• 제목/요약/키워드: F.V.M

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$Sm^2+$이온이 첨가된 $KMgF_3$ 결정의 성장 및 레이저 분광학 연구

  • 장만송;허성욱;장경혁;서효진;문병기;이성수;장기완
    • 한국광학회:학술대회논문집
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    • 한국광학회 2003년도 하계학술발표회
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    • pp.180-181
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    • 2003
  • Czochralski 방법으로 KMg $F_3$:S $m^{2+}$ 결정을 성장시키고 고 분해 레이저 분광법을 이용하여, 형광특성을 조사하였다. S $m^{2+}$ 이온이 KMg $F_3$ 결정에서 $C_{4v}$, $C_{2v}$, $C_{3v}$$O_{h}$ 형광 방출 사이트를 가진다는 것을 확인하였고, 아울러 각 사이트의 에너지 준위를 구하였다. 구하였다.

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EXISTENCE OF SOLUTIONS FOR FRACTIONAL p&q-KIRCHHOFF SYSTEM IN UNBOUNDED DOMAIN

  • Bao, Jinfeng;Chen, Caisheng
    • 대한수학회보
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    • 제55권5호
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    • pp.1441-1462
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    • 2018
  • In this paper, we investigate the fractional p&q-Kirchhoff type system $$\{M_1([u]^p_{s,p})(-{\Delta})^s_pu+V_1(x){\mid}u{\mid}^{p-2}u\\{\hfill{10}}={\ell}k^{-1}F_u(x,\;u,\;v)+{\lambda}{\alpha}(x){\mid}u{\mid}^{m-2}u,\;x{\in}{\Omega}\\M_2([u]^q_{s,q})(-{\Delta})^s_qv+V_2(x){\mid}v{\mid}^{q-2}v\\{\hfill{10}}={\ell}k^{-1}F_v(x,u,v)+{\mu}{\alpha}(x){\mid}v{\mid}^{m-2}v,\;x{\in}{\Omega},\\u=v=0,\;x{\in}{\partial}{\Omega},$$ where ${\Omega}{\subset}{\mathbb{R}}^N$ is an unbounded domain with smooth boundary ${\partial}{\Omega}$, and $0<s<1<p{\leq}q$ and sq < N, ${\lambda},{\mu}>0$, $1<m{\leq}k<p^*_s$, ${\ell}{\in}R$, while $[u]^t_{s,t}$ denotes the Gagliardo semi-norm given in (1.2) below. $V_1(x)$, $V_2(x)$, $a(x):{\mathbb{R}}^N{\rightarrow}(0,\;{\infty})$ are three positive weights, $M_1$, $M_2$ are continuous and positive functions in ${\mathbb{R}}^+$. Using variational methods, we prove existence of infinitely many high-energy solutions for the above system.

토끼 단일 심실근 세포에서 cyclic GMP의 $Ca^{2+}$ 전류 조절기전에 관한 연구 (Modulation of Calcium Current by Cyclic GMP in the Single Ventricular Myocytes of the Rabbit)

  • 안재호;서경필;엄융의
    • Journal of Chest Surgery
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    • 제25권4호
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    • pp.364-382
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    • 1992
  • In order to investigate the effect of intracellular cyclic GMP on the calcium channel, whole cell patch clamp technique with internal perfusion method was used in the single ventricular myocytes of the rabbit. Cyclic GMP, cGMP analogues, cAMP, isopernaline and forskolin were perfused into cells and their effects on the calcium current were analysed by applying depolarizing step pulse of 10 mV in amplitude for 200 msec from holding potential of -40 mV. Calcium currents usually activated from -30 mV and then reached a peak at +10 mV. Amplitude of the calcium current was standardized with membrane capacitance, 50 pF. Peak amplitude at +10 mV in control was -0.15 nA/50pF. When 100 mM cAMP was applied from the pipette, peak amplitude of calcium current increased to -0.32 nA and addition of 1 mM isoprenaline further increased its amplitude. In the presence of cGMP it alone also produced an increase of the calcium current to -0.52 nA/50pF and addition of isoprenaline or forskolin increased its magnitude to -[0.55~0.95] nA/50pF. Simultaneous application of cGMP and cAMP increased the calcium current to -0.67 nA/50pF. Among the cGMP analogues, 8-Br-cGMP was the most potent stimulant for the calcium current activation. From the above results it could be concluded tlat cGMP increases the calcium current not through cAMP dependent protein kinase nor cAMP dependent phosphodiesterase pathway, but through independent phosphorylation pathway, possibly cGMP dependent protein kinase pathway.

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쌍끌이 중층트롤어법의 연구 ( 1 ) - 모형어구의 망구형상에 관하여 - ( A Study on the Pair Midwater Trawling ( 1 ) - Mouth Performance of the Model Net - )

  • 이병기
    • 수산해양기술연구
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    • 제31권1호
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    • pp.29-44
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    • 1995
  • A model experiment on the pair midwater trawl net applicable to 800 PS class Korean pair bottom trawlers was carried out in the special-prepared experimental thank. the tank was prepared as a reverse trapezoid shape in its vertical section by digging out flat soil. The dimension of the tank showed the 9.6 W$\times$43.0 L(m) of the upper fringe and the 4.8 W$\times$38.0 L(m) of the bottom with 3.0m in depth. The depth of water was maintained 2.7m during experiment. The model net was prepared based on the Tauti's similarity law of fishing gear in 1/30 scale considering the dimension of the experimental tank. Mouth performance of the model net during towing were determined by the photographs taken in front of the net mouth with the combinations of towing velocity, warp length and distance between paired boats. The results obtained can be summarized as follows: 1. Vertical opening of the model nets A and B was varied in the range of 0.18~0.88 m and 0.21~0.78 m (which can be converted into 5.4~26.4m and 6.3~23.4 m in the full-scale net) respectively, and was varied predominantly by towing speed. Vertical opening (H which is appendixed m for the model net. f for the full-scale net. A and B for the types of the model net) can be expressed as the function of towing velocity$V_t$as in the model net $V_t$ : m/ sec)$H_{mA}$=1.67$e^{-1.65V_t}$ $H_{mB}$=1.15$e^{-1.13V_t}$, in the full-scale net ($V_t$ : k't) $H_{fA}$=50.27$e^-0.37V_t$ $H_{fB}$=34.46$e^{-0.26Vt}$. 2. Horizontal opening of the model nets An and b was varied in the range of 1.03~1.54m and 1.04~1.55 m (which can be converted into 30.9~46.2 m and 31.2~46.5m in the full-scale net) respectively, and was varied predominantly by distance between paired boats. Horizontal opening (W, appendixes are as same as the former) an be expressed as the function of distance between paired boats $D_b$as in the model net $W_{mA}$=0.69+0.09$D_b$ $W{mB}$=0.73+0.09$D_b$, in the full-scale net $W_{fA}$=20.81+0.09$D_b$ $W_{fB}$=22.11+0.09$D_b$ 3. Net opening area of the model net A and B was varied in the range of 0.28~1.04 $m^2$ and 0.33~0.94$m^2$(which can be converted into 252~936$m^2$ and 297~846$m^2$ in the full-scale net) respectively, and was varied predominantly by towing velocity. Net opening area ($S$, appendixes are as same as the former) van be expressed as the function of towing velocity$V_t$ as in the model net $v_t$ : m/sec) $S_{Ma}$=2.01$e^{-1.54V_T}$ $S_{mA}$=1.40$e^{-1.65V_t}$, in the full-scale net ($V_t$ : k't) $S_{fA}$=1.807$e^-0.35V_t$ $S_{fA}$=1.265$e^{-0.24V_t}$. 4. Filtering volume of the model nets A and B was varied in the range of 0.32~0.55 $m^3$ and 0.37~0.55$m^3$(which can be converted into 8.640~14.850 $m^3$ and 9.990~14.850$m3$in the full~scale net) respectively, and was predominantly varied by towing speed. filtering volume of the model net-A showed the maximum at the towing speed 0.69 m/sec(3 k't in the full-scale net), compared with that of the model net B showed at 0.92 m/sec(4 k't in the full-scale net).

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솔-젤법으로 제조한 PZT박막의 유전 및 전기적 특성 (Dielectric and electric properties of sol-gel derived PZT thin Films)

  • 홍권;김병호
    • E2M - 전기 전자와 첨단 소재
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    • 제9권3호
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    • pp.251-258
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    • 1996
  • Sol-Gel derived ferroelectric Pb(Z $r_{0.52}$ $Ti_{0.48}$) $O_{3}$ thin films have been fabricated on Pt/Ti/ $SiO_{2}$/Si substrate. Two kinds of fast annealing methods, F-I (six times of intermediate and final annealing) and F-II(one final annealing after six times of intermediate annealing) were used for preparation of multi-coated PZT thin films. As the annealing temperature was increased, high capacitance could be obtained, for instance, 2700.angs.-thick PZT thin film annealed at 680.deg. C had a capacitance value of approximately 20nF at 1kHz. In addition, it is found that the dielectric constant is a function of the perovskite phase fraction. In case of F-I method, PZT thin film had a remanent polarization(Pr) of 8-15.mu.C/c $m^{2}$ and a coercive field( $E_{c}$) of 35-44kV/cm according to annealing temperature, whereas PZT film fabricated by F-II method had as high as 24-25.mu.C/c $m^{2}$ and 48-59kV/cm, respectively. As a result of measuring Curie temperature, PZT thin film had a range of 460-480.deg. C by F-I method and more or less higher range of 525-530.deg. C by F-II method, which implied that different microstructures could cause the different Curie temperature. Through I-V measurement, leakage current of PZT thin film fabricated by F-I and F-II methods was 64nA/c $m^{2}$ and 2.2.mu.A/c $m^{2}$ in the electric field of 100kV/cm, respectively.y.y.y.

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System-On-Glass를 위한 Poly-Si TFT 소 면적 DC-DC 변환회로 (An Area-Efficient DC-DC Converter with Poly-Si TFT for System-On-Glass)

  • 이균렬;김대준;유창식
    • 대한전자공학회논문지SD
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    • 제42권2호
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    • pp.1-8
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    • 2005
  • System-on-glass를 위해 poly-Si TFT로 면적이 작으면서도 리플전압을 최소화한 DC-DC 전압 변환회로를 개발하였다. 전압 변환회로는 전하 펌핑 회로, 문턱전압 변화를 보상한 비교기, 오실레이터, 버퍼, 다중 위상 클럭을 만들기 위한 지연 회로로 구성된다. 제안한 다중 위상 클럭킹을 적용함으로써 클럭 주파수 또는 필터링 캐패시터의 증가 없이도 낮은 출력 리플전압을 얻음으로써 DC-DC 변환기의 면적을 최소화 하였다. 제안한 DC-DC 변환회로를 제작하여 측정한 결과 $R_{out}=100k\Omega,\;C_{out}=100pF$, 그리고 $f_{clk}=1MHz$에서 Dickson 구조와 기존의 cross-coupled 구조에서의 리플전압은 각각 590mv와 215mv인 반면 4-위상 클럭킹을 적용한 구조에서는 123mV이다. 그리고 50mV의 리플전압을 가지기 위해 필요한 필터링 캐패시터의 크기는 $I_{out}=100uA$$f_{clk}=1MHz$에서 Dickson 구조와 기존의 cross-coupled 구조에서는 각각 1029pF와 575pF인 반면 4-위상과 6-위상 클럭킹을 적용한 구조에서는 단지 290pF와 157pF만이 각각 요구된다. 구조별 효율로는 Dickson 구조의 전하 펌프에서는 $59\%$, 기존의 cross-coupled 구조와 본 논문에서 제안한 4-위상을 적용한 cross-coupled 구조의 전하 펌프에서는 $65.7\%$$65.3\%$의 효율을 각각 가진다.

EXISTENCE AND NON-EXISTENCE FOR SCHRÖDINGER EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENTS

  • Zou, Henghui
    • 대한수학회지
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    • 제47권3호
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    • pp.547-572
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    • 2010
  • We study existence of positive solutions of the classical nonlinear Schr$\ddot{o}$dinger equation $-{\Delta}u\;+\;V(x)u\;-\;f(x,\;u)\;-\;H(x)u^{2*-1}\;=\;0$, u > 0 in $\mathbb{R}^n$ $u\;{\rightarrow}\;0\;as\;|x|\;{\rightarrow}\;{\infty}$. In fact, we consider the following more general quasi-linear Schr$\ddot{o}$odinger equation $-div(|{\nabla}u|^{m-2}{\nabla}u)\;+\;V(x)u^{m-1}$ $-f(x,\;u)\;-\;H(x)u^{m^*-1}\;=\;0$, u > 0 in $\mathbb{R}^n$ $u\;{\rightarrow}\;0\;as\;|x|\;{\rightarrow}\;{\infty}$, where m $\in$ (1, n) is a positive number and $m^*\;:=\;\frac{mn}{n-m}\;>\;0$, is the corresponding critical Sobolev embedding number in $\mathbb{R}^n$. Under appropriate conditions on the functions V(x), f(x, u) and H(x), existence and non-existence results of positive solutions have been established.

ODD-EVEN GRACEFUL GRAPHS

  • Sridevi, R.;Navaneethakrishnan, S.;Nagarajan, A.;Nagarajan, K.
    • Journal of applied mathematics & informatics
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    • 제30권5_6호
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    • pp.913-923
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    • 2012
  • The Odd-Even graceful labeling of a graph G with $q$ edges means that there is an injection $f:V (G)$ to $\{1,3,5,{\cdots},2q+1\}$ such that, when each edge $uv$ is assigned the label ${\mid}f(u)-f(v){\mid}$, the resulting edge labels are $\{2,4,6,{\cdots},2q\}$. A graph which admits an odd-even graceful labeling is called an odd-even graceful graph. In this paper, we prove that some well known graphs namely $P_n$, $P_n^+$, $K_{1,n}$, $K_{1,2,n}$, $K_{m,n}$, $B_{m,n}$ are Odd-Even graceful.

Acclimation of maximum quantum yield of PSII and photosynthetic pigments of Panax quinquefolius L. to understory light

  • Fournier, Anick R.;T.A., John;Khanizadeh, Shahrokh;Gosselin, Andre;Dorais, Martine
    • Journal of Ginseng Research
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    • 제32권4호
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    • pp.347-356
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    • 2008
  • Forest-grown American ginseng (Panax quinquefolius L.) is exposed to daily and seasonal light variations. Our goal was to determine the effect of understory light changes on the maximum quantum yield of photosystem II, expressed as $F_v/F_m$, and photosynthetic pigment composition of two-year-old plants. Understory light photon flux density and sunfleck durations were characterized using hemispherical canopy photography. Our results showed that understory light significantly affected the $F_v/F_m$ of American ginseng, especially during the initial development of the plants when light levels were the highest, averaging 28 mol $m^{-2}d^{-1}$. Associated with low $F_v/F_m$ during its initial development, American ginseng had the lowest levels of epoxidation state of the xanthophyll cycle of the season, suggesting an active dissipation of excess light energy absorbed by the chlorophyll pigments. As photon flux density decreased after the deployment of the forest canopy to less than 10 mol $m^{-2}d^{-1}$, chlorophyll a/b decreased suggesting a greater investment in light harvesting pigments to reaction centers in order to absorb the fleeting light energy.

한국산 나비나물속(콩과)의 세포분류학적 연구 (A cytotaxonomic study of Vicia L. (Fabaceae) in Korea)

  • 남보미;박명순;오병운;정규영
    • 식물분류학회지
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    • 제42권4호
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    • pp.307-315
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    • 2012
  • 한국산 나비나물속(Vicia)에 속하는 10분류군의 체세포 염색체수와 그 중 6분류군에 대한 핵형분석을 실시하였다. 본 연구에서 밝혀진 나비나물속의 체세포 염색체수는 2n = 12, 14 또는 24로서, 기본 염색체수 x = 6 또는 7의 이배체와 사배체로 밝혀졌다. 한국특산식물인 나래완두(V. hirticalycina, 2n = 2x = 12)의 염색체수는 본 연구에서 처음으로 밝혀졌다. 가는살갈퀴(V. angustifolia, 2n = 2x = 12), 등갈퀴나물(V. cracca, 2n = 4x = 24), 새완두(V. hirsuta, 2n = 2x = 14), 얼치기완두(V. tetrasperma, 2n = 2x = 14 + 2B), 벌완두(V. amurensis, 2n = 2x = 12), 노랑갈퀴(V. chosenensis, 2n = 2x = 12, 12 + 2B), 나비나물(V. unijuga, 2n = 4x = 24), 애기나비나물(V. unijuga f. minor, 2n = 4x = 24), 광릉갈퀴(V. venosa var. cuspidata, 2n = 4x = 24)의 체세포 염색체수는 기존의 보고들과 일치하였다. 핵형분석 결과, 등갈퀴나물은 2 m + 8 sm+ 2 st, 벌완두는 2 m + 2 sm + 2st, 나래완두는 3 m + 1 sm+ 2 st, 나비나물과 애기나비나물은 4 m + 6 sm + 2 st, 광릉갈퀴는 4 m + 8 sm로 각각 조사되었다.