• 분석과학
• /
• 제6권5호
• /
• pp.515-520
• /
• 1993

Rene 80 주조블레이드가 고온에서 사용중인 사용 온도에 의해 ${\gamma}^{\prime}$이라는 석출물이 기지(${\gamma}^{\prime}$) 내에서 생성되기 때문에 고온강도는 그 석출물에 좌우된다. 즉, 석출물의 격자상수는 기지의 격자상수보다 크기 때문에 석출물이 생성되거나 성장할 때에 ${\gamma}-{\gamma}^{\prime}$ 격자어긋남(lattice misfit)에 의해 전위가 발생한다고 일반적으로 알려져 있다. 이러한 격자어긋남은 석출물(${\gamma}^{\prime}$)의 크기가 클수록 원형${\rightarrow}$사각형${\rightarrow}$판상형으로 바뀌어 가면서 증가한다. 따라서 본 연구에서는 이러한 격자어긋남의 양을 주사투과전자현미경에서 수렴성 빔전자 회절(CBED)을 사용하여 측정하여, 석출물과 인접한 기지의 전위밀도의 증가가 기지 내에서 석출물이 생성하고 성장함에 따른 격자어긋남이 원인인가를 관찰하였다.

• 대한수학회지
• /
• 제54권1호
• /
• pp.69-86
• /
• 2017

The point $P{\in}{\mathbb{P}}^2$ is referred to as a Galois point for a nonsingular plane algebraic curve C if the projection ${\pi}_P:C{\rightarrow}{\mathbb{P}}^1$ from P is a Galois covering. In contrast, the point $P^{\prime}{\in}C^{\prime}$ is referred to as a weak Galois Weierstrass point of a nonsingular algebraic curve C' if P' is a Weierstrass point of C' and a total ramification point of some Galois covering $f:C^{\prime}{\rightarrow}{\mathbb{P}}^1$. In this paper, we discuss the following phenomena. For a nonsingular plane curve C with a Galois point P and a double covering ${\varphi}:C{\rightarrow}C^{\prime}$, if there exists a common ramification point of ${\pi}_P$ and ${\varphi}$, then there exists a weak Galois Weierstrass point $P^{\prime}{\in}C^{\prime}$ with its Weierstrass semigroup such that H(P') = or , which is a semigroup generated by two positive integers r and 2r + 1 or 2r - 1, such that P' is a branch point of ${\varphi}$. Conversely, for a weak Galois Weierstrass point $P^{\prime}{\in}C^{\prime}$ with H(P') = or , there exists a nonsingular plane curve C with a Galois point P and a double covering ${\varphi}:C{\rightarrow}C^{\prime}$ such that P' is a branch point of ${\varphi}$.

• Korean Journal of Mathematics
• /
• 제24권3호
• /
• pp.409-445
• /
• 2016

The class $\mathcal{W}^{\delta}_{\beta}({\alpha},{\gamma})$ defined in the domain ${\mid}z{\mid}$ < 1 satisfying $Re\;e^{i{\phi}}\((1-{\alpha}+2{\gamma})(f/z)^{\delta}+\({\alpha}-3{\gamma}+{\gamma}\[1-1/{\delta})(zf^{\prime}/f)+1/{\delta}\(1+zf^{\prime\prime}/f^{\prime}\)\]\)(f/z)^{\delta}(zf^{\prime}/f)-{\beta}\)$ > 0, with the conditions ${\alpha}{\geq}0$, ${\beta}$ < 1, ${\gamma}{\geq}0$, ${\delta}$ > 0 and ${\phi}{\in}{\mathbb{R}}$ generalizes a particular case of the largest subclass of univalent functions, namely the class of $Bazilevi{\check{c}}$ functions. Moreover, for 0 < ${\delta}{\leq}{\frac{1}{(1-{\zeta})}}$, $0{\leq}{\zeta}$ < 1, the class $C_{\delta}({\zeta})$ be the subclass of normalized analytic functions such that $Re(1/{\delta}(1+zf^{\prime\prime}/f^{\prime})+1-1/{\delta})(zf^{\prime}/f))$ > ${\zeta}$, ${\mid}z{\mid}$<1. In the present work, the sucient conditions on ${\lambda}(t)$ are investigated, so that the non-linear integral transform $V^{\delta}_{\lambda}(f)(z)=\({\large{\int}_{0}^{1}}{\lambda}(t)(f(tz)/t)^{\delta}dt\)^{1/{\delta}}$, ${\mid}z{\mid}$ < 1, carries the fuctions from $\mathcal{W}^{\delta}_{\beta}({\alpha},{\gamma})$ into $C_{\delta}({\zeta})$. Several interesting applications are provided for special choices of ${\lambda}(t)$. These results are useful in the attempt to generalize the two most important extremal problems in this direction using duality techniques and provide scope for further research.

• 정보보호학회논문지
• /
• 제30권6호
• /
• pp.1255-1261
• /
• 2020

캐시 부채널 공격은 CPU의 공유 캐시 자원을 이용하여 시스템에서 민감한 정보를 획득해내는 공격 유형이다. 최근 모바일 시스템에서 클라우드까지 다양한 환경에 공격이 가해짐에 따라 많은 탐지 전략이 제안되었다. 기존의 캐시 부채널 공격들은 많은 수의 캐시 이벤트를 발생시키는 특징을 가지고 있었기 때문에 기존의 탐지 기법은 대부분 캐시 이벤트를 주의 깊게 모니터링하는 것에 기반하여 설계되었다. 그러나 최근에 제안된 공격은 공격 중에 캐시 이벤트를 적게 유발하는 경향이 있다. 예를 들어 PRIME+ABORT 공격은 캐시에 접근하여 액세스 시간을 측정하는 대신 Intel TSX를 활용한다. 이러한 특징으로 인해 캐시 이벤트 기반 탐지 기법은 해당 공격을 탐지하기 어렵다. 본 논문에서는 PRIME+ABORT 공격에 대한 심층 분석을 수행하여 캐시 이벤트 이외에 공격 탐지에 활용 가능한 유용한 하드웨어 이벤트를 밝힌다. 이를 기반으로, PRIME+ABORT 공격 탐지 기법인 PRIME+ABORT Detector를 제시하고, 실험을 통해 제안한 탐지 기법이 0.3%의 성능 오버헤드로 99.5%의 탐지 성공률을 달성할 수 있음을 보인다.

• 한국재료학회지
• /
• 제32권9호
• /
• pp.396-402
• /
• 2022

In this study, surface roughness and interfacial defect characteristics were analyzed after forming a high-k oxide film on the surface of a prime wafer and a test wafer, to study the possibility of improving the quality of the test wafer. As a result of checking the roughness, the deviation in the test after raising the oxide film was 0.1 nm, which was twice as large as that of the Prime. As a result of current-voltage analysis, Prime after PMA was 1.07 × 10 A/cm² and Test was 5.61 × 10 A/cm², which was about 5 times lower than Prime. As a result of analyzing the defects inside the oxide film using the capacitance-voltage characteristic, before PMA Prime showed a higher electrical defect of 0.85 × 10¹² cm^-2 in slow state density and 0.41 × 10¹³ cm^-2 in fixed oxide charge. However, after PMA, it was confirmed that Prime had a lower defect of 4.79 × 10¹¹ cm^-2 in slow state density and 1.33 × 10¹² cm^-2 in fixed oxide charge. The above results confirm the difference in surface roughness and defects between the Test and Prime wafer.

• 대한수학회보
• /
• 제42권3호
• /
• pp.477-484
• /
• 2005

Let R be a ring with an automorphism 17. An ideal [ of R is ($\sigma$-ideal of R if $\sigma$(I).= I. A proper ideal P of R is ($\sigma$-prime ideal of R if P is a $\sigma$-ideal of R and for $\sigma$-ideals I and J of R, IJ $\subseteq$ P implies that I $\subseteq$ P or J $\subseteq$ P. A proper ideal Q of R is $\sigma$-semiprime ideal of Q if Q is a $\sigma$-ideal and for a $\sigma$-ideal I of R, I$^{2}$ $\subseteq$ Q implies that I $\subseteq$ Q. The $\sigma$-prime radical is defined by the intersection of all $\sigma$-prime ideals of R and is denoted by P$_{(R). In this paper, the following results are obtained: (1) For a principal ideal domain R, P$_{(R) is the smallest $\sigma$-semiprime ideal of R; (2) For any ring R with an automorphism $\sigma$ and for a skew Laurent polynomial ring R[x, x$^{-1}$; $\sigma$], the prime radical of R[x, x$^{-1}$; $\sigma$] is equal to P$_{(R)[x, x$^{-1}$; $\sigma$ ].

• 대한수학회논문집
• /
• 제32권3호
• /
• pp.543-552
• /
• 2017

Let R be a commutative ring with identity, and ${\phi}:{\mathfrak{I}}(R){\rightarrow}{\mathfrak{I}}(R){\cup}\{{\varnothing}\}$ be a function where ${\mathfrak{I}}(R)$ is the set of all ideals of R. Following [2], a proper ideal P of R is called a ${\phi}$-prime ideal if $x,y{\in}R$ with $xy{\in}P-{\phi}(P)$ implies $x{\in}P$ or $y{\in}P$. For an ideal I of R, we define the ${\phi}$-radical ${\sqrt[{\phi}]{I}}$ to be the intersection of all ${\phi}$-prime ideals of R containing I, and show that this notion inherits most of the essential properties of the usual notion of radical of an ideal. We also investigate when the set of all ${\phi}$-prime ideals of R, denoted $Spec_{\phi}(R)$, has a Zariski topology analogous to that of the prime spectrum Spec(R), and show that this topological space is Noetherian if and only if ${\phi}$-radical ideals of R satisfy the ascending chain condition.

• 열처리공학회지
• /
• 제5권2호
• /
• pp.85-94
• /
• 1992

Microstructural evolution of wrought Inconel 718 superalloy with different heat treatment conditions was studied. Heat treatment was performed via conventional(CHT), modified(MHT), Merrick(MeHT) and modified Merrick (MMeHT) methods. The size of ${\gamma}^{\prime}$ and ${\gamma}^{\prime\prime}$ precipitates which are principal strengthening phases in Inconel 718 superalloy increase in order of CHT, MHT, MeHT. For the case of MMeHT, a coexistence of fine ${\gamma}^{\prime\prime}$ precipitate and very coarse particles due to exess growth of ${\gamma}^{\prime\prime}$, which is called bimodal distribution, was observed. CHT gave the finest grain size. (Ti, Nb)C carbide and needle-like ${\delta}$ phase were formed together at grain boundaries for CHT, and were formed both inside and at boundaries of grains for MHT, MeHT and MMeHT. Morphology of partially serrated grain boundaries was developed in all heat treatment conditions except CHT.

• 한국대기환경학회지
• /
• 제29권2호
• /
• pp.171-185
• /
• 2013

Wetland has been known as a major biogenic source of $CH_4$ in globe. In a global scale, the amounts of 55~150 Tg $CH_4$ are released into the atmosphere annually from wetlands; and it accounts for about 21% of total $CH_4$ annual global emission. From August 2010 to August 2011, measurements of major greenhouse gas ($CO_2$, $CH_4$, $N_2O$) emissions were conducted from a freshwater wetland at Kunsan ($35^{\circ}56^{\prime}38.94^{\prime\prime}N$, $126^{\circ}43^{\prime}16.62^{\prime\prime}E$), Korea by using floating closed static chamber method. Flux measurements for these gases from western coastal tidal flat at Seocheon ($36^{\circ}07^{\prime}13.85^{\prime\prime}N$, $126^{\circ}35^{\prime}43.18^{\prime\prime}E$), Korea were managed from July 2011 to February 2012 by using closed static chamber method. The average gas fluxes and ranges from freshwater wetland experiment were $0.155{\pm}0.29\;mg\;m^{-2}\;hr^{-1}$ (-0.054~0.942 $mg\;m^{-2}\;hr^{-1}$) for $CH_4$, $17.30{\pm}73.27\;mg\;m^{-2}\;hr^{-1}$ (-52.44~261.66 $mg\;m^{-2}\;hr^{-1}$) for $CO_2$, and $0.004{\pm}0.01\;mg\;m^{-2}\;hr^{-1}$ (-0.02~0.07 $mg\;m^{-2}\;hr^{-1}$) for $N_2O$, respectively. Monthly base flux measurement results revealed that $CH_4$ fluxes during summer months in high water temperature were significantly high, and at least order of one higher than those during other months. The average fluxes and ranges of these greenhouse gases from tidal flat during the experimental period were $0.002{\pm}0.08\;mg\;m^{-2}\;hr^{-1}$ (-0.16~0.22 $mg\;m^{-2}\;hr^{-1}$) for $CH_4$, $-31.18{\pm}75.33\;mg\;m^{-2}\;hr^{-1}$ (-298.87~101.93 $mg\;m^{-2}\;hr^{-1}$) for $CO_2$, and $0.001{\pm}0.01\;mg\;m^{-2}\;hr^{-1}$ (-0.017~0.03 $mg\;m^{-2}\;hr^{-1}$) for $N_2O$, respectively. Comparing the results of gas emissions from tidal flat to those from freshwater wetland, we found significantly lower emissions from tidal flat based on the experiment. Physicochemical parameters of water and soil at these experimental plots were also sampled and analyzed for understanding their correlation with these gas emissions.

• 한국자기학회지
• /
• 제26권4호
• /
• pp.115-118
• /
• 2016

본 연구에서는 순수한 ${\alpha}^{{\prime}{\prime}}-Fe_{16}N_2$의 띠구조와 자기결정이방성에 대한 총 퍼텐셜 선형보강 평면파(Full-potential Linearized Augmented Plane Wave; FLAPW) 방법을 이용하여 연구하였다. 혼성화된 질소원자로 인해 Fe(4e), Fe(8h) 영역의 자기모멘트가 감소되었지만 z-축 방향의 격자 확장으로 인해 Fe(4d) 영역의 자기모멘트가 매우 커짐을 확인할 수 있었다. 각각의 Fe 영역들(4d, 4e, 8h) 스핀 자기모멘트들은 이전에 알려진 값들과 잘 일치함을 알 수 있다. 정방정계 왜곡으로 인해 $0.58 MJ/m^3$의 매우 큰 일축이방성상수를 구할 수 있었다. 게다가 1.76 MA/m의 매우 큰 자화량 또한 얻을 수 있었다. 또한 순수한 ${\alpha}^{{\prime}{\prime}}-Fe_{16}N_2$의 6.51 kOe의 예측 보자력과 71.7 MGOe의 최대에너지적을 얻을 수 있었다. 이러한 결과는 ${\alpha}^{{\prime}{\prime}}-Fe_{16}N_2$ 구조가 희토류 대체 영구자석으로 이용될 가능성이 있다는 것을 의미한다.