• Journal of Magnetics
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• 제21권1호
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• pp.40-45
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• 2016

Nickel substituted nano-sized ferrite powders, $Co_{1-x}Ni_xFe_2O_4$, $Mn_{1-x}Ni_xFe_2O_4$ and $Mn_{1-2x}Zn_xNi_xFe_2O_4$ ($0.0{\leq}x{\leq}0.2$), were fabricated using a sol-gel method, and their crystallographic and magnetic properties were subsequently compared. The lattice constants decreased as quantity of nickel substitution increased, while the particle size decreased in $Co_{1-x}Ni_xFe_2O_4$ ferrite but increased for the $Mn_{1-x}Ni_xFe_2O_4$ and $Mn_{1-2x}Zn_xNi_xFe_2O_4$ ferrites. For the $Co_{1-x}Ni_xFe_2O_4$ and $Mn_{1-x}Ni_xFe_2O_4$ ($0.0{\leq}x{\leq}0.2$) ferrite powders, the $M{\ddot{o}}ssbauer$ spectra could be fitted as the superposition of two Zeeman sextets due to the tetrahedral and octahedral sites of the $Fe^{3+}$ ions. However, the $M{\ddot{o}}ssbauer$ spectrum of $Mn_{0.8}Zn_{0.1}Ni_{0.1}Fe_2O_4$ consisted of two Zeeman sextets and one single quadrupole doublet due to the ferrimagnetic and paramagnetic behavior. The area ratio of the $M{\ddot{o}}ssbauer$ spectra could be used to determine the cation distribution equation, and we also explain the variation in the $M{\ddot{o}}ssbauer$ parameters by using this cation distribution equation, the superexchange interaction and the particle size. The saturation magnetization decreased in the $Co_{1-x}Ni_xFe_2O_4$ and $Mn_{1-2x}Zn_xNi_xFe_2O_4$ ferrites but increased in the $Mn_{1-x}Ni_xFe_2O_4$ ferrite with nickel substitution. The coercivity decreased in the $Co_{1-x}Ni_xFe_2O_4$ and $Mn_{1-2x}Zn_xNi_xFe_2O_4$ ferrites but increased in the $Mn_{1-x}Ni_xFe_2O_4$ ferrite with nickel substitution. These variations could thus be explained by using the site distribution equations, particle sizes and spin magnetic moments of the substituted ions.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.713-716
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• 2001

In many papers, the electrochemical analysis of LiMn$_2$O$_4$shows the transition results of Mn$^{3+}$ ion. Charge ordering is accompanied by simultaneous orbital ordering due to the Jahn-Teller effect in Mnl$^{3+}$ ions. To analyze the cycle performance of LiMn$_{2-x}$Cu$_{x}$ O$_4$as the cathode of 4 V class lithium secondary batteries, XRD, TGA analysis were conducted. Although the cycle performance of the LiMn$_{2-x}$Cu$_{x}$ O$_4$was improved from pure LiMn$_2$O$_4$, the discharge capacity was significantly lower than LiCoO$_2$. In this paper, We study the Electrochemical characterization and enhanced stability of Cu-doped spinels in the LiMn$_{2-x}$Cu$_{x}$ O$_4$upon initial cycling.l cycling.

• Transactions on Electrical and Electronic Materials
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• 제18권1호
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• pp.46-50
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• 2017

The Zn1-xMnxO ($0.00{\leq}x{\leq}0.06$) samples have been synthesized in the form of powder by the coprecipitation method at low temperature using $Zn(CH_3COO)_2$. $2H_2O$ and $Mn(CH_3COO)_2$. $4H_2O$ powders, as well as HCl and $NH_4OH$ solutions as starting materials. Characterization was conducted using XRD, TEM, XRF, FTIR and VSM. The result shows that the $Zn_{(1-x)}Mn_xO$ ($0.00{\leq}x{\leq}0.06$) nanoparticles have the wurtzite phase with a hexagonal structure and particle sizes ranging from 17.48 to 118.83 nm. In a qualitative analysis of XRF, the peaks that confirm the existence of the manganese element in Mn-doped ZnO samples were observed. Meanwhile, FTIR test result shows that there are peaks at around $500cm^{-1}$ and $400cm^{-1}$ in the FTIR spectra for Mn doped ZnO samples which clearly reveal the existence of the (Zn, Mn)-O strain mode. The (Zn, Mn)-O absorption peak positions have shifted to a lower wave number with increasing Mn doping content. The peak intensity is also lower if compared to that of the ZnO sample without doping. From the VSM test, it is shown that $Zn_{(1-x)}Mn_xO$ ($0.00{\leq}x{\leq}0.06$) nanoparticles are all paramagnetic having monotonically increased susceptibility as increasing Mn content.

• 한국자기학회지
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• 제6권3호
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• pp.145-150
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• 1996

Ferrite plating 방법은 진공이 불필요하고, 저온(< $100^{\circ}C$)에서 페라이트 박막을 제작할 수 있다. 이 방법으로 유리 기판위에 $80^{\circ}C$에서 $Fe_{3-x}Mn_{x}O_4(x=0.0~0.023)$의 페라이트 박막을 제작하였다. 박막은 60분간 성장시켰으며, 막의두께는 약 $9000\AA$이었고, 거울면과 같은 광택을 지녔다. X-선 회절 실험으로 스피넬 구조의 단일상을 확인하였다. $Fe_{3-x}Mn_{x}O_4$ 박막의 구성비 x는 반응용액에서의 구성비 x'에 비해 매우낮다(x/x'=0.04). $Fe_{3}O_{4}$ ferrite 박막의 포화자화($M_{s}$)는 480 emu/cc로써 bulk 시료와 비슷한 값을 가졌다.

• Corrosion Science and Technology
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• 제9권2호
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• pp.81-86
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• 2010

The mechanisms of selective oxidation of intercritically annealed CMnAl TRIP steels in a Continuous Galvanizing Line (GCL) were studied by cross-sectional observation of the surface and sub-surface regions by means of High Resolution Transmission Electron Microscopy (HR-TEM). The selective oxidation and nitriding of an intercritically annealed CMnAl TRIP steel in a controlled dew point 10%$H_2+N_2$ atmosphere resulted in the formation of c-xMnO.$MnO_2$ (1${\leq}$x<3) and c-xMnO.$Al_2O_3$ ($x{\geq}1$) particles on the steel surface. Single crystal c-xMnO.$SiO_2$ ($2{\leq}x{\leq}4$) oxide particles were also observed on the surface. A thin film of crystalline c-xMnO.$SiO_2$ (2${\leq}$x<3) and c-xMnO.$Al_2O_3$ ($x{\geq}1$) was present between these particles. In the sub-surface region, internal oxidation, nitriding and intermetallic compound formation were observed. In the first region, large crystalline c-xMnO.$SiO_2$ ($1{\geq}x{\geq}2$) and c-xMnO.$Al_2O_3$ ($x{\geq}1$) oxides particles were present. In the second region, c-AlN particles were observed, and in a third region, small $MnAl_x$ (x>1) intermetallic compound particles were observed.

• Journal of Magnetics
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• 제14권1호
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• pp.1-6
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• 2009

The magnetic properties of ${Bi_x}{Ca_{1-x}}{MnO_3}$ for x = 0.12, 0.13, 0.14, 0.15, and 0.16 were examined by measuring magnetic susceptibility, resistivity and electron magnetic resonance at different temperatures. ${Bi_x}{Ca_{1-x}}{MnO_3}$ showed complicated magnetic structure that varies with temperature and composition, particularly around Bi composition x. 0.15. The aim of this study was to determine how the magnetic and physical properties of ${Bi_x}{Ca_{1-x}}{MnO_3}$ change in this region. In addition, first principles calculations of the magnetic phase of ${Bi_x}{Ca_{1-x}}{MnO_3}$ for x = 0, 0.125, 0.25 were carried out, and the spin state, electric and magnetic characteristics are discussed.

• Journal of Magnetics
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• 제18권1호
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• pp.26-29
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• 2013

$Mn_xFe_{3-x}O_4$ powders have been fabricated by using sol-gel methods; their crystallographic and magnetic properties were investigated by using X-ray diffraction, scanning electron microscopy, M$\ddot{o}$ssbauer spectroscopy, and vibrating sample magnetometer. The $Mn_xFe_{3-x}O_4$ ferrite powders annealed at $500^{\circ}C$ had a single spinel structure regardless of the $Mn^{2+}$-doping amount and their lattice constants became larger as the $Mn^{2+}$ concentration was increased. Their Mossbauer spectra measured at room temperature were fitted with 2 Zeeman sextets due to the tetrahedral and octahedral sites of Fe ions, which made them ferrimagnetic. The magnetic behavior of $Mn_xFe_{3-x}O_4$ powders showed that the $Mn^{2+}$-doping amount made their saturation magnetization increase, but there were no severe effects on their coercivities. The saturation magnetization of the $Mn_xFe_{3-x}O_4$ powder varied from 38 emu/g to 70.0 emu/g and their minimum coercivity was 111.1 Oe.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2000년도 하계학술대회 논문집
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• pp.726-729
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• 2000

Though L $a_{1+x}$S $r_{2-x}$M $n_2$ $O_{7}$ n=2 R-P phases have been well known to have CMR effect, it was generally believed that n=1 phase was insulating. But recently monolayered perovskite $Ca_{2-x}$L $n_{x}$Mn $O_4$phase has been reported to show magnetoresistance. In this study, layered perovskite $Ca_{2-x}$L $n_{x}$Mn $O_4$ (x=0, 0.5, Ln=Pr, Nd, Sm, Gd) phases were synthesized by solid state reaction and their structures were refined by Rietveld method. The space groups of $Ca_2$Mn $O_4$, N $d_{0.5}$C $a_{1.5}$Mn $O_4$phases were refined as C2cb and Fmmm, respectively.y.ely.y.y.y.y.y.y.

• 한국세라믹학회지
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• 제41권2호
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• pp.170-175
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• 2004

Y-acetate, Yb-acetate와 Mn-acetate를 출발물질로 사용하여 sol-gel 법으로 강유전성 (Y $b_{x}$ $Y_{1-x}$)Mn $O_3$ 박막을 제조하였다. Acetylaceton을 촉매로 사용하고 Reflux 법을 이용하여 안정한 (Y $b_{x}$ $Y_{1-x}$)Mn $O_3$ 전구체 용액을 얻었으며, 박막은 스핀 코팅방법으로 Si(100) 기판 위에 제조하였다 열처리 온도, 코팅용액의 Rw($H_2O$/alkoxide moi ratio)변화 등을 실험변수로 하여 박막의 결정상 변화를 연구하였다. X-선 회절분석 결과 YbMn $O_3$의 결정상을 얻기 위한 최저 열처리온도는 7$50^{\circ}C$이었으며, 최적 열처리 조건은 80$0^{\circ}C$였다 Rw를 1∼6 범위 내에서 조절하여 첨가한 결과, Rw=1의 조건에서 c-축 배향이 잘 발달된 hexagonal YbMn $O_3$ 단일 결정상을 얻었다. Si(100)기판 위에 제조된 (Y $b_{x}$ $Y_{1-x}$)Mn $O_3$ 박막은 x=0 또는 1인 경우 잔류분극(Pr)값이 약 200 nC/$ extrm{cm}^2$을 나타내었으나 0

• 한국자기학회지
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• 제10권2호
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• pp.81-85
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• 2000

Orthoferrite LaFeO$_3$ 화합물에서 Fe 이온의 미량을 Mn 이온으로 치환시킨 시료인 LaFe$_{1-x}$Mn$_{x}$ O$_3$(0.0$\leq$x$\leq$0.4)을 제조하여 Mn 이온의 치환에 따른 결정학적 및 자기적 특성의 변화를 밝히기 위하여 x-선 회절기, M ssbauer 분광기, 진동자력계와 초전도 양자간섭계 등을 이용한 연구를 하였다. 제조한 시료는 모든 조성비 범위에서 단일상의 orthorhombic distorted perovskite 구조를 보였다. M ssbauer 스펙트럼은 상온에서 한 개의 육중선(x=0.0)에서 두 개의 육중선 세트(x=0.1, 0.2, 0.4)로 변했다. 특히 x=0.4에서는 상자성의 이중선과 육중선이 중첩된 모양을 보였다. 본 시료에서 Fe는 모두 Fe$^{3+}$ 상태로 팔면체자리에 위치함을 알았다. 또 LaFe$_{1-x}$Mn$_{x}$ O$_3$에서 Mn의 양이 증가함에 따라 포화자화 값은 증가하지만 보자력은 감소함을 알아냈다.