5\;cm^2$로 절단하여 Photo-lithography 공정을 통하여 감광제 (Photo-resist)로 패턴하였다. 식각 반응기 내부에 패턴 된 아크릴(PMMA) 과 폴리카보네이트 (Polycabonate)를 넣은 후 반응기 내부 진공 상태로 만들었다. 그 후 5 sccm $O_2$ 가스를 유량조절기 (Mass flow controller)를 통하여 식각 반응기 내부로 유입하여 실험을 하였다. 이때 식각 공정 변수는 식각 반응기 내부 압력과 샘플 척 파워이다. 특성평가 항목은 식각 후 기판 (Substrate)의 식각율 (Etch rate), 식각 선택비 (Selectivity) 그리고 기판 표면 거칠기 (RMS roughness)이다. 실험 결과는 표면 단차 분석기(Surface profiler)를 이용하여 기판 (Substrate)의 표면을 분석 하였다. 또한 OES (Optical Emission Spectroscopy) 를 이용하여 식각 중 내부 플라즈마의 상태를 분석하였다. 본 실험 결과에 따르면 5 sccm $O_2$ 가스와 100 W 척 파워를 고정한 후 반응기 내부의 압력을 25 mTorr에서 180 mTorr까지 변화시켜 실험한 결과 40 mTorr의 반응기 내부 압력에서 실험 자료 중 가장 높은 식각율로 아크릴 (PMMA)은 $0.46\;{\mu}m/min$, 폴리카보네이트 (Polycabonate)는 $0.28\;{\mu}m/min$의 결과를 얻었다. 또한 이 자료를 바탕으로 5 sccm $O_2$ 가스와 반응기 내부 압력을 40 mTorr로 고정시키고 RIE 척 파워를 25 W에서 150 W로 증가시켰을 때 아크릴 (PMMA)의 식각율은 $0.15\;{\mu}m/min$에서 $0.72\;{\mu}m/min$까지 증가하였고, 폴리카보네이트 (Polycabonate) 의 식각율은 $0.1\;{\mu}m/min$에서 $0.36\;{\mu}m/min$까지 증가하였다.

• Korean Journal of Materials Research
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• v.11 no.6
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• pp.441-447
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• 2001

A study on the TiN coating layer in small holes on the Purpose of die-casting dies application has been performed with a PACVD process. For the hole having diameter of 4 mm. the uniform TiN coating layer in the hole to the depth of 20 mm was achieved using DC pulsed power source. To understand the forming mechanism of TiN coating layer, plasma diagnosis on Ti, $N_{2}^{+}$ and A $r^{+}$ emissions was carried out during plasma coaling process by optical emirssion spectroscopy. When the duty ratio was equal or over 50%, the Peaks of Ti,$ N_{2}^{+}$ and A $r^{+}$ emission were obviously observed. While duty ratio was equal or under 28.6%, no peaks for Ti, $N_{2}^{+}$ and A $r^$ were observed and the formation of TiN coating layer was rarely observed. For the coating in 4 mm hole diameter, the coating layer with bipolar process was two times deeper than that with unipolar process.

• Transactions of the Korean hydrogen and new energy society
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• v.27 no.1
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• pp.127-134
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• 2016

Most of reconstruction algorithms for the calculation of temperature distributions in CT (computed tomography)-TDLAS (tunable diode laser absorption spectroscopy) are based upon two-line thermometry method. This method gives unstable calculation convergence due to signal noise, bias error, and signal mis-matches. In this study, a new reconstruction algorithm based on cross-correlation for temperature calculation is proposed. The patterns of the optical signals at all wave lengths were used to reconstruct the temperature distribution. Numerical test has been made using phantom temperature distributions. Using these phantom temperature data, absorption spectra for all wave lengths were constructed, and these spectra were regarded as the signals that would be obtained in an actual experiments. Using these virtually generated experimental signals, temperature distribution was once again reconstructed, and was compared with those of the original phantom data. Calculation errors obtained by the newly proposed algorithm were slightly large at high temperatures with small errors at low temperature.

• Proceedings of the Korean Institute of Surface Engineering Conference
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• 2001.11a
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• pp.35-35
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• 2001

agnesium Oxide (MgO) with a NaCI structure is well known to exhibit high secondary electron emission, excellent high temperature chemical stability, high thermal conductance and electrical insulating properties. For these reason MgO films have been widely used for a buffer layer of high $T_c$ superconducting and a protective layer for AC-plasma display panels to improve discharge characteristics and panel lifetime. Up to now MgO films have been synthesized by lE-beam evaporation, Molecular Beam Epitaxy (MBE) and Metalorganic Chemical Vapor Deposition (MOCVD), however there have been some limitations such as low film density and micro-cracks in films. Therefore magnetron sputtering process were emerged as predominant method to synthesis high density MgO films. In previous works, we designed and manufactured unbalanced magnetron source with high power density for the deposition of high quality MgO films. The magnetron discharges were sustained at the pressure of O.lmtorr with power density of $110W/\textrm{cm}^2$ and the maximum deposition rate was measured at $2.8\mu\textrm{m}/min$ for Cu films. In this study, the syntheses of MgO films were carried out by unbalanced magnetron sputtering with various $O_2$ partial pressure and specially target power densities, duty cycles and frequency using pulsed DC power supply. And also we investigated the plasma states with various $O_2$ partial pressure and pulsed DC conditions by Optical Emission Spectroscopy (OES). In order to confirm the relationships between plasma states and film properties such as microstructure and secondary electron emission coefficient were analyzed by X-Ray Diffraction(XRD), Transmission Electron Microscopy(TEM) and ${\gamma}-Focused$ Ion Beam (${\gamma}-FIB$).

• Journal of the Korean institute of surface engineering
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• v.36 no.1
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• pp.79-84
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• 2003

$WC-Ti_{1}$ -xA $l_{x}$ N multilayered coatings are performed by their periodically repeated structures of lamellae of WC-Ti/$WC-Ti_{1}$ -xA $l_{x}$ Nmaterials. The $WC-Ti_{1}$ -xA $l_{x}$ N coatings with variable Al content were deposited onto AISI D2 steel by cathodic arc deposition (CAD) method. The electrochemical behavior of multilayered $WC-Ti_{1}$ -xA $l_{x}$ N coatings with different phases (WC- Ti$0.6/Al_{0.4}$ N, $WC-Ti_{0.53}$$Al_{0.47}$N, $WC-Ti_{0.5}$ $Al_{0.5}$ N and $WC-Ti_{ 0.43}$$Al_{0.57}$ N) was investigated in deaerated 3.5% NaCl solution at room temperature. The corrosion behaviors for the multilayered coatings were investigated by electrochemical techniques (potentiodynamic polarization) and surface analyses (X-ray diffraction (XRD), scanning electron microscopy (SEM), and glow discharge optical emission spectroscopy (GDOES)). In the petentiodynamic polarization test, the corrosion current density of $WC-Ti_{0.5}$$Al_{0.5}$N was lower than others.