• 한국세라믹학회지
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• 제56권4호
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• pp.412-420
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• 2019

In this study, the dielectric and polarization properties of manganese (Mn% = 0.0, 0.1, 0.2, 0.5) doped (Pb_0.93La_0.07)(Zr_0.82Ti_0.18)O₃ (PLZT 7/82/18) anti-ferroelectric ceramics were studied for energy storage capacitor and pyroelectric applications. A systematic investigation demonstrated that the electric properties of PLZT 7/82/18 ceramics are affected significantly by the Mn-doping content. A maximum dielectric constant of ~ 2,128 at 1 kHz was found for 0.1% Mn-doped PLZT ceramics with a low dielectric loss of 0.018. The bipolar polarization versus electric field (P-E) hysteresis loops were traced for all compositions showing a typical anti-ferroelectric nature. The breakdown field was found to decrease with Mn-doping. The energy storage density and efficiency were found to be 460 J/㎤ and ~ 63%, respectively, for 0.2% Mn-doped PLZT ceramics. The pyroelectric coefficient of PLZT ceramics shows an increase based on the amount of Mn-doping.

• 한국재료학회지
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• 제20권3호
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• pp.137-141
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• 2010

The $(1-x)La_{0.7}Sr_{0.3}MnO_3(LSMO)/xZnFe_2O_4$(ZFO) (x = 0, 0.01, 0.03, 0.06 and 0.09) composites were prepared by a conventional solid-state reaction method. We investigated the structural properties, magnetic properties and electrical transport properties of (1-x)LSMO/xZFO composites using X-ray diffraction (XRD), scanning electron microscopy (SEM), field-cooled dc magnetization and magnetoresistance (MR) measurements. The XRD and SEM results indicate that LSMO and ZFO coexist in the composites and the ZFO mostly segregates at the grain boundaries of LSMO, which agreed well with the results of the magnetic measurements. The resistivity of the samples increased by the increase of the ZFO doping level. A clear metal-to-insulator (M-I) transition was observed at 360K in pure LSMO. The introduction of ZFO further downshifted the transition temperature (350K-160K) while the transition disappeared in the sample (x = 0.09) and it presented insulating/semiconducting behavior in the measured temperature range (100K to 400K). The MR was measured in the presence of the 10kOe field. Compared with pure LSMO, the enhancement of low-field magnetoresistance (LFMR) was observed in the composites. It was clearly observed that the magnetoresistance effect of x = 0.03 was enhanced at room temperature range. These phenomena can be explained using the double-exchange (DE) mechanism, the grain boundary effect and the intrinsic transport properties together.

• Transactions on Electrical and Electronic Materials
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• 제11권4호
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• pp.182-185
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• 2010

$Pb_{0.99}[(Zr_{0.6}Sn_{0.4})_{0.9}Ti_{0.1}]_{0.98}Nb_{0.02}O_3$ (PNZST) thin films were deposited by radio frequency magnetron sputtering on a $(La_{0.5}Sr_{0.5})CoO_3$ (LSCO)/Pt/Ti/$SiO_2$/Si substrate using a PNZST target with an excess PbO of 10 mole%. The thin films deposited at the substrate temperature of $500^{\circ}C$ crystallized to a perovskite phase after rapid thermal annealing (RTA). The thin films, which annealed at $650^{\circ}C$ for 10 seconds in air, exhibited good crystal structures and ferroelectric properties. The remanent polarization and coercive field of the fabricated PNZST capacitor were approximately $20uC/cm^2$ and 50 kV/cm, respectively. The reduction of the polarization after $2.2\;{\times}\;10^9$ switching cycles was less than 10%.

• 한국재료학회지
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• 제26권1호
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• pp.29-34
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• 2016

$NaLa_{1-x}{(MoO_4)}_2$:$Ho^{3+}/Yb^{3+}$ phosphors with the correct doping concentrations of $Ho^{3+}$ and $Yb^{3+}$ ($x=Ho^{3+}+Yb^{3+}$, $Ho^{3+}=0.05$ and $Yb^{3+}=0.35$, 0.40, 0.45 and 0.50) were successfully synthesized by the microwave-modified sol-gel method. Well-crystallized particles formed after heat-treatment at $900^{\circ}C$ for 16 h showed a fine and homogeneous morphology with particle sizes of $3-5{\mu}m$. The optical properties were examined using photoluminescence emission and Raman spectroscopy. Under excitation at 980 nm, the UC intensities of the doped samples exhibited strong yellow emissions based on the combination of strong emission bands at 545-nm and 655-nm emission bands in green and red spectral regions, respectively. The strong 545-nm emission band in the green region corresponds to the $^5S_2/^5F_4{\rightarrow}^5I_8$ transition in $Ho^{3+}$ ions, while the strong emission 655-nm band in the red region appears due to the $^5F_5{\rightarrow}^5I_8$ transition in $Ho^{3+}$ ions. Pump power dependence and Commission Internationale de L'Eclairage chromaticity of the upconversion emission intensity were evaluated in detail.

• 한국표면공학회지
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• 제50권4호
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• pp.282-288
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• 2017

$Eu^{3+}$- or $Sm^{3+}$-doped $La_2MoO_6$ phosphors were synthesized with different concentrations of activator ions via a solid-state reaction. The X-ray diffraction patterns exhibited that crystalline structures of all the phosphors were tetragonal systems with the dominant peak occurring at (103) plane, irrespective of the concentration and the type of activator ions. The crystallites showed the pebble-like crystalline shapes and the average crystallite size increased with a tendency to agglomerate as the concentration of $Eu^{3+}$ ions increased. The excitation spectra of $Eu^{3+}$-doped $La_2MoO_6$ phosphors contained an intense charge transfer band centered at 331 nm in the range of 250-370 nm and three weak peaks at 381, 394, and 415 nm, respectively, due to the $^7F_0{\rightarrow}^5L_7$, $^7F_0{\rightarrow}^5L_6$, and $^7F_0{\rightarrow}^5D_3$ transitions of $Eu^{3+}$ ions. The emission spectra under excitation at 331 nm exhibited a strong red band centered at 620 nm and two weak bands at 593 and 704 nm. As the concentration of $Eu^{3+}$ increased from 1 to 20 mol%, the intensities of all the emission bands gradually increased. For the $Sm^{3+}$-doped $La_2MoO_6$ phosphors, the emission spectra consisted of an intense emission band at 607 nm arising from the $^4G_{5/2}{\rightarrow}^6H_{7/2}$ transition and three relatively small bands at 565, 648, and 707 nm originating from the $^4G_{5/2}{\rightarrow}^6H_{5/2}$, $^4G_{5/2}{\rightarrow}^6H_{9/2}$, and $^4G_{5/2}{\rightarrow}^6H_{11/2}$ transitions of $Sm^{3+}$, respectively. The intensities of all the emission bands approached maxima when concentration of $Sm^{3+}$ ions was 5 mol%. These results indicate that the optimum concentrations for highly-luminescent red and orange emission are 20 mol% of $Eu^{3+}$ and 5 mol% of $Sm^{3+}$ ions, respectively.

• 한국초전도ㆍ저온공학회논문지
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• 제8권3호
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• pp.13-17
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• 2006

The effect of the addition of the nano size $Y_2O_3$ powder on the microstructurte and superconducting properties of YBCO thin film deposited on LAO single crystalline substrate by TFA-MOD method was studied. Nano size $Y_2O_3$ powder was added to the stoichiometric precursor solution with a cation ratio of Y : Ba . Cu = 1 : 2 : 3 prepared using TFA as chelating agent. Precursor solutions with and without $Y_2O_3$ addition were coated on $LaAlO_3(100)$ single crystalline substrates by dip coating method. Calcination and conversion heat treatments were performed in controlled atmosphere containing moisture Current carrying capacity(Jc) of YBCO film was enhanced about 50% by $Y_2O_3$ doping and it is thought to be due to the better connectivity of YBCO grains and/or the flux pinning by the $Y_2O_3$ particles embedded in YBCO grains.

• 한국세라믹학회지
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• 제56권2호
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• pp.111-129
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• 2019

Recently, all-solid-state batteries (ASSBs) have attracted increasing interest owing to their higher energy density and safety. As the core material of ASSBs, the characteristics of the solid electrolyte largely determine the performance of the battery. Thus far, a variety of inorganic solid electrolytes have been studied, including the NASICON-type, LISICON-type, perovskite-type, garnet-type, glassy solid electrolyte, and so on. The garnet Li₇La₃Zr₂O₁₂ (LLZO) solid electrolyte is one of the most promising candidates because of its excellent comprehensively electrochemical performance. Both, experiments and theoretical calculations, show that cubic LLZO has high room-temperature ionic conductivity and good chemical stability while contacting with the lithium anode and most of the cathode materials. In this paper, the crystal structure, Li-ion transport mechanism, preparation method, and element doping of LLZO are introduced in detail based on the research progress in recent years. Then, the development prospects and challenges of LLZO as applied to ASSBs are discussed.

• 공업화학
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• 제19권5호
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• pp.477-483
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• 2008

구연산법을 이용하여 $La_{0.7}Sr_{0.3}Co_{0.2}Fe_{0.8}O_{3-{\delta}$ 산화물을 합성하였으며, 합성된 분말은 압축 성형 후 $1300^{\circ}C$에서 소결하여 치밀한 페롭스카이트 분리막을 제조하였다. 구연산법으로 제조한 $La_{0.7}Sr_{0.3}Co_{0.2}Fe_{0.8}O_{3-{\delta}$의 전구물질은 TGA와 XRD로 분석하였다. $260{\sim}410^{\circ}C$ 온도 영역에서 전구물질의 금속-구연산 복합체가 분해되며 페롭스카이트 산화물이 얻어지나 XRD 분석결과 $900^{\circ}C$ 이하에서는 $SrCO_3$가 불순물로 존재하였다. 분리막의 전기전도도는 온도가 증가함에 따라 증가하다. 결정격자의 산소 손실로 인해 공기분위기에서는 $700^{\circ}C$ ($Po_2=0.2atm$)부터, 헬륨분위기에서는 $600^{\circ}C$ ($Po_2=0.01atm$) 부터 각각 감소하였다. 산소투과량은 온도가 증가할수록 증가하였고, 두께 1.6 mm의 $La_{0.7}Sr_{0.3}Co_{0.2}Fe_{0.8}O_{3-{\delta}$ 분리막은 $950^{\circ}C$에서 $0.31cm^3/cm^2{\cdot}min$의 최대 투과도를 보였다. 산소투과에 대한 활성화 에너지는 $750{\sim}950^{\circ}C$ 온도 영역에서 88.4 kJ/mol이었다. 40 h의 투과실험 후에 분리막의 페롭스카이트 결정 구조는 변하지 않았으며 0.3 mol Sr doping 시 2차상이 생성되지 않고 안정하였다.

• 한국방사선학회논문지
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• 제4권4호
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• pp.5-10
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• 2010

$Ca_2SiO_4$를 모체로 한 열형광체에도 활성제로 La를 0.1 wt.%, 0.3 wt.%, 0.5 wt.%, 1.0 wt.%의 농도로 첨가하여 $1000^{\circ}C$의 질소 분위기의 전기로에서 90분 동안 소결한 후 입자의 크기를 $100{\mu}m$로 일정하게 선별한 후 측정에 사용하였다. 저에너지 X-선을 조사한 후 측정한 경우 0.1 wt.%에서 상대적으로 열형광 강도가 크게 나타났다. peak shape 법으로 구한 활성화 에너지는 0.434 ~ 0.516 eV이며, 주파수 인자는 0.5 ~ 0.56으로 2차 발광이었다. 자외선을 조사한 후 측정한 경우 0.3 wt.%에서 상대적인 열형광 강도가 크게 나타났고, 활성화 에너지는 0.415 ~ 0.477 eV이며, 주파수 인자는 0.5 ~ 0.53 으로 2차 발광이었다. 저에너지 방사선에 대한 방사선량과 열형광 강도는 선형적임을 나타내어 열형광선량계로서 좋은 특성을 나타내고 있다. 본 연구에서 제작한 $CaB_4O_7$, $Ca_2SiO_4 열형광체는 저에너지 영역의 방사선에 대하여 우수한 열형광 특성을 가짐을 알 수 있었고, 향후 선량계의 제작에 좋은 물질이 될 것으로 생각한다.

• 한국결정성장학회지
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• 제22권2호
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• pp.78-83
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• 2012

$La_{1-x}Sr_xMn_{0.8}Cu_{0.2}O_{3-{\delta}}$(LSMCu)에서 Sr 함량에 따른 구조적 변화와 전기전도도에 대해 연구, 고찰하였다. EDTA citric complexing process(ECCP)로 페로브스카이트 구조를 갖는 $La_{0.8}Sr_{0.2}MnO_3$(LSM)와 $La_{1-x}Sr_xMn_{0.8}Cu_{0.2}O_3$($0.1{\leq}x{\leq}0.4$)을 제조하였다. Sr 함량이 증가할수록 격자상수와 격자부피는 감소하는 경향을 나타내었으며, 이는 Sr 함량이 증가함에 따라 B-site에서 증가하는 $Mn^{4+}$ 이온과 $Cu^{3+}$ 이온의 영향인 것으로 판단하였다. $0.1{\leq}x{\leq}0.3$ 범위의 조성에서 Sr 함량이 증가할수록 $500{\sim}1000^{\circ}C$에서 측정된 전기전도도는 증가하였고, x = 0.3 조성에서는 $750^{\circ}C$와 $950^{\circ}C$에서 각각 172.6 S/cm와 177.7 S/cm (최고값)를 나타내었다. 반면, x = 0.4 조성에서는 전기전도도가 감소하였는데 이는 입계에 발생한 산화물에 의한 영향으로 판단하였다. Sr 함량이 증가함에 따라 B-site에 존재하는 $Mn^{4+}$ 이온과 $Cu^{3+}$ 이온의 증가로 인해 격자수축이 발생하고, hopping mechanism에 관여하는 charge carrier들이 늘어나 전기전도도가 증가한 것으로 판단하였다.