• 대한화학회지
• /
• 제43권6호
• /
• pp.636-643
• /
• 1999

PDP(plasma display panel)의 녹색 광원으로 유망한 $Zn_{2-x}Mn_xSiO_4$ 헝광체를 1300$^{\circ}C$에서 고상반응법으로 제조한 후 900$^{\circ}C$에서 후속 열처리를 실시하면 녹색 형광의 강도가 현저히 증가한다. 열처리를 통한 형광 강도의 향상과 망간의 산화 상태 및 국부 구조 변화와의 관계를 파악하고자 망간 K 흡수단의 엑스선 흡수 스펙트럼을 분석하였다. $1s{\rightarrow}3d$ 전이에 해당하는 프리엣지(preedge) 봉우리와 XANES 스펙트럼을 분석한 결과, 망간은 열처리와 무관하게 +2가의 산화 상태를 유지하였으며 Zn 자리를 치환하는 것으로 밝혀졌다. 또한 EXAFS 스펙트럼의 분석을 통하여, Mn은 $MnO_4$ 사면체를 형성하고 Mn-O 쌍의 결합 길이와 디바이월러 인자(Debye-Waller factor)는 열처리 후 공히 감소함을 알 수 있었다.

• 대한전기학회:학술대회논문집
• /
• 대한전기학회 1999년도 추계학술대회 논문집 학회본부 C
• /
• pp.882-884
• /
• 1999

금속 다층박막과 미세입상 합금박막에서 발견된 Giant Magnetoresistance(GMR)현상에 고무되어 최근에는 50년대에 밝혀졌던 산화물 자기저항 재료에 관하여 새롭게 연구하고 있다. Perovskite 구조를 가지는 $La_{1-x}Ca_{x}MnO_{3}$ 박막에서 큰 자기저항을 얻었으며 이를 Colossal Magentoresistance (CMR)이라 한다. 본 연구에서는 $La_{1-x}Ca_{x}MnO_{3}$ 분말을 고상반응법과 자발착화연소 합성법(Glycine-Nitrate Process)으로 각각 제조하였으며 비교 분석하였다. TGA을 이용하여 불순물과 미반응 물질을 확인하여 적당한 하소온도를 결정하였고 XRD를 이용하여 결정상을 분석하였다. Dilatometer를 이용해 $1400^{\circ}C$까지의 열팽창율을 측정하였다. BET로 비 표면적을 비교하였으며, 주사전자현미경(SEM)으로 각각 제조된 분말의 입자상태와 입자성장을 확인하였다. GNP법으로 합성한 경우가 고상반응법을 이용한 경우보다 입자의 크기가 submicron 단위로 미세하고 비표면적도 수배 컸으며, 고순도의 perovskite 구조를 갖는 $La_{1-x}Ca_{x}MnO_{3}$ 분말을 얻을 수 있었다.

• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 1999년도 춘계학술대회 논문집
• /
• pp.137-141
• /
• 1999

금속 다층박막과 미세입상 합금박막에서 발견된 Giant Magnetoresistance(GMR) 현상에 고무되어 최근에는 50년대에 밝혀졌던 산화물 자기저항 재료에 관하여 새롭게 연구하고 있으며 perovskite 구조를 가지는 La$_{1-x}$ Ca/xub x/MnO$_{3}$ 박막에서 큰 자기저항을 얻었으며 이를 Colossal Magentoresistance (CMR) 이라 부른다. 본 연구에서는 La$_{1-x}$ Ca/xub x/MnO$_{3}$ 분말을 하소온도를 700-90$0^{\circ}C$로 변화시킨 고상반응법과 자발착화연소합성법(Glycine-Nitrate Process) 으로 각각 제조하였으며 비교 분석하였다. TG-DTA을 이용하여 불순물과 미반응 물질을 확인하여 적당한 하소 온도를 결정하였고 XRD를 이용하여 결정상을 분석하였다. 주사전자현미경(SEM)으로 각각 제조된 분말의 하소후 입자의 크기를 비교하였다. GNP법으로 합성한 경우가 고상반응법을 이용한 경우보다 입자의 크기가 submicron 단위로 미세하고 균질하며 고순도의 perovskite 구조를 갖는 La$_{1-x}$ Ca/xub x/MnO$_{3}$ 분말을 얻을 수 있었다.었다.

• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 1999년도 춘계학술대회 논문집
• /
• pp.133-136
• /
• 1999

We report on the electrochemical properly of LiZ $n_{x}$Mn $_{2-x}$ $O_4$ for different degrees of Zn substitution(x) Though all cathode material showed spinel phase based on cubic phase in X-ray diffraction, other peaks(M $n_2$ $O_3$ or M $n_3$ $O_4$) gradually exhibited and became intense with the increase of x vague in LiZ $n_{x}$Mn $_{2-x}$ $O_4$. In addtion, TG-DTA analysis exhibited that both LiM $n_2$ $O_4$ and LiZ $n_{0.1}$ M $n_{1.9}$ $O_4$ occurred the weight loss(TG) and the endothermic and exothermic reaction(DTA) until 80$0^{\circ}C$ When x=0.1 in LiZ $n_{x}$Mn $_{2-x}$ $O_4$ cathode materials showed the charge and discharge capacity of about 100mAh/g at first cycle and about 70mAh/g after tooth cycle.cle.e.cle.e.e.e.

• 한국전기화학회:학술대회논문집
• /
• 한국전기화학회 2004년도 춘계총회 및 학술발표회
• /
• pp.59-59
• /
• 2004

• 한국세라믹학회지
• /
• 제34권5호
• /
• pp.461-466
• /
• 1997

Dielectric and piezoelectric properties of (Pb1-1.5xLnx)(Ti0.98Mn0.02)O3 ceramics with x=0~0.2 have been investigated. Pb(Ti0.98Mn0.02)O3 showed poor sinterability and cracking on cooling, but the substitution of Nd3+ ions into Pb2+ sites resulted in dense microstructures without cracking through reducing crystallographic anisotropy. The Nd3+ substitution, however, deteriorated the temperature stability of the piezoelectric properties because of lowering the Curie point. Electromechanical anisotropy(Kt/Kp) indicated a maximum value of 10 when x=0.1. This result might be attributed to the counteracting effects that with increasing x, the lattice anisotropy decreases while the poling becomes easier due to the increase in O2- vacancy concentration. Thickness-shear mode resonators with (Pb0.85Nd0.1)(Ti0.98Mn0.02)O3 composition showed good resonant characteristics around 4.5 MHz.

• 전기화학회지
• /
• 제7권1호
• /
• pp.1-8
• /
• 2004

This paper deals with the recent development of high-voltage cathode materials of mono- and di- metal ions substituted spinel $LiMn_2O_4$ for lithium batteries. $LiCu_xMn_{2-x}O_4(0{\leq}x{\leq}0.5)$ shows reversible intercalation/deintercalation in two potential regions, $3.9\~43\;and\;4.8-5.0V$ and stable electrochemical cycling behavior but with low capacity. $LiNi_{0.5}Mn_{1.5}O_4$ obtained by a sol-gel process delivers a capacity of 127mAh $g^{-1}$ on the first cycle and sustains a value of 124 mAh $g^{-1}$ even after the 60th cycle. The $Li_xCr_yMn_{2-y}O_4(0{\leq}x{\leq}0.5)$ solid-solutions exhibit enhanced specific capacity, larger average voltage, and improved cycling behaviors for low Cr content. $LiCr_yMn_{2-y}O_4$ presents a reversible Li deintercalation process at 4.9V, whose capacity is proportional to the Cr content in the range of $0.25{\leq}x{\leq}0.5$ and delivers higher capacities. $LiM_yCr_{0.5-y}Mn_{1.5}O_4(M=Fe\;or\;Al)$ shows that the capacity retention is lowered compared with lithium manganate. The cumulative capacities obtainable with Al-substitutted materials are less than those with Fe-substituted materials. $LiCr_xNi_{0.5-x}Mn_{1.5}O_4(x=0.1)$ delivers a high initial capacity of 1$152mAh\;g^{-1}$ with excellent cycleability.

• 한국진공학회:학술대회논문집
• /
• 한국진공학회 2009년도 제38회 동계학술대회 초록집
• /
• pp.226-226
• /
• 2010

Microstructure, magnetic and transport properties of as-deposited electron-doped $La_{1-x}Ce_xMnO_3$ and hole-doped $La_{1-x}Ce_xMnO_3$ films prepared by pulse laser deposition, with x = 0.1 and 0.3, have been investigated. The microstructural analysis reveals that the $La_{1-x}Ce_xMnO_3$ films have a column-like microstructure and a strip-domain phase with a periodic spacing of about 3c, which were not found for the $La_{1-x}Ce_xMnO_3$ ones. At the same time, the experimental results manifest that there is no fundamental difference in the magnetic and the transport properties between electron- and hole-doped manganite films, except the appearance of ferromagnetic response in the low-doped $La_{0.9}Ce_{0.1}MnO_3$ film at temperatures above the Curie point. The observed magnetic behavior, typical for the Griffiths-like phase, for this film is explained by the percolation mechanism of the ferromagnetic transition and by the presence of strip-domain phase which stimulates the magnetic phase separation.

• 한국전기전자재료학회논문지
• /
• 제14권4호
• /
• pp.309-315
• /
• 2001

Crystallized $LiMn_{2-y}Mg_{y}O_4$ powder was prepared by calcing the mixture of LiOH.$H_2O$, $MnO_2$ and MgO at $800^{\circ}C$ for 36h in an air atmosphere. The structure of $LiMn_{2-y}Mg_{y}O_4$ crystallites was analyzed from powder X-ray diffraction data as a cubic spinel, space group Fd3m. Though all cathode material showed spinel phase based on cubic phase in X-ray diffraction, other peaks gradually exhibited and became intense with increasing y value in $LiMn_{2-y}Mg_{y}O_4$. However, ununiform which calculated by (111) face and (222) face was constant in spite of the increase of y value, except pure $LiMn_2O_4$. AC impedance of Li/$LiMn_{2-y}Mg_{y}O_4$ cells revealed the similar resistance of about $70\Omega$ before cycling. In addition, The impedance of Li/$LiMn_{1.9}Mg_{0.1}O_4$ cell changed during charge and discharge or after cycling.

• 한국표면공학회지
• /
• 제25권1호
• /
• pp.1-7
• /
• 1992

The formation of manganese ferrite has been performed to investigate some properties according to the variation of compositions, pH, current density by electrolysis. It has been found that the amount of oxidized weight of anode were increased with increasing current density. The amount of oxidized weight of anode were most in pH 10. As the result of X-ray diffraction Mn Fe₂O₄ crystal composition in pH13. When the particles of Mn/sub x/ Fe/sub 3-x/O₄ were heated at 300℃, it has been shown typical Mn Fe₂O₄(JCPDS Card No. 10-319) in X=1 composition. As the result of SEM observation, the size of MnFe₂O₄ particles were about 0.1㎛, the shape of particles were spherical type. According to the above mentioned experimental condition, 0.1-0.5㎛ sub-micron particles of manganese ferrite were formed from the wasted manganese dry cell, through washing → reduction → electrloysis.