• Title/Summary/Keyword: $BaMO_3$

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The Sintering Behavior of Ba(Cu, Mo)O3 Flux Added (Ba, Sr)TiO3 Ceramic Dielectrics (Ba(Cu, Mo)O3 Flux가 첨가된 (Ba,Sr)TiO3계 유전체의 소결)

  • 안진용
    • Journal of the Microelectronics and Packaging Society
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    • v.3 no.1
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    • pp.25-32
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    • 1996
  • 본 연구에서는 BaTiO3에 Sr과 Pb를 치환시켜TiO3 조성의 세라믹 유전체를 제조한 후 페로브스카이트형 Ba(Cu, Mo)O3를 저융점 flux 로 첨가하여 120$0^{\circ}C$ 이하의 여러온도에 서 소결을 행하였으며 flux 첨가량의 변화에 따른 소결거동 및 유전 특성의변화를 조사하였 다. 이러한 저온 소결용 유전체 세라믹스가 MLCC의 응용시 Pt-Pd계의합금을 내부전극으로 사용가능성을 검토하였다. Flux를 4mol%첨가한 TiO3-0.04Ba(Cu,Mo)O3 조성의 유전체는 120$0^{\circ}C$의 온도에서 2시간 소결했을 경우 소결밀도는 이론밀도의 95% 에 근접하였으며 이때 의 비유전율은 8000이상을 나타내었다. 이러한 소결 온도의 감소는 저융점인 ba(Cu,Mo)O3 계의 flux가 첨가되면서 비교적 낮은 온도에서 액상을 형성하여 소결을 촉진시켰기 때문으 로 사료된다.

Preparation and Characterization of $(Ba_{0.5}La_{0.5}) (Mg_0.5}Mo_{0.5})O_3$ ($(Ba_{0.5}La_{0.5}) (Mg_0.5}Mo_{0.5})O_3$의 합성 및 특성연구)

  • 최진호
    • Journal of the Korean Ceramic Society
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    • v.22 no.3
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    • pp.25-28
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    • 1985
  • The new compound $(Ba_{0.5}La_{0.5}) (Mg_0.5}Mo_{0.5})O_3$ is synthesized under the $H_2$-atmosphere and reveals to have a cation ordering between Mg and Mo in cubic lattic of ordered perovskite (a0=8.009(2)$\AA$) and obeys Curie-Weiss law below the room temperature with the effective magnetic moment of 1.60(5) Bohr Magneton.

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Effect of Mn Addition on the Dielectric Loss characteristics of $BaTiO_3$ Ceramics ($BaTiO_3$ 세라믹의 유전손실에 미치는 Mn 첨가의 영향)

  • 김태중;한주환;이재열;이희영
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.07a
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    • pp.436-439
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    • 2000
  • Change of dielectric loss of use in high relative permitivity capacitor BaTiO$_3$ ceramic depends on Mn doping have been investigated. The powders used in this study were commercial BaTiO$_3$, TiO$_2$and, MnCO$_3$. Sample was fabricated by conventional ceramic process. The quantity of Mn was changed gradually from 0.lmol% to 10mo1%. The sintering densities were reduced with increasing amount of MnCO$_3$. This result is because of increase of low density second phase BaMnO$_3$. When the samples were doped by over 0.2mol% of MnCO$_3$, average grain sizes were enlarge to several tens ${\mu}{\textrm}{m}$. The dielectric losses were reduced by Mn doping to lmol% but, increased from lmol% to 10mo1% gradually.

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Preparation, Structural and Magnetic Properties of Ordered Perovskite (BaLa)(MgMo)O$_6$

  • Choy Jin-Ho;Hong Seung-Tae
    • Bulletin of the Korean Chemical Society
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    • v.10 no.1
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    • pp.8-12
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    • 1989
  • The polycrystalline powder of (BaLa)(MgMo)$O_6$ has been prepared at $1350^{\circ}C$ in a nitrogen flowing atmosphere. The powder X-ray diffraction pattern indicates that (BaLa)(MgMo)$O_6$ has a cubic perovskite structure ($a_0$ = 8.019(3) $\AA)$ with 1:1 ordering or $Mg^{2+}$ and $Mo^{5+}$ in the oxide lattice. The infrared spectrum shows two strong absorption bands with their maxima at 600(${\nu}3$) and 365(${\nu}4$) cm-1, which are attributed to $2T_{1U}$, modes of molybdenum octahedra MoO6 in the crystal lattice. According to the magnetic susceptibility measurement, the compound shows a paramagnetic behavior which follows the Curie-Weiss law below room temperature with the effective magnetic moment 1.60(1){$\mu}B$, which is consistent with that of spin only value ($1.73{\mu}B$) for $Mo^{5+}$ ($4d^1$ electronic configuration). From the thermogravimetric and X-ray diffraction analyses, it has been found that (BaLa)(MgMo)$O_6$ decomposes gradually into $BaMoO_4$, $MoO_3$ and unidentified phases above $900^{\circ}C$ in an ambient atmosphere, absorbing about 0.25 mole $O_2$ per mole of Mo ion, which also supports that oxidation state of $Mo^{5+}$ in the (BaLa)(MgMo)$O_6$.

Superconducting and Normal-state Properties of Y(Sr$_{2-x}$Ba$_x$)Cu$_{2.7}$Mo$_{0.3}$O$_z$

  • Her, Hark-Moo;Lee, Ho-Keum
    • 한국초전도학회:학술대회논문집
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    • v.10
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    • pp.76-79
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    • 2000
  • The effect of Ba substitution for Sr on the lattice parameters and the temperature dependence of the thermoelectric power and electrical resistivity has been investigated for Y(Sr$_{2-x}$Ba$_x$)Cu$_{2.7}$Mo$_{0.3}$O$_z$ (x=0${\sim}$2.0). Both a and c lattice parameters increase as the Ba content, x increases. The correlation between Tc and the carrier concentration estimated from the thermoelectric power data indicates that the change of hole concentration is negligible for x ${\le}$ 1.0 in contrast to the large change for x > 1.

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AC & DC Electrical Characterization of PTC $BaTiO_3$ and Electrodes (PTC $BaTiO_3$ 및 전극의 직류 및 교류 특성)

  • 전표용;최경만
    • Journal of the Korean Ceramic Society
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    • v.28 no.2
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    • pp.101-108
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    • 1991
  • 0.2 mo1% La doped BaTiO3 samples were prepared by a wet chemical process (Pechini process) and electrical conductivity were measured from annealing temperatures(800-110$0^{\circ}C$) to room temperature continuously. 2 probe I-V characteristics showed that Pt electrodes were non-ohmic below about 80$0^{\circ}C$ for Ladoped sample. I-V curves showed varistor behavior and breakdown voltages showed PTC-like behavior. AC complex impedance of 0.2 La and 0.05 Mn mo1% doped BaTiO3 samples with three different electrodes (electroless Ni, Pt, Ag electrodes) were measured with temperature variation. Complex impedance plots showed that the samples with electroless Ni electrodes have negligible electrode resistance. Samples with Ag or Pt paste electrodes showed large electrode resistance. PTC effect, which is defined as the ratio of maximum resistance to minimum resistance, was found to be less than 10 for 0.2 mo1% La doped dense sample however greater than 105 with codoping of 0.05 mo1% Mn and 0.2 mol% La.

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Effect of MoO3 Addition and Their Frequency Characteristics in Nb+5 doped Semiconductive BaTiO3 Ceramics (Nb+5첨가된 반도성 BaTiO3세라믹스에서 MoO3의 영향과 주파수 특성)

  • 윤상옥;정형진;윤기현
    • Journal of the Korean Ceramic Society
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    • v.24 no.1
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    • pp.63-69
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    • 1987
  • Effect of MoO3 additiion on the semiconductive BaTiO3 ceramics doped with 0.2 mole% Nb2O5 and their frequency characteristics have been investigated on the view of intergranular barrier layer model through the observation of changes in their electrical properties. The resistivity increases with the increase of MoO3 addition, but the capacitance, the frequency dependence of capacitance and the effect of positive temperature coefficient of resistivity (PTCR) decrease. It is explained by the possible increase in the thickness of potential barrier due to the formation of insulating layer and thus decrease in the degree of energy band bending. Both the PTCR effect and resistivity decrease with the increase of frequency due to the possible elimination of barrier layer at the grain boundary.

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$A_{2-x}La_xFeMoO_6$(A=Ca and Ba)의 자기적 특성

  • Yang, Hyeon-Mo;Han, Hyeok;Lee, U-Yeong;Lee, Bo-Hwa
    • Proceedings of the Korean Magnestics Society Conference
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    • 2002.12a
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    • pp.86-87
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    • 2002
  • Fe과 Mo이 교대로 정렬해 있는 이중 페로브스카이트 구조를 갖는 $A_{2-x}$FeMo $O_{6}$(A=Ca, Sr, Ba) 화합물들은 망간 산화물들에 비해 높은 $T_{c}$ (310-420K)의 준강자성 상태를 갖는다.$^{1.3}$ 이 화합물들은 F $e^{3+}$ (S=5/2) 와 M $o^{5+}$(S=1/2) 스핀들 사이의 커다란 반강자성 상호작용으로 이론적으로 4$\mu$$_{B}$/f.u.의 $M_{s}$ 값을 갖는다. A-site의 평균 이온 반경( $r_{A}$)이 증가함에 따라 이 화합물들의 결정구조는 Monoclinic(A=Ca)에서 Tetragonal(Sr)과 Cubic(Ba)으로 점진적으로 변화한다.$^3$(중략)(중략)략)략)

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