• The Korean Journal of Ceramics
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• 제5권2호
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• pp.189-194
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• 1999

Crystallization of glasses in the system (Ca, Sr, Ba)$O-Al_2O_3-B_2O_3-SiO_2-TiO_2$ and dielectric properties of crystallized glasses were investigated. As increasing B2O3 content and decreasing SiO2 content in the glass, the major crystalline phase changed from $(Sr, Ba)_2TiSi_2O_8$ to (Ca, Sr, Ba)TiO3, the dielectric constant of crystallized glasses increased and the Temperature Coefficient of Capacitance (TCC) changed to negative. The dielectric constant and TCC was estimated for (Sr, Ba)2TiSi2O8 phase as 18 and -440 $ppm/^{\circ}C$, respectively and for (Ca, Sr, Ba)TiO3 phase as 307 and -1900 $ppm/^{\circ}C$, respectively. The dielectric properties of (Ca, Sr, Ba)TiO3 phase (in this study) were similar to those of (Ca, Ba) TiO_3 solid-solution^12)$, but $(Sr, Ba)_2TiSi_2O_8$ phase (in this study) and $Sr_2TiSi_2O_\;8^4$ showed the different properties.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 추계학술대회 논문집 Vol.14 No.1
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• pp.402-405
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• 2001

$(Ba_{0.6-x}Sr_{0.4}Ca_{x})TiO_{3}$ (x=0.10, 0.15, 0.20) ceramics were fabricated by the mixed-oxide method and their stuctural and dielectric properties were investigated with variation of composition ratio and an amount of $Al_{2}O_{3}$ (0.5, 1.0, 1.5. 2.0, 3.0 wt%) doping content. As a result of the X-ray diffraction BSCT specimens showed dense and homogeneous structure without presence of the second phase. The sintered density was decreased with increase an $Al_{2}O_{3}$ doping content. The Curie temperature and relative dielectric constant at room temperature were decreased with increasing an amount of $Al_{2}O_{3}$ doping content. The dielectric loss is minimum for BSCT doped with 1.5wt% $Al_{2}O_{3}$ content. The tunability was decreased with increasing an Ca content and is about 4.2% for BSCT(50/40/10) doped with 2.0wt% $Al_{2}O_{3}$ content.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 추계학술대회 논문집
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• pp.402-405
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• 2001

(Ba$\_$0.6-x/Sr$\_$0.4/Ca$\_$x/)TiO$_3$(x=0.10, 0.15, 0.20) ceramics were fabricated by the mixed-oxide method and their structural and dielectric properties were investigated with variation of composition ratio and an amount of Al$_2$O$_3$(0.5, 1.0, 1.5, 2.0, 3.0 wt%) doping content. As a result of the X-ray diffraction BSCT specimens showed dense and homogeneous structure without presence of the second phase. The sintered density was decreased with increase an Al$_2$O$_3$ doping content. The Curie temperature and relative dielectric constant at room temperature were decreased with increasing an amount of Al$_2$O$_3$ doping content. The dielectric loss is minimum for BSCT doped with 1.5wt% Al$_2$O$_3$ content. The tunability was decreased with increasing an Ca content and is about 4.2% for BSCT(50/40/10) doped with 2.0wt% Al$_2$O$_3$ content.

• 방사성폐기물학회지
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• 제16권1호
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• pp.49-58
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• 2018

본 연구는 고온 열분해를 통한 Cs, Sr 등 고방사성핵종의 고정화를 위하여 각각 Cs이 흡착된 CHA (K형 Chabazite zeolite)-Cs, CHA-PCFC (potassium cobalt ferrocyanide)-Cs 및 Sr이 흡착된 4A-Sr, BaA-Sr 등의 제올라이트 계에서 TGA 및 XRD에 의한 배소 온도 변화에 따른 상변환을 고찰하였다. CHA-Cs 제올라이트 계의 경우 $900^{\circ}C$ 까지는 CHA-Cs의 형태를 유지하고 있으며, $1,000^{\circ}C$에서 무정형 단계를 거친 후 $1,100^{\circ}C$에서 pollucite ($CsAlSi_2O_6$)로 재결정 되었다. 반면에 CHA-CFC-Cs 제올라이트 계는 $700^{\circ}C$ 까지는 CHA-PCFC-Cs 형태를 유지하고 있으나, $900{\sim}1,000^{\circ}C$ 사이에서 구조가 파괴되어 무정형으로 상변환된 후 $1,100^{\circ}C$에서 pollucite로 재결정 되었다. 한편 4A-Sr 제올라이트 계의 경우 $700^{\circ}C$ 까지는 4A-Sr의 구조를 유지하고 있으며, $800^{\circ}C$에서 무정형으로 상변환 된 다음 $900^{\circ}C$에서는 Sr-feldspar ($SrAl_2Si_2O_8$, hexagonal)으로, $1,100^{\circ}C$에서 $SrAl_2Si_2O_8$ (triclinic)로 재결정 되었다. 그러나 BaA-Sr 제올라이트 계의 경우는 $500^{\circ}C$ 이하부터 구조가 파괴되기 시작하여 $500{\sim}900^{\circ}C$에서 무정형 단계를 거친 후, $1,100^{\circ}C$에서 Ba/Sr-feldspar ($Ba_{0.9}Sr_{0.1}Al_2Si_2O_8$ 및 $Ba_{0.5}Sr_{0.5}Al_2Si_2O_8$ 공존)로 재결정 되었다. 상기 제올라이트 계 모두 온도 증가에 따라 탈수/(분해)${\rightarrow}$ 무정형${\rightarrow}$ 재결정의 단계를 거쳐 광물상으로 재결정 되었으며, 고온 열분해 과정에서의 Cs 및 Sr의 휘발성, 침출성 등의 추가 연구가 요구되지만 각 제올라이트 계에 흡착된 Cs 및 Sr은 pollucite나 Sr-feldspar, Ba/Sr-feldspar 등으로 광물화 하여 Cs과 Sr을 배소체/(고화체) 내에 완전히 고정화 시킬 수 있을 것으로 보인다.

• 한국결정학회지
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• 제9권1호
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• pp.48-52
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• 1998

Nd2O3, BaCo3, Co3O4를 출발물질로 하여 새로운 Nd3Ba5Co4O15상을 고상반응법에 의하여 합성하였다. 반응 온도는 1200℃ 로 하였고 열처리 중 반복적인 혼합을 실시하였다. Nd3Ba5Co4O15상의 결정구조는 분말 X-선회절법에 의한 데이터를 Rietveld법을 이용하여 정밀화하였다. 출발 모델은 Nd3.43Ba4.42Co2.23Al1.77O15의 결정구조를 따랐고 공간군 P63mc(186), 격자상수 a=11.636(5) Å, c=6.846(3) Å. 최종 신뢰도 R값은 Rwp=0.097, Rp=0.068로 나타났다. 이 상의 결정구조는 CoVICoIV3O15 클러스터로 구성되어 있고 이 클러스터는 CoVI 육면체가 3개의 CoIV 사면체와 corner sharing하는 형태를 보인다.

• 한국세라믹학회지
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• 제22권4호
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• pp.61-65
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• 1985

$BaTiO_3$ powders doped with $BaTiO_3$ and $Nb_2O_5$ at 9$0^{\circ}C$ for 1hr. were synthesized by Direct Wet Process. These powders were very homogeneous and fine particle size. To obtain the highe PTCR effect AST($1/3Al_2O_3$.$3/4SiO_2$.$1/4TiO_2$) and $MnO_2$ were added in the semiconduc-ting $BaTiO_3$. In this case $Bi_2O_3$ and $MnO_2$ were used in the form of $Bi(NO)_3$ and $MnCl_2$.$4H_2O$ solution for Direct Wet Process. $BaTiO_3$ doped Nb2O5 and $MnO_2$ demostrated greater PTCR effect than $BaTiO_3$ doped $Nn_2O_5$ only.

• 대한화학회지
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• 제47권4호
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• pp.370-375
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• 2003

보라색 발광 다이오드에 의해 여기되어 청색, 녹색, 적색을 발광하는 형광체로 각각 $BaMg_2Al_16O_27:Eu,\SrGa_2S_4:Eu$, ZnCdS:Ag,Cl 형광체를 선택하였다. 보라색 발광 다이오드의 발광에서 형광체에 의해서 완전히 흡수되지 않고 나오는 보라색 발광과 $BaMg_2Al_16O_27:Eu,\SrGa_2S_4:Eu$, ZnCdS:Ag,Cl 형광체에서 나오는 청색, 녹색, 적색 발광을 조합하여 사파장 백색 발광 다이오드를 만들었다. 사파장 백색 발광 다이오드의 발광 특성을 확인하였다.

• 한국세라믹학회지
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• 제45권3호
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• pp.146-149
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• 2008

Strontium-substituted $Sr_{1-x}Ba_xAl_2O_4:Eu^{2+},\;Dy^{3+}$ compositions were prepared by the solid state synthesis method. These compositions were characterized for their phase, crystallinity and morphology using powder x-ray diffraction (XRD) and scanning electron microscopy (SEM) techniques. Photoluminescence properties were investigated by measuring excitation spectra, emission spectra and decay time for varying Ba/Sr concentrations. Photoluminescence results show higher luminescence and long decay time for $Sr_{1-x}Ba_xAl_2O_4:Eu^{2+},\;Dy^{3+}$(x=0). This is probably due to the influence of the 5d electron states of $Eu^{2+}$ in the crystal field. Long persistence was observed for these compositions due to $Dy^{3+}$ co-doping.

• 한국재료학회지
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• 제12권11호
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• pp.840-844
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• 2002

A spherical $BaMgAl_{10}$ $O_{17}$ :Eu phosphor has been synthesized by a multi-step precipitation route. In order to successfully synthesize the phosphor with spherical shape, the hydrated-alumina particles should be controlled for spherical shape. In this process, the hydroxypropyl cellulose (HPC) was used as a dispersing reagent. This reagent plays an important role in that the particles were controlled to have the uniform size of sub-micron. The final product prepared by the multi-step precipitation method maintained spherical shape with uniform size of 0.4$\mu\textrm{m}$. It can be seen in X-ray diffraction patterns, formation of the single phase of $BaMgAl_{10}$ $O_{17}$ :Eu phosphor prepared by the multi-step precipitation method at $1350^{\circ}C$. Also, the emission spectra of spherical $BaMgAl_{O}$ $10_{17}$ :Eu phosphor in the present case was compared with those of commercially-available blue phosphor under VUV (Vacuum Ultra Violet) excitation. The luminescence process of the $BaMgAl_{10}$ $O_{17}$ :Eu phosphor is characterized by the $4f^{6}$$5d^1$longrightarrow4f$^{7}$ transition (blue) of the $Eu^{2+}$ ion acting as an activating center and the maximum luminescence intensity was obtained by reduction treatment at 145$0^{\circ}C$.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2001년도 하계학술대회 논문집 C
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• pp.1493-1495
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• 2001

$(Ba_{0.6-x}Sr_{0.4}Ca_x)TiO_3+yAl_2O_3$ wt% (x=0.10, 0.15, 0.20, y=0.5 $\sim$ 3.0) specimens were fabricated by the mixed-oxide method and then the structural properties as a function of the composition ratio and $Al_2O_3$ contents were studied. All BSCT specimens showed dense and homogeneous structure without the presence of the seconds phase. The sintered density was decreased with increase ad $Al_2O_3$ content. The Curie temperature and dielectric constant at room temperature decreased with increasing $Al_2O_3$ content. The dielectric constant and dielectric loss of the doped-0.5 wt% $Al_2O_3$ BSCT(50/40/10) specimen were about 3131 and 0.932% at 1KHz, respectively.