• Journal of Magnetics
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• 제8권4호
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• pp.129-132
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• 2003

We investigated the crystallographic and magnetic properties of double perovskite $Sr_2Fe_{l-x}Cr_{x}MoO_{6}$ (x=0.0, 0.01, 0.03, 0.05, and 0.10). Mossbauer spectra of the $Sr_2Fe_{l-x}Cr_{x}MoO_{6}$ have been taken at various temperatures ranging from 15 to 415 K. As the temperature increased towards $T_{c}$(415 K), the Mossbauer spectra showed line broadening and 1, 6 and 3, 4 line-width differences because of anisotropic hyperfine field fluctuation. The Mossbauer spectra indicated that an anisotropic field fluctuation of +H ( $P_{+}$=0.85) was greater than that of -H ($P_{-}$=0.15). We also calculated the field fluctuation frequency factors and the temperature dependence of anisotropy energies from its relaxation rate. We interpreted the effect of Cr ($t^3$$_{2g}$) doping as a decrease in the anisotropy energy.

• 대한수학회지
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• 제57권6호
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• pp.1551-1571
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• 2020

This paper is concerned with the following Kirchhoff-Schrödinger-Poisson system $$\begin{cases} -(a+b{\displaystyle\smashmargin{2}\int\nolimits_{\mathbb{R}^3}}{\mid}{\nabla}u{\mid}^2dx){\Delta}u+V(x)u+{\mu}{\phi}u={\lambda}f(x){\mid}u{\mid}^{p-2}u+g(x){\mid}u{\mid}^{p-2}u,&{\text{ in }}{\mathbb{R}}^3,\\-{\Delta}{\phi}={\mu}{\mid}u{\mid}^2,&{\text{ in }}{\mathbb{R}}^3, \end{cases}$$ where a > 0, b, µ ≥ 0, p ∈ (1, 2), q ∈ [4, 6) and λ > 0 is a parameter. Under some suitable assumptions on V (x), f(x) and g(x), we prove that the above system has at least two different nontrivial solutions via the Ekeland's variational principle and the Mountain Pass Theorem in critical point theory. Some recent results from the literature are improved and extended.

• Bulletin of the Korean Chemical Society
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• 제22권7호
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• pp.709-715
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• 2001

We have been studied photosensitization mechanism's additive effect, of perylene 3,4,9,10-tetracarboxyl-diimide and X-phthalocyanine (charge generation materials), using the photochemical and photoelectrochemical approach. It was found that the photoreceptor on the excited state reacts with metal oxide, which creates the charge transfer on the interface of SnO2/electrolyte. In the electrode (X5P1) made of five X-phthalocyanine and single perylene 3,4,9,10-tetracarboxyldiimide layers, the cathodic photocurrent of X-phthalocyanine in the 400-600 nm region was increased by the addition of perylene 3,4,9,10-tetracarboxyldiimide. The maximum wavelength of fluorescence of perylene 3,4,9,10-tetracarboxyldiimide showed no dependence on the temperature. The addition of 4-dibenzylamino-2-methylbenzaldehyde diphenylhydrazone known as charge transport material was represented as decreasing photocurrent for X-phthalocyanine and perylene 3,4,9,10-tetracarboxyldiimide, respectively. In the electrode (X1P1) made of single X-phthalocyanine and single perylene 3,4,9,10-tetracarboxyldiimide layers, an anodic photocurrent of about 10.5 nA was generated by addition of hydroquinone at 550 nm. And the characteristic of photoinduced discharge was shown to decrease by a factor of 5 and the speed of dark decay was increased by a factor of 1.2.

• 한국표면공학회지
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• 제24권1호
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• pp.1.2-1.2
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• 1991

The formation of managanese 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 pH10. As the result of X-ray diffraction Mn Fe2O4 crystal composition in pH13. When the particles of Mnx Fe3-x O4 were heated at 30$0^{\circ}C$, it has been shown typical MnFe2O4(JCPDS Card No. 10-319) in X-1 composition. As the result of SEM observation, the size of MnFe2O4 particles were about 0.1$\mu\textrm{m}$, the shape of particles were spherical type. According to the above mentioned experimental condition, 0.1-0.5$\mu\textrm{m}$ sub-micron particles of manganese ferrite were formed from the wasted manganese dry cell, through washing longrightarrow reduction longrightarrow electrloysis.

• 대한화학회지
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• 제17권3호
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• pp.154-162
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• 1973

치환된 염화벤젠술포닐 $XC_6H_4SO_2Cl$(X:p-MeO, H, p-Cl, p-Br, p-NO_2)의 할라이드 교환 반응을 무수 아세톤 중에서 행하여 반응속도 상수와 활성화 계수를 구하였다. 금속 할라이드의 이온쌍 $M^{+}X^{-}$의 반응성은 할라이드 이온에 비하여 무시할 수 있음을 보았다. EH 친핵성도가 전자를 밀어내는 치환기를 가진 경우에 $Cl>Br^{-}>I^{-}$이고, 전자를 끌어주는 치환기를 가진 경우에는 $Cl>I^{-}>Br^{-}$이었다. 이들 결과와 Hammett그림표가 위로 볼록한 것을 결합 약화 과정이 크게 기여하는 단순 $S_N2$메커니즘으로 설명하였다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2000년도 추계학술대회 논문집
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• pp.555-558
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• 2000

Layered perovskite La$_{2-x}$Ca$_{l-x}$Mn$_2$O$_{7}$ phases were synthesized by solid state reaction. Single phase R-P could be obtained in the range of 0.4$_{2-x}$Ca$_{l-x}$Mn$_2$O$_{7}$. About 30% of MR ratio was obtained at 270K when 5 T of magnetic field was applied.ied.ied.ied.

• 대한수학회보
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• 제54권4호
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• pp.1323-1330
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• 2017

For a nondegenerate projective irreducible variety $X{\subset}{\mathbb{P}}^r$, it is a natural problem to find an upper bound for the value of $${\ell}_{\beta}(X)=max\{length(X{\cap}L){\mid}L={\mathbb{P}}^{\beta}{\subset}{\mathbb{P}}^r,\;{\dim}(X{\cap}L)=0\}$$ for each $1{\leq}{\beta}{\leq}e$. When X is locally Cohen-Macaulay, A. Noma in [10] proves that ${\ell}_{\beta}(X)$ is at most $d-e+{\beta}$ where d and e are respectively the degree and the codimension of X. In this paper, we construct some surfaces $S{\subset}{\mathbb{P}}^5$ of degree $d{\in}\{7,{\ldots},12\}$ which satisfies the inequality $${\ell}_2(S){\geq}d-3+{\lfloor}{\frac{d}{2}}{\rfloor}$$. This shows that Noma's bound is no more valid for locally non-Cohen-Macaulay varieties.

• 대한화학회지
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• 제47권6호
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• pp.614-618
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• 2003

고상반응으로 $Sr_2Ru_{1-x}Cu_xO_{4-y}(0.0{\le}x{\le}0.5)$ 화합물을 합성하였다. X-선 회절 분석 결과에 대한 Rietveld 정밀화로부터 합성된 $Sr_2Ru_{1-x}Cu_xO_{4-y}$ 화합물은 $0{\le}x{\le}0.30$의 Cu 치환 범위에서는 모두 단일상의 정방정계 구조를 갖는 $K_2NiF_4$ 형태의 구조를 취하지만, $0.4{\le}x{\le}0.5$의 범위에서는 미량의 $Sr_2CuO_3$ 화합물의 회절 피이크가 관찰되는 이중상을 갖는 화합물로 존재한다는 사실을 알 수 있었다. $Sr_2RuO_4$ 화합물의 Ru자리에 Cu 이온을 부분적으로 치환할 때의 전이금속 이온인, Ru와 Cu이온의 원자가 상태는 X-선 전자 분광법으로 확인하였다. $Ru\; 3p_{3/2}$ 전자와 $Cu\; 2p_{3/2}$ 전자의 결합에너지 측정으로부터 $Ru^{4+},\;Cu^{2+}$를 갖는 것으로 확인되었다. $Sr_2RuO_4$ 화합물의 Ru 자리에 치환하는 Cu 이온의 농도를 증가할수록 $Ru-O1({\times}4)$ 와 $Ru-O_2({\times}2$)의 결합길이 차이가 ${\Delta}=0.1329 {\AA}Sr_2RuO_4$ 경우)에서 ${\Delta}=0.0383 {\AA}(Sr_Ru_{0.7}Cu_{0.3}O_{4-y}$ 경우)으로 변하며, c/a 역시 감소하는 경향을 나타내고 있다. 따라서, $Sr_2RuO_4$ 화합물의 Ru 자리에 Cu 이온을 치환함에 따라 $RuO_6$ 팔면체의 국부 대칭성의 변화에 의해 결정구조가 정방정계로의 변화를 수반하면서, 이에 따른 $Sr_2Ru_{1-x}Cu_xO_{4-y}$의 전달특성이 금속에서 반도체로 변화한다.

• Korean Journal of Mathematics
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• 제30권2호
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• pp.403-412
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• 2022

In this paper, we introduce the following cubic-quartic functional equation of the form $$f(x+4y)+f(x-4y)=16[f(x+y)+f(x-y)]{\pm}30f(-x)+\frac{5}{2}[f(4y)-64f(y)]$$. Further, we investigate the general solution and the Ulam stability for the above functional equation in non-Archimedean spaces by using the direct method.

• 대한화학회지
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• 제55권3호
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• pp.502-508
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• 2011

[ $Nd_{2x}Cd_{2-3x}SiO_4$ ]($0.01{\leq}x{\leq}0.21$) [S1-S3: x=0.01, 0.11 and 0.21] 고용체를 졸-겔 방법을 통해 합성하였다. X선 분말회절(XRD) 측정은 $P2_1$/m 공간군의 단사정계를 보여준다. 평균 결정 크기는 20-45 nm이다. 주사전자현미경(SEM)으로 살펴본 모양은 구형의 특성을 보인다. 에너지 분산 X 선 분광기(EDS) 결과로부터 모든 구성 원소의 존재를 확인하였다. ~750 nm에서의 흡수 밴드는 $Nd^{3+}$ 이온의 $^4I_{9/2}{\rightarrow}^4F_{7/2}+^4S_{3/2}$ 전이에 기인한다. 10, 40, 77, 300 K에서 S1-S3의 전자 상자성 공명 (EPR) 선모양은 $Nd^{3+}$ 이온의 빠른 스핀 격자 이완에 기인하는 폭이 넓은 구분되지 않은 등방성의 선모양을 보여준다.