• 대한수학회논문집
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• 제9권2호
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• pp.419-421
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• 1994

Recently Hong and Oh [5] provided a fairly general weak law for arrays in the following form: Let {(X/sub ni/, l ≤ i ≤ k/sub n/), n ≥ l}, k/sub n/ → ∞ as n → ∞, be an array of random variables on (Ω, F, P) and set F/sub nj/ = σ{X/sub ni/, 1 ≤ i ≤ j}, 1 ≤ j ≤ k/sub n/, n ≥ 1, and F/sub n0/ = {ø, Ω}, n ≥ 1. Suppose that (equation omitted) aP { X/sub ni/ /sup p/ ＞ a} → 0 as a → ∞ uniformly in n for some 0 < p < 2. Then S/sub n//(equation omitted) → 0 in probability as n → ∞ where S/sub n/ = (equation omitted)(X/sub ni/ - E(X/sib ni/I( X/sub ni/ /sub p/ ≤ k/sub n/) F/sub n,i-l/)). In this note, we will prove the following result under the same domination condition of Hong and Oh [5].(omitted)

• 자연과학논문집
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• 제8권2호
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• pp.5-7
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• 1996

{X,$X_n$,n$\geq$1}은 독립이고 평균이 영으로 같은 확률분포를 갖는 확률변수 열이고, {$a_ni$, 1$\leq$i$\leq$n,n$\geq$1}은 수열일 때 가중합 $sum_{i=1}^n$$a_{ni}$$X_i$가 0에 확률 1로 수렴할 충분조건을 제시한다.

• Bulletin of the Korean Chemical Society
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• 제27권11호
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• pp.1747-1751
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• 2006

The dinuclear tetraazadiphenol macrocyclic nickel(II) complexes [$Ni_2$([20]-DCHDC)]$Cl_2$ (I), [$Ni_2$([20]-DCHDC)]$(ClO_4)_2{\cdot}2CH_3CN $ (II(b)) and [$Ni_2$([20]-DCHDC)$(NCS)_2$] (III) {$H_2$[20]-DCHDC = 14,29-dimethyl-3,10,18,25-tetraazapentacyclo-[25,3,1,$0^{4,9}$,$1^{12,16}$,$0^{19,24}$]ditriacontane-2,10,12,14,16(32),17,27(31), 28,30-decane-31,32-diol} have been synthesized by self-assembly and characterized by elemental analyses, conductances, FT-IR and FAB-MS spectra, and single crystal X-ray diffraction. The crystal structure of II(b) is determined. It crystallizes in the monoclinic space group P2(1)/c. The coordination geometries around Ni(II) ions in I and II(b) are identical and square planes. In complex III each Ni(II) ion is coordinated to $N_2O_2$ plane from the macrocycle and N atoms of NCS- ions occupying the axial positions, forming a square pyramidal geometry. The nonbonded Ni…Ni intermetallic separation in the complex II(b) is 2.8078(10) $\AA$. The FAB mass spectra of I, II and III display major fragments at m/z 635.1, 699.4 and 662.4 corresponding to [$Ni_2$([20]-DCHDC)(Cl + 2H)]$^+$, [$Ni_2$([20]-DCHDC)$(ClO_4\;+\;2H)]^+$ and [$Ni_2$([20]-DCHDC)(NCS) + 6H]$^+$, respectively.

• 대한수학회보
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• 제41권2호
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• pp.275-282
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• 2004

Let {$a_{ni},\;u_n\;{\leq}\;{\upsilon}_n,\;n\;{\geq}\;1$} be an arry of constants. Let {X_{ni},\;u_n\;{\leq}\;i\;{\leq}\;{\upsilon}_n,\;n\;{\geq}\;1$} be {$a_{ni}$}-uniformly integrable random variables. Weak laws for the weighted sums ${{\Sigma}_{i=u_n}}^{{\upsilon}_n}\;a_{ni}X_{ni}$ are obtained.

• 한국초전도ㆍ저온공학회논문지
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• 제19권2호
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• pp.48-52
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• 2017

Discrepancy between a power supply current and an actual "spiral" coil current makes the conventional 4-probe measurement of a critical current ($I_c$) of a no-insulation (NI) high temperature superconductor (HTS) coil inaccurate and time-consuming. This paper presents a fast and accurate approach for $I_c$ measurement of NI HTS coils. With an NI HTS coil energized at a constant ramping rate, a complete analytic expression for the spiral coil current was obtained from a first-order partial differential equation that derived from an equivalent circuit model of the NI coil. From the analytic solution, both spiral coil current and radial leak current can be obtained simultaneously, which enables fast and accurate measurement of the NI coil $I_c$. To verify the proposed approach, an NI double-pancake (DP) coil, wound with GdBCO tapes of $6mm{\times}0.1mm$, was constructed and its $I_c$ was repeatedly measured with various ramping rates in a bath of liquid nitrogen at 77 K. The measured results agreed well with the calculated ones, which validates the proposed approach to measure $I_c$ of an NI HTS coil.

• 한국재료학회지
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• 제21권2호
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• pp.78-82
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• 2011

Mono- and few-layer graphenes were grown on Ni thin films by rapid-thermal pulse chemical vapor deposition technique. In the growth steps, the exposure step for 60 s in $H_2$ (a flow rate of 10 sccm (standard cubic centimeters per minute)) atmosphere after graphene growth was specially established to improve the quality of the graphenes. The graphene films grown by exposure alone without $H_2$ showed an intensity ratio of $I_G/I_{2D}$ = 0.47, compared with a value of 0.38 in the films grown by exposure in H2 ambient. The quality of the graphenes can be improved by exposure for 60 s in $H_2$ ambient after the growth of the graphene films. The physical properties of the graphene films were investigated for the graphene films grown on various Ni film thicknesses and on 260-nm thick Ni films annealed at 500 and $700^{\circ}C$. The graphene films grown on 260-nm thick Ni films at $900^{\circ}C$ showed the lowest $I_G/I_{2D}$ ratio, resulting in the fewest layers. The graphene films grown on Ni films annealed at $700^{\circ}C$ for 2 h showed a decrease of the number of layers. The graphene films were dependent on the thickness and the grain size of the Ni films.

• 한국자기학회지
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• 제5권6호
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• pp.937-946
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• 1995

본 연구에서는 NiCuZn Ferrite 제조공정의 제어를 위하여 제조공정 변수에 따른 NiCuZn Ferrite의 물성 및 자기적특성의 변화를 검토하여, 겉보기밀도(bulk density)와 초기투자율의 관계를 명확하게 하는 것을 목적으로 하였다. $700^{\circ}C$에서 3시간 하소 한 NiCuZn Ferrite를 약 60시간 볼밀링하여 약 $0.5\mu\textrm{m}$ 입자크기로 분쇄한 후 분무 건조하여 과립화하였다. 본 연구에서는 (1)NiCuZn Ferrite 과립의 크기와 성형압력 변화와 (2)일정한 성형조건에서 소성온도의 변화에 따른 성형체 및 소성체의 물성측정, 그리고 자기적 특성을 검토하였다. NiCuZn Ferrite의 green density는 과립의 크기보다는 성형압력에 더 의존하였으며, 과립의 크기가 $150\mu\textrm{m}$ 이하 일 때 성형압력이 증가 함에 따라 green density는 $2.484\;g/cm^{3}$에서 $3.002\;g/cm^{3}$로 크게 증가하 였다. NiCuZn Ferrite의 bulk density는 소성온도에 의하여 거의 직선적으로 $3.470\;g/cm^{3}$에서 $4.754\;g/cm^{3}$로 증가하였다. 성형압력 변화 및 소성온도 변화에 따른 NiCuZn Ferrite 초기투자율과 겉보기밀도 관계를 비교 검토한 결과, NiCuZn Ferrite의 초기투자율($\mu_{i}$)과 겉보기밀도($\rho$)의 관계를 $\mu_{i}=a+b_{\rho}+c_{\rho}^2$와 같이 실험식으로 표현할 수 있었다.

• 한국자기학회지
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• 제9권2호
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• pp.98-103
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• 1999

DC, RF 스퍼터링 방법으로 제조한 glass/Ta/NiFeI/CoI(t)/Cu/CoII(3/4 t)/NiFeII/FeMn 스핀밸브구조에서 아르곤(Ar)가스압력과 코발트(Co)층의 두께에 변화를 주어 보자력(Hc)과 교환이방성자계(Hex) 그리고 자기저항변화율(MR)에 대해 연구하였다. 아르곤가스 압력에 대한 보자력은 4mTorr에서 2.8Oe로 가장 작았으며 교환이방성자계는 6mTorr에서 약 50.0Oe, 자기저항변화율은 10mTorr에서 5.3%를 얻을 수 있었다. 또한 코발트층의 두께변화에 대한 보자력은 코발트층(CoI)의 두께가 40$\AA$일 때 3.0Oe, 교환이방성자계는 13$\AA$두께에서 65.9Oe 그리고 자기저항변화율은 27$\AA$과 34$\AA$의 두께에서 4.7%를 얻을 수 있었다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1996년도 추계학술대회 논문집
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• pp.378-381
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• 1996

This study is to research Li$_{x}$Ni$_{2-x}$O$_2$ cathode for lithium chargeable battery. We investigated morphology and cell resistance, capacity and Ah efficiency of Li$_{x}$Ni$_{2-x}$O$_2$/Li cells using Li$_{x}$Ni$_{2-x}$O$_2$ prepared under air and $O_2$ flow. The (003)I/(104)I intensity ratio was 1.4. The cell resistance was increased with increasing Li in Li$_{x}$Ni$_{2-x}$O$_2$. The discharge capacity based on Li$_{x}$Ni$_{2-x}$O$_2$of 1st and 15th cycles was 135㎃h/g and 108㎃h/g, respectively. The Li$_{x}$Ni$_{2-x}$O$_2$ prepared with hexan under $O_2$ flow had a good properties. properties. properties.

• Bulletin of the Korean Chemical Society
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• 제28권7호
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• pp.1119-1126
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• 2007

Hydrogen gas and carbon nanotubes along with nanocarbon were produced from commercial natural gas using fixed bed catalyst reactor system. The maximum amount of carbon (491 g/g of catalyst) formation was achieved on 25% Ni, 3% Cu supported catalyst without formation of CO/CO2. Pure carbon nanotubes with length of 308 nm having balloon and horn type shapes were also formed at 673 K. Three sets of catalysts were prepared by varying the concentration of Ni in the first set, Cu concentration in the second set and doping with K in the third set to investigate the effect on stabilization of the catalyst and production of carbon nanotubes and hydrogen by copper and potassium doping. Particle size analysis revealed that most of the catalyst particles are in the range of 20-35 nm. All the catalysts were characterized using powder XRD, SEM/EDX, TPR, CHN, BET and CO-chemisorption. These studies indicate that surface geometry is modified electronically with the formation of different Ni, Cu and K phases, consequently, increasing the surface reactivity of the catalyst and in turn the Carbon nanotubes/H2 production. The addition of Cu and K enhances the catalyst dispersion with the increase in Ni loadings and maximum dispersion is achieved on 25% Ni: 3% Cu/Al catalyst. Clearly, the effect of particle size coupled with specific surface geometry on the production of hydrogen gas and carbon nanotubes prevails. Addition of K increases the catalyst stability with decrease in carbon formation, due to its interaction with Cu and Ni, masking Ni and Ni:Cu active sites.