• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 1997년도 추계학술대회 논문집
• /
• pp.68-72
• /
• 1997

In this paper, to obtain the YbB $a_2$C $u_3$ $O_{x}$ superconductor, the mixed Powders of Y $b_2$ $O_3$, BaC $O_3$, CuO and Y $b_2$BaCu $O_{5}$, BaCu $O_2$ were used and the various calcining conditions were applied for the 123 phase of YbB $a_2$C $u_3$ $O_{x}$. Samples were prepared by the mixed oxide method and calcined with various temperatures of 88$0^{\circ}C$ ~91$0^{\circ}C$ . It was observed that the distribution of YbB $a_2$C $u_3$ $O_{x}$ phase which was calcined at 90$0^{\circ}C$ for 12 hours and 99 hours. But the result of long time calcination(99 hrs), the 123 phase of YbB $a_2$C $u_3$ $O_{x}$ was existed between 89$0^{\circ}C$ and 91$0^{\circ}C$ . And the best case could be obtained at the calcination temp. of 90$0^{\circ}C$ from the mixed Powder of YbB $a_2$C $u_3$ $O_{5}$ and Bacu $O_2$ which were prepared individually.idually.

• 한국세라믹학회지
• /
• 제31권3호
• /
• pp.249-256
• /
• 1994

By surface structure and X-ray topographic observation, growth mechanism of NAB single crystal grown by TSSG technique using a BaB4O7 flux was studied. Surface structure of grown crystals were investigated by optical microscope. Growth history and crystal defects included within grown crystal were investigated using X-ray topography. The {001} faces were grown by 2-D nucleation growth. As decreasing cooling rate, growth mechanism of {111} and {11} was changed from 2-D nucleation growth to the growth by screw dislocation. Only surface striations developed parallel to a-axis were observed on {010} faces. Growth sector of NAB crystals were divided into {001}, {111}, {010}, {021}, {11}. The inclusion which was usually trapped between {001} faces was investigated.

• Kyungpook Mathematical Journal
• /
• 제56권2호
• /
• pp.507-516
• /
• 2016

In this paper, we introduce an explicit formula for the solutions and discuss the global behavior of solutions of the difference equation $$x_{n+1}={\frac{ax_{n-3}}{b-cx_{n-1}x_{n-3}}}$$, $n=0,1,{\ldots}$ where a, b, c are positive real numbers and the initial conditions $x_{-3}$, $x_{-2}$, $x_{-1}$, $x_0$ are real numbers.

• 한국자기학회지
• /
• 제6권4호
• /
• pp.218-224
• /
• 1996

새로운 고성능 자심용 연자성 합금을 개발하기 위해, 급냉응고 방식에 의해 제조된 $Fe_{83-x}Al_{x}Nb_{5}B_{12}(X=1~5at%)$ 합금의 결정화거동 및 자기적 특성을 조사하였다. 3at% Al의 $Fe_{80}Al_{3}Nb_{5}B_{12}$ 합금이 조사된 Fe-Al-Nb-B계 합금중에서 가장 우수한 연자기 특성을 가지며, 이때 미세한 $\alpha-Fe$상 결정립 조직을 가지는 것으로 판명되었다. 또, 이 조성의 합금에 1 at%의 Cu를 첨가하면, 약 6~7 nm정도의 크기를 가지는 극히 미세한 결정립의 $\alpha-Fe$ 상조직이 얻어졌으며 이에 따라 대단히 현저한 연자기 특성의 향상이 실현되었다. 이때 초미세 결정구조 $Fe_{79}Al_{3}Nb_{5}B_{12}Cu_{1}$ 합금의 자기적 특성은 다음과 같다 : ${\mu}_{eff}(1\;kHz)=26,000,\;B_{10}=1.45\;T,\;H_{c}=25\;mOe,\;P_{c}(100\;kHz,\;0.2\;T)=55\;W/kg$.

• Bulletin of the Korean Chemical Society
• /
• 제23권6호
• /
• pp.845-851
• /
• 2002

The synthesis of the intramolecular donor - stabilized silyl and germyl complexes of the type ($Cab^c.p) MMe_2X$ (2a:M=Si, X=Cl;2b;M= Ge, X=Cl;2e;M=Si,X=H) was achieved by the reaction of $LiCab^c,p$ (1) with $Me_2SiClX$ and $Me_2GeCl_2$ respectively. The intramolecular M←P interacion in 2a-2c is provided by $^1H$, $13^C.$, $31^P$ and $29^Si$ NMR spectroscopy. The salt elimination reactions of dichlorotetramethyldisilane and -digermane with 1 afforded the $bis(\sigma-carboranylphosphino)disilane$ and disgermane [$(Cab^C.P)MMe_2]_2(4a;M$ = Si;4b: M=Ge). The oxidative addition reaction of 4a-4b with $pd_2(dba)_3CHCl_3afforded$ the bis(silyl)-and bis(germyl)-palladium complexes. The chloro-bridged dipalladium complexes were obtained by the reaction of 2a-2b with $pd_2(dba)_3CHCl_3$ The crystal structures of 5a and 7b were determined by X-ray structural studies.

• 호남수학학술지
• /
• 제39권3호
• /
• pp.417-430
• /
• 2017

In this paper, we investigate the stability of a functional equation $$2f(ax+by)+abf(x-y)+abf(y-x)-{\frac{2af((a+b)x)}{a+b}}-{\frac{bf((a+b)y)}{a+b}}-{\frac{bf(-(a+b)y)}{a+b}}=o$$ by applying the direct method in the sense of Hyers and Ulam.

• Journal of applied mathematics & informatics
• /
• 제25권1_2호
• /
• pp.383-388
• /
• 2007

A (g, f)-factor F of a graph G is Called a Hamiltonian (g, f)-factor if F contains a Hamiltonian cycle. The binding number of G is defined by $bind(G)\;=\;{min}\;\{\;{\frac{{\mid}N_GX{\mid}}{{\mid}X{\mid}}}\;{\mid}\;{\emptyset}\;{\neq}\;X\;{\subset}\;V(G)},\;{N_G(X)\;{\neq}\;V(G)}\;\}$. Let G be a connected graph, and let a and b be integers such that $4\;{\leq}\;a\;<\;b$. Let g, f be positive integer-valued functions defined on V(G) such that $a\;{\leq}\;g(x)\;<\;f(x)\;{\leq}\;b$ for every $x\;{\in}\;V(G)$. In this paper, it is proved that if $bind(G)\;{\geq}\;{\frac{(a+b-5)(n-1)}{(a-2)n-3(a+b-5)},}\;{\nu}(G)\;{\geq}\;{\frac{(a+b-5)^2}{a-2}}$ and for any nonempty independent subset X of V(G), ${\mid}\;N_{G}(X)\;{\mid}\;{\geq}\;{\frac{(b-3)n+(2a+2b-9){\mid}X{\mid}}{a+b-5}}$, then G has a Hamiltonian (g, f)-factor.

• Journal of Magnetics
• /
• 제18권4호
• /
• pp.395-399
• /
• 2013

The metallic glass ribbons of $[(Fe_xCo_{1-x})_{0.75}B_{0.2}Si_{0.05}]_{96}Mo_4$ (x = 0, 0.3, 0.6, 0.9 at.%) and $[(Fe_xCo_{1-x})_{0.75}B_{0.2}Si_{0.05}]_{96}Nb_4$ (x = 0, 0.3, 0.6, 0.9 at.%) were obtained by melt spinning with 25-30 ${\mu}m$ thickness. The thermal stability, mechanical properties and magnetic properties of Fe-Co-B-Si based systems were investigated. The values of thermal stability were measured using differential scanning calorimetry (DSC), including glass transition temperature ($T_g$), crystallization temperature ($T_x$) and supercooled liquid region (${\Delta}T_x=T_x-T_g$). These amorphous ribbons were identified as fully amorphous, using X-ray diffraction (XRD). The mechanical properties of Febased samples were measured by nano-indentation. Magnetic properties of the amorphous ribbons were measured by a vibrating sample magnetometer (VSM). The amorphous ribbons of $[(Fe_xCo_{1-x})_{0.75}B_{0.2}Si_{0.05}]_{96}Mo_4$ (x = 0, 0.3, 0.6, 0.9 at.%) and $[(Fe_xCo_{1-x})_{0.75}B_{0.2}Si_{0.05}]_{96}Nb_4$ (x = 0, 0.3, 0.6, 0.9 at.%) exhibited soft magnetic properties with low coercive force ($H_c$) and high saturation magnetization (Ms).

• Journal of Magnetics
• /
• 제16권3호
• /
• pp.229-233
• /
• 2011

Phase evolution during the hydrogen-assisted disproportionation of $Nd_{12.5}Fe_{80.6}B_{6.4}Ga_{0.3}Nb_{0.2}$ alloy was investigated mainly by using a magnetic balance-type thermomagnetic analyser (TMA). In order to avoid any undesirable phase change in the course of heating for TMA, a swift TMA technique with very high heating rate (around 2 min to reach $800^{\circ}C$ from room temperature) was adopted. The hydrided $Nd_{12.5}Fe_{80.6}B_{6.4}Ga_{0.3}Nb_{0.2}$ alloy started to be disproportionated in hydrogen from around $600^{\circ}C$, and the alloy after the early disproportionation (from 600 to $660^{\circ}C$) has been partially disproportionated. The partially disproportionated alloy consisted of a mixture of $NdH_x$, $Fe_3B$, ${\alpha}$-Fe, and the remaining undisproportionated $Nd_2Fe_{14}BH_x$-phase. During the subsequent heating to $800^{\circ}C$ in hydrogen, two additional phases of $Fe_{23}B_6$ and $Fe_2B$ were formed, and the material consisted of a mixture of $NdH_x$, $Fe_{23}B_6$, $Fe_3B$, $Fe_2B$, and ${\alpha}$-Fe phases. During the subsequent isothermal holding at $800^{\circ}C$ for 1 hour, the phase constitution was further changed, and one additional unknown magnetic phase was formed. Eventually, the fully disproportionated $Nd_{12.5}Fe_{80.6}B_{6.4}Ga_{0.3}Nb_{0.2}$ alloy consisted of $NdH_x$, $Fe_{23}B_6$, $Fe_3B$, $Fe_2B$, ${\alpha}$-Fe, and one additional unknown magnetic phase.

• 한국재료학회지
• /
• 제5권7호
• /
• pp.880-887
• /
• 1995

융체방사법으로 제작한 YB $a_2$C $u_3$A $g_{15}$과 YbB $a_2$C $u_3$A $g_{x}$(x=5, 16 and 53) 예비 합금 리본(precursor alloy ribbon)을 263~322$^{\circ}C$에서 산화시키고, 산소 1기압 온도 872~89$0^{\circ}C$에서 열처리하였다. 또한 약 10개의 리본을 층으로 쌓아 프레스로 압축.접착시켜 다층 시편(multilayered specimen)을 제작하였다. 이 다충 시편도 위의 리본과 같은 조건에서 열처리하였다. YB $a_2$C $u_3$ $O_{7-{\delta}}$ 혹은 YbB $a_2$C $u_3$ $O_{7-{\delta}}$상이 모든 리본과 모든 다층 시편에서 형성되었다. 이 1-2-3상들은 모든 리본에서 집합조직(texture)을 나타내지 않았으나, 다층 시편들에서는 약간의 집합조직을 나타내었다. 모든 리본은 0 자장 77K에서 임계 전류 밀도 $J_{c}$가 0을 나타내었다. 다층 시편 중에서 YB $a_2$C $u_3$A $g_{15}$과 YbB $a_2$C $u_3$A $g_{16}$시편이 각각 260, 180A/$\textrm{cm}^2$의 임계 전류 밀도를 나타내었다. 여러 리본들 중에서 YB $a_2$C $u_3$A $g_{15}$ 과 YbB $a_2$C $u_3$A $g_{16}$ 리본이, 프레스 변형으로 집합조직을 가지게 함으로써 향상된 $J_{c}$를 가진 초전도 산화물을 만들 수 있는 적절한 조성을 가지고 있다. 다층 YB $a_2$C $u_3$A $g_{15}$ 시편의 개시 임계 온도 ( $T_{on}$ )는 92K 이었으며, 다층 YbB $a_2$C $u_3$A $g_{x}$(x=5, 16 and 53)의 $T_{on}$ 은 88~90K이었다.