• 한국결정성장학회지
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• 제33권1호
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• pp.1-16
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• 2023

LED용 비희토류 기반 strontium-aluminate 계 적색 발광 형광체를 고상반응법으로 합성하였고, 합성온도 및 Mn⁴⁺ 활성제 첨가량이 형광체의 발광특성에 미치는 영향에 대하여 조사하였다. 합성된 SrAl₂O₄:Mn⁴⁺ 형광체는 330 및 460 nm 근처 파장에서 피크가 나타나는 근자외선 및 청색 영역의 광대역 흡광 특성과 644, 658, 및 673 nm 근처의 세 개의 피크로 이루어진 삼중밴드 형태의 deep red 발광 특성을 나타내었다. 합성온도 1600℃, 0.5 mol% Mn⁴⁺ 이온 첨가량에서 합성된 SrAl₂O₄:Mn⁴⁺ 형광체가 가장 우수한 발광 특성을 나타내었고, 0.7 mol% 이상의 첨가량에서는 농도소광이 관찰되었다. FE-SEM 및 DLS 입도크기분포 분석 결과 합성된 SrAl₂O₄:Mn⁴⁺ 형광체 2~6.4 ㎛의 입도 분포 및 불규칙한 구형을 나타내며 약 4 ㎛의 평균 입자 크기를 갖는 것으로 조사되었다.

• 한국광학회지
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• 제35권3호
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• pp.115-120
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• 2024

자기광학(magneto-optical, MO) 효과가 우수한 광학소재는 자기장센서, 광전류센서, 광 고립기(optical isolator), 그리고 광서큘레이터와 같은 다양한 응용 분야에서 활용될 수 있어 많은 관심을 받고 있다. 본 연구에서는 일반적인 유리용융법을 사용하여 Dy³⁺ 이온이 고농도로 함유된 알루미노보로실리케이트(alumino-borosilicate, ABS) 광학유리를 제조하고, Dy³⁺ 이온 농도에 따른 ABS-Dy 유리의 열 특성, 광 특성 및 자기광학 특성을 분석하였으며 1550 nm 파장 대역에서 유리의 MO 특성을 패러데이 회전각 측정을 통하여 분석하였다. 패러데이 회전각은 유리의 Dy³⁺ 이온 농도가 증가함에 따라 선형적으로 증가하는 것으로 나타났으며, 특히 Dy₂O₃ 함량이 30 mol%인 유리는 -6.86 rad/(T·m) 가량의 높은 베르데 상수를 갖는 것으로 확인되었다. 또한 제조된 ABS-Dy 유리는 128 ℃ 이상의 우수한 열안정성(∆T= T_x-T_g)과 파장 대역이 각각 490-710, 1390-1560, 1800-2400 nm일 때 70% 이상의 높은 광투과특성을 보여주었다. 이상의 높은 베르데 상수와 우수한 열안정성은 본 연구에서 제안한 ABS-Dy 유리가 1550 nm MO 소자용 광학소재로 사용 가능함을 시사한다.

• Bulletin of the Korean Chemical Society
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• 제32권spc8호
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• pp.3039-3044
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• 2011

This study suggests the prediction model for the concentration variation of $NO_2{^-}$ and $NO_3{^-}$ along with the rate constants of all reactions during ozonation under UV radiation ($O_3$/UV process). While $NO_2{^-}$ was completely converted into $NO_3{^-}$ during the $O_3$-only process, the production of $NO_2$ radical or $N_2O_4$ was expected in the $O_3$/UV process. In addition, the quenching of OH radicals, by $NO_2$ radical in the $O_3$/UV process, resulted in regeneration of $NO_2{^-}$. However, the regeneration of $NO_2{^-}$ was not observed in the $O_3$/UV process in the presence of $C_6H_6$ where the concentrations of $NO_2{^-}$ and $NO_3{^-}$ were significantly reduced compared to in the process without $C_6H_6$. The pseudo-first order rate constants of all species were calculated with and without the presence of $C_6H_6$ to predict the variation of concentrations of all species during the $O_3$/UV process. It was suggested that $NO_2{^-}$ and $NO_3{^-}$ in the $O_3$/UV process can be more effectively removed from an aqueous system with an OH radical scavenger such as $C_6H_6$.

• 대한환경공학회지
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• 제22권7호
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• pp.1213-1223
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• 2000

CDQ 분진을 흡착제로 사용하여 페놀의 흡착제거 양상을 검토하였다. CDQ 분진의 흡착능은 300 ppm의 페놀 용액에 대해 흡착평형시간 60분에서 약 42%의 흡착율을 보이는 것으로 나타났다. 페놀의 초기농도를 달리하여 흡착실험한 결과, 실험조건범위에서 농도가 증가함에 따라 흡착제거율이 증가하였으며 흡착양상은 Freundlich 등온흡착식에 잘 적용되었다. 흡착의 속도론적 해석시, 시간에 따른 속도식의 차수는 1차, 1.5차, 그리고 2차로 변화하는 것으로 파악되었다. 온도에 따른 흡착에서는 온도가 상승함에 따라 흡착제거량이 증가하여 흡열임을 보였으며, 이의 결과를 바탕으로 흡착에 대한 열역학적 데이터를 도출하였다. pH변화에 따른 페놀의 흡착량은 거의 변화가 없는 것으로 관찰되었으나, pH 11 이상의 영역에서는 다소 감소하는 것으로 나타났다.

• 한국재료학회지
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• 제23권8호
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• pp.430-434
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• 2013

Quantum dots(QDs) with their tunable luminescence properties are uniquely suited for use as lumophores in light emitting device. We investigate the microstructural effect on the electroluminescence(EL). Here we report the use of inorganic semiconductors as robust charge transport layers, and demonstrate devices with light emission. We chose mechanically smooth and compositionally amorphous films to prevent electrical shorts. We grew semiconducting oxide films with low free-carrier concentrations to minimize quenching of the QD EL. The hole transport layer(HTL) and electron transport layer(ETL) were chosen to have carrier concentrations and energy-band offsets similar to the QDs so that electron and hole injection into the QD layer was balanced. For the ETL and the HTL, we selected a 40-nm-thick $ZnSnO_x$ with a resistivity of $10{\Omega}{\cdot}cm$, which show bright and uniform emission at a 10 V applied bias. Light emitting uniformity was improved by reducing the rpm of QD spin coating.At a QD concentration of 15.0 mg/mL, we observed bright and uniform electroluminescence at a 12 V applied bias. The significant decrease in QD luminescence can be attributed to the non-uniform QD layers. This suggests that we should control the interface between QD layers and charge transport layers to improve the electroluminescence.

• Bulletin of the Korean Chemical Society
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• 제34권3호
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• pp.810-814
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• 2013

The thermodynamic parameters for the intercalative interaction of structurally related well known intercalators, 9-aminoacridine (9AA) and proflavine (PF) were determined by means of fluorescence quenching study. The fluorescence intensity of 9AA decreased upon intercalation to DNA, poly[$d(A-T)_2$] and poly[$d(G-C)_2$]. A van't Hoff plot was constructed from the temperature-dependence of slope of the ratio of the fluorophore in the absence and presence of a quencher molecule with respect to the quencher concentration, which is known as a Stern-Volmer plot. Consequently, the thermodynamic parameters, enthalpy and entropy change, for complex formation was calculated from the slope and y-intercept of the van't Hoff plot. The detailed thermodynamic profile has been elucidated the exothermic nature of complex formation. The complex formation of 9AA with DNA, poly[$d(A-T)_2$] and poly[$d(G-C)_2$] was energetically favorable with a similar negative Gibb's free energy. On the other hand, the entropy change appeared to be unfavorable for 9AA-poly[$d(G-C)_2$] complex formation, which was in contrast to that observed with native DNA and poly[$d(A-T)_2$] cases. The equilibrium constant for the intercalation of PF to poly[$d(G-C)_2$] was larger than that to DNA, and was the largest among sets tested despite the most unfavorable entropy change, which was compensated for by the largest favorable enthalpy. The favorable hydrogen bond contribution to the formation of the complexes was revealed from the analyzed thermodynamic data.

• 대한기계학회논문집B
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• 제26권5호
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• pp.742-749
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• 2002

Numerical Study with detailed chemistry has been conducted to investigate the flame structure and NOx formation characteristics in oxygen -enhanced(CH$_4$/O$_2$-$N_2$) and oxygen-enhanced-EGR(CH$_4$/O$_2$-$CO_2$) counter diffusion flame with various strain rates. A small amount of $N_2$is included in oxygen-enhanced-EGR combustion, in order to consider the inevitable $N_2$contamination by $O_2$production process or air infiltration. The results are as follows : In CH$_4$/O$_2$-$CO_2$flame it is very important to adopt a radiation effect precisely because the effect of radiation changes flame structure significantly. In CH$_4$/O$_2$-$N_2$flame special strategy to minimize NO emission is needed because it is very sensitive to a small amount of $N_2$. Special attention is needed on CO emission by flame quenching, because of increased CO concentration. Spatial NO production rate of oxygen-enhanced combustion is different from that of air and oxygen-enhanced-EGR combustion in that thermal mechanism plays a role of destruction as well as production. In case CH$_4$/O$_2$-$CO_2$flame contains more than 40% $CO_2$it is possible to maintain the same EINO as that of CH$_4$/Air flame with accomplishing higher temperature than that of CH$_4$/Air flame. EINO decreases with increasing strain rate, and those effects are augmented in CH$_4$/O$_2$flame.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 추계학술대회논문집B
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• pp.185-190
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• 2001

Numerical Study with detailed chemistry has been conducted to investigate the flame structure and NOx formation characteristics in oxygen-enhanced$(CH_4/O_2-N_2)$ and oxygen-enhanced-EGR$(CH_4/O_2-CO_2)$ counter diffusion flame with various strain rates. A small amount of $N_2$ is included in oxygen-enhanced-EGR combustion, in order to consider the inevitable $N_2$ contamination by $O_2$ production process or air infiltration. The results are as follows : In $CH_4/O_2-CO_2$ flame it is very important to adopt a radiation effect precisely because the effect of radiation changes flame structure significantly. In $CH_4/O_2-N_2$ flame special strategy to minimize NO emission is needed because it is very sensitive to a small amount of $N_2$. Special attention is needed on CO emission by flame quenching, because of increased CO concentration. Spatial NO production rate of oxygen-enhanced combustion is different from that of air and oxygen-enhanced-EGR combustion in that thermal mechanism plays a role of destruction as well as production. In case $CH_4/O_2-CO_2$ flame contains more than 40% $CO_2$ it is possible to maintain the same EINO as that of $CH_4/Air$ flame with accomplishing higher temperature than that of $CH_4/Air$ flame. EINO decreases with increasing strain rate, and those effects are augmented in $CH_4/O_2$ flame. Complementary study is needed with extending the range of strain rate variation.

• BMB Reports
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• 제37권5호
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• pp.603-611
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• 2004

Fluorescence probes located in different membrane regions were used to evaluate the effects of chlorpromazine HCl on structural parameters (transbilayer lateral mobility, annular lipid fluidity, protein distribution, and lipid bilayer thickness) of synaptosomal plasma membrane vesicles (SPMVs) isolated from bovine cerebral cortex. The experimental procedure was based on the selective quenching of 1,3-di(1-pyrenyl)propane (Py-3-Py) by trinitrophenyl groups, radiationless energy transfer from the tryptophan of membrane proteins to Py-3-Py, and energy transfer from Py-3-Py monomers to 1-anilinonaphthalene-8-sulfonic acid (ANS). In this study, chlorpromazine HCl decreased the lateral mobility of Py-3-Py in a concentration dependent-manner, showed a greater ordering effect on the inner monolayer than on the outer monolayer, decreased annular lipid fluidity in a dose dependent-manner, and contracted the membrane lipid bilayer. Furthermore, the drug was found to have a clustering effect on membrane proteins.

• 열처리공학회지
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• 제17권5호
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• pp.271-277
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• 2004

Zr-xNb alloys (x = 0.2, 0.8, 1.5 wt.%) were prepared to study the characteristics of the phase transformation in Zr-Nb system. The samples were heat treated at ${\beta}$-temperature ($1020^{\circ}C$) for 20 min and then cooled with different cooling rate. The microstructures of the specimens having the same compositions were changed with cooling rate and Nb content. The Widmanst$\ddot{a}$tten structure was observed on the furnace-cooled sample. The relationship between ${\alpha}$-Widmanst$\ddot{a}$tten and ${\beta}$-phase was the {0001}${\alpha}$//{110}${\beta}$, <11$\bar{2}$0>//<111>. The ${\beta}$-phase in Widmanst$\ddot{a}$tten structure of Zr-Nb alloys containing Nb more than solubility limit was identified as ${\beta}_{Zr}$ phase which was a stable phase at high temperature. In the water quenched samples, two kinds of martensite structures were observed depending on the Nb-concentration. The lath martensite was formed in Zr-0.2, 0.8 wt.% Nb alloys and the plate martensite having twins was formed in Zr-1.5 wt.% Nb alloy.