• Title/Summary/Keyword: SrO

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Synthesis, Structure and Electrical Properties of $Sr_1-_xY_xMnO_3$ System ($Sr_1-_xY_xMnO_3$의 합성 및 조성에 따른 결정구조와 전기적 성질변화)

  • Park, So Jeong;Kim, Seong Jin
    • Journal of the Korean Chemical Society
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    • v.38 no.11
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    • pp.785-791
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    • 1994
  • The $Sr_1-_xY_xMnO_3$ (x = 0.0∼1.0) system was synthesized using amorphous citrate process. The stability of various structures and the electronic transport properties of this system were investigated. X-ray diffraction study indicated that the $Sr_1-_xY_xMnO_3$ system has three different structures depending on composition, namely, 4L-hexagonal perovskite (when x is less than 0.3), pseudocubic perovskite (when x is 0.3∼0.7), and hexagonal nonperovskite (when x is larger than 0.7) structures. The structural changes and electronic properties were interpreted based on two factors, i.e., the size of cations and the oxidation state of manganese ion. When the concentration of Y substitution exceeds 30%, the Mn-Mn repulsive interaction dominates over intermetallic attraction, and thus structure changes to pseudocubic perovskite. In perovskite phase the unit cell dimensions increases with increasing $Mn^{3+}$ ions due to yttrium substitution. The band gap of $Sr_{0.9}Y_{0.1}MnO_3$ is greater than that of $Sr_{0.5}Y_{0.5}MnO_3$. The greater band gap of $Sr_{0.9}Y_{0.1}MnO_3$ indicates that the 4L-hexagonal structure is more stabilized than cubic perovskite due to the Mn-Mn bond.

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Photoluminescence and long after -glow characteristics of $Sr_{1-x}Eu_xAl_2O_4$phosphor ($Sr_{1-x}Eu_xAl_2O_4$ 형광체의 발광 및 장잔광특성)

  • 이영기;김병규
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.8 no.3
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    • pp.493-497
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    • 1998
  • The synthesis of $Sr_{1-x}Eu_xAl_2O_4$ (x=0.005~0.2;mol%) phosphors and its properties of both photoluminescence and long-phosphorescent were investigated as a function of $Eu_2O_3$ composition. The peak wavelengths (520 nm) of phosphorescence spectra were found not to vary with the $Eu_2O_3$ composition (x) of $Sr_{1-x}Eu_xAl_2O_4$ crystals. Single phase of $SrAl_2O_4$ which determined by XRD and PL was obtained with the compositions of x<0.05 mol%. After the removal of light excitation (360 nm), the excellent after-glow characteristics of the phosphorescence were obtained with the $Eu_2O_3$ compositions of x<0.05 mol%, although the after-glow intensities for all phosphors vary exponentially with the times.

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Synthesis and Luminescent Characteristics of Sr4Al14O25 Phosphor (Sr4Al14O25 형광체의 합성과 발광특성)

  • Han Sang Hyuk;Kim Young Jin
    • Korean Journal of Materials Research
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    • v.14 no.8
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    • pp.529-534
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    • 2004
  • $Sr_{4}Al_{14}O_{25}$ was synthesized by solid state reaction with flux. $H_{3}BO_3$ was used to synthesize $SrO-Al_{2}O_{3}$ phosphor system as a flux. The effect of doping system such as Eu+Dy, Eu, and Ce on the luminescent properties of $Sr_{4}Al_{14}O_{25}$ was investigated. Both PL spectra of $Sr_{4}Al_{14}O_{25}$:Eu and $Sr_{4}Al_{14}O_{25}$:Eu+Dy excited at 390 nm showed greenish-blue emission at about 490 nm, while the emission wavelength was shifted to 400 nm by doping Ce. The reduction of $Eu^{3+}$ ions to $Eu^{2+}$ could be accomplished by the annealing process under $N_{2}^{+}$ vacuum atmosphere, and attributed to the emission at 490 nm. It is verified that $Sr_{4}Al_{14}O_{25}$:Eu phosphor is suitable for white LEDs became of a broad absorption band peaking at 390 nm.

Preparation of Conductive SrMoO3 Thin Films by RF Magnetron Sputtering and Evaluation of Their Electrical Conduction Properties (RF 마그네트론 스퍼터법을 사용한 전도성 SrMoO3 박막 제조 및 전기전도특성 평가)

  • Ryu, Hee-Uk;Sun, Ho-Jung
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.24 no.6
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    • pp.468-472
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    • 2011
  • Conductive $SrMoO_3$ thin films were fabricated by RF magnetron sputtering with the powder-type sputtering target, and annealed for crystallization. When RTP (rapid thermal processing) in vacuum was applied, the fabricated thin films showed the mixed phases of $SrMoO_3$ and $SrMoO_4$, but $SrMoO_3$ phase could be promoted by the lowering of the working pressure during deposition. In order to eliminate $O_2$ gas during deposition and annealing, further lowering of the working pressure and furnace annealing in hydrogen atmosphere were tried. With the optimization of the deposition and annealing conditions, the thin film with nearly single-phase of $SrMoO_3$ was obtained, and it showed good electrical conduction properties with a low resistivity of $2.5{\times}10^{-3}{\Omega}{\cdot}cm$ at room temperature.

Preparation and Luminescent Properties of (Sr,Ba)TiO3:Pr, Al Phosphors ((Sr,Ba)TiO3:Pr,Al 형광체의 제조와 발광특성)

  • Park, Chang-Sub;Yu, Il
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.21 no.9
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    • pp.825-828
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    • 2008
  • $Sr_xBa_{(1-x)}TiO_3$ red phosphors doped with Pr(0.13 mol%) and Al(O.23 mol%) were synthesized by solid state reaction method. Orthorhombic perovskite structure with increasing value of x in $Sr_xBa_{(1-x)}TiO_3$:Pr,Al phosphors changed to cubic perovskite structure. Emission bands at 615 nm and 492 nm in $Sr_{0.25}Ba_{0.75}TiO_3$:Pr,Al and $BaTiO_3$:Pr,Al phosphors were observed at room temperature. The main cause of green luminescence at 492 nm was explained by the change of the 4f5d band.

Analysis of Spin state of SrCoO2.5+x by DFT Calculation

  • Ryu, Ji-Hun;Im, Jin-Yeong
    • Proceeding of EDISON Challenge
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    • 2014.03a
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    • pp.430-433
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    • 2014
  • Perovskite 구조를 가진 코발트 산화물 $SrCoO_3$와 Brownmillerite 구조인 $SrCoO_{2.5}$의 electronic structure를 제1원리 계산을 통해 분석하였다. 이들의 magnetic structure를 계산하여 실험을 통해 알려진 값과 비교하였고, 각 구조에서 코발트 이온이 갖는 spin state를 확인할 수 있었다. 코발트 이온은 $SrCoO_3$에서 intermediate spin state(IS)를, $SrCoO_{2.5}$에서는 high spin state(HS)를 갖는데 이것이 lattice constant의 차이에 의한 것인지, 아니라면 차이의 원인은 무엇인지 density of state를 분석함으로써 알아보았다.

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Cathodic Polarization of $La_{0.5}Sr_{0.5}MnO_{3-\delta}$ on $Ce_{0.8}Gd_{0.2}O_{1.9}$ Electrolyte ($Ce_{0.8}Gd_{0.2}O_{1.9}$ 전해질에서 $La_{0.5}Sr_{0.5}MnO_{3-\delta}$ 양극의 과전압특성)

  • 윤희성;노의범;김병호
    • Journal of the Korean Ceramic Society
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    • v.35 no.9
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    • pp.981-987
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    • 1998
  • $La_{0.5}Sr_{0.5}MnO_{3-\delta}$ as air electrode for soild oxide fuel cell was synthesized by a citrate process and its cathodic polarization was determinated by the current interruption method on the Gd-doped ceria as electrolyte. The addition of citric acid increased the exothermic heat for the formation of $La_{0.5}Sr_{0.5}MnO_{3-\delta}$ perovskite oxide. The degree of the initial particle agglomeration was affected by the exothermic heat. Also the increase of cal-cination temperature enlarged the particle size and the higher sintering temperature accelerated the den-sification of $La_{0.5}Sr_{0.5}MnO_{3-\delta}$ layer after its being painted on $Ce_{0.8}Gd_{0.2}O_{1.9}$ electrolyte. In this study $La_{0.5}Sr_{0.5}MnO_{3-\delta}$ synthesized by citrate process of which the molar ratio of citric acid to metal nitrate was 2 calcined at $650^{\circ}C$ for 2hr and sintered at 1100 at $1200^{\circ}C$ for 4 hrs after slurry coating on Ce0.8Gd0.2O1.9 electrlyte showed the lowest cathodic polarization.

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Microwave Dielectric Properties of the MgTiO$_3$-SrTiO$_3$Ceramics (MgTiO$_3$-SrTiO$_3$세라믹스의 마이크로파 유전특성)

  • 최의선;이문기;정장호;김강;이영희
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.07a
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    • pp.843-846
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    • 2000
  • The (1-x)MgTiO$_3$-xSrTiO$_3$(x=0.02∼0.08) ceramics were fabricated by conventional mixed oxide method. The sintering temperature and time were 1250$^{\circ}C$∼1400$^{\circ}C$, 2hr., respectively. The structural and microwave dielectric properties were investigated by varying sintering temperature and composition ratio. In the (1-x)MgTiO$_3$-xSrTiO$_3$(x=0.02) ceramics, the cubic SrTiO$_3$and hexagonal MgTiO$_3$phases were coexisted. The dielectric constant was increased and the temperature coefficient of resonant frequency( $\tau_f$) was decreased with addition of SrTiO$_3$. The temperature coefficient of resonant frequency($\tau_f$) was gradually varied from negative value to positive value with increasing the SrTiO$_3$.

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