• 한국분말재료학회지
• /
• 제9권6호
• /
• pp.449-454
• /
• 2002

$MnxZn_{1-x}Fe_2O_4$ (x=0.69~0.74) powders synthesized by the thermal decomposition of organic acid salts. The obtained powders were uniform in composition and ultra-fine particle with about 400 nm. The amount of spinel phase of these powders was about 50% in X-ray diffraction patterns. The calcination of powder was carried out at $900^{\circ}C$ for 2 hours in air. After the powders were calcined. the mean size of powder was about 500 nm and the amount of spinel phase was increased over about 65%. The maximum amount of spinel phase was about 75% in the specimen of X=0.72. The magnetic properties of calcined $Mn_{0.72}Zn_{0.28}Fe_2O_4$ powders were the best among the different among the different compositions.

• 한국전기전자재료학회논문지
• /
• 제29권6호
• /
• pp.337-341
• /
• 2016

In this study, $ Ni_{0.79}(Mn_{2.21-x}Cu_x)O_4$ (x=0~0.25) specimens were prepared by using a conventional mixed oxide method. All specimens were sintered in air at $1,200^{\circ}C$ for 12 h and cooled at a rate of $2^{\circ}C/min$ to $800^{\circ}C$, subsequently quenching to room temperature. We investigated the structural and electrical properties of $ Ni_{0.79}(Mn_{2.21-x}Cu_x)O_4$ specimens with variation of CuO amount for the application of NTC thermistors. As results of X-ray diffraction patterns, all specimens showed the formation of a complete solid solution with cubic spinel phase. The relationship between ln ${\rho}$ and the reciprocal of absolute temperature(1/T) for the NTC thermistors was shown linearity, which exhibited the typical NTC thermistor properties. With increasing the amount of CuO, resistivity at room temperature, B-value, and temperature coefficient resistance decreased.

• 한국자기학회:학술대회 개요집
• /
• 한국자기학회 2005년도 하계학술연구발표회 논문개요집
• /
• pp.194-195
• /
• 2005

• 한국자기학회:학술대회 개요집
• /
• 한국자기학회 2005년도 하계학술연구발표회 논문개요집
• /
• pp.214-215
• /
• 2005

• 한국세라믹학회지
• /
• 제28권8호
• /
• pp.603-610
• /
• 1991

An oxygen deficient perovskite (CaLa)(MgMn)O5.43, with the cubic unit cell parameter of 3.826$\AA$, was prepared 115$0^{\circ}C$ for 10 hrs under the ambient oxygen gas pressure. The average oxidation state of manganese was determined to be 3.86 by the iodometric titration, so that the perovskite could be formulated as (CaLa) ({{{{ { MgMn}`_{ chi } ^{II } }}{{{{ { Mn}`_{ y} ^{III } }}{{{{ { Mn}`_{1- chi -y } ^{IV } }})O5.43 (2x+y=0.14). From X-ray photoelectron spectroscopy, the manganese ions in the lattice are mostly tetravalent, but two paramagnetic configurations were observed in the EPR spectrum: One sharp isotropic signal with hyperfines (ΔH 50 G, g=1.997$\pm$0.002 and │A│=82(4)$\times$10-4 cm-1) and a broad isotropic one (ΔH 1600 G, g=1.994$\pm$0.002), those which correspond respectively to Mn(II) and Mn(IV) ions. According to the magnetic susceptibility measurement, it follows the Curie-Weiss law from 20 K up to room temperature with $\mu$eff=5.23 $\mu$B, which is relatively larger than spin-only value({{{{ { mu }`_{eff} ^{s.o } }}=4.04 $\mu$B) due to the effect of weak ferromagnetic coupling. Such a result is in accord with a theory of semicovalence exchange.

• 한국결정학회지
• /
• 제12권4호
• /
• pp.212-215
• /
• 2001

NaOAC·3H₂O 존재 하에서, manganese nitrate(Mn(NO₃)₂·H₂O )와 imidzole-4,5-dicarboxylic acid(IDCH₂)가 수열반응하여, 실험식 [Mn(IDC)(H₂O)]을 가지는 2차원 배위고분자 합성되었다. 화합물 1의 구조가 분광학적 방법(IR) 및 X-ray 회절법으로 규명되었다. 화합물의 1의 결정학적 자료: 사방정계 공간군 Pbca, a=7.257(5) Å b=13.687(5)Å, c=14.332(6)Å Z=8, R(wR₂)=0.0498(0.0999).

• 자원환경지질
• /
• 제21권1호
• /
• pp.29-44
• /
• 1988

석류석과 사방휘석의 평형관계를 20-45kb, $975-1400^{\circ}C$, FMAS시스템에서 상호역반응 실험을 통해서 연구하였으며 반응 촉매제로써 사용한 PbO와 0.55 $PbF_2$의 혼합물은 매우 효과적이었다. Fe-Mg의 교환반응은 이 실험온도, 압력범위 내에서는 조성성분의 영향을 받지 않는다. 실험결과와 석류석의 혼합 모델을 사용한 석류석-사방휘석의 지질온도계는 다음과 같다. $$T^{\circ}C=(1971+11.91P(Kb)+1510(X_{Ca}+X_{Mn})^{Gt}/(lnK_D+0.96)-273$$.

• Journal of Magnetics
• /
• 제18권1호
• /
• pp.34-38
• /
• 2013

This paper studies the effects of the Mn-site substitution by nickel on the magnetic properties and the magnetocaloric properties of $La_{0.7}Ca_{0.3}Mn_{1-x}Ni_xO_3$ (x = 0, 0.05 and 0.1). The orthorhombic crystal structures of the samples are confirmed by the room temperature X-ray diffraction. The dependence of the Curie temperature ($T_C$) and the magnetic entropy change (${\Delta}S_M$) on the Ni doping content was investigated. The samples with x = 0 had the first order phase transition, while the samples with x = 0.05 and 0.1 had the second order phase transition. As the concentration of Ni increased, the maximum entropy change (${\mid}{\Delta}S_M{\mid}_{max}$) decreased gradually, from 2.78 $J{\cdot}kg^{-1}{\cdot}K^{-1}$ (x = 0) to 1.02 $J{\cdot}kg^{-1}{\cdot}K^{-1}$ (x = 0.1), in a magnetic field change of 15 kOe. The measured value of $T_C$ was 185 K, 150 K and 145 K for x = 0, 0.05 and 0.1, respectively. The phase transition temperatures became wider as x increased. It indicates that the Mn-site substitution by Ni may be used to tailor the Curie temperature in $La_{0.7}Ca_{0.3}Mn_{1-x}Ni_xO_3$.

• 한국세라믹학회지
• /
• 제36권7호
• /
• pp.698-704
• /
• 1999

Li rich Li1+xMn2-xO4(x=0.07) spinel powders were prepared by an oxalate precipitation of wet chemical methods at temperature lower than $600^{\circ}C$. The FTIR results showed that the powders prepared at $600^{\circ}C$ had high degree of crystal quality comparing with the spinel powders prepared by solid state reaction at 75$0^{\circ}C$ which was the lowest synthesis temperature of the solid state reaction method. The particle size of powders prepared by the oxalate precipitation at $600^{\circ}C$ was smaller than 0.2${\mu}{\textrm}{m}$ and the specific surface area was 11.01 m2/g A heat treatment over 90$0^{\circ}C$ formed second phase in the precipitates. It was shown that there were phase transitions at temperatures. T1,T2 and T2. The transitions involved weight loss and gain during heating and cooling. The low temperature synthesis below $600^{\circ}C$ avoided the second phase formation and the prepared powders showed improved compositional and physical properties for secondary lithium battery applications.

• 한국자기학회지
• /
• 제8권6호
• /
• pp.335-340
• /
• 1998

거대 자기 저항 La0.67Ca0.33Mn0.9957Fe0.01O3물질을 졸-겔법을 이용하여 제조하였다. La0.67Ca0.33Mn0.9957Fe0.01O3의 자기적 성질을 X-선 회절 분석, 리더퍼스 분광 측정, 자화 측정, Mossbauer 분광 측정으로 연구하였다. 단일상 La0.67Ca0.33Mn0.9957Fe0.01O3의 결정구조는 cubic 페롭스카이트 구조이고, 격자상수 a0=3.868$\AA$이었다. 1%철 이온의 치환에 의한 격자상수의 변화는 관측할 수 없겠지만, 큐리온도는 282K에서 270K로, 77K에서의 포화 자화는 84emu/g에서 81emu/g으로 감소함을 알 수 있었다. Mossbauer 분광 측정은 4.2K에서 상온 온도 영역까지 여러 온도 구간에서 측정하였다. Mossbauer 스펙트럼의 분석은 57Fe 이온에 분포에 의한 상호작용 모델을 고려하여 분석하였다. 이성질체 이동값에 의해 철 이온은 모든 구간에서 +3가 이었다. La0.67Ca0.33Mn0.9957Fe0.01O3의 반도체-금속 전이온도는 250K이엇으며, 자기 저항비는 33%이었다..