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Luminescence Wavelength Control of $CaAlSiN_3:Eu^{2+}$ by Ca-replacing: Computational and Experimental Study

  • Onuma, Hiroaki;Suehiro, Takayuki;Suzuki, Ai;Tsuboi, Hideyuki;Hatakeyama, Nozomu;Endou, Akira;Takaba, Hiromitsu;Kubo, Momoji;Sato, Tsugio;Miyamoto, Akira
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2009년도 9th International Meeting on Information Display
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    • pp.290-293
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    • 2009
  • We both theoretically and experimentally investigated the luminescence wavelength control of the $Eu^{2+}$-doped $CaAlSiN_3$ (CASN:$Eu^{2+}$). To modify emission wavelength, Na-doped and Mg-doped CASN:$Eu^{2+}$ (NCASN:$Eu^{2+}$ and MCASN:$Eu^{2+}$) have been studied. According to quantum chemistry calculation result, we synthesized NCASN:$Eu^{2+}$ and MCASN:$Eu^{2+}$. NCASN:$Eu^{2+}$ and MCASN:$Eu^{2+}$ showed shorter emission wavelength than that of CASN:$Eu^{2+}$.

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Hexagonal Ferrite에 관한 연구 (I) Ferroxplana $Zn_{I-X}$$Mn_X$Y($Ba_2$$Zn_{2(1-X)}$$Mn_{2X}$$Fe_12$$O_22$)의 자성 (Studies on the Hexagonal Ferrites (I) The Magnetic Properties ofFerroxplana $Zn_{I-X}$$Mn_X$Y($Ba_2$$Zn_{2(1-X)}$$Mn_{2X}$$Fe_12$$O_22$))

  • 김태옥
    • 한국세라믹학회지
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    • 제13권3호
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    • pp.13-20
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    • 1976
  • The magnetic properties, especially the magnetostriction, of ferroxplana $Zn_{1-x}$$M_X$Y(x=0.0, 0.2, 0.4, 0.6) were investigated at room temperature. In general, the Curie temperature and the permeability of ferroxplana $Zn_{1-X}$$Mn_X$Y increased while the amount of the other phase decrease with increased concentration of dopant $Mn^{2+} for $Zn^{2+}. The magnetostriction constnats K1, K2, K3 and K4 for ZnY were +0.3, -5.0, -4.3 and $-4.8{\times}$$10^{-6} while that for 4Zn^0.8$ $Mn^0.2$Y were +2.5, -5.4, -6.0 and $-3.4{\times}10^{-6}$, respectively.

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REVISIT TO ALEXANDER MODULES OF 2-GENERATOR KNOTS IN THE 3-SPHERE

  • Song, Hyun-Jong
    • East Asian mathematical journal
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    • 제36권3호
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    • pp.359-364
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    • 2020
  • It is known that a 2-generator knot K has a cyclic Alexander module ℤ[t, t―1]/(Δ(t)) where Δ(t) is the Alexander polynomial of K. In this paper we explicitly show how to reduce 2-generator Alexander modules to cyclic ones by using Chiswell, Glass and Wilsons presentations of 2-generator knot groups $$<\;x,\;y\;{\mid}\;(x^{{\alpha}_1})^{y^{{\gamma}_1}},\;{\cdots}\;,\;(x^{{\alpha}_k})^{y^{{\gamma}_k}}\;>$$ where ab = bab-1.

터널 산화막 두께에 따른 Al2O3/Y2O3/SiO2 다층막의 메모리 특성 연구 (A Study of the Memory Characteristics of Al2O3/Y2O3/SiO2 Multi-Stacked Films with Different Tunnel Oxide Thicknesses)

  • 정혜영;최유열;김형근;최두진
    • 한국세라믹학회지
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    • 제49권6호
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    • pp.631-636
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    • 2012
  • Conventional SONOS (poly-silicon/oxide/nitride/oxide/silicon) type memory is associated with a retention issue due to the continuous demand for scaled-down devices. In this study, $Al_2O_3/Y_2O_3/SiO_2$ (AYO) multilayer structures using a high-k $Y_2O_3$ film as a charge-trapping layer were fabricated for nonvolatile memory applications. This work focused on improving the retention properties using a $Y_2O_3$ layer with different tunnel oxide thickness ranging from 3 nm to 5 nm created by metal organic chemical vapor deposition (MOCVD). The electrical properties and reliabilities of each specimen were evaluated. The results showed that the $Y_2O_3$ with 4 nm $SiO_2$ tunnel oxide layer had the largest memory window of 1.29 V. In addition, all specimens exhibited stable endurance characteristics (program/erasecycles up to $10^4$) due to the superior charge-trapping characteristics of $Y_2O_3$. We expect that these high-k $Y_2O_3$ films can be candidates to replace $Si_3N_4$ films as the charge-trapping layer in SONOS-type flash memory devices.

고온초전도체 $SmBa_2Cu_2O_y$ 교류자화율 (AC susceptibility of the $high-T_c$ superconductor $SmBa_2Cu_2O_y$)

  • 김홍;이부영;이준호;김영철
    • Progress in Superconductivity
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    • 제6권1호
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    • pp.89-94
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    • 2004
  • The policrystalline$SmBa_2$$Cu_2$$O_{y}$ was synthesized by the solid state reaction method. The dependence of AC susceptibility on temperature and applied ac field was studied. The critical temperature $T_{c}$ is about 92 K. As the ac field is increased, the slope and the value of real part of susceptibility become smaller and the peak position of imaginary part $T_{P}$ was shifted to a lower temperature with peak broadening. Using Bean's model, we determined intergrain critical current density $J_{c}$ and obtained $44 A/{cm}^2$ at 75 K. From the relation of the $J_{c}$ (T)=($1-T/T_{c}$ )$^{\beta}$ we obtained $\beta$=0.8 and found that the Josephson junction type of the $SmBa_2$$Cu_2$$O_{y}$ is SIS junction. The peak of the imaginary part shifts to higher temperature with increasing frequency, f. from Arrhenius plot, we obtained the activation energy of about 0.96 eV.

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Local Moves and Gordian Complexes, II

  • Nakanishi, Yasutaka
    • Kyungpook Mathematical Journal
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    • 제47권3호
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    • pp.329-334
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    • 2007
  • By the works of Levine [2] and Rolfsen [5], [6], it is known that a local move called a crossing-change is strongly related to the Alexander invariant. In this note, we will consider to what degree the relationship is strong. Let K be a knot, and $K^{\times}$ the set of knots obtained from a knot K by a single crossing-change. Let MK be the Alexander invariant of a knot K, and MK the set of the Alexander invariants $\{MK\}_{K{\in}\mathcal{K}}$ for a set of knots $\mathcal{K}$. Our main result is the following: If both $K_1$ and $K_2$ are knots with unknotting number one, then $MK_1=MK_2$ implies $MK_1^{\times}=MK_2^{\times}$. On the other hand, there exists a pair of knots $K_1$ and $K_2$ such that $MK_1=MK_2$ and $MK_1^{\times}{\neq}MK_2^{\times}$. In other words, the Gordian complex is not homogeneous with respect to Alexander invariants.

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THE DIMENSION OF THE CONVOLUTION OF BIPARTITE ORDERED SETS

  • Bae, Deok-Rak
    • 대한수학회지
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    • 제36권3호
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    • pp.633-648
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    • 1999
  • In this paper, for any two bipartite ordered sets P and Q, we define the convolution P * Q of P and Q. For dim(P)=s and dim(Q)=t, we prove that s+t-(U+V)-2 dim(P*Q) s+t-(U+V)+2, where U+V is the max-mn integer of the certain realizers. In particular, we also prove that dim(P)=n+k- {{{{ { n+k} over {3 } }}}} for 2 k n<2k and dim(Pn ,k)=n for n 2k, where Pn,k=Sn*Sk is the convolution of two standard ordered sets Sn and Sk.

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Nonstoichimetry (x) of Nuclear Materials UO2+x and $(Ce_yU_{1-y})O_{2+x}$ at High Temperatures as a Function of Oxygen Activity$(a_o_2)$

  • Kang, Sun-Ho;Yoo, Han-Ill;Kim, Han-Soo;Lee, Young-Woo
    • The Korean Journal of Ceramics
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    • 제4권2호
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    • pp.78-82
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    • 1998
  • The oxygen nonstoichiometry (x) of UO$_{2+x}$ and $(Ce_yU_{1-y})O_{2+x}$ (y=0.05, 0.25) has been measured as a function of oxygen activity (a02) at 100$0^{\circ}C$ by a solid state coulometri titration technique. The results for UO$_{2+x}$ are in a good agreement with literature data and the ao2-dependence of the nonstoichimetry has been well explained with (2:2:2) cluster model. The equilibrium oxygen activity of $(Ce_yU_{1-y})O_{2+x}$ increases with Ce-content (y) for given nonstoichiometry (x), which is ascribed to the fact that Ce is present as Ce$^{3+}\; and\; Ce^{4+}$, and, therefore, the addition of Ce reduces the oxidation capacity of UO$_{2+x}$. From the oxygen activity dependence of x in $(Ce_yU_{1-y})O_{2+x}$ the defect structure of $(Ce_yU_{1-y})O_{2+x}$ is discussed.

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