• Korean Journal of Materials Research
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• v.13 no.8
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• pp.531-536
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• 2003

The electromagnetic properties and microstructures of the ferrites based on ($Ni_{0.2}$ $Cu_{0.2}$ $Zn_{0.6}$)$_{1.085}$($Fe_2$$O_3$)$_{0.915}$ were investigated by changing the amount of additive SnO$_2$and CaO and the sintering temperatures. Addition of $SnO_2$caused pores in the specimen. There was no variation of grain size by changing the amount of additives. Total loss was reduced when ($Ni_{0.2} $Cu_{0.2}$ $Zn_{ 0.6}$)$_{1.085}$ ($Fe_2$$O_3$)$_{0.915}$ composition was sintered at $1150^{\circ}C$ rather than $1300^{\circ}C$. Addition of CaO was useful to reduce the total loss because it increased the sintering density. The lowest total loss was obtained when 0.06 wt% $SnO_2$and 0.4 wt% CaO were added at the same time.

• Journal of Integrative Natural Science
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• v.9 no.4
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• pp.223-227
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• 2016

The Zn, Sn, and ZnSn thin films were deposited on Si(100) substrate using radio frequency (RF) magnetron co-sputtering method. A surface profiler and X-ray photoelectron spectroscopy (XPS) were used to investigate the Zn, Sn, and ZnSn thin films. Thickness of the thin films was measured by a surface profiler. The deposition rates of pure Zn and Sn thin films were calculated with thickness and sputtering time for optimization. From the survey XPS spectra, we could conclude that the thin films were successfully deposited on Si(100) substrate. The chemical environment of the Zn and Sn was monitored with high resolution XPS spectra in the binding energy regions of Zn 2p, Sn 3d, O 1s, and C 1s.

• Journal of the Korean Ceramic Society
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• v.31 no.11
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• pp.1293-1298
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• 1994

(Zr, Sn)TiO4 powders were prepared in 0.05~0.13 ${\mu}{\textrm}{m}$ by coprecipitating (Zr4+, Ti4+)hydroxide on SnO2 particles and followed by calcination at 90$0^{\circ}C$ for 2 h. They sinter to 95% of relative density at 140$0^{\circ}C$ for 2 h. and shows dielectric constant, $\varepsilon$r=37.5 and quality factor, Qxf(GHz)=46,000. With 3 mol% of ZnO it sinters to rel=97.5%, $\varepsilon$r=39 and Qxf(GHz)=40,050 at 135$0^{\circ}C$ for 2 h., but raising sintering temperature to 140$0^{\circ}C$ deteriorates quality factor, relative density and microstructure with developing second phase.

• Korean Chemical Engineering Research
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• v.55 no.1
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• pp.93-98
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• 2017

This experiment investigated characteristic changes in a $Cu_2ZnSnS_4$(CZTS) solar cell by applying a $Zn(O_x,S_{1-x})$ butter layer with various compositions on the upper side of the absorber layer. Among the four single layers such as $Zn(O_{0.76},S_{0.24})$, $Zn(O_{0.56},S_{0.44})$, $Zn(O_{0.33},S_{0.67})$, and $Zn(O_{0.17},S_{0.83})$, the $Zn(O_{0.76},S_{0.24})$ buffer layer was applied to the device due to its bandgap structure for suppressing electron-hole recombination. In the application of the $Zn(O_{0.76},S_{0.24})$ buffer layer to the device, the buffer layer in the device showed the composition of $Zn(O_{0.7},S_{0.3})$ because S diffused into the buffer layer from the absorber layer. The $Zn(O_{0.7},S_{0.3})$ buffer layer, having a lower energy level ($E_V$) than a CdS buffer layer, improved the $J_{SC}$ and $V_{OC}$ characteristics of the CZTS solar cell because the $Zn(O_{0.7},S_{0.3})$ buffer layer effectively suppressed electron-hole recombination. A substitution of the CdS buffer layer by the $Zn(O_{0.7},S_{0.3})$ buffer layer improved the efficiency of the CZTS solar cell from 2.75% to 4.86%.

• Journal of Ceramic Processing Research
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• v.20 no.1
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• pp.80-83
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• 2019

The Mn4+-activated Li2ZnSn2O6 (LZSO:Mn4+) red phosphors were synthesized by the solid-state reaction at temperatures of 1100-1400 ℃ in air. The synthesized LZSO:Mn4+ phosphors were confirmed to have a single hexagonal LZSO phase without the presence of any secondary phase formed by the Mn4+ addition. With near UV and blue excitation, the LZSO:Mn4+ phosphors exhibited a double band deep-red emission peaked at ~658 nm and ~673 nm due to the 2E → 4A2 transition of Mn4+ ion. PL emission intensity showed a strong dependence on the Mn4+ doping concentration and the 0.3 mol% Mn4+-doped LZSO phosphor produced the strongest PL emission intensity. Photoluminescence emission intensity was also found to be dependent on the calcination temperature and the optimal calcination temperature for the LZSO:Mn4+ phosphors was determined to be 1200 ℃. Dynamic light scattering (DLS) and field-effect scanning electron microscopy (FE-SEM) analysis revealed that the 0.3 mol% Mn4+-doped LZSO phosphor particles have an irregularly round shape and an average particle size of ~1.46 ㎛.

• Proceedings of the Korean Vacuum Society Conference
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• 2010.02a
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• pp.205-205
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• 2010

투명 전극(transparent conducting oxide, TCO)은 높은 전기전도도 및 낮은 비저항 ($10^{-4}{\sim}10^{-3}\;{\Omega}cm$)과 가시광영역에서의 우수한 광투과도(> 80%) 특성을 가지며, 주로 디스플레이, 태양전지, 가스 센서 소자 등에 쓰인다. 투명전극으로 쓰이는 대표적인 물질로서는 ITO, ZnO, $SnO_2$ 등이 있으며, ITO는 전기적 특성이 우수하여 널리 사용되고 있으나 가격이 비싸고 화학적으로 불안정하고, ZnO는 ITO에 비해 가격이 저렴하지만 고온에서 불안정한 특성을 가지고 있다. 반면, $SnO_2$는 ITO와 ZnO에 비해 전기적 특성은 떨어지지만, 우수한 열적, 화학적 안정성 및 높은 내마모성을 가지고 제조단가가 저렴하여 TCO 재료로 많은 연구가 진행되고 있다. TCO 박막을 증착시키는 방법으로 CVD, ion plating, sputtering, spray pyrolysis 등이 있으며, 이 중 sputtering 방법은 균일한 입자로 균질의 박막을 입힐 수 있고 우수한 재현성과 낮은 온도에서도 증착이 가능하여 박막 제조 방법으로 널리 이용되고 있다. 본 연구에서는 $SnO_2$ 박막을 실리콘 (100) 및 글라스 (Eagle 2000) 기판 위에 RF magnetron sputtering 방법을 사용하여 제작하였다. 박막 증착을 위해 99.99%의 2 인치 un-doped $SnO_2$ 타겟을 사용하였고, 기판은 20 rpm 으로 회전시켜 균일한 박막이 형성될 수 있도록 하였으며, 초기 진공도는 $1{\times}10^{-6}\;Torr$가 되도록 하였다. 증착 변수로 기판-타겟간 거리, RF 파워, $O_2/(Ar+O_2)$ 비, 공정압력, 기판 온도 등을 각각 변화 시키며 $SnO_2$ 박막을 증착하였다. 증착된 박막의 구조적 및 광학적 특성을 분석하기위해 FE-SEM, AFM, XRD, UV/VIS spectrophotometer, Photoluminescence 등을 사용하였다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2002.08a
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• pp.25-30
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• 2002

The ternary semiconducting compounds of the $A_{4}BX_{6}$(A=Cd, Zn, Hg; B=Si, Sn, Ge; X=S, Se, Te) type exhibit strong fluorescence and high photosensitivity in the visible and near infrared ranges, so these are supposed to be materials applicable to photoelectrical devices. These materials were synthesized and single crystals were first grown by Nitsche, who identified the crystal structure of the single crystals. In this paper. author describe the undoped and $Co^{2+}$-doped $Zn_{4}SnSe_{6}$ single crystals were grown by the chemical transport reaction(CTR) method using iodine of $6mg/cm^{3}$ as a transport agent. For the crystal. growth, the temperature gradient of the CTR furnace was kep at $700^{\circ}C$ for the source aone and at $820^{\circ}C$ for the growth zone for 7-days. It was found from the analysis of x-ray diffraction that undoped and $Co^{2+}$-doped $Zn_{4}SnSe_{6}$ compounds have a monoclinic structure. The optical absorption spectra obtained near the fundamental absorption edge showed that these compounds have a direct energy gaps. These temperature dependence of the optical energy gap were closely investigated over the temperature range 10[K]~300[K]

• Journal of Sensor Science and Technology
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• v.17 no.4
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• pp.281-288
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• 2008

Polyacrylonitrile(PAN)/metal oxide(MO) nanocomposite mats with a thickness of 0.12 mm were electrospun by adding 0 to 10 wt% of MO nanoparticles ($Fe_2O_3$, ZnO, $SnO_2$, $Sb_2O_3-SnO_2$) into PAN. Pt electrode was patterned on $Al_2O_3$ substrate by DC sputtering and then the PAN(/MO) mats on the Pt patterned $Al_2O_3$ were electrically wired to investigate the $CO_2$ gas sensing properties. As the MO content rose, the fiber diameter decreased due to the presence of lumps caused by the presence of MOs in the fiber. The PAN/2% ZnO mat revealed a faster response time of 93 s and a relatively short recovery of 54 s with a ${\Delta}R$ of 0.031 M${\Omega}$ at a $CO_2$ concentration of 200 ppm. The difference in sensitivity was not observed significantly for the PAN/MO fiber mats in the $CO_2$ concentration range of 100 to 500 ppm. It can be concluded that an appropriate amount of MO nanoparticles in the PAN backbone leads to improvement of the $CO_2$ gas sensing properties.

• 한국전자현미경학회:학술대회논문집
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• 2005.05a
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• pp.59-65
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• 2005

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2004.07b
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• pp.998-1001
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• 2004

ZnO, $SnO_2$ 타겟 각각의 RF 파워를 50 W, 38 W로 고정시킨 후 combinatorial RF magnetron sputtering법을 사용하여 기판 위치에 따라서 조성 구배를 주어 여러 가지 조성의 Zn-Sn-O(ZTO) 박막을 제작하였다. 시편의 열처리에 따른 물성 변화를 분석하기 위해 Rapid Thermal Annealer(RTA)을 이용하여 450, $650{^\circ}C$의 온도 및 $10^{-2}$ Ton의 진공 분위기에서 각각 1 시간 동안 열처리하였다. XRD 분석 결과 상온에서 제작된 ZTO 박막은 Sn 18 at%의 조성을 갖는 시편을 제외하고 모두 비정질상으로 나타났다. $450^{\circ}C$에서 열처리 후 구조적인 변화는 보이지 않았으나, 캐리어 농도와 이동도는 증가하였으며 Sn 54 at%의 조성에서 최고 $25.4cm^2/Vsec$의 전자 이동도를 나타내었다. $26{\leq}Sn$ $at%{\leq}65$의 조성 범위를 갖는 박막은 가시광 영역에서 80 % 이상의 투과도를 가졌으며 $650^{\circ}C$에서 결정화가 되면서 투과도가 증가하였다.