• 대한화학회지
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• 제38권4호
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• pp.276-282
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• 1994

Citrate sol-gel법을 이용하여 perovskite형 복합산화물 LaBO$_3$(B = Mn, Fe, Co)을 공기 중 $850^{\circ}C$에서 24시간 동안 소성하여 제조하였다. X-선 회절분석(XRD)과 TPR결과에 의하면 이들 산화물의 결정구조와 산소화학양론은 LaMnO$_{3.16}$(a = 5.507, c = 13.329 $\AA$, hexagonal), LaFeO$_{3.17}$(a = 5.554, b = 5.555, c = 7.863 $\AA$, orthorhomibic), LaCoO$_{3.0}$(a = 5.436, c = 13.095 $\AA$, hexagonal)으로 수소 분위기(300torr)에서의 TPR결과에 의하면 이들 산화물은 2단계 환원반응으로 반응이 진행되며, 열적안정성은 LaMnO$_3$ > LaFeO$_3$ > LaCoO$_3$순으로 나타났고, 반응속도론적 결과 역시 LaCoO$_3$의 활성화에너지 값이 가장 낮음을 보였다.

• 한국전기전자재료학회논문지
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• 제14권4호
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• pp.316-322
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• 2001

Cathode materials $LiMn_{2-y}$$M_{y}$ $O_4$(M=Zn and Mg) were obtained by reacting the mixture of LiOH.$H_2O$, Mn $O_2$ and MgO ar ZnO at 80$0^{\circ}C$ for 36h in an air atmosphere. These materials showed an extended cycle life in lithium-anode cells working at room temperatue in a 3.0 to 4.3V potential window. Among these materials, LiM $n_{1.9}$M $g_{0.1}$ $O_4$ showed the best cycle performance in terms of the capacity and cycle life. The discharge capacities of the cathode for the Li/LiM $n_{1.9}$ $M_{0.1}$ $O_4$ cell at the 1st cycle and at the 70th cycle were about 120 and 105mAh/g, respectively. This cell capacity is retained by 88% after 70th cycle. In cyclic voltammetry measurement, all cells revealed tow oxidation peaks and reduction peaks. However, Li/$LiMn_{2-y}$$M_{y}$ $O_4$ cell substituted with Zn and Mg showed new reaction peak during reduction reaction.eaction.ion.ion.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1998년도 추계학술대회 논문집
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• pp.271-274
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• 1998

Metallic ferromagnet LA$_{1-x}$ Sr$_{x}$MnO$_3$ has received considerable attentions because of its metallic conductivity and giant magnetic resistivity. It is generally believed that layered perovskite SrO(LA$_{1-x}$ Sr$_{x}$MnO$_3$)$_{n}$ phase is insulating and shows no metallic transition. But recent report revealed that some single crystal SrO(LA$_{1-x}$ Sr$_{x}$MnO$_3$)$_{n}$ phase showed MR effect. In this study, layered perovskite SrO(LA$_{1-x}$ Sr$_{x}$MnO$_3$)$_2$ Phases were synthesized by solid state reaction at 140$0^{\circ}C$ in air atmosphere, for wide range of x and their phases were confirmed by X-ray diffraction. Electrical and magnetic properties were measured down to 10K and the possibility of MR effects was investigated.as investigated.

• 한국세라믹학회지
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• 제36권8호
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• pp.843-847
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• 1999

The dc resistivity dc magnetization and thermopower of layered perovskite La1.6Ca1.4Mn2O7.07 have been studied. The ceramic sample of La1.6Ca1.4Mn2O7.07 undergoes the metal-insulator transition at 120K while a first-order phase transition from a ferromagnetic phase to a paramagnetic phae is observed at 260 K=TC This behavior is quite different from that of the well-known double exchange ferromagnets such as La1-xCaxMnO3 This phenomenon could be understood by considering the effects of the anisotropic double exchange interaction caused by two dimensional Mn-O-Mn networks in this materials. The dc magnetization between 120K and 250K is nearly constant and decreases rapidly with increasing temperature above 250K The measurements of dc resistivity and thermopower indicate that Zener polaron hopping conduction takes place above 260 K.

• Journal of Magnetics
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• 제21권2호
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• pp.168-172
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• 2016

$BiMnO_3$ has been a promising candidate as a magnetoelectric multiferroic while there have been many controversial reports on its ferroelectricity. The detailed analysis of its film growth, especially the growth of thin film having monoclinic symmetry has not been reported. We studied the effect of miscut angle, the substrate surface, and film thickness on the symmetry of $BiMnO_3$ thin film. A flat $SrTiO_3$ (110) substrate resulted in a thin film with three domains of $BiMnO_3$ and 1 degree miscut in the $SrTiO_3$ (110) substrate resulted in dominant domain preference in the $BiMnO_3$ thin film. The larger miscut resulted in a nearly perfect detwinned $BiMnO_3$ film with a monoclinic phase. This strong power of domain selection due to the step edge of the substrate was efficient even for the thicker film which showed a rather relaxed growth behavior along the $SrTiO_3$ [1-10] direction.

• 한국세라믹학회지
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• 제36권1호
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• pp.82-88
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• 1999

본 연구에서는 fine ceramics의 합성법을 traditional ceramics 합성에 적용하여 합성한 내화재료용 mullite에 광화제를 첨가함으로서 광화제가 mullite 생성에 미치는 영향을 관찰하고자 한다. 출발물질로 하동 kaolin과 boehmite를 사용하였으며, 여기에 광화제로 MnO와 TiO2를 액상으로 첨가하였다. 그 결과 3.5 wt% MnO를 첨가한 경우, 1,25$0^{\circ}C$에서 미반응 silica와 alumina가 존재하지 않는 단일상의 mullite를 합성할 수 있었으며, TiO2 첨가시 2~3.5wt% MnO의 경우 mullite 생성 온도를 약 10$0^{\circ}C$ 낮출 수 있었다. 이때의 mullite 생성율은 1$650^{\circ}C$에서 84%이며, 부피 비중과 흡수율 및 상온에서 꺾임강도는 각각 2.72, 0.27%, 180MPa을 나타내어 광화제를 첨가하지 않은 경우보다 특성도 향상함을 알 수 있었다.

• 한국세라믹학회지
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• 제37권8호
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• pp.774-780
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• 2000

In order to improve luminescence prperty of phosphors, we have synthesized Zn2SiO4:Mn phosphors by a new chemical synthetic route, i.e., the homogeneous precipitation method. This method has featured that the formation of phosphoris completed at relatively low temperature of 105$0^{\circ}C$ and the particle morphology exhibits spherical shape to be well-dispersed and uniform size. At all the Mn concentration explored, phosphors prepared by this method have exhibited the improved emission intensities. In particular, the emission intensities of phosphors with Mn doping contents between 1 at% and 3.5 at% were higher about 40% than that of commercial phosphor. On the other hand, the decay time has been decreased from 23 ms to 11 ms with increasing Mn concentration. In addition, the phosphor composition containing 3 at% Mn has displayed the most saturated color.

• E2M - 전기 전자와 첨단 소재
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• 제3권3호
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• pp.205-214
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• 1990

본 논문은 저손실 Mn-Zn-Fe 페라이트 제조에 관하여 연구한 것이다. Mn-Zn-Fe 페라이트는 16mol% Xno, 31mol% MnO 및 53mol% Fe$_{2}$O$_{3}$로 조성하였으며 0.1wt% $Na_{2}$SiO$_{3}$ 0.05wt% $Na_{2}$SiO$_{3}$ 0.1%wt% CaO 0.05% SiO$_{2}$ 및 0.05wt% SiO$_{2}$ 및 0.05wt% $Na_{2}$SiO$_{3}$ 0.1% CaO 0.05wt% $Al_{2}$O$_{3}$를 미량 첨가하였다. 그리고 하소와 분쇄과정을 거친 분말은 충진성을 높이기 위하여 과립화하였다. 소결 1250, 1300 및 1350.deg.C에서 이루어졌고, 평형 산소분압은 소오킹 시 PO$_{2}$는 6%부터 시작하여 점차 감소시켰으며 900.deg.C에서 순수한 질소 분위기로 냉각시켰다. 초투자율, 손실계수 및 고유저항 등의 자기적인 특성은 1300.deg.C에서 소결했을 경우의 것이 가장 우수하였다. 즉, 초투자율은 2*$10^{3}$~$10^{3}$의 높은 값을 얻을 수 있었으며 tan.delta./.mu.i값은 100KHz~ 400KHz의 고파수대에서 9*10$_{-6}$~21*10$_{-6}$이었으며 고유저항 값은 485~680 .OMEGA.-cm의 높은 값을 나타내어 중간주파수대의 자심재료에 적합한 페라이트임을 확인하였다.

• 한국자기학회지
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• 제24권2호
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• pp.46-50
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• 2014

Sol-gel법을 이용하여 $Fe_3O_4$과 $M_{0.2}Fe_{2.8}O_4$(M =Mn, Ni, Cu) 박막 시료을 만들어 M 치환에 따른 $Fe_3O_4$의 결정구조적 특성 및 양이온 분포를 X-ray diffraction(XRD)과 conversion electron M$\ddot{o}$ssbauer(CEMS) 분광법을 이용하여 조사하였다. CEMS 분광법을 이용하여 Fe 이온의 전하상태와 거동과 초미세 자기적 특성을 분석하였다. $M_{0.2}Fe_{2.8}O_4$(M =Mn, Ni, Cu) 시료들은 $Fe_3O_4$에서와 같이 입방정 스피넬 구조를 나타내었으며, Ni 이온 치환된 시료에서는 격자상수 값이 $Fe_3O_4$에서의 값과 비교하여 감소하였고, Mn 및 Cu 이온 치환된 시료에서는 증가하였다. CEMS 분석 결과 $Mn^{2+}$ 및 $Ni^{2+}$ 이온들은 주로 팔면체 자리를 치환하는 것으로 나타났으며, $Cu^{2+}$ 이온들은 팔면체, 사면체 자리를 모두 치환하는 것으로 나타났다. 부스펙트럼들의 세기비 $A_B/A_A$는 계산값과 측정값에 다소 차이가 있었으며, 이것은 M 치환이 A와 B자리의 Debye 온도에 영향을 주는 것으로 해석된다. B-자리 부스펙트럼의 비교적 큰 선폭값은 M 이온 치환에 기인한 B-자리의 M 이온분포가 초미세자기장에 미치는 분포효과로 나타났다.

• Transactions on Electrical and Electronic Materials
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• 제4권2호
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• pp.35-39
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• 2003

This paper is contents on the orthorhombic crystalline calcined by the solid phase method with LiMnO$_2$ thin film structured as the result which an average pore diameter of power was 132.3${\AA}$ in porosity analysis. Voltage ranges are able to get the properties of charge and discharge for experimental results of LiMnO$_2$ thin film were 2.2V 4.3V. The current density and scan speed were 0. 1㎃/$\textrm{cm}^2$ and 0.2㎷/sec respectively. Properties of the charge and discharge are obtained by optimum experiment condition parameters. Li dense ratio of the LiMnO$_2$ thin film that discharged capacities were 87㎃h/g have been 96.9［ppm］ at 670.784［nm］ wavelength. The dense ratio of Mn analyzed to 837［ppm］ at 257.610［nm］ wavelength. It can be estimated the quality of the LiMnO$_2$ thin film as that the wrong LiMnO$_2$ thin film pulled up from cell of electrolyte and became dry it at 800$^{\circ}C$. The results of SEM and XRD were the same as that of original researchers.